TABLE OF NUCLEAR MOMENTS

E. F. Kyul'ts, V. V. Kunts, V. G. Hartman

Submitted 1955 | SovietRxiv: ru-195501.92771 | Translated from Russian

Abstract

In compiling the table, use was made chiefly of works published and abstracted in Physics Abstracts up to September 1954. The table contains nuclear moments, with an indication of the method and accuracy of their measurements. For each moment, the numerical value reported in the literature as the most accurate is given.

Full Text

TABLE OF NUCLEAR MOMENTS

E. F. Kholtz, V. V. Kunts, V. G. Khartman

In compiling the table, use was made mainly of works published and abstracted in Physics Abstracts up to September 1954. The table contains nuclear moments with an indication of the method and accuracy of their measurements. For each moment the numerical value given is that which is reported in the literature as the most accurate. In addition, all works on the determination of a given moment that were published after the appearance of the review by I. E. Mack (50MA) are indicated, except in those cases where the moments were determined by means of nuclear reactions. In such cases only one or several new works containing references to the older works are indicated.

Other tables, namely:

H. L. Poss, Brookhaven Report, BNL—26 (T—10);

G. J. Béné, P. M. Denis, R. C. Extermann, J. phys. et rad. 11, 41D (1950);

K. Way, L. Fano, M. R. Scott, K. Thew, Nuclear Data NBS Circular 499 (1950); Suppl. I (1950); Suppl. II (1950); Suppl. III (1951);

W. F. Meggers, Journ. Opt. Soc. Amer. 41, 143 (1951);

P. F. A. Klinkenberg, Rev. mod. Phys. 24, 63 (1952),

were used only in those cases where their data were not published in the original papers.

Works in which moments are predicted are included in the list only when there are no experimental data (or when only inaccurate experimental data are available). Some older experimental data that were not included in Mack’s table (50MA) are nevertheless given if, by the time the compilation of the table was completed, no newer results were available.

In general, only the moments of the ground states of nuclei are indicated. Exceptions are isotopes for which the ground states—

measurements are still imprecisely determined, and measurements whose moments are determined not by means of nuclear reactions. The numerical values are given in the table as they are reported by the authors of the papers, i.e., the magnetic moments have not been recalculated to one and the same magnetic moment of the proton. If an author gave his result with an expression of doubt, such results are enclosed in parentheses.

In the bibliography the first letter denotes the method of measurement. The designations essentially correspond to those already used by Mack (50MA):

A — magnetic resonance on molecular or atomic beams,
B — band spectra,
D — double resonance,
E — electric resonance on molecular beams,
N — kinetics of nuclear reactions,
Q — nuclear quadrupole resonance,
R — nuclear paramagnetic resonance absorption and nuclear induction,
S — hyperfine structure of line spectra,
T — predictions, corrections, and treatments,
W — microwave absorption,
X — hyperfine structure of electron paramagnetic resonance,
Z — “zero moments” on atomic beams.

There is no first letter if the reference pertains to some table or if it was impossible to establish exactly by which method the cited value was obtained.

The number after the first letter denotes the year of publication of the given work. The following letters, of which the first usually corresponds to the initial letter in the surname of one of the authors, serve only to place the references in the bibliographic list. A reference in parentheses indicates that the given work contains corrections to, or processing of, the data of the work indicated in the preceding reference.

If, when there are several references for one moment, one reference is given in boldface, then the value of the moment or its sign given in the table is taken precisely from this work.

The following is placed in the individual columns:

Column 1 — serial number and designation of the atom.
Column 2 — mass number. “†” denotes a radioactive isotope.
Column 3 — abundance in %, and for radioactive isotopes—the half-life (yr—years, d—days, h—hours, m—minutes, s—seconds, ms—milliseconds, μs—microseconds).

TABLE OF NUCLEAR MOMENTS

Column 4 — nuclear spin in units of $\hbar$. When there are several values, the less probable ones are given in parentheses, and the more probable ones are set in bold type.

Column 5 — literature references to works on the determination of the spin.

Column 6 — magnetic dipole moment $\mu$, in nuclear magnetons; “cor” after a value measured by methods of nuclear paramagnetic absorption or nuclear induction indicates that, for the given value of the moment, the author applied a diamagnetic correction. If the magnetic moment is calculated by the Goudsmit–Fermi–Segrè formula from the hyperfine splitting of the optical spectrum, then “cor” means application of a correction for the finite size of the nucleus (T49BI, T49CS, T50BW). Other corrections are indicated in the footnotes. If the dipole moment is determined from a measured $j$-factor using an inaccurately known value for the nuclear spin, or if only the $j$-factor was measured at all, then its numerical value is given under the value of the dipole moment in parentheses.

Column 7 — literature references to works on the determination of the magnetic moment. If in col. 7 a reference is placed without a numerical value in col. 6, then the given work contains certain possible results for the magnetic moment.

Column 8 — nuclear electric quadrupole moment in units of $e \cdot 10^{-24}\ \mathrm{cm}^2$. “cor” after a result obtained from the hyperfine splitting of the optical spectrum indicates that a correction has been applied for shielding of the nucleus by inner electrons (T50SR, T51SR, T52SR).

Column 9 — literature references to works on the determination of the quadrupole moment.

After the data for each element are placed the ratios of nuclear moments and the ratios of experimentally measured quantities that lead to ratios of moments. These ratios for isotopes of different elements are given under both elements, with only one exception—if one of the elements is hydrogen. Literature references for ratios of dipole moments, resonance frequencies, and hyperfine splittings, as well as for ratios of quadrupole moments, coupling constants, and quadrupole resonance frequencies, are given immediately after the corresponding values. Ratios of nuclear quadrupole moments are denoted by the subscript $Q$. Values taken from works in which the measurements were carried out with the greatest accuracy are presented.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
$0^n$	$1^+$	10,4 min	$1/2$	50MA, N50HA	$-1,912\ 80 \pm 9$	50MB, R50SR
$1\mathrm{H}$	1	99,99%	$1/2$	50MA	$2,792\ 76 \pm 6$ corr.$^*)$	50MA, R50SR, R50TD, R51GA, R51BJ, (R51TS), R51TS, T53MC
$1\mathrm{H}$	2	0,01%	1	50MA, R50LV	$0,857\ 354 \pm 9$ corr.	50MA, R50LV	$(2,738 \pm 14)\times 10^{-3}$	50MA, T50NW, A52RK
$1\mathrm{H}$	$3^+$	12,4 yr	$1/2$	50MA	$2,978\ 643 \pm 28$ corr.	50MA

\[ {}^{2}\nu_{\mathrm{D}}/{}^{1}\nu_{\mathrm{H}} =0,307\ 012\ 192 \pm 15\ \text{(in HD)},\quad \mathrm{R50LI,\ R50LV,\ R51LI,\ R51SA,\ R52LI,\ A52KP,\ R53WI,\ X54LZ} \]

\[ {}^{9}\nu_{\mathrm{Be}}/{}^{2}\nu_{\mathrm{D}}=0,915\ 475 \pm 7\quad \mathrm{R51SW} \]

\[ {}^{14}\nu_{\mathrm{N}}/{}^{2}\nu_{\mathrm{D}}=0,470\ 70 \pm 5\quad \mathrm{R50PY,\ R51PY} \]

\[ {}^{135}\nu_{\mathrm{Cs}}/{}^{2}\nu_{\mathrm{D}}=0,638\ 27 \pm 6\quad \mathrm{R51PY} \]

\[ {}^{47}\nu_{\mathrm{Ti}}/{}^{2}\nu_{\mathrm{D}}=0,367\ 21 \pm 6\quad \mathrm{R53JL} \]

\[ {}^{50}\nu_{\mathrm{V}}/{}^{2}\nu_{\mathrm{D}}=0,649\ 203 \pm 12\quad \mathrm{R52WL,\ R52WM} \]

\[ {}^{75}\nu_{\mathrm{As}}/{}^{2}\nu_{\mathrm{D}}=1,115\ 69 \pm 5\quad \mathrm{R53TW} \]

\[ {}^{87}\nu_{\mathrm{Sr}}/{}^{2}\nu_{\mathrm{D}}=0,282\ 32 \pm 3\quad \mathrm{R53JS} \]

\[ {}^{109}\nu_{\mathrm{Ag}}/{}^{2}\nu_{\mathrm{D}}=0,303\ 16 \pm 3\quad \mathrm{R54JS} \]

\[ {}^{127}\nu_{\mathrm{I}}/{}^{2}\nu_{\mathrm{D}}=1,303\ 37 \pm 2\quad \mathrm{R51SW,\ R51WL} \]

\[ {}^{10}\nu_{\mathrm{B}}/{}^{2}\nu_{\mathrm{D}}=0,700\ 065 \pm 70\quad \mathrm{R53TW} \]

\[ {}^{29}\nu_{\mathrm{Si}}/{}^{2}\nu_{\mathrm{D}}=1,294\ 10 \pm 7\quad \mathrm{R51DV,\ R53WV} \]

\[ {}^{43}\nu_{\mathrm{Ca}}/{}^{2}\nu_{\mathrm{D}}=0,438\ 32 \pm 4\quad \mathrm{R53JE} \]

\[ {}^{49}\nu_{\mathrm{Ti}}/{}^{2}\nu_{\mathrm{D}}=0,367\ 32 \pm 6\quad \mathrm{R53JL} \]

\[ {}^{73}\nu_{\mathrm{Ge}}/{}^{2}\nu_{\mathrm{D}}=0,227\ 24 \pm 2\quad \mathrm{R53JL,\ R54AW} \]

\[ {}^{77}\nu_{\mathrm{Se}}/{}^{2}\nu_{\mathrm{D}}=1,242\ 11 \pm 10\quad \mathrm{R53WA} \]

\[ {}^{99}\nu_{\mathrm{Tc}}/{}^{2}\nu_{\mathrm{D}}=1,466\ 28 \pm 10\quad \mathrm{R52WA} \]

\[ {}^{123}\nu_{\mathrm{Sb}}/{}^{2}\nu_{\mathrm{D}}=0,844\ 23 \pm 8\quad \mathrm{R50CK,\ R50PU,\ R51PY} \]

\[ {}^{129}\nu_{\mathrm{I}}/{}^{2}\nu_{\mathrm{D}}=0,867\ 44 \pm 1\quad \mathrm{R51WL} \]

Table of nuclear moments

\[ \nu_{\mathrm{Cs}^{133}}/\nu_D = 0.854\,49 \pm 4 \quad \mathrm{R51SW} \]

\[ \nu_{\mathrm{Hg}^{199}}/\nu_D = 1.164\,7 \pm 1 \quad \mathrm{R51PY} \]

\[ \nu_{\mathrm{La}^{139}}/\nu_D = 0.920\,25 \pm 6 \quad \mathrm{R51SW} \]

\[ \nu_{\mathrm{Bi}^{209}}/\nu_D = 1.046\,84 \pm 5 \quad \mathrm{R50PU,\ R51PY,\ R53TW} \]

Element	Mass number	Abundance or half-life	Spin	References	Magnetic moment	References	Quadrupole moment	References
${}^{2}\mathrm{He}$	3	$1.3\cdot 10^{-4}\%$	$1/2$	50MA, B50DR, S51FT, A53WH	$-2.127\,414$ $\pm 3$ corr.	50MA, S51FT
${}^{2}\mathrm{He}$	4	$100\%$	0	50MA
${}^{2}\mathrm{He}$	$5^{+}$	$\ll 10^{-8}\ \mathrm{s}$	$3/2$	T52DA	$-1.59 \pm 9$	T52DA
${}^{3}\mathrm{Li}$	$5^{+}$	$\ll 10^{-8}\ \mathrm{s}$	$3/2$	N52AL, T54KC
${}^{3}\mathrm{Li}$	6	$7.4\%$	1	50MA	$0.821\,89$ $\pm 4$ corr.	50MA	$(-)\,4.6\cdot 10^{-4}$	50MA, R51SP, A53KU, T53IN, T54MT
${}^{3}\mathrm{Li}$	7	$92.6\%$	$3/2$	50MA	$3.256\,33$ $\pm 9$ corr.	50MA, R52LI )	$(<0)$	50MA, T50AB, T53HM, A53KU, T53IN, T53SF
${}^{3}\mathrm{Li}$	$8^{+}$	$0.83\ \mathrm{s}$	(3)	T51GA, T52KW, N53CH

\[ \gamma_7/\gamma_6 = 2.640\,91 \pm 1 \quad \mathrm{R51WP} \]

\[ \mu_7/\mu_H = 1.165\,989 \pm 7 \ \text{corr.}\quad \mathrm{R51LI,\ R52LI,\ R52MY^{**})} \]

\[ \nu_{\mathrm{psa}}/\nu_7 = 1.041\,82 \pm 5 \quad \mathrm{R51SW}^{*} \]

\[ Q_6/Q_7 = (1.9 \pm 1)\cdot 10^{-2}\quad \mathrm{R51SP,\ R53CR,\ A63KU} \]

\[ \nu_{\mathrm{B}^{11}}/\nu_7 = 0.825\,615 \pm 4 \quad \mathrm{R51SW} \]

* Correction according to T50RA or T50NX. The correction according to T50NY gives $\mu_H = 2.792\,77 \pm 6$.

** According to measurements by V. G. Hartmann with the participation of N. L. Olifirchuk (1951), by method R.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(h)$	Literature data	$\mu$ nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{4}\mathrm{Be}$	$7+$	53.6 d	$1/2;$ $3/2$	T51MU, T52FL, T52DA, N52AL	$-1.59 \pm 9$	T50AB, T51MU, T52FL, T52DA	$\approx Q(\mathrm{Li}^{7})$	T50AB
${}_{4}\mathrm{Be}$	$8+$	$< 2\cdot 10^{-14}$ s	$(0)$	N52AL
${}_{4}\mathrm{Be}$	$9$	$100\%$	$3/2$	R51GC, R51HR, R51ST, R54WO	$-1.17746$ $\pm 9$ corr.	50MA, R51AV, R51SW	$\approx \|0.02\|$	R51HR, R53KN
${}_{4}\mathrm{Be}$	$10+$	$2.7\cdot 10^{6}$ yr	$(0)$	N52AL
$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$	$\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}$
${}_{5}\mathrm{B}$	$9+$	Very short	$3/2$	T51MU		T51MU
${}_{5}\mathrm{B}$	$10$	$\approx 19.0\%$	$3$	50MA, W50WS, W50GR	$1.80066$ $\pm 15$ corr.	50MA, R51TW, R53TW	$0.0740 \pm 5$	50MA, (T50SR, T52SR), W50GR, Q52DE, (Q53DE), A53WE
${}_{5}\mathrm{B}$	$11$	$\approx 81.0\%$	$3/2$	50MA, W50GR, N54BR	$2.68853$ $\pm 7$ corr.	50MA, R51SW, R52LI	$0.0355 \pm 2$	50MA, (T50SR, T52SR), W50GR, (T53BA), Q52DE, (Q53DE), A53WE
${}_{5}\mathrm{B}$	$12+$	22 ms	$1$	T51NH, T52KW
$Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}$	$Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}$	$Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}$	$Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}$	$Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}$	$\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}$	$\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}$	$\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}$	$\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}$

\[ \gamma_{10}/\gamma_D = 0.700\,065 \pm 70 \ \mathrm{R53TW} \]

\[ \gamma_{11}/\gamma_H = 0.320\,838\,1 \pm 8 \ \mathrm{R51LI,\ R52LI} \]

\[ \gamma_{11}/\gamma_{\mathrm{Nb}^{93}} = 0.761\,87 \pm 40 \ \mathrm{R50SH} \]

\[ \gamma_{10}/\gamma_{\mathrm{Rb}^{85}} = 1.112\,82 \pm 5 \ \mathrm{R53TW} \]

\[ \gamma_{11}/\gamma_{\mathrm{Li}^{7}} = 0.825\,615 \pm 4 \ \mathrm{R51SW} \]

Element	Isotope	Half-life / abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
${}_{6}\mathrm{C}$	$11^{+}$	20.4 min	$3/2$	T49BE	$-1.1$	T49BE
${}_{6}\mathrm{C}$	12	98.9%	0	50MA, N54HR
${}_{6}\mathrm{C}$	13	1.1%	$1/2$	50MA, N52AL	$0.702\,25 \pm 14$ cor	50MA
${}_{6}\mathrm{C}$	$14^{+}$	$5.650 \cdot 10^{3}$ yr	0	50MA
${}_{6}\mathrm{C}$	$15^{+}$	2.4 s	$5/2$	T53IN, N54RH
${}_{7}\mathrm{N}$	$12^{+}$	12.75 ms	1	T51NH
${}_{7}\mathrm{N}$	$13^{+}$	10.1 min	$1/2$	N52AL
${}_{7}\mathrm{N}$	14	99.6%	1	50MA, W54GB, N54ST	$0.403\,69 \pm 3$ cor	50MA, R50PR, R51PY, R53TW	0.01	50MA, (T52SR), W50GS, W54KI
${}_{7}\mathrm{N}$	15	0.4%	$1/2$	50MA, R54OG, N52GO	$-0.283\,12 \pm 4$	50MA, R50PR, R51PY
${}_{7}\mathrm{N}$	$16^{+}$	7.4 s	(2)	T49FH, T51NH, N53HP

\[ \gamma_{15}/\gamma_{14} = 1.402\,6 \pm 1 \ \mathrm{R50PR,\ R51PY} \]

\[ \gamma_{14}/\gamma_H = 0.072\,257 \pm 4 \ \mathrm{R53TW} \]

\[ \gamma_{14}/\gamma_D = 0.470\,70 \pm 5 \ \mathrm{R50PR,\ R51PY} \]

\[ \gamma_{\mathrm{K}^{39}}/\gamma_{14} = 0.645\,80 \pm 6 \ \mathrm{R50CO} \]

\[ \gamma_{14}/\gamma_{\mathrm{Rb}^{85}} = 0.748\,37 \pm 4 \ \mathrm{R53TW} \]

\[ \gamma_{15}/\gamma_D = 0.660\,04 \pm 6 \ \mathrm{R50PR,\ R51PY} \]

\[ \gamma_{\mathrm{Mg}^{25}}/\gamma_{14} = 0.847\,14 \pm 8 \ \mathrm{R51AY} \]

\[ \gamma_{\mathrm{Cr}^{53}}/\gamma_{14} = 0.782\,26 \pm 5 \ \mathrm{R53AH} \]

\[ \gamma_{\mathrm{Mo}^{97}}/\gamma_{14} = 0.920\,8 \pm 1 \ \mathrm{R51PY} \]

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$ nuclear magnetons	Literature data	$Q$ $(e \cdot 10^{-24}\,\mathrm{cm}^2)$	Literature data
${}_{8}\mathrm{O}$	$15^{+}$	118 s	$\leqslant 5/2$	N52AL
${}_{8}\mathrm{O}$	16	99.76%	0	50MA
${}_{8}\mathrm{O}$	17	0.04%	$5/2$	50MA, W51MJ, R51AU, W52GG, W53MT, N52BB	$-1.8928 \pm 1.9$	R51AU	$-4 \cdot 10^{-3}$	50MA, W52GG, W54BT
${}_{8}\mathrm{O}$	18	0.20%	0	50MA, W51MJ			$< \|4 \cdot 10^{-3}\|$	50MA
${}_{8}\mathrm{O}$	$19^{+}$	27 s	$(1/2; 3/2; 5/2)$	T49FH, T52DA, T54FL	$-0.73 \pm 8$	T52DA *)
${}_{8}\mathrm{O}$				$\nu_{17}/\nu_{\mathrm{D}} = 0.88313 \pm 4$ R51AU
${}_{9}\mathrm{F}$	$17^{+}$	70 s	$3/2; 5/2$	N52AL
${}_{9}\mathrm{F}$	$18^{+}$	112 min	1	T52BE, N53ST, T53KP, T54MP,	0.8	T49BE, T52BE	$> 0$	T54MT
${}_{9}\mathrm{F}$	19	100%	$1/2$	50MA	$2.62895 \pm 10$ cor	50MA, R51SW**), R52LI
${}_{9}\mathrm{F}$	$20^{+}$	10.7 s	1	T49FH, T53KP N53FB, T54SC
${}_{9}\mathrm{F}$				$\nu_{\mathrm{H}}/\nu_{19} = 1.062917 \pm 1$ R50GA, R51BD, R51MY, R51SW, R52LI *)

TABLE OF NUCLEAR MOMENTS

Element	Mass number	Abundance or half-life	$I$
${}_{10}\mathrm{Ne}$	20	90,9%	(0)	50MA, A52WT	$<12\cdot 10^{-4}$	50MA, A52WT
${}_{10}\mathrm{Ne}$	21	0,3%	3/2	50MA, T51ST, T52BE, T52DA, N52MT	$-0,73 \pm 8$	50MA, T51ST, T52FL, T52BE, T52DA, T54SH	$-0,195$	T54SH
${}_{10}\mathrm{Ne}$	22	8,8%	(0)	50MA	$\approx 0$	50MA
${}_{10}\mathrm{Ne}$	$23^{+}$	40,2 s	(5/2)	N53HP
${}_{11}\mathrm{Na}$	$22^{+}$	2,60 y	3	50MA	$1,745\ 82 \pm 22\ \mathrm{cor}$	50MA
${}_{11}\mathrm{Na}$	23	100%	3/2	50MA, R51GC	$2,217\ 54 \pm 10\ \mathrm{cor}$	50MA, R52LI, R51SW	$0,10 \pm 6$ $(-2,3)$	S53MW ) T53IN *) D54SA T54MT, T54SH
${}_{11}\mathrm{Na}$	$24^{+}$	15,1 h	4	A51SB, A53SB, N54NY	$1,688 \pm 5$	A53SB
${}_{11}\mathrm{Na}$	$25^{+}$	58,2 s	3/2	A51SB, A53SB, N54NY

\[ \nu_{23}/\nu_{\mathrm{H}}=0,264\ 518\ 2 \pm 7 \quad \text{R51LI, A51LK, R52LI, R52MY} \]

\[ \nu_{23}/\nu_{\mathrm{Al}^{27}}=1,015\ 081 \pm 1 \quad \text{R50GA} \]

\[ \nu_{23}/\nu_{\mathrm{Sc}^{45}}=1,088\ 83 \pm 5 \quad \text{R50PU, R51PY, R51SW} \]

\[ \nu_{\mathrm{V}^{51}}/\nu_{23}=0,993\ 855 \pm 25 \quad \text{R52WM} \]

) $I=3/2$ adopted.
) According to the measurement of V. G. Hartmann with the participation of N. L. Olifertchuk (1951), by method R.
) Value predicted, not obtained from the hyperfine structure of line spectra.
**) Mean value according to unpublished measurement data of P. Kusch.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(h)$	Literature data	$\mu$, nuclear magnetons	Literature data
				$\nu_{\mathrm{Mn}^{55}}/\nu_{23}=0.9372\pm1$ R50PR, R51PY		$\nu_{\mathrm{Co}^{59}}/\nu_{23}=0.89709\pm9$ R51PY
				$\nu_{\mathrm{As}^{75}}/\nu_{23}=0.64745\pm15$ R51DW, R53WV		$\nu_{\mathrm{Se}^{77}}/\nu_{23}=0.72193\pm2$ R52DW, R53WV
				$\nu_{\mathrm{Cd}^{111}}/\nu_{23}=0.8016\pm1$ R50PY		$\nu_{\mathrm{Cd}^{113}}/\nu_{23}=0.8386\pm1$ R50PY
				$\nu_{\mathrm{In}^{113}}/\nu_{23}=0.82667\pm8$ R51PY		$\nu_{\mathrm{In}^{115}}/\nu_{23}=0.82841\pm8$ R51PY
				$\nu_{\mathrm{Sn}^{115}}/\nu_{23}=1.2362\pm1$ R50PY		$\nu_{\mathrm{Sn}^{117}}/\nu_{23}=1.3468\pm1$ R50PY
				$\nu_{\mathrm{Sn}^{119}}/\nu_{23}=1.4090\pm1$ R50PY		$\nu_{\mathrm{Sb}^{121}}/\nu_{23}=0.90469\pm4$ R50CL, R50CK, R50PU, R51PY
				$\nu_{\mathrm{Te}^{123}}/\nu_{23}=0.99085\pm3$ R51DV, R53DW		$\nu_{\mathrm{Te}^{125}}/\nu_{23}=1.19457\pm4$ R51DV, R53DW
				$\nu_{\mathrm{Xe}^{129}}/\nu_{23}=1.0457\pm1$ R50PU, R51PY		$\nu_{\mathrm{Re}^{185}}/\nu_{23}=0.85114\pm9$ R51AY
				$\nu_{\mathrm{Re}^{187}}/\nu_{23}=0.85987\pm9$ R51AY		$\nu_{\mathrm{Pt}^{195}}/\nu_{23}=0.81273\pm8$ R51PY
				$\nu_{\mathrm{Pb}^{207}}/\nu_{23}=0.7901\pm1$ R51PY
${}^{12}\mathrm{Mg}$	24	78.6%	(0)	50MA	$\approx 0$	50MA
${}^{12}\mathrm{Mg}$	25	10.1%	$5/2$	50MA, S50KS, N54EK	$-0.85466\pm15$	50MA, S50KS, R51AY
${}^{12}\mathrm{Mg}$	26	11.3%	(0)	50MA, N54EK	$\approx 0$	50MA
${}^{12}\mathrm{Mg}$	$27+$	9.5 m	$1/2$	T52DA, N54EK	$-0.62\pm7$	T52DA
				$\nu_{25}/\nu_{\mathrm{N}^{14}}=0.84714\pm8$ R51AY

Table of Nuclear Moments

Element	Isotope	Abundance or half-life	Spin	References	Magnetic moment	References	Quadrupole moment	References
$^{13}\mathrm{Al}$	$25+$	7.3 s	$3/2;\ 5/2$	T51MU, N53GO		T51MU		50MA, (T50SR, T52SR), A53LE, T52KO
$^{13}\mathrm{Al}$	$26+$	109 y	5	T49BE, T52BE, T53KP, N54EK	3.0	T49BE
$^{13}\mathrm{Al}$	27	100%	$5/2$	50MA, R53PC, R54WO	$3.641\,33 \pm 15$ cor	50MA, R51SV, S51SV, R52LI, R54WO	$0.149 \pm 2$	50MA, (T50SR, T52SR), A53LE, T52KO
$^{13}\mathrm{Al}$	$28+$	2.3 m	3	N54SH, N54EG, N54EK
$^{13}\mathrm{Al}$	$29+$	6.6 m	$5/2$	N54EK

\[ \gamma_{27}/\gamma_{\mathrm H} = 0.260\,569 \pm 10 \quad \text{R51LI, R52MY, R52LI} \]

\[ \gamma_{27}/\gamma_{\mathrm{Sc}} = 1.072\,61 \pm 5 \quad \text{R51SW} \]

\[ \gamma_{27}/\gamma_{\mathrm{Na}^{23}} = 1.015\,081 \pm 1 \quad \text{R50GA} \]

\[ \gamma_{\mathrm{Rb}^{87}}/\gamma_{27} = 1.255\,29 \pm 6 \quad \text{R51SW} \]

Element	Isotope	Abundance or half-life	Spin	References	Magnetic moment	References	Quadrupole moment	References
$^{14}\mathrm{Si}$	28	92.2%	0	50MA, W50SP, R54OR	$(r < 0.05)$	R54WG	$\approx 0$	50MA
$^{14}\mathrm{Si}$	29	4.7%	$1/2$	50MA, W50SP, R53WV, W53WT, R54OR, R54WG, N54EK	$-0.554\,92 \pm 4$	R51DV, R51HR, R53WV	$< 1.1 \cdot 10^{-4}$	50MA, W53WT
$^{14}\mathrm{Si}$	30	3.1%	0	50MA, W50SP, R54OR, N54EK		R54WG	$\approx 0$	50MA
$^{14}\mathrm{Si}$	$31+$	157 m	$1/2;\ 3/2$	N54EK

\[ \gamma_{29}/\gamma_{\mathrm D} = 1.294\,10 \pm 7 \quad \text{R51DV, R53WV} \]

$Z$	$A$	$p\%$ or $T_{1/2}$	$I$ $(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\,\mathrm{cm}^2)$	Literature data
${}_{15}\mathrm{P}$	$29^\dagger$	4.5 s	$(1/2)$	N54EK
${}_{15}\mathrm{P}$	$30^\dagger$	2.5 min	1	T52BE; T54MP, N54EL	0.65	T52BE	0	T54MT
${}_{15}\mathrm{P}$	31	100%	$1/2$	50MA	$1.131\,65 \pm 7$ corr.	50MA, R51SW
${}_{15}\mathrm{P}$	$32^\dagger$	14.3 d	$(1;2)$	T53SK, N54KB, T52BB, N54EG		T53SK
${}_{15}\mathrm{P}$	$33^\dagger$	25.0 d	$(3/2)$	N54NJ
${}_{15}\mathrm{P}$	$34^\dagger$	12.7 s	$(1)$	N54EK
		$\gamma_{31}/\gamma_{\mathrm{H}} = 0.404\,804 \pm 10$ R52MY				$\gamma_{31}/\gamma_{\mathrm{Li}^7} = 1.041\,82 \pm 5$ R51SW
${}_{16}\mathrm{S}$	$31^\dagger$	2.66 s	$1/2$	T52DA	$-0.62 \pm 7$	T52DA
${}_{16}\mathrm{S}$	32	95.00%	0	50MA			—
${}_{16}\mathrm{S}$	33	0.74%	$3/2$	50MA, W50EH, N54EK	$0.642\,92 \pm 14$	50MA, W50EH, W50JN, R51DR, W52EH, R53WV	$-0.064$ corr.	50MA, (T52SR), Q53DH, W53GB, W54BT
${}_{16}\mathrm{S}$	34	4.24%	$(0)$	50MA			$<\lvert 2\cdot 10^{-3}\rvert$	50MA
${}_{16}\mathrm{S}$	$35^\dagger$	87.1 d	$3/2$	50MA, W50CK, T51ST, W51CK	$(+)1.00 \pm 4^*)$	T51ST, T52BE, W54CK, T52DA	0.045 corr.	50MA, (T52SR), W51CK, Q53DH, W53GB, W54BT
${}_{16}\mathrm{S}$	36	0.017%	$(0)$	50MA			$<0.01$	50MA
		$Q_{35}/Q_{36} = -0.695$ W51CK, (Q53DH)				$\gamma_{33}/\gamma_{\mathrm{N}^{14}} = 1.061\,74 \pm 13$ R51DR, R53WV


${}^{17}\mathrm{Cl}$	$33^{\dagger}$	$1,8\ \mathrm{s}$	$(3/2;\ 5/2)$	N54EK
${}^{17}\mathrm{Cl}$	$34^{\dagger}$	$1,50\ \mathrm{s}$	$0$	T52MA, T53KP, T54MP, N54EK			$0$	T54MT
${}^{17}\mathrm{Cl}$	$35$	$75,39\%$	$3/2$	50MA	$0,821\ 80 \pm 5\ \text{sog}$	50MA, R50PR, R51PY, R53TW, Q53TM, Q54TM	$-0,084\ 31 \pm 2\ \text{sog}$	50MA, T52KO, A51JK, (T51SR, T52SR)
${}^{17}\mathrm{Cl}$	$36^{\dagger}$	$4,4\cdot 10^{5}\ \mathrm{yr}$	$2$	50MA, W51JG, W52GT	$0,9$	T52KL	$-0,0168 \pm 1$	50MA, (T51SR, T52SR), W51JG, W52GT
${}^{17}\mathrm{Cl}$	$37$	$24,61\%$	$3/2$	50MA	$0,684\ 10 \pm 5\ \text{sog}$	50MA, R50PR, R51PY, R53TW	$-0,066\ 35 \pm 2\ \text{sog}$	50MA, T52KO, A51JK, (T51SR, T52SR)
${}^{17}\mathrm{Cl}$	$38^{\dagger}$	$37,3\ \mathrm{min}$	$(2)$	T53KU, N50LA, T50FE, T52BB

\[ \Delta \nu_{35}/\Delta \nu_{37}=1,201\ 357 \pm 13 \quad \text{R50PR, R51PY, A51JK} \]
\[ \text{Q51DK, R51WP, R53TW} \]

\[ (\gamma_{35}/\gamma_{37})_{Q}=1,268\ 78 \pm 15 \quad \text{W50SW, A51JK, Q51DH,} \]
\[ \text{Q51DK, Q51LV, W51GG,} \]
\[ \text{A52ZR, E52CL, Q52DP,} \]
\[ \text{Q52WT, Q53BB, R53MA} \]

\[ \nu_{35}/\nu_{\mathrm{H}}=0,097\ 982 \pm 5 \quad \text{R53TW} \]

\[ \nu_{\mathrm{Ti}^{47}}/\nu_{35}=0,574\ 93 \pm 6 \quad \text{R53JL} \]

\[ \nu_{\mathrm{V}^{51}}/\nu_{35}=1,017\ 58 \pm 1 \quad \text{R52WL} \]

\[ \nu_{\mathrm{Ge}^{73}}/\nu_{35}=0,355\ 72 \pm 4 \quad \text{R53JL} \]

\[ \nu_{37}/\nu_{\mathrm{Rb}^{85}}=0,844\ 77 \pm 5 \quad \text{R53TW} \]

\[ \nu_{35}/\nu_{\mathrm{D}}=0,638\ 27 \pm 6 \quad \text{R51PY} \]

\[ \nu_{\mathrm{Ti}^{49}}/\nu_{35}=0,575\ 08 \pm 6 \quad \text{R53JL} \]

\[ \nu_{35}/\nu_{\mathrm{Rb}^{85}}=1,014\ 81 \pm 5 \quad \text{R52WL, R53TW} \]

\[ \nu_{\mathrm{Os}^{189}}/\nu_{35}=0,791\ 896 \pm 93 \quad \text{R54LS} \]

\[ \nu_{37}/\nu_{\mathrm{H}}=0,081\ 564 \pm 6 \quad \text{R53TV} \]

*) If negative, then $\mu=-1,07 \pm 4$.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}^{18}\mathrm{Ar}$	$35^{+}$	$1.90\ \mathrm{s}$	$(3/2)$	T51MU	$\approx 0$	T51MU
${}^{18}\mathrm{Ar}$	$36$	$0.34\%$	$(0)$	50MA		50MA, S53ME
${}^{18}\mathrm{Ar}$	$37^{+}$	$35.0\ \mathrm{d}$	$3/2$	T51MU, T52DA	$0.98 \pm 7$	T51MU, T52DA
${}^{18}\mathrm{Ar}$	$38$	$0.06\%$	$0$	T50FE	$\approx 0$	S53ME
${}^{18}\mathrm{Ar}$	$39^{+}$	$265\ \mathrm{y}$	$7/2$	N50BZ
${}^{18}\mathrm{Ar}$	$40$	$99.60\%$	$(0)$	50MA	$\approx 0$	50MA, S53ME
${}^{18}\mathrm{Ar}$	$41^{+}$	$110\ \mathrm{min}$	$5/2;$ $7/2$	T49FI, T52DA, N54EK	$-1.17 \pm 12$	T52DA
${}^{19}\mathrm{K}$	$38^{+}$	$0.95\ \mathrm{s}$	$0$	T53KP, T53KU, T54MP, N54EK	$1.4$	T52BE	$>0$	T54MT
${}^{19}\mathrm{K}$	$39$	$93.08\%$	$3/2$	50MA	$0.390\,873 \pm 13$	50MA, A52EB, R54BO	$(\approx -0.03)$	49GH, T52WB T52PI
${}^{19}\mathrm{K}$	$40^{+}$	$1.25\cdot 10^{9}\ \mathrm{y}$ $0.01\%$	$4$	50MA, N54EG	$-1.298\,2$ $\pm 4\ \mathrm{cor}$	50MA A52EB
${}^{19}\mathrm{K}$	$41$	$6.91\%$	$3/2$	50MA	$+0.214\,53 \pm 3$	50MA, R54BO	$(\approx -0.02)$	49GH, T52WB
${}^{19}\mathrm{K}$	$42^{+}$	$12.5\ \mathrm{h}$	$2$	A53SB, N54EK	$-1.137 \pm 5$	A53SB
${}^{19}\mathrm{K}$	$43^{+}$	$22.0\ \mathrm{h}$	$(3)$	N54LT

\[ \Delta \nu_{39}/\Delta \nu_{41}=1.817\,68 \pm 1\ \text{A50LO, R54BO} \]

\[ Q_{41}/Q_{39}=1.220 \pm 2\ \text{E53CL} \]

\[ \gamma_{40}/\gamma_{39}=-1.243\,46 \pm 24\ \text{A52EB} \]

\[ \mu_{39}/\mu_{\mathrm H}=0.139\,99 \pm 2\ \text{R50CO} \]

\[ \gamma_{39}/\gamma_{\mathrm{N}^{14}}=0.645\,80 \pm 6\ \text{R50CO} \]

TABLE OF NUCLEAR MOMENTS

Element	Isotope	Abundance or half-life	Spin	Method	Magnetic moment	References	Additional value	Additional references
$^{20}\mathrm{Ca}$	40	96.92%	(0)	50MA N54EK	$\approx 0$	50MA, R51GC
$^{20}\mathrm{Ca}$	41+	$\left\{\begin{array}{l}<7\cdot 10^{-4}\%\\ 1.1\cdot 10^{5}\ \text{yr}\end{array}\right.$	(5/2; 7/2)	N54EK
$^{20}\mathrm{Ca}$	42	0.64%	0	T50FE
$^{20}\mathrm{Ca}$	43	0.13%	7/2	R53JE, S54KK	$-1.3152 \pm 2$	R53JE, S54KK
$^{20}\mathrm{Ca}$	45+	164 d	5/2	T52DA	$0.87 \pm 6$	T52DA
$^{20}\mathrm{Ca}$	49+	2.5 h	3/2	T52DA	$-0.85 \pm 9$	T52DA
$^{21}\mathrm{Sc}$	43+	3.92 h	7/2	N54IM
$^{21}\mathrm{Sc}$	44+	3.92 h	(2; 3)	N54SD, T54HC, T54SC
$^{21}\mathrm{Sc}$	45	100%	7/2	50MA	$4.75611 \pm 6\ \mathrm{cor}^{**)}$	50MA, R50PU, R50SW, (T50RA), R51HU, R51PY	$(-0.31)$	T52WB
$^{21}\mathrm{Sc}$	46+	84 d	4	N54KS, T52RB		R51SW
$^{21}\mathrm{Sc}$	47+	3.43 d	(7/2)	N53CB
$^{21}\mathrm{Sc}$	48+	43.7 h	$>6$	T52KU, T53KU, N52JW, N52RP, N53CG, N52JK

\[ \gamma_{43}/\gamma_{\mathrm{D}} = 0.43832 \pm 4 \quad \text{R53JE} \]

\[ \gamma_{43}/\gamma_{\mathrm{H}} = -0.242939 \pm 3 \quad \text{R51HU} \]

\[ \gamma_{\mathrm{Al}^{27}}/\gamma_{43} = 1.07261 \pm 5 \quad \text{R51SW} \]

\[ \gamma_{\mathrm{Na}^{23}}/\gamma_{43} = 1.08883 \pm 5 \quad \text{R50PU, R51PY, R51SW} \]

\[ \gamma_{\mathrm{V}^{51}}/\gamma_{43} = 1.08156 \pm 5 \quad \text{R51SW} \]

*) R51SW calculated from data borrowed from R51HU.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \text{cm}^2)$	Literature data
${}_{21}\mathrm{Sc}$		$\gamma_{\mathrm{Mn}^{55}}/\gamma_{45}=1{,}020$	$28\pm 5$	R51SW	$\gamma_{\mathrm{Cu}^{63}}/\gamma_{45}=1{,}091$	$25\pm 6$ R51SW
${}_{21}\mathrm{Sc}$		$\gamma_{\mathrm{Cu}^{65}}/\gamma_{45}=1{,}169$	$51\pm 6$	R51SW	$\gamma_{45}/\gamma_{\mathrm{Br}^{79}}=0{,}969$	$54\pm 6$ R50SW, R51SW
${}_{21}\mathrm{Sc}$		$\gamma_{\mathrm{Br}^{81}}/\gamma_{45}=1{,}111$	$65\pm 6$	R51SW	$\gamma_{\mathrm{Nb}^{93}}/\gamma_{45}=1{,}006$	$13\pm 5$ R51SW
${}_{21}\mathrm{Sc}$		$\gamma_{\mathrm{In}^{115}}/\gamma_{45}=0{,}901$	$877\pm 50$	R52TB, R53TW
${}_{22}\mathrm{Ti}$	$45^{+}$	$3{,}08$ h	$7/2$	T52DA	$-1{,}17\pm 12$	T52DA
${}_{22}\mathrm{Ti}$	47	$7{,}75\%$	$5/2$	R53JL, T53WI	$-0{,}787\ 06\pm 10$	R53JL
${}_{22}\mathrm{Ti}$	48	$73{,}45\%$	0	N54SB
${}_{22}\mathrm{Ti}$	49	$5{,}51\%$	$7/2$	R52JE *), R53JL, N54SB	$-1{,}102\ 2\pm 2$	R52JE *), R52ST R53JL	$(0{,}34)$	T52WB
${}_{22}\mathrm{Ti}$	$51^{+}$	$5{,}79$ min	$3/2$	T52DA	$-0{,}85\pm 9$	T52DA
${}_{22}\mathrm{Ti}$		$\gamma_{47}/\gamma_{\mathrm{D}}=0{,}367$	$21\pm 6$	R53JL	$\gamma_{47}/\gamma_{\mathrm{Cr}^{53}}=0{,}574$	$93\pm 6$ R53JL
${}_{22}\mathrm{Ti}$		$\gamma_{49}/\gamma_{\mathrm{H}}=0{,}056$	$38\pm 1$	R52JE *)	$\gamma_{49}/\gamma_{\mathrm{D}}=0{,}367$	$32\pm 6$ R53JL
${}_{22}\mathrm{Ti}$		$\gamma_{49}/\gamma_{\mathrm{Cl}^{35}}=0{,}575$	$08\pm 6$	R53JL
${}_{23}\mathrm{V}$	$48^{+}$	$16{,}0$ d	$4; 5$	N53CG
${}_{23}\mathrm{V}$	$49^{+}$	635 d	$7/2$	N54NN, T54FL,
${}_{23}\mathrm{V}$	50	$0{,}23\%$	6	X52KS, X52BT, T52HC	$3{,}347$ corr. **)	R52WL, R52WM
${}_{23}\mathrm{V}$	51	$99{,}77\%$	$7/2$	50MA, X51BE, X51BS	$5{,}145\ 03\pm 23$ corr.	50MA, R51PY, R51SW, R52WM	$0{,}3\pm 2$	S53MW

TABLE OF NUCLEAR MOMENTS (continued)

Element	Isotope	Half-life / abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
	52+	3.75 min	(3)	N54KB, T52BB
		$\nu_{50}/\nu_{51}=0.379\,074\pm17$ X52KS, X52BT, R52WM			$\nu_{50}/\nu_D=0.649\,203\pm12$ R52WL, R52WM
		$\nu_{50}/\nu_{\mathrm{Cr}^{53}}=1.017\,58\pm10$ R52WL			$\nu_{50}/\nu_{\mathrm{Rb}^{85}}=1.032\,62\pm10$ R52WL
		$\gamma_{51}/\gamma_{\mathrm H}=0.262\,65$ 50BE			$\nu_{51}/\nu_{\mathrm{Na}^{23}}=0.993\,855\pm25$ R52WM
		$\nu_{51}/\nu_{\mathrm{Sc}^{45}}=1.081\,56\pm5$ R51SW
${}_{24}\mathrm{Cr}$	49+	41.9 min	$5/2$	T52DA, N54NN	$0.87\pm6$	T52DA
${}_{24}\mathrm{Cr}$	51+	27.75 days	$7/2$	T52DA	$-1.20\pm12$	T52DA
${}_{24}\mathrm{Cr}$	53	9.55%	$3/2$	X51BW, X52BW, R53JS, R54HB	$-0.473\,51\pm6$	X51BE, X51BW, X52BW, R53AH, R53JS	$(-0.09)$	T52WB
${}_{24}\mathrm{Cr}$	55+	3.52 min	$3/2$	T52DA	$-0.66\pm9$	T52DA
${}_{24}\mathrm{Cr}$		$\nu_{53}/\nu_D=0.368\,20\pm3$ R53JS			$\nu_{53}/\nu_{14}=0.782\,26\pm5$ R53AH
${}_{25}\mathrm{Mn}$	52+	6.0 days	5	N52GH, T54HC, T54SC			—
${}_{25}\mathrm{Mn}$	55	100%	$5/2$	50MA, X51BI, X51BE, X50AK, X50ES, W52JT, X54UE	$3.467\,53\pm17$ corr.	50MA, R50PR, R51PY, R51SW	$0.4\pm2$	W53JT, T53TR, S53MW
${}_{25}\mathrm{Mn}$	56+	2.58 h	$3\pm1$	N54KB
${}_{25}\mathrm{Mn}$		$\nu_{55}/\nu_{\mathrm H}=0.247\,86\pm12$ R50SC			$\nu_{55}/\nu_{\mathrm{Na}^{23}}=0.937\,2\pm1$ R50PR, R51PY
${}_{25}\mathrm{Mn}$		$\nu_{55}/\nu_{\mathrm{Sc}^{45}}=1.020\,28\pm5$ R51SW

*) The value from R52JE for $\mathrm{Ti}^{49}$ may be assigned on the basis of R53JL.

**) In R52WM, $I_{50}=7$ was adopted and $\mu=3.905$ nuclear magnetons, corr., was obtained. The value of $\mu$ adopted here is obtained for $I_{50}=6$.

$Z$	$A$	$\rho\%$ or $T_{1/2}$	$I$ ($\hbar$)	Literature data	$\mu$ nuclear magnetons	Literature data	$Q$ $(e \cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{26}\mathrm{Fe}$	$53^{\dagger}$	8.9 min	$7/2$	T52DA	$-1.20 \pm 12$	T52DA
${}_{26}\mathrm{Fe}$	$55^{\dagger}$	2.94 yr	$3/2$	T52DA	$-0.85 \pm 9$	T52DA
${}_{26}\mathrm{Fe}$	57	2.21%	$\leq 5/2;\ \neq 1/2$	T51ST, T52DA, T53WA, X54BT, N54KB	$<0.05$	50MA, T51ST, T52DA, X54BT	$(0.10)$	T52WB
${}_{26}\mathrm{Fe}$	$59^{\dagger}$	45.1 d	$3/2$	T52DA	$-0.10 \pm 9$	T52DA	—	—
${}_{27}\mathrm{Co}$	$55^{\dagger}$	18.1 h	$7/2$	N54CM
${}_{27}\mathrm{Co}$	$56^{\dagger}$	80 d	(5)	N53MT
${}_{27}\mathrm{Co}$	$57^{\dagger}$	270 d	$7/2$	X53BB	$\lvert 4.6 \pm 2\rvert$	X53BB
${}_{27}\mathrm{Co}$	$58^{\dagger}$	72 d	2	N50SH, N52GA, N52DG	$\lvert 3.5 \pm 3\rvert$	N52GA, N52DG
${}_{27}\mathrm{Co}$	59	100%	$7/2$	50MA, X51BK, X51BE, R50PR, R51PY	$4.639\,9 \pm 9$	50MA, R50PR, R51PY
${}_{27}\mathrm{Co}$	$60^{\dagger}$	5.24 yr	$5;4$	N51DS, N52FN, N54KS	$I=5;\ \mu=\lvert 3.5 \pm 5\rvert$	N52BD, (N52DG), N52GT, N52GS, T52KI, N54BD	$0.5 \pm 2$	S53MW
${}_{27}\mathrm{Co}$	$60^{\dagger}$	5.24 yr	$5;4$	N51DS, N52FN, N54KS	$I=4;\ \mu=3.5 \pm 5\ (3.2 \pm 5)$	N54BD	$0.5 \pm 2$	S53MW

\[ |\gamma_{56}/\gamma_{57}| = 1.00 \pm 5 \quad \text{X53BB} \]

\[ \gamma_{59}/\gamma_{\mathrm{Na}^{23}} = 0.897\,09 \pm 9 \quad \text{R50PR, R51PR} \]

\[ |\gamma_{60}/\gamma_{59}| = 32/67 \quad \text{N52GT} \]

Table of nuclear moments

Element	Mass number	Half-life or abundance	Spin	References	Magnetic moment	References	Electric quadrupole moment	References
${}_{28}\mathrm{Ni}$	$57+$	$36.4$ h	$3/2$	N51CM
${}_{28}\mathrm{Ni}$	$59+$	$7.5\cdot 10^{4}$ yr	$3/2$	T52DA, N54ES	$-0.66 \pm 9$	T52DA
${}_{28}\mathrm{Ni}$	$61$	$1.25\%$	$5/2$	T51ST, T52DA, T53WA, N53SP	$<0.25$	50MA, S50KF, T51ST, T52DA
${}_{29}\mathrm{Cu}$	$58+$	$7.9$ min or $3.04$ s $3.04$ s	$(1)$	T54MP
${}_{29}\mathrm{Cu}$	$60+$	$24.6$ min	$2$	N54NV
${}_{29}\mathrm{Cu}$	$62+$	$10.1$ min	$0;\ 1$	T52MA, N54NW,
${}_{29}\mathrm{Cu}$	$63$	$68.94\%$	$3/2$	50MA, X51BE	$2.226\,28 \pm 13\ \mathrm{cor}$	50MA, R51SW	$-0.157 \pm 31$	50MA, (T51SR, T52SR), T51AP, Q51BE, X51BU, (T52KL), S53KS, X53BT
${}_{29}\mathrm{Cu}$	$64+$		$1$	A54LP, N54KB	$\lvert 0.40 \pm 5\rvert$	A54LP
${}_{29}\mathrm{Cu}$	$65$	$31.1\%$	$3/2$	50MA, X51BE	$2.385\,94 \pm 13\ \mathrm{cor}$	50MA, R51SW	$-0.145 \pm 29$	50MA, (T51SR, T52SR), T51AP, Q51BE, X51BU, (T52KL), X53BT
${}_{29}\mathrm{Cu}$	$66+$	$5.08$ min	$(1)$	T53MA, N54KB

\[ Q_{63}/Q_{65}=1.080\,6 \pm 3 \quad \text{Q51BE, T51AP, X51BU, **Q52KM**} \]

\[ \nu_{63}/\nu_{\mathrm{Sc}^{45}}=1.091\,25 \pm 6 \quad \text{R51SW} \]

\[ \nu_{65}/\nu_{63}=1.071\,78 \pm 5 \quad \text{R51SW} \]

\[ \nu_{65}/\nu_{\mathrm{Sc}^{45}}=1.169\,51 \pm 6 \quad \text{R51SW} \]

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{30}\mathrm{Zn}$	$63^{+}$	38.3 min	$3/2$	T52DA	$-0.10 \pm 9$	T52DA
${}_{30}\mathrm{Zn}$	64	48.89%	$(0)$	50MA	$\approx 0$	50MA
${}_{30}\mathrm{Zn}$	$65^{+}$	250 d	$5/2$	T52DA, N53PH, N54KB	$-0.62 \pm 9^{*}$	T52DA
${}_{30}\mathrm{Zn}$	66	27.81%	$(0)$	50MA	$\approx 0$	50MA
${}_{30}\mathrm{Zn}$	67	4.16%	$5/2$	50MA	$0.873\,78 \pm 13$	50MA, R52DV, R53WV
${}_{30}\mathrm{Zn}$	68	18.51%	$(0)$	50MA	$\approx 0$	50MA
${}_{30}\mathrm{Zn}$	$69^{+}$	57 min	$1/2$	T49FH, T51GS, T52DA, N53DD	0.48	T52DA
${}_{30}\mathrm{Zn}$		$\gamma_{67}/\gamma_{\mathrm{N}^{14}} = 0.865\,80 \pm 1$ R52DV, R53WV
${}_{31}\mathrm{Ga}$	$66^{+}$	9.2 h	1	T53SK, N52MP		T53SK
${}_{31}\mathrm{Ga}$	$67^{+}$	3.26 d	$3/2$	N53KB
${}_{31}\mathrm{Ga}$	$68^{+}$	67 min	1	T53SK, N52MP		T53SK
${}_{31}\mathrm{Ga}$	69	60.2%	$3/2$	50MA	$2.016\,7 \pm 11$ corr.	50MA	0.243 corr.	50MA, (T50SR, T52SR), T52KO
${}_{31}\mathrm{Ga}$	71	39.8%	$3/2$	50MA	$2.561\,4 \pm 10$ corr.	50MA	0.152 corr.	50MA, (T50SR, T52SR), T52KO
${}_{31}\mathrm{Ga}$	$73^{+}$	4.9 h	$3/2$	N53HP
${}_{31}\mathrm{Ga}$		$(\gamma_{69}/\gamma_{71})_{Q}=1.586\,7 \pm 4$ Q53DM			$\mu_{69}/\mu_{\mathrm{H}}$ see T50KS		$\mu_{71}/\mu_{\mathrm{H}}$ see T50KS

TABLE OF NUCLEAR MOMENTS

Element	A	Half-life / abundance	I	References	μ	References	Q	References
${}_{32}\mathrm{Ge}$	$67^{+}$	20 min	3/2	T52DA	$-0.62 \pm 9$	T52DA	$\lvert < 7 \cdot 10^{-3} \rvert$	50MA, W51MA
${}_{32}\mathrm{Ge}$	70	20.52%	0	50MA, W50ST, W51MA
${}_{32}\mathrm{Ge}$	$71^{+}$	11 d	1/2	T49FH, T52DA, N53SV	$0.48 \pm 7$	T52DA
${}_{32}\mathrm{Ge}$	72	27.43%	0	50MA, W50ST, W51MA			$\lvert < 7 \cdot 10^{-3} \rvert$	50MA, W51MA
${}_{32}\mathrm{Ge}$	73	7.76%	9/2	50MA, W51MA	$-0.876\,77 \pm 9$	R53JL, R54AW	$-0.22 \pm 10$ concord.	50MA, (T52SR) W51MA
${}_{32}\mathrm{Ge}$	74	36.54%	0	50MA, W50ST, W51MA			$\lvert < 7 \cdot 10^{-3} \rvert$	50MA, W51MA
${}_{32}\mathrm{Ge}$	$75^{+}$	80 min	(1/2)	N52SC
${}_{32}\mathrm{Ge}$	76	7.76%	0	50MA, W50ST, W51MA			$\lvert < 7 \cdot 10^{-3} \rvert$	50MA, W51MA
${}_{32}\mathrm{Ge}$	$77^{+}$	12 h	(7/2)	T52DA, N53HP	$0.52 \pm 7$	T52DA *)

\[ \nu_{73}/\nu_{\mathrm{D}}=-0.227\,24 \pm 2 \ \text{R53JL, R54AW} \]

\[ \nu_{73}/\nu_{\mathrm{Cl}^{35}}=0.355\,72 \pm 4 \ \text{R53JL.} \]

Element	A	Half-life / abundance	I	References	μ	References	Q	References
${}_{33}\mathrm{As}$	$72^{+}$	25.8 h	2	T53SK		T53SK
${}_{33}\mathrm{As}$	$73^{+}$	76 d	(3/2; 5/2)	N53BB
${}_{33}\mathrm{As}$	75	100%	3/2	50MA, R52JE	$1.438\,93$ $\pm 8$ concord.	50MA, R51DW R52JE, Q52KB R53WV, R53TW	$0.3 \pm 2$ concord.	50MA, (T52SR)

) Adopted $I=3/2$.
*) Adopted $I=1/2$.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e \cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{33}\mathrm{As}$	$76^{+}$	$26.8\ \mathrm{h}$	$2$	N53HP
${}_{33}\mathrm{As}$	$77^{+}$	$38.7\ \mathrm{h}$	$3/2$	N52SA
${}_{33}\mathrm{As}$		$\nu_{75}/\nu_{\mathrm H}=0.17129 \pm 3$		R52JE, R53TW	$\nu_{75}/\nu_{\mathrm D}=1.11569 \pm 5$	R53TW	$\nu_{75}/\nu_{\mathrm{Na}^{23}}=0.64745 \pm 15$	R51DW, R53WV
${}_{34}\mathrm{Se}$	$73^{+}$	$7.1\ \mathrm{h}$	$1/2$	T52DA	$0.48 \pm 7$	T52DA
${}_{34}\mathrm{Se}$	$74$	$0.87\%$	$0$	50MA, W50GM			$\lvert <2 \cdot 10^{-3} \rvert$	W50GM
${}_{34}\mathrm{Se}$	$75^{+}$	$127\ \mathrm{y}$	$5/2$	N52SC, N54JI, W54AS	$-1.61 \pm 14^{*)}$	T52DA	$0.9$	W54AS
${}_{34}\mathrm{Se}$	$76$	$9.02\%$	$0$	50MA, W50GM	$\approx 0$	50MA	$\lvert <2 \cdot 10^{-3} \rvert$	50MA, W50GM
${}_{34}\mathrm{Se}$	$77$	$7.58\%$	$1/2$	50MA, W50GM, B51DJ, N51CH, B54DV	$0.53326 \pm 5$	R52DW, R53WV	$\lvert <2 \cdot 10^{-3} \rvert$	50MA, W50GM
${}_{34}\mathrm{Se}$	$78$	$23.5\%$	$0$	50MA, W50GM, B54DV, B51DJ	$\approx 0$	50MA	$\lvert <2 \cdot 10^{-3} \rvert$	50MA, W50GM
${}_{34}\mathrm{Se}$	$79^{+}$	$<6.5 \cdot 10^{4}\ \mathrm{y}$	$7/2$	W52HS, W53HS	$-1.015 \pm 15$	W53HS	$0.7 \pm 1$	W52HS, W53HS, W54BT
${}_{34}\mathrm{Se}$	$80$	$49.82\%$	$0$	50MA, W50GM, B54DV	$\approx 0$	50MA	$\lvert <2 \cdot 10^{-3} \rvert$	50MA, W50GM
${}_{34}\mathrm{Se}$	$81^{+}$	$17.5\ \mathrm{min}$	$1/2$	T51GS, N52GH
${}_{34}\mathrm{Se}$	$82$	$9.19\%$	$0$	50MA, W50GM	$\approx 0$	50MA	$\lvert <2 \cdot 10^{-3} \rvert$	W50GM
${}_{34}\mathrm{Se}$	$83^{+}$	$25\ \mathrm{min}$	$(7/2);\ 9/2$	T49FN
${}_{34}\mathrm{Se}$		$\nu_{77}/\nu_{\mathrm D}=1.24211 \pm 10$		R53WA	$\nu_{77}/\nu_{\mathrm{Na}^{23}}=0.72193 \pm 2$	R52DW, R53WV

Table of nuclear moments


$_{35}\mathrm{Br}$	79	50.40%	3/2	50MA, W50ST, A54KJ	$2.105\ 74 \pm 10$ cor	50MA, R51SW, A54KJ	$0.33 \pm 2$ cor	50MA, (T51SR), T52SR), Q51DH, T51GO, A54KJ
$_{35}\mathrm{Br}$	$80^{+}$	18.0 min	1	T51GS, N53SK
$_{35}\mathrm{Br}$	81	49.59%	3/2	50MA, W50ST, A54KJ	$2.269\ 47 \pm 13$ cor	50MA, R51SW, A54KJ	$0.28 \pm 2$ cor	50MA, (T51SR, T52SR), Q51DH, T51GO, A54KJ
$_{35}\mathrm{Br}$	$83^{+}$	2.30 h	3/2	T49FH, N53SW
$_{35}\mathrm{Br}$	$87^{+}$	185 s	(3/2)	N53SS
$_{35}\mathrm{Br}$	?	?			1.8	S51RN	0.28	S51RN
$_{35}\mathrm{Br}$		$\mu_{81}/\mu_{79}=1.077\ 938 \pm 20$ R51SW, R53WH, A54KJ			$Q_{79}/Q_{81}=1.197\ 07 \pm 3$ Q51DH, Q53KT, Q53MW, E53CL, Q54BB, Q54DR, A54KJ, Q54DB, Q54SC
$_{35}\mathrm{Br}$		$\nu_{79}/\nu_{\mathrm{Sc}^{45}}=1.031\ 45 \pm 5$ R51SW			$\nu_{81}/\nu_{\mathrm{Sc}^{45}}=1.111\ 65 \pm 6$ R51SW
$_{36}\mathrm{Kr}$	$77^{+}$	1.1 h	9/2	T52DA	$-1.61 \pm 14$	T52DA
$_{36}\mathrm{Kr}$	$79^{+}$	34.5 h	(1/2)	T51GS, N52BS
$_{36}\mathrm{Kr}$	$81^{+}$	$2.1\cdot 10^{5}$ yr	(7/2)	T51GS, N52GH
$_{36}\mathrm{Kr}$	82	11.56%	(0)	50MA	$\approx 0$	50MA
$_{36}\mathrm{Kr}$	83	11.55%	9/2	50MA	$-0.967\ 06 \pm 4^{**})$	50MA, R54BR	0.16 cor	50MA, (T52SR)
$_{36}\mathrm{Kr}$	84	56.90%	(0)	50MA	$\approx 0$	50MA
$_{36}\mathrm{Kr}$	$85^{+}$	10.27 yr	1/2; 9/2	T51GS, N52BS
$_{36}\mathrm{Kr}$	86	17.37%	(0)	50MA	$\approx 0$	50MA
$_{36}\mathrm{Kr}$	$87^{+}$	78 min	(5/2)	N52TH, T52DA	$-0.58 \pm 11$	T52DA
$_{37}\mathrm{Rb}$	$82^{+}$	6.4 h	(3)	N52HM
$_{37}\mathrm{Rb}$	$84^{+}$	36 d	(2)	N53HP
$_{37}\mathrm{Rb}$	85	72.8%	5/2	50MA	$1.353\ 2 \pm 4$ cor	50MA	(0.33)	T52WB
$_{37}\mathrm{Rb}$	$86^{+}$	19.5 d	2	A51BL, A53SB N50MR, N54PL	$-1.69 \pm 1$	A51BL, A53SB

*) Adopted $I=9/2$.

**) The indication in R54BR that $\mu>0$ is probably a misprint. All preceding works (50MA) consistently indicate $\mu<0$.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\,\mathrm{cm}^2)$	Literature data
${}_{37}\mathrm{Rb}$	$87+$	$6.25\cdot 10^{10}$ y	$3/2$	50MA, N52CD	$2.749\,37 \pm 19$ corr	50MA, R51SW	$(0.170)$	49GH, T52WB T52PI
${}_{37}\mathrm{Rb}$	$88+$	$17.8$	$2$	N52TL
${}_{37}\mathrm{Rb}$				$\mu_{87}/\mu_{85}=2.033\,390\,5\pm75$ R51AB, R51YS, A52OK			$Q_{85}/Q_{87}=2.07\pm1$ E50HG
${}_{37}\mathrm{Rb}$				$\nu_{\mathrm{H}}/\nu_{85}=10.357\,105\pm30$ R51YS, R52WL			$\nu_{\mathrm{H}}/\nu_{87}=3.0561\,097\pm55$ R51YS, R51WL, R51WS
${}_{37}\mathrm{Rb}$				$\nu_{85}/\nu_{\mathrm{Cl}^{35}}=0.985\,41\pm15$ R52WL			$\nu_{87}/\nu_{\mathrm{Al}^{27}}=1.255\,29\pm6$ R51SW
${}_{37}\mathrm{Rb}$				$\nu_{\mathrm{V}^{50}}/\nu_{85}=1.032\,62\pm10$ R52WL			$\nu_{\mathrm{B}^{10}}/\nu_{85}=1.112\,82\pm5$ R53TW
${}_{37}\mathrm{Rb}$				$\nu_{\mathrm{N}^{14}}/\nu_{85}=0.748\,37\pm4$ R53TW
${}_{38}\mathrm{Sr}$	$85+$	$65$ d	$9/2$	N52SM
${}_{38}\mathrm{Sr}$	$86$	$9.75\%$	$(0)$	50MA	$\approx 0$	50MA
${}_{38}\mathrm{Sr}$	$87$	$6.96\%$	$9/2$	50MA	$-1.089\,2\pm15$	50MA, R53JS	$0.85$	T52WB
${}_{38}\mathrm{Sr}$	$88$	$82.7\%$	$(0)$	50MA	$\approx 0$	50MA
${}_{38}\mathrm{Sr}$	$89+$	$54.5$ d	$5/2$	T49FH, T50FE, T52DA, N52GH	$-0.58\pm11$	T52DA
${}_{38}\mathrm{Sr}$	$90+$	$19.9$ y	$0$	T50FE
${}_{38}\mathrm{Sr}$	$91+$	$9.67$ h	$5/2$	T50FE, N53SP
${}_{38}\mathrm{Sr}$				$\nu_{87}/\nu_{\mathrm{D}}=0.282\,32\pm3$ R53JS

Table of nuclear moments

Element	Mass number	Half-life or abundance	Spin	References	Moment	References	Moment	References
$_{39}\mathrm{Y}$	$87^{+}$	80 h	$(1/2)$	T51GS, N51MA
$_{39}\mathrm{Y}$	$88^{+}$	105 d	4	N51BL
$_{39}\mathrm{Y}$	89	100%	$1/2$	50MA, S50KW	$-0.136\ 825 \pm 4$	50MA, S50KW, R54BO
$_{39}\mathrm{Y}$	$90^{+}$	60.5 h	2	T52MA, T53SK, N49BS, T50FE		T53SK
$_{39}\mathrm{Y}$	$91^{+}$	61 d	$1/2$	T50FE, T51GS, N54BM
$_{39}\mathrm{Y}$				$\gamma_{9/2}^{H}=0.048\ 994 \pm 1$ R54BO
$_{40}\mathrm{Zr}$	$89^{+}$	79.7 h	$9/2$	T51GS, N51SB
$_{40}\mathrm{Zr}$	91	11.2%	$5/2$	50MA	$-1.3 \pm 3$	S52SU, S53SU	$-0.46$	T52WB
$_{40}\mathrm{Zr}$	$93^{+}$	$9.5 \cdot 10^{5}$ yr	$(5/2)$	N53HP
$_{40}\mathrm{Zr}$	$95^{+}$	65 d	$(5/2)$	N53CA
$_{41}\mathrm{Nb}$	$89^{+*}$	0.8 h	$(1/2)$	N54DM
$_{41}\mathrm{Nb}$	$89^{+*}$	1.9 h	$(9/2)$	N54DM
$_{41}\mathrm{Nb}$	$91^{+}$	$\approx 8$ yr	$(1/2)$	T51GS, N52GH
$_{41}\mathrm{Nb}$	$92^{+}$	10.0 d	2	T52MA
$_{41}\mathrm{Nb}$	93	100%	$9/2$	50MA	$6.166\ 70$ $\pm 30$ corr.	50MA, R50SH, R51SW	$\approx 0$	50MA, T52WB

*) It is still unclear which of the states is the ground state.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(t_i)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\,\mathrm{cm}^2)$	Literature data
${}_{41}\mathrm{Nb}$	$94^{\dagger}$	$2.2\cdot 10^4$ yr	$(6; 7)$	N52GH
${}_{41}\mathrm{Nb}$	$95^{\dagger}$	35 d	$9/2$	T51GS, N51SP
${}_{41}\mathrm{Nb}$	$97^{\dagger}$	72.1 min	$9/2$	T51GS, N52GH
${}_{41}\mathrm{Nb}$		$\nu_{93}/\nu_{\mathrm{B}^{11}}=0.761\,87\pm40$	R50SH			$\nu_{93}/\nu_{45}=1.006\,13\pm5$ R51SW
${}_{42}\mathrm{Mo}$	92	15.8%	$(0)$	50MA	$\approx 0$	50MA
${}_{42}\mathrm{Mo}$	$93^{\dagger}$	$>2$ yr	$(7/2)$	T52DA, N53KH	$0.83\pm6$	T52DA
${}_{42}\mathrm{Mo}$	94	9.04%	$(0)$	50MA	$\approx 0$	50MA
${}_{42}\mathrm{Mo}$	95	15.72%	$5/2$	50MA, S50AE, S50AO, S50MK, R51PY, S54WO, N51SP	$-0.909\,8\pm2$	R51PY, S54WO
${}_{42}\mathrm{Mo}$	96	16.53%	$(0)$	50MA	$\approx 0$	50MA
${}_{42}\mathrm{Mo}$	97	9.46%	$5/2$	50MA, S50AE, S50AO, R51PY, S54WO	$-0.928\,9\pm2$	R51PY, S54WO	$(0.50)$	T52WB
${}_{42}\mathrm{Mo}$	98	23.78%	$(0)$	50MA	$\approx 0$	50MA
${}_{42}\mathrm{Mo}$	$99^{\dagger}$	67 h	$1/2$	N54CK
${}_{42}\mathrm{Mo}$	100	9.63%	$(0)$	50MA	$\approx 0$	50MA
${}_{42}\mathrm{Mo}$		$\nu_{97}/\nu_{95}=1.021\,0\pm1$	R51PY, S51MC, S54WO			$\lvert Q_{97}/Q_{95}\rvert>1$ R51PY
${}_{42}\mathrm{Mo}$		$\nu_{97}/\nu_{\mathrm{N}^{14}}=0.920\,8\pm1$	R51PY

Table of nuclear moments

Element	Isotope	Half-life or abundance	Spin	References	Value	References	Value	References
$^{43}\mathrm{Tc}$	$93^{+}$	2.7 h	$(9/2)$	N54LN
$^{43}\mathrm{Tc}$	$94^{+}$	52.5 min	$(3)$	N50MP
$^{43}\mathrm{Tc}$	$95^{+}$	20 h	$(9/2)$	T51GS, N50MP
$^{43}\mathrm{Tc}$	$96^{+}$	104 h	$(3; 5; 6); 7$	N53EM
$^{43}\mathrm{Tc}$	$97^{+}$	$>10^{4}$ yr	$9/2$	T51GS, N54BY
$^{43}\mathrm{Tc}$	$99^{+}$	$2.12\cdot10^{5}$ yr	$9/2$	S53MT	$5.6805 \pm 4$ cor	R52WA, S53MT, (T52KL)	$0.34 \pm 34$ *)	S53MT
$^{44}\mathrm{Ru}$	$95^{+}$	1.65 h	$5/2,\ 7/2$	T52DA		T52DA
$^{44}\mathrm{Ru}$	99	12.8%	$5/2$	N52GH, X52GO, S53MU	$<0$	S53MU	$(-0.84)$	T52WB
$^{44}\mathrm{Ru}$	101	16.98%	$5/2$	X52GO, S53MU	$<0$	S53MU
$^{44}\mathrm{Ru}$	$103^{+}$	39.8 d	$(5/2)$	T49FH, N52CM
$^{44}\mathrm{Ru}$	$105^{+}$	4.4 h	$(1/2)$	N52GH
$^{44}\mathrm{Ru}$		$\mu_{101}/\mu_{99}=1.09\pm3$	X52GO
$^{45}\mathrm{Rh}$	103	100%	$1/2$	50MA, S51KW	$\approx -0.10\pm3$	50MA, S51KW, T52BE
$^{45}\mathrm{Rh}$	$104^{+}$	42 s	1	N53JC
$^{45}\mathrm{Rh}$	$105^{+}$	36.5 h	$(7/2)$	N52GH
$^{45}\mathrm{Rh}$	$106^{+}$	30 s	1	N52GH

*) Small $Q<0$ are not excluded.

$Z$	$A$	p% or $T_{1/2}$	$I$ $(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data
${}_{46}\mathrm{Pd}$	$103^\dagger$	15.5 d	$5/2$	N54RB
${}_{46}\mathrm{Pd}$	105	22.2%	$5/2$	S52ST, S53BC	$-0.57 \pm 5$	S52ST, S53BC
${}_{46}\mathrm{Pd}$	$107^\dagger$	$7 \cdot 10^6$ y	$(5/2)$	N52GH
${}_{46}\mathrm{Pd}$	$109^\dagger$	13.1 h	$(5/2)$	N52GH
${}_{46}\mathrm{Pd}$	$111^\dagger$	26 min	$5/2;\ (1/2)$	N51GN
${}_{47}\mathrm{Ag}$	$103^\dagger$	66 min	$1/2$	N54HW
${}_{47}\mathrm{Ag}$	$106^\dagger$	24 min	1	N53BS
${}_{47}\mathrm{Ag}$	107	51.35%	$1/2$	50MA, S50CK	$-0.113\ 014 \pm 4$	50MA, S50CK, S51BK, A53LW, R54BO, R54JS
${}_{47}\mathrm{Ag}$	$108^\dagger$	2.44 min	1	N53PB
${}_{47}\mathrm{Ag}$	109	48.65%	$1/2$	50MA, S50CK	$-0.129\ 924 \pm 4$	50MA, S50CK, S51BK, A53LW, R54BO, R54JS
${}_{47}\mathrm{Ag}$	$110^\dagger$	24 s	$(1)$	T51GS, N52GH
${}_{47}\mathrm{Ag}$	$111^\dagger$	181 h	$1/2$	N51GN, A54LP	$\lvert 0.144 \pm 7 \rvert$	A54LP
${}_{47}\mathrm{Ag}$	$112^\dagger$	3.2 h	2	N53NW
${}_{47}\mathrm{Ag}$	$113^\dagger$	5.3 h	$(1/2)$	N52GH
${}_{47}\mathrm{Ag}$	$115^\dagger$	20 min	$(1/2)$	N52GH
${}_{47}\mathrm{Ag}$	$\gamma_{109}/\gamma_{107}$	$\begin{cases}=1.149\ 61 \pm 4\ \text{(in metal)}\\=1.149\ 62 \pm 4\ \text{(in } \mathrm{AgNO}_3 \text{ in } \mathrm{H}_2\mathrm{O}\text{)}\end{cases}$				S51BK, R54JS, R54BO

\[ \frac{\nu_{107}}{\nu_{\mathrm H}} \begin{cases} = 0.040\,684 \pm 1 \quad \text{(in the metal)}\\ = 0.040\,468 \pm 1 \quad \text{(in AgNO}_3 \text{ in H}_2\text{O)} \end{cases} \qquad \text{R54BO} \]

\[ \frac{\nu_{109}}{\nu_{\mathrm H}} \begin{cases} = 0.046\,771 \pm 1 \quad \text{(in the metal)}\\ = 0.046\,533 \pm 1 \quad \text{(in AgNO}_3 \text{ in H}_2\text{O)} \end{cases} \qquad \text{R54BO} \]

\[ \frac{\nu_{109}}{\nu_{\mathrm D}} = 0.303\,16 \pm 3 \qquad \text{R54JS} \]

Table of Nuclear Moments

Element	Isotope	Abundance or half-life	Spin	Reference	Moment	Reference
$_{48}\mathrm{Cd}$	$107^{\dagger}$	6.7 h	$5/2;$ $7/2$	N52GH
$_{48}\mathrm{Cd}$	$109^{\dagger}$	470 d	$3/2;$ $(5/2)$	T49FH
$_{48}\mathrm{Cd}$	110	12.39%	$(0)$	50MA	$\approx 0$	50MA
$_{48}\mathrm{Cd}$	111	12.75%	$1/2$	50MA, R50PY, N50SR	$-0.592\,3 \pm 1$	50MA, R50PY
$_{48}\mathrm{Cd}$	112	24.07%	$(0)$	50MA	$\approx 0$	50MA
$_{48}\mathrm{Cd}$	113	12.3% ($>10^3$ y)	$1/2$	50MA, R50PY	$-0.619\,6 \pm 1$	50MA, R50PY
$_{48}\mathrm{Cd}$	114	28.86%	$(0)$	50MA	$\approx 0$	50MA
$_{48}\mathrm{Cd}$	$115^{\dagger}$	52.6 h	$1/2$	N52GH
$_{48}\mathrm{Cd}$	116	7.58%	$(0)$	50MA	$\approx 0$	50MA
$_{48}\mathrm{Cd}$	$117^{\dagger}$	2.83 h	$(1/2)$	N52GH

\[ \frac{\nu_{113}}{\nu_{111}} = 1.046\,1 \pm 1 \quad \text{R50PY} \qquad\qquad \frac{\nu_{111}}{\nu_{\mathrm{Na}^{23}}} = 0.801\,6 \pm 1 \quad \text{R50PY} \]

\[ \frac{\nu_{113}}{\nu_{\mathrm{Na}^{23}}} = 0.838\,6 \pm 1 \quad \text{R50PY} \]

Element	Isotope	Abundance or half-life	Spin	Reference
$_{49}\mathrm{In}$	$110^{\dagger}$	9 min	$(1)$	N52GH
$_{49}\mathrm{In}$	$111^{\dagger}$	2.84 d	$9/2$	N51GN
$_{49}\mathrm{In}$	$112^{\dagger}$	14.5 min	$(1)$	N52GH

$Z$	$A$	p% or $T_{1/2}$	$I$ $(\hbar)$	Literature data	$\mu$ nuclear magnet.	Literature data	$Q$ $(e \cdot 10^{-24}\,\text{cm}^2)$	Literature data
${}_{49}\mathrm{In}$	$113^{+}$	$4,23\%$ $(>10^{12}\ \text{yr})$	$9/2$	50MA	$5,522\ 2$ $\pm 5$ corr.	50MA, R51PY, R53TW	$1,181$ corr.	50MA, (T50SR, T52SR), T52KO
${}_{49}\mathrm{In}$	$114^{+}$	$72\ \text{s}$	$1$	N52GH
${}_{49}\mathrm{In}$	$115^{+*}$	$95,77\%$ $(6 \cdot 10^{14}\ \text{yr})$	$9/2$	50MA	$5,533\ 9 \pm 4$	50MA, R51PY, R52TB, R53TW,	$1,198$ corr.	50MA, (T50SR, T52SR), T52KO
${}_{49}\mathrm{In}$	$116^{+}$	$13\ \text{s}$	$(1)$	N52GH
${}_{49}\mathrm{In}$	$117^{+}$	$1,95\ \text{h}$	$(1/2)$	N52GH
${}_{49}\mathrm{In}$				$\mu_{115}/\mu_{113}=1,002\ 13 \pm 4$ corr. R51PY, R53TW $\nu_{115}/\nu_{\mathrm{Sc}^{45}}=0,901\ 877 \pm 50$ R52TB, R53TW			$Q_{115}/Q_{113}=1,014\ 6$ A50KM $\nu_{113}/\nu_{\mathrm{Na}^{23}}=0,826\ 67 \pm 8$ R51PY $\nu_{115}/\nu_{\mathrm{Na}^{23}}=0,828\ 41 \pm 8$ R51PY
${}_{50}\mathrm{Sn}$	$111^{+}$	$35,0\ \text{min}$	$7/2;$ $9/2;$ $11/2$	N51GN				.
${}_{50}\mathrm{Sn}$	$115$	$0,34\%$	$1/2$	50MA, R50PY	$-0,913\ 4 \pm 2$	50MA, R50PY
${}_{50}\mathrm{Sn}$	$116$	$14,2\%$	$(0)$	50MA	$\approx 0$	50MA
${}_{50}\mathrm{Sn}$	$117$	$7,57\%$	$1/2$	50MA, R50PY	$-0,995\ 1 \pm 2$	50MA, R50PY
${}_{50}\mathrm{Sn}$	$118$	$24,0\%$	$(0)$	50MA	$\approx 0$	50MA
${}_{50}\mathrm{Sn}$	$119$	$8,58\%$	$1/2$	50MA, R50PY	$-1,041\ 1 \pm 2$	50MA, R50PY
${}_{50}\mathrm{Sn}$	$120$	$33,0\%$	$(0)$	50MA	$\approx 0$	50MA

Table of Nuclear Moments

A	Half-life or abundance	Spin	References
$121^{+}$	27,5 h	$3/2$	50ND **)
$123^{+}$ ***)	126 d	$(11/2)$	N52GH
$123^{+}$ ***)	40,0 min	$3/2$	N52GH
$125^{+}$	9,8 min	$(11/2)$	N52GH

\[ \nu_{117}/\nu_{115}=1,089\,4 \pm 1 \ \mathrm{R50PY} \]

\[ \nu_{115}/\nu_{\mathrm{Na}^{23}}=1,236\,2 \pm 1 \ \mathrm{R50PY} \]

\[ \nu_{119}/\nu_{\mathrm{Na}^{23}}=1,409\,0 \pm 1 \ \mathrm{R50PY} \]

\[ \nu_{119}/\nu_{117}=1,046\,5 \pm 1 \ \mathrm{R50PY} \]

\[ \nu_{117}/\nu_{\mathrm{Na}^{23}}=1,346\,8 \pm 1 \ \mathrm{R50PY} \]

Element	A	Half-life or abundance	Spin	References		References		References
${}_{51}\mathrm{Sb}$	$117^{+}$	2,8 h	$(5/2)$	N52GH
	121	57,3%	$5/2$	50MA, W51LS	$3,359\,5$ $\pm 4$ cor	50MA, R50PU, R50CK, R50CL, R51PY, (T52KL)	$-0,52 \pm 10$	50MA, (T52SR), W51LS, S53ST, S54MW
	$122^{+}$	2,80 d	2	T52MA, N52GH
	123	42,8%	$7/2$	50MA, W51LS	$2,547\,0$ $\pm 3$ cor	50MA, R50CK, R50PU, R51PY, (T52KL)	$-0,67 \pm 10$	50MA, (T52SR), W51LS, S53ST, S54MW
	$124^{+}$	60 d	$(3;4)$	T51GS, T53SK, N53MZ, N54LZ		T53SK
	$125^{+}$	2,7 y	$7/2$	N52GH

\[ \nu_{121}/\nu_{123}=1,319\,1 \pm 1 \ \mathrm{R50CK,\ \mathbf{R50PU},\ R51PY} \]

\[ \nu_{121}/\nu_{\mathrm{Na}^{23}}=0,904\,69 \pm 4 \ \mathrm{R50CL,\ \mathbf{R50CK},\ R50PU,\ R51PY} \]

\[ \nu_{123}/\nu_{\mathrm{D}}=0,844\,23 \pm 8 \ \mathrm{R50CK,\ \mathbf{R50PU},\ R51PY} \]

\[ Q_{123}/Q_{121}=1,275\,1 \pm 2 \ \mathrm{\mathbf{Q51DK},\ W51LS,\ S54MW,\ W54WT^{****})} \]

) An octupole moment exists, A54KE.
) p. 33.
) It is still unclear which of the states is the ground state.
**) W54WT gives refined values for different molecules.

$Z$	$A$	$p\%$ or $t_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{52}\mathrm{Te}$	$121^{+}$	17 d	$1/2$	N52GH
${}_{52}\mathrm{Te}$	123	0.87%	$1/2$	50MA, S50FW, N49HL	$-0.731\ 88 \pm 4$	R51DV; S52RM, S53WV
${}_{52}\mathrm{Te}$	125	6.99%	$1/2$	50MA, S50FW	$-0.882\ 35 \pm 4$	R51DV, S52RM, R53WV
${}_{52}\mathrm{Te}$	126	18.72%	(0)	50MA	$\approx 0$	50MA
${}_{52}\mathrm{Te}$	$127^{+}$	9.3 h	$(3/2)$	T51GS, N52GH	0.8	T49BE
${}_{52}\mathrm{Te}$	128	31.79%	(0)	50MA	$\approx 0$	50MA
${}_{52}\mathrm{Te}$	$129^{+}$	72 min	$(3/2)$	N52GH	0.8	T49BE
${}_{52}\mathrm{Te}$	130	34.49%	(0)	50MA	$\approx 0$	50MA
${}_{52}\mathrm{Te}$	$131^{+}$	24.8 min	$(3/2)$	N53HP	0.8	T49BE
${}_{52}\mathrm{Te}$	$133^{+}$	$\approx 2$ min	$(3/2)$	N52PP
${}_{52}\mathrm{Te}$		$\nu_{125}/\nu_{123}=1.205\ 60 \pm 7$		S50FW, R51DV, S52RM, R53WV.
${}_{52}\mathrm{Te}$		$\nu_{123}/\nu_{\mathrm{Na}^{23}}=0.990\ 85 \pm 3$		R51DV, R53WV		$\nu_{125}/\nu_{\mathrm{Na}^{23}}=1.194\ 57 \pm 4$ R51DV, R53WV
${}_{53}\mathrm{I}$	$125^{+}$	60 d	$(5/2;\ 7/2)$	N52BS
${}_{53}\mathrm{I}$	$126^{+}$	13 d	2	N54PW
${}_{53}\mathrm{I}$	127*)	100%	$5/2$	50MA, A53JS	$2.808\ 38 \pm 13\ \mathrm{cor}$	50MA, R51WL, R51YS, R51SW	$-0.75 \pm 2\ \mathrm{cor}^{**})$	50MA, (T52SR) T51GO, Q52KE S54MZ

TABLE OF NUCLEAR MOMENTS

Isotope	Half-life or abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
$129^{+}$	$1.72\cdot 10^{7}$ yr	$7/2$	50MA	$2.617\ 3\pm3$ agree.	50MA, R51WL	$-0.47$	50MA, (T52SR), T51GO
$130^{+}$	12.6 h	6	N54CM
$131^{+}$	8.14 d	$7/2$	W53LB, N52BR			$-0.412^{***}$	W53LB
$133^{+}$	22.4 h	$(7/2)$	N52GH

\[ \mu_{127}/\mu_{129}=1.0732 \quad \text{agree. R51WL} \]

\[ \nu_{\mathrm H}/\nu_{127}=4.997\ 63\pm15\ \mathrm{R51YS} \]

\[ \nu_{129}/\nu_{\mathrm D}=0.867\ 44\pm1\ \mathrm{R51WL} \]

\[ Q_{129}/Q_{127}=0.701\ 213\pm15\ \mathrm{Q53LZ} \]

\[ Q_{131}/Q_{127}=0.5031\ \mathrm{W53LB} \]

\[ \nu_{127}/\nu_{\mathrm D}=1.303\ 37\pm2\ \mathrm{R51SW,\ R51WL} \]

Element	Isotope	Half-life or abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
${}_{54}\mathrm{Xe}$	$127^{+}$	32 d	$1/2$	T51GS
${}_{54}\mathrm{Xe}$	129	26.44%	$1/2$	50MA, S50KR	$-0.772\ 55\pm5$	50MA, R50PU, R51PY, R54BS
${}_{54}\mathrm{Xe}$	131	21.18%	$3/2$	50MR, S50KR, N54SF	$0.686\ 80\pm2$	50MA, R54BS	$-0.12$ agree.	50MA, S50KR, S52BK
${}_{54}\mathrm{Xe}$	132	26.89%	$(0)$	50MA	$\approx 0$	50MA
${}_{54}\mathrm{Xe}$	$133^{+}$	5.27 d	$3/2,\ 9/2,\ 11/2$	T51GS, N52BS
${}_{54}\mathrm{Xe}$	134	10.44%	$(0)$	50MA	$\approx 0$	50MA
${}_{54}\mathrm{Xe}$	$135^{+}$	9.15 h	$3/2$	T51GS, N52GH
${}_{54}\mathrm{Xe}$	136	8.87%	$(0)$	50MA	$\approx 0$	50MA

\[ \nu_{129}/\nu_{131}=-1.124\ 85\pm2\ \mathrm{S52BK,\ R54BS} \]

\[ \nu_{129}/\nu_{\mathrm{Na}^{23}}=1.045\ 7\pm1\ \mathrm{R50PU,\ R51PY} \]

\[ \nu_{129}/\nu_{\mathrm H}=0.276\ 633\pm5\ \mathrm{R54BS} \]

\[ \nu_{131}/\nu_{\mathrm H}=0.081\ 976\pm1\ \mathrm{R54BS} \]

) Octupole moment: $0.3$ nuclear magnetons $\cdot 10^{-24}\ \mathrm{cm}^{2}$, A54JK.
) Refined value, see ).
*) With $Q_{127}=-0.819\cdot 10^{-24}\ \mathrm{cm}^{2}$ (Jaccarino, King, Stroke, unpublished), one obtains $Q_{131}/Q_{127}=0.5031$.

Z	A	p% or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e \cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{55}\mathrm{Cs}$	$127+$	6.1 h	$(5/2)$	N53WP
${}_{55}\mathrm{Cs}$	$129+$	31 h	$(5/2)$	N53WP
${}_{55}\mathrm{Cs}$	$130+$	30 min	1	N52SB
${}_{55}\mathrm{Cs}$	$131+$	9.6 d	$(5/2)$	A53SB, N52GH	$3.48 \pm 4$	A53SB
${}_{55}\mathrm{Cs}$	133	100%	$(7/2)$	50MA *)	$2.578\,77 \pm 12$ cor	50MA *) R51SW	$-0.003$	50MA, D54AK
${}_{55}\mathrm{Cs}$	$134+$	2.3 yr	4	Z52JB, A53SB	$2.96 \pm 1$	Z52JB, A53SB
${}_{55}\mathrm{Cs}$	$134^n$	3.1 h	8	A54CG, A54GW	$\lvert 1.10 \pm 1\rvert$	A54CG, A54GW
${}_{55}\mathrm{Cs}$	$135+$	$2.1 \cdot 10^6$ yr	$7/2$	50MA, N52GH, N54SF	$2.727\,1 \pm 33$ cor	50MA
${}_{55}\mathrm{Cs}$	$137+$	33 yr	$7/2$	50MA, N49PM	$2.839\,7 \pm 30$ cor	50MA	$\ll 0.2$	49GH

\[ \gamma_{133}/\gamma_D = 0.854\,49 \pm 4 \quad \text{R51SW} \]

Z	A	p% or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e \cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{56}\mathrm{Ba}$	$133+$	$\approx 10$ yr	$1/2$	T51GS, N52GH,
${}_{56}\mathrm{Ba}$	134	2.42%	$(0)$	50MA	$\approx 0$	50MA
${}_{56}\mathrm{Ba}$	135	6.59%	$3/2$	50MA, S50AR	$0.834\,6 \pm 25$ cor	50MA	$(0.51)$	T52WB
${}_{56}\mathrm{Ba}$	136	7.81%	$(0)$	50MA	$\approx 0$	50MA
${}_{56}\mathrm{Ba}$	137	11.32%	$3/2$	50MA, S50AR	$0.935\,1 \pm 27$ cor	50MA	$(0.51)$	T52WB
${}_{56}\mathrm{Ba}$	138	71.66%	$(0)$	50MA	$\approx 0$	50MA

\[ \lvert Q_{137}/Q_{135}\rvert < 1 \quad \text{T54BD} \]


${}^{57}\mathrm{La}$	$135^{+}$	19 h	$(5/2)$	N53WP
${}^{57}\mathrm{La}$	$138^{+}$	$2.0\cdot 10^{11}$ yr	5	N52MK
${}^{57}\mathrm{La}$	139	99.9%	$7/2$	50MA	$2.77802 \pm 18$ corr.	50MA, R51SW	$0.9 \pm 1$	49GH, 50MA, S53MW
${}^{57}\mathrm{La}$	$140^{+}$	40.0 h	3	N53HP
${}^{57}\mathrm{La}$	$141^{+}$	3.6 h	$5/2;\ 7/2$	N51DL
${}^{57}\mathrm{La}$		$\gamma_{139}/\gamma_D = 0.920$	$25 \pm 6$	R51SW
${}^{58}\mathrm{Ce}$	$141^{+}$	33.1 d	$7/2$	N51DL
${}^{58}\mathrm{Ce}$	$143^{+}$	33 h	$(5/2;\ 7/2;\ 9/2)$	N51KH
${}^{59}\mathrm{Pr}$	$140^{+}$	3.4 min	1	N52BR
${}^{59}\mathrm{Pr}$	141	100%	$5/2$	50MA, X51DK, X52BE	$3.9 \pm 3$ corr.	50MA, R50WS, (R51WS) A53LH, T53BX, S54MS	$-0.054$	A53LH, S54MS
${}^{59}\mathrm{Pr}$	$142^{+}$	19.2 h	2	N54PL
${}^{59}\mathrm{Pr}$	$143^{+}$	13.6 d	$7/2$	N51KH
${}^{59}\mathrm{Pr}$	$144^{+}$	17.5 min	1; 0	N52AK, N52PC,
${}^{59}\mathrm{Pr}$	$146^{+}$	24.4 min	3	N54BK

*) According to measurements by V. G. Hartmann with the participation of A. G. Kucheryaev and Yu. K. Sazhenov (1951), by method Z.

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(h)$	Literature data	$\mu$ nuclear magn.	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{60}\mathrm{Nd}$	142	27,09%	0	X50BE
${}_{60}\mathrm{Nd}$	143	12,14%	7/2	S51MU, X51BE, X50BE	$-1,0 \pm 2$ cor	S51MU, (T52KL), T51ES, (T53ES), X54BE	$\lvert 1\rvert$	X52BA, T52WB, T51ES, (T53ES), X54BE
${}_{60}\mathrm{Nd}$	144	23,83%	0	X50BE
${}_{60}\mathrm{Nd}$	145	8,29%	7/2	S51MU, X51BE, X50BE	$-0,65 \pm 9$ cor	S51MU, (T52KL), T51ES, (T53ES), X54BE	$\lvert 1\rvert$	X52BA, T51ES, (T53ES), X54KL
${}_{60}\mathrm{Nd}$	146	17,26%	0	X50BE
${}_{60}\mathrm{Nd}$	148	5,74%	0	X50BE
${}_{60}\mathrm{Nd}$	150	$>2\cdot 10^{15}$ yr 5,63%	0	X50BE

$\mu_{143}/\mu_{145}=1,608\ 3 \pm 12$ X50BE, X51BE, S51MU, X54BE

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(h)$	Literature data	$\mu$ nuclear magn.	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{62}\mathrm{Sm}$	144	2,87%	0	X52BL
${}_{62}\mathrm{Sm}$	$147+$	14,94% $1,3\cdot 10^{11}$ yr	7/2	50MA, S51MU, X52BL, T52ES, S54MW	$-0,76 \pm 8$	S51MU, (T52KL), T52ES, (T53ES), S54MW	$\lvert <0,72\rvert$	T52ES, (T53ES), S54MW
${}_{62}\mathrm{Sm}$	148	11,24%	0	X52BL

TABLE OF NUCLEAR MOMENTS


	149	13.85%	7/2	50MA, S51MU, X52BL, T52ES, S54MW	$-0.64 \pm 6$	S51MU, (T52KL), T52ES, (T53ES), S54MW	$\lvert <0.72 \rvert$	T52ES, (T53ES), S54MW
	150	7.36%	0	X52BL
	152	26.90%	0	X52BL
	154	22.84%	0	X52BL
				$\mu_{147}/\mu_{149} = 1.222 \pm 8$ S51MU, X52BL, S54MW		$\lvert Q_{149}/Q_{147} \rvert > 1$ T54BD
${}_{63}\mathrm{Eu}$	151	47.77%	5/2	50MA	3.6 agr.	50MA, (T52KL)	1.2 agr.	50MA, (T50SR, T52SR)
${}_{63}\mathrm{Eu}$	153	52.23%	5/2	50MA, N53KL	1.6 agr.	50MA, (T52KL)	2.6 agr.	50MA, (T50SR, T52SR)
				$\lvert \mu_{153}/\mu_{151} \rvert = 0.443$ T52BR		$\lvert Q_{153}/Q_{151} \rvert = 2.0$ T52BR
${}_{64}\mathrm{Gd}$	155	14.73%	$>3/2$	S52SU, T52ES	$\lvert 0.25 \pm 15 \rvert$	S52SU
${}_{64}\mathrm{Gd}$	157	15.68%	$>3/2$	S52SU, T52ES	$\lvert 0.3 \pm 2 \rvert$	S52SU	$-1.56$	T52WB
${}_{64}\mathrm{Gd}$	159+	18.0 h	(7/2)	T52ES, N53JD
${}_{65}\mathrm{Tb}$	159	100%	3/2	50MA	$\begin{array}{r}0.45\\ 1.0\end{array}\ \Bigg\}$	$\begin{array}{r}\text{T52BE}\\ \text{T50RI}\end{array}\ \Bigg\}$	$(-0.42)$	T52WB
${}_{66}\mathrm{Dy}$	161	18.73%	(7/2)	S53MW, T52ES
${}_{66}\mathrm{Dy}$	163	24.91%	(7/2)	S53MW, T52ES,
${}_{66}\mathrm{Dy}$	165+	139 min	7/2	T51GS, T52ES, N52GH
				$\mu_{161}/\mu_{163} \approx 1$ S53MW

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{67}\mathrm{Ho}$	165	100%	7/2	50MA	$2.4\ \}$ $3.3\ \}$	T50RI $\}$ T52BE $\}$
${}_{67}\mathrm{Ho}$	$166+$	27.5 h	(2)	N54SN	$2.4\ \}$ $3.3\ \}$	T50RI $\}$ T52BE $\}$
${}_{68}\mathrm{Er}$	166	33.4%	0	T51GS	$(-)\,0.50 \pm 12^*)$	T51ES, (T53ES)	$\|10 \pm 2\|$	X52BS, T52WB, T51ES, (T53ES)
${}_{68}\mathrm{Er}$	167	22.9%	7/2	X51BD	$(-)\,0.50 \pm 12^*)$	T51ES, (T53ES)	$\|10 \pm 2\|$	X52BS, T52WB, T51ES, (T53ES)
${}_{69}\mathrm{Tm}$	169	100%	1/2	50MA	$0.8\ \}$ $-0.15\ \}$	T50RI $\}$ T52BE $\}$
${}_{69}\mathrm{Tm}$	$170+$	127 d	1	T52MA, N52RR, N54PL	$0.8\ \}$ $-0.15\ \}$	T50RI $\}$ T52BE $\}$
${}_{69}\mathrm{Tm}$	$171+$	680 d	(1/2)	N52GN	$0.8\ \}$ $-0.15\ \}$	T50RI $\}$ T52BE $\}$
${}_{70}\mathrm{Yb}$	170	3.0%	0	T51GS
${}_{70}\mathrm{Yb}$	171	14.3%	1/2	50MA	0.45	50MA
${}_{70}\mathrm{Yb}$	173	16.1%	5/2	50MA	$-0.65$	50MA	$4.0 \pm 4$ agree.	50MA, (T52SR)

Table of Nuclear Moments

Element	Mass number	Abundance or half-life	Spin	Source	Moment	Source	Moment	Source
$_{71}\mathrm{Lu}$	175	97.4%	$7/2$	50MA, N54BH	$2.9 \pm 5$ sog	50MA, (T52KL)	6.5 sog	50MA, (T50SR, T51SR, T52SR)
$_{71}\mathrm{Lu}$	176†	$2.4 \cdot 10^{10}$ yr	$\geqslant 7$	50MA, N54DN, N54AR	$4.2 \pm 8$ sog	50MA, (T52KL)	$7.7 \pm 10$ sog	50MA, (T50SR, T51SR, T52SR)
$_{71}\mathrm{Lu}$	177†	6.98 d		N52GH
$_{72}\mathrm{Hf}$	177	18.6%	$(1/2;\ 3/2)$	50MA	$[0.6]$	T49BE
$_{72}\mathrm{Hf}$	178	27.2%	$(0)$	50MA	$\approx 0$	50MA
$_{72}\mathrm{Hf}$	179	13.7%	$(1/2;\ 3/2)$	50MA	$[0.6]$	T49BE
$_{72}\mathrm{Hf}$	180	35.1%	$(0)$	50MA	$\approx 0$	50MA
$_{72}\mathrm{Hf}$	181†	45 d	$1/2$	N53BA
$_{73}\mathrm{Ta}$	180†	8.15 h	$(1?)$	N51BB
$_{73}\mathrm{Ta}$	181	100%	$7/2$	50MA	2.3 sog **)	50MA (T52KL) S53BT	6.6 sog	50MA, (T52SR), S53BT, (T53TR), T52WB
$_{74}\mathrm{W}$	182	26.3%	$(0)$	50MA
$_{74}\mathrm{W}$	183	14.3%	$1/2$	50MA, S50FW	$0.08 \pm 2$	S51MV
$_{74}\mathrm{W}$	184	30.6%	$(0)$	50MA
$_{74}\mathrm{W}$	185†	73 d	$(3/2)$	N53LM
$_{74}\mathrm{W}$	186	28.6%	$(0)$	50MA

) According to the shell model, the magnetic dipole moment is close to zero.
*) Value from 50MA with the correction indicated in T52KL. In the T52KL tables, apparently through oversight, the value 2.1 nuclear magnetons, indicated in 50MA, is given.

$Z$	$A$	p% or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{75}\mathrm{Re}$	185	37.0%	$5/2$	50MA, W53JT	$3.1714 \pm 6$ corr	50MA, R50BL, R51AY, (T52KL)	2.9 corr	50MA, (T52SR), R51AY
${}_{75}\mathrm{Re}$	$186^{+}$	92.8 h	1	N54GK, N54KT
${}_{75}\mathrm{Re}$	$187^{+}$	$4\cdot10^{12}$ y 62.9%	$5/2$	50MA, W53JT	$3.1755 \pm 6$	50MA, R50BL, R51AY	2.7 corr	50MA, (T52SR), R51AY
${}_{75}\mathrm{Re}$		$\gamma_{187}/\gamma_{185}=1.01026 \pm 8$ R51AY $\gamma_{185}/\gamma_{\mathrm{Na}^{23}}=0.85114 \pm 9$ R51AY				$Q_{185}/Q_{187}=1.06 \pm 5$ W53JT $\gamma_{187}/\gamma_{\mathrm{Na}^{23}}=0.85987 \pm 9$ R51AY
${}_{76}\mathrm{Os}$	187	1.64%	$(1/2?)$	T49BE, N52GH	0.6	T49BE
${}_{76}\mathrm{Os}$	189	16.1%	$3/2$	50MA, S51SU, S52MW, R54LS	$0.650655 \pm 81$	S51SU, (T52KL), S52MW, R54LS	$2.0 \pm 8$	S52MW
${}_{76}\mathrm{Os}$	$191^{+}$	16 d	$7/2$	N52SH
${}_{76}\mathrm{Os}$	193	32 h	$3/2$	N54WW
${}_{76}\mathrm{Os}$		$\gamma_{189}/\gamma_{\mathrm{C}^{13}}=0.791896 \pm 93$ R54LS
${}_{77}\mathrm{Ir}$	191	38.5%	$3/2$	50MA, S50BQ, S50MS, S52MW, S53SE
${}_{77}\mathrm{Ir}$	193	61.5%	$3/2$	50MA, S50BQ, S5JMS, S52MW, S53SE	$0.17 \pm 3$ corr	S50BQ, S52MW, S53SE	$1.5 \pm 1$	S52MW, S53SE
${}_{77}\mathrm{Ir}$	$194^{+}$	19 h	$(1?)$	N54BP
${}_{77}\mathrm{Ir}$		$\mu_{193}/\mu_{191}=1.04 \pm 4$ S50BQ, S50MS, S52MW, S53SE				$Q_{193}/Q_{191}=1.0 \pm 3$ S50BQ, S52MW, S53SE

Element	Isotope	Value	Spin	Reference	Value	Reference	Value	Reference
$_{78}\mathrm{Pt}$	$191^{+}$	2,90 days	$1/2$	N54CB	$\approx 0$	50MA
$_{78}\mathrm{Pt}$	194	32,8%	$(0)$	50MA
$_{78}\mathrm{Pt}$	195	33,7%	$1/2$	50MA, R51PY	$0,600\ 5 \pm 1$	50MA, R51PY
$_{78}\mathrm{Pt}$	196	25,4%	$(0)$	50MA	$\approx 0$	50MA
$_{78}\mathrm{Pt}$	$197^{+}$	18 h	$(1/2)$	N52SS
$_{78}\mathrm{Pt}$		$\gamma_{195}/\gamma_{\mathrm{Na}^{23}} = 0,812\ 73 \pm 8$ R51PY
$_{79}\mathrm{Au}$	$191^{+}$	18 h	$(3/2)$	N54GG
$_{79}\mathrm{Au}$	$192^{+}$	4,13 h	$(1;\ 2;\ 3)$	T53SK, N54GG		T53SK
$_{79}\mathrm{Au}$	$193^{+}$	15,8 h	$(3/2)$	N54GG
$_{79}\mathrm{Au}$	$194^{+}$	39,5 h	2	T53SK		T53SK
$_{79}\mathrm{Au}$	$195^{+}$	185 days	$3/2$	N52ST
$_{79}\mathrm{Au}$	$196^{+}$	133 h	2	T53SK		T53SK
$_{79}\mathrm{Au}$	197	100%	$3/2$	50MA	$0,13 \pm 1$ cor	50MA, (T52KU), S51SI, S52KE, S53SI, A53LW	$0,56 \pm 10$	S51SI, S53SI
$_{79}\mathrm{Au}$	$198^{+}$	2,73 days	3	N52FN, T53SK, N54EP		T53SK
$_{79}\mathrm{Au}$	$199^{+}$	3,15 days	$3/2$	N53HP

$Z$	$A$	$p\%$ or $T_{1/2}$	$I(\hbar)$	Literature data	$\mu$ nuclear magnetons	Literature data	$Q$ $(e \cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
${}_{80}\mathrm{Hg}$	$193^{+}$	6 h	$3/2$	N54GG
${}_{80}\mathrm{Hg}$	$195^{+}$	9.5 h	$3/2$	N54GG
${}_{80}\mathrm{Hg}$	$197^{+}$	64.5 h	$1/2$	S53BY, N53MS
${}_{80}\mathrm{Hg}$	$197i$	24 h	$13/2$	S53BY
${}_{80}\mathrm{Hg}$	198	10.0%	0	50MA, W50GO	$\approx 0$	50MA
${}_{80}\mathrm{Hg}$	199	18.9%	$1/2$	50MA, W50GO, R51PY	$0.499\ 4 \pm 1$	50MA, R51PY, S51FO
${}_{80}\mathrm{Hg}$	200	23.1%	0	50MA, W50GO	$\approx 0$	50MA
${}_{80}\mathrm{Hg}$	201	13.2%	$3/2$	50MA	$-0.553\ 8$	50MA, R51PY	0.6	50MA, (T52SR), S50MW, Q54RG
${}_{80}\mathrm{Hg}$	202	29.8%	0	50MA, W50GO	$\approx 0$	50MA
${}_{80}\mathrm{Hg}$	$203^{+}$	46 d	$(1/2;\ 3/2;\ 5/2)$	N54WM
${}_{80}\mathrm{Hg}$	204	6.85%	0	50MA, W50GO	$\approx 0$	50MA
${}_{80}\mathrm{Hg}$	$205^{+}$	5.5 mo	$1/2$	N53KD
				$\gamma_{199}/\gamma_D = 1.164\ 7 \pm 1\ \mathrm{R51PY}$	$\gamma_{199}/\gamma_D = 1.164\ 7 \pm 1\ \mathrm{R51PY}$	$\gamma_{199}/\gamma_D = 1.164\ 7 \pm 1\ \mathrm{R51PY}$	$\gamma_{199}/\gamma_D = 1.164\ 7 \pm 1\ \mathrm{R51PY}$	$\gamma_{199}/\gamma_D = 1.164\ 7 \pm 1\ \mathrm{R51PY}$
${}_{81}\mathrm{Tl}$	$198^{+}$	5.3 h	$(1;\ 2)$	N54PM
${}_{81}\mathrm{Tl}$	203	29.5%	$1/2$	50MA, R50PY	$1.611\ 36 \pm 11\ \mathrm{cor}$	50MA, R50PY, R51SW


204+	4.02 y 2.71 y	2	T53SG, T53SK, N54KR		T53SK
205+	70.5%	1/2	50MA, R50PY	1.627 33 ± 8 cor	50MA, R50PY, R51SW
206+	4.19 mo	(0)	T54KP
207+	4.79 mo	(1/2; 3/2)	T52PY, N52TF
208+	3.1 mo	(5, 4)	T52PY, T54KS

\[ \gamma_{205}/\gamma_{203}=1.009\,838 \pm 1 \quad \text{R50PY, R51SW, R52WL, A52KB, \textbf{R53GG}} \]

\[ \gamma_{203}/\gamma_{\mathrm H}=0.571\,40 \pm 4 \quad \text{R50PY, R51SW} \qquad \gamma_{205}/\gamma_{\mathrm H}=0.577\,02 \pm 3 \quad \text{R50PY, R51SW} \]


${}_{82}\mathrm{Pb}$	203+	252 h	(5/2; 3/2)	N54VA, N54WM
	204	1.37%	(0)	50MA	$\approx 0$	50MA
	205+	$T_{1/2}$ very large	(5/2)	N54SP
	206	25.1%	(0)	50MA	$\approx 0$	50MA
	207	21.1%	1/2	50MA, R50PY,	0.583 7 ± 1	50MA, R50PY
	208	52.4%	0	50MA	$\approx 0$	50MA
	209+	3.32 h	(9/2, 11/2)	T52PY, N53BT

\[ \gamma_{207}/\gamma_{\mathrm{Na}^{23}}=0.790\,1 \pm 1 \quad \text{R50PY} \]

Z	A	p% or $T_{1/2}$	$I\;(\hbar)$	Literature data	$\mu$, nuclear magnetons	Literature data	$Q$ $(e\cdot 10^{-24}\ \mathrm{cm}^2)$	Literature data
$_{83}\mathrm{Bi}$	204+	12 h	3	T53SK	3.85	T53SK
$_{83}\mathrm{Bi}$	206+	6.4 d	(6?)	N54AP
$_{83}\mathrm{Bi}$	207+	$>40$ y	9/2	N54WP
$_{83}\mathrm{Bi}$	208+	$T_{1/2}$ large	5	T52PY
$_{83}\mathrm{Bi}$	209+	$2.7\cdot 10^{17}$ y; 100%	9/2	50MA	$4.081\ 0 \pm 4$ corr.	50MA, S50CR, R50PU, (T52KL), R51PY, R53TW	$-0.4$ corr.	50MA, (T52SR)
$_{83}\mathrm{Bi}$	210+	$2.6\cdot 10^{6}$ y	$(>)\,4$	N54LP, T52PY
$_{83}\mathrm{Bi}$	210ᵢ	5.02 d *)	(0)	T52MA, N53WB, S53FT, T53SK, T54BR, T54KP, T54RO, T54KS	$<0.18$	S53FT, (T54RO), T53SK, T54KP
$_{83}\mathrm{Bi}$	211+	2.16 min	(1/2; 3/2)	N54FV
$_{83}\mathrm{Bi}$	212+	60.5 min	1	N53HS
$_{83}\mathrm{Bi}$				$\gamma_{209}/\gamma_D = 1.046\ 84 \pm 5$ R50PU, R51PY, R53TW
$_{84}\mathrm{Po}$	215+	1.83 μs	5/2	N54MR
$_{85}\mathrm{At}$	210+	8.3 h	4; 5; 6	N54MS
$_{89}\mathrm{Ac}$	227+	22.0 y	3/2	S51TF, N54MR

TABLE OF NUCLEAR MOMENTS

Element	Mass number	Half-life	Spin	Source	Magnetic moment	Source	Existence	Source
${}_{90}\mathrm{Th}$	$229+$	$7.34 \cdot 10^{3}$ y	$5/2$	N54MR
${}_{91}\mathrm{Pa}$	$231+$	$3.43 \cdot 10^{4}$ y	$3/2$	50MA
${}_{91}\mathrm{Pa}$	$234+$	$6.7$ h	$(5)$	N52GH
${}_{92}\mathrm{U}$	$233+$	$1.62 \cdot 10^{5}$ y	$5/2$	S54SN			exists	S54SN
${}_{92}\mathrm{U}$	$235+$	$7.07 \cdot 10^{8}$ y	$(7/2)$	50MA, S50SK, 54NA	$-0.8 \pm 2$	S50SK, (S54SN)	$\approx 8$	S50SK, (S54SN)
${}_{92}\mathrm{U}$				$\mu_{233}/\mu_{235} < 0$ S54SN
${}_{93}\mathrm{Np}$	$237+$	$2.25 \cdot 10^{6}$ y	$5/2$	50MA, X54BR	$\|6 \pm 2.5\|$	X54BR
${}_{94}\mathrm{Pu}$	$239+$	$24.4 \cdot 10^{3}$ y	$1/2$	S54VK, S54VR, X54BL	$(-) 0.4 \pm 2$	S54VK, X54BL, (X54BP)
${}_{94}\mathrm{Pu}$	$241+$	$13$ y	$5/2$	X54BP	$\|1.4 \pm 6\|$	X54BP
${}_{94}\mathrm{Pu}$				$\|\mu_{241}/\mu_{239}\| = 3.53 \pm 2$ X54BP
${}_{95}\mathrm{Am}$	$241+$	$470$ y	$(5/2)$	S53FS
${}_{95}\mathrm{Am}$	$242+$	$\sim 400$ y	$(\leq 2); \ne 3$	N52GH
${}_{95}\mathrm{Am}$	$243+$	$8.8 \cdot 10^{3}$ y	$5/2$	S54CL
${}_{95}\mathrm{Am}$				$\|\mu_{241}/\mu_{243}\| = 1$, S54CL

*) According to the data of N54LP, the $5.02$-d state may not be the ground state, as has been assumed until now.

E. F. KOLTS, V. V. KUNTS, V. G. HARTMAN

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Q54BB — H. Benoit, M. Buyle-Bodin, C. R. Acad. Sci. 238, 671.

Q54DB — D. Dautreppe, A. Blaise, C. R. Acad. Sci. 239, 493.

Q54DR — H. G. Dehmelt, H. G. Robinson, W. Gordy, J. Chem. Phys. 22, 511.

Q54RG — H. G. Dehmelt, H. G. Robinson, W. Gordy, Phys. Rev. 93, 480, 93, 920A.

Q54SC — A. L. Shalow, J. Chem. Phys. 22, 1211.

Q54TM — E. Manring, Y. Ting, D. Williams, Phys. Rev. 93, 360.

R50BL — F. Bloch, cited in 50BE.

R50CK — V. W. Cohen, W. D. Knight, T. Wentink, Jr., Phys. Rev. 79, 191.

R50CL — T. L. Collins, Phys. Rev. 79, 226A.

R50CO — T. L. Collins, Phys. Rev. 80, 103.

R50GA — E. W. Guptil, W. J. Archibald, E. S. Warren, Can. J. Res. A. 28, 359.

R50LI — G. Lindström, Phys. Rev. 78, 817.

R50LV — E. C. Levinthal, Phys. Rev. 78, 204.

R50PR — W. G. Proctor, A. C. Yu, Phys. Rev. 77, 716.

R50PU — W. G. Proctor, A. C. Yu, Phys. Rev. 78, 471.

R50PY — W. G. Proctor, A. C. Yu, Phys. Rev. 79, 35.

R50SC — W. H. Chambers, R. E. Sheriff, D. Williams, Phys. Rev. 78, 640.

R50SH — R. E. Sheriff, W. H. Chambers, D. Williams, Phys. Rev. 78, 476.

R50SR — H. H. Staub, E. H. Rogers, Helv. Phys. Acta 23, 63.

R50SW — R. E. Sheriff, D. Williams, Phys. Rev. 79, 175.

R50TD — H. A. Thomas, R. L. Driscoll, J. A. Hipple, Phys. Rev. 78, 787; J. Res. NBS 44, 569; H. A. Thomas, Phys. Rev. 80, 901.

R50WS — W. H. Chambers, R. S. Sheriff, D. Williams, Phys. Rev. 78, 482.

R51AB — N. L. Adams, T. F. Wimett, F. Bitter, Phys. Rev. 82, 343A.

R51AU — F. Alder, A. C. Yu, Phys. Rev. 81, 1067.

R51AY — F. Alder, A. C. Yu, Phys. Rev. 82, 105.

R51BD — G. J. Béné, P. M. Denis, R. C. Extermann, Helv. Phys. Acta 24, 304; G. J. Béné, Helv. Phys. Acta 24, 367.

R51BJ — F. Bloch, C. D. Jeffries, Phys. Rev. 80, 305 (1950); F. Bloch, Physica 17, 272 (1951); C. D. Jeffries, Phys. Rev. 81, 1040 (1951).

R51DR — S. S. Dharmatti, H. E. Weaver, Phys. Rev. 83, 845.

R51DW — S. S. Dharmatti, H. E. Weaver, Phys. Rev. 84, 367.

R51DV — S. S. Dharmatti, H. E. Weaver, Phys. Rev. 84, 843.

R51GA — J. H. Gardner, Phys. Rev. 83, 996.

R51GC — H. S. Gutowsky, R. E. McClure, C. J. Hoffman, Phys. Rev. 81, 635.

R51HR — J. Hatton, B. V. Rollin, E. F. W. Seymour, Phys. Rev. 83, 672.

E. F. Külz, V. V. Kunz, V. G. Hartmann

R51HU — D. M. Hunten, Phys. Rev. 78, 806 (1950); Can. J. Phys. 29, 463 (1951).
R51LI — G. Lindström, Physica 17, 412.
R51MY — T. Kandan, Y. Masuda, R. Kusaka, Y. Yamagata, J. Itoh, J. Phys. Soc. Japan, 7, 296 (1952); Phys. Rev. 83, 1066 (1951).
R51PY — W. G. Proctor, A. C. Yu, Phys. Rev. 81, 20.
R51SA — B. Smaller, E. Yasaitis, H. L. Anderson, Phys. Rev. 80, 137A (1950); 81, 896 (1951); B. Smaller, Phys. Rev. 83, 812 (1951).
R51SP — N. A. Schuster, G. E. Pake, Phys. Rev. 81, 157.
R51ST — N. A. Schuster, G. E. Pake, Phys. Rev. 81, 886.
R51SW — R. E. Sheriff, D. Williams, Phys. Rev. 82, 651; D. Williams, Physica 17, 454.
R51TS — H. Sommer, H. A. Thomas, J. A. Hipple, Phys. Rev. 80, 487 (1950); 82, 697 (1951).
R51TW — Y. Ting, D. Williams, Phys. Rev. 82, 131A.
R51WL — H. E. Walchli, R. Livingston, G. Hebert, Phys. Rev. 82, 97.
R51WP — G. D. Watkins, R. V. Pound, Phys. Rev. 82, 343A.
R51WS — D. Williams, Phys. Rev. 83, 858.
51YS — E. Yasats, B. Smaller, Phys. Rev. 82, 750.
R52DV — S. S. Dharmatti, H. E. Weaver, Phys. Rev. 85, 927.
R52DW — S. S. Dharmatti, H. E. Weaver, Phys. Rev. 86, 259.
R52JE — C. D. Jeffries, H. Loeliger, H. H. Staub, Helv. Phys. Acta 24, 643 (1951); Phys. Rev. 85, 478 (1952).
R52LI — G. Lindström, Ark. f. Fys. 4, 1.
R52MY — Y. Masuda, R. Kusaka, Y. Yamagata, J. Itoh, T. Kanda, Phys. Rev. 85, 938.
R52ST — H. H. Staub, Lucerne 1951; cited in J. phys. et rad. 13, 161 (1952).
R52TB — Y. Ting, F. K. Biard, D. Williams, Phys. Rev. 86, 618A.
R52WA — H. E. Walchli, R. Livingston, W. J. Martin, Phys. Rev. 85, 479.
R52WI — H. E. Walchli, A table of nuclearmoment data, Preliminary issue, Oct. 1, 1952, p. 89; cited in R53GG.
R52WL — H. E. Walchli, W. E. Leyshon, F. M. Scheitlin, Phys. Rev. 85, 922; 86, 618A.
R52WM — H. E. Walchli, H. W. Morgan, Phys. Rev. 87, 541.
R53AH — F. Alder, K. Halbach, Helv. Phys. Acta 26, 426.
R53CR — N. G. Cranna, Can. J. Phys. 31, 1185.
R53GG — H. S. Gutowsky, B. R. McGarvey, Phys. Rev. 91, 81.
R53JE — C. D. Jeffries, Phys. Rev. 90, 1130.
R53JL — C. D. Jeffries, Phys. Rev. 92, 1096A; 92, 1262.
R53JS — C. D. Jeffries, P. B. Sogo, Phys. Rev. 91, 1286.
R53KN — W. D. Knight, Phys. Rev. 92, 539A.
R53MA — H. C. Meal, H. C. Allen, Phys. Rev. 90, 348A.
R53PC — H. E. Petch, N. G. Cranna, G. M. Volkoff, Can. J. Phys. 31, 837.
R53TW — Y. Ting, D. Williams, Phys. Rev. 89, 595.
R53WA — H. E. Walchli, Phys. Rev. 90, 331.
R53WH — H. E. Walchli, Oak Ridge Nat. Lab. Rep. ORNL—1469; unpublished; cited in A54KJ.
R53WI — T. F. Wimett, Phys. Rev. 91, 499A.
R53WV — H. E. Weaver, Phys. Rev. 89, 923.
R54AW — C. I. Aksenov, K. V. Vladimirskii, DAN 96, 37.
R54BO — E. Brun, J. Oeser, H. W. Staub, C. G. Telschow, Phys. Rev. 93, 172.
R54BR — E. Brun, J. Oeser, H. W. Staub, C. G. Telschow, Helv. Phys. Acta 27, 173.

TABLE OF NUCLEAR MOMENTS

R54BS — E. Brun, J. Oeser, H. W. Staub, C. G. Telschow, Phys. Rev. 93, 904.
R54HB — K. Halbach, Helv. Phys. Acta 27, 259.
R54JS — P. B. Sogo, C. D. Jeffries, Phys. Rev. 93, 174.
R54LS — H. R. Loeliger, L. R. Sowles, Phys. Rev. 95, 291.
R54OG — R. A. Ogg, Jr., J. Chem. Phys. 22, 560.
R54OR — R. A. Ogg, Jr., J. D. Ray, J. Chem. Phys. 22, 147.
R54WG — G. A. Williams, D. W. McCall, H. S. Gutowsky, Phys. Rev. 93, 1428.
R54WO — L. C. Brown, D. Williams, Phys. Rev. 95, 1110.
S50AE — O. H. Arroe, Phys. Rev. 79, 212A.
S50AO — O. H. Arroe, unpublished; cited in 50BE and Amer. J. Phys. 20, 152 (1952).
S50AR — O. H. Arroe, Phys. Rev. 77, 745A; 79, 836.
S50BQ — P. Brix, H. Kopfermann, W. V. Siemens, Naturwiss. 37, 397.
S50CK — M. F. Crawford, A. L. Schawlow, F. M. Kelly, W. M. Gray, Can. J. Res. A 28, 558.
S50CR — F. M. Kelly, R. Richmond, M. F. Crawford, Phys. Rev. 80, 295.
S50FW — G. R. Fowles, Phys. Rev. 78, 744.
S50KE — K. Kessler, Phys. Rev. 79, 167.
S50KR — J. Koch, E. Rasmussen, Phys. Rev. 77, 722.
S50KS — F. M. Kelly, A. L. Schawlow, W. M. Gray, M. F. Crawford, Phys. Rev. 77, 745A.
S50KW — H. Kuhn, G. K. Woodgate, Proc. Phys. Soc. A 63, 830.
S50MK — J. E. Mack, unpublished; cited in Phys. Rev. 77, 771 (1950); Helv. Phys. Acta 23, 299 (1950).
S50MS — K. Murakawa, cited in 50BE.
S50MW — K. Murakawa, S. Suwa, J. Phys. Soc. Japan 5, 429.
S50SK — G. L. Stukenbroeker, J. R. McNally, J. Opt. Soc. 40, 226 A; 40, 336.
S51BK — P. Brix, H. Kopfermann, Naturwiss. 38, 68; P. Brix, H. Kopfermann, R. Martin, W. Walcher, Zeits. f. Phys. 130, 88.
S51FO — E. W. Foster, Proc. Roy. Soc. A 208, 367.
S51FT — M. Fred, F. S. Tomkins, J. K. Brody, Phys. Rev. 79, 212A (1950); M. Fred, F. S. Tomkins, J. K. Brody, M. Hamermesh, Phys. Rev. 82, 406 (1951).
S51KL — P. F. A. Klinkenberg, Physica 17, 715.
S51KW — H. Kuhn, G. K. Woodgate, Nature 166, 906 (1950); Proc. Phys. Soc. A 64, 1090 (1951).
S51MC — J. E. Mack, unpublished, cited in Phys. Rev. 81, 20.
S51MU — K. Murakawa, J. S. Ross, Phys. Rev. 82, 967.
S51MV — J. A. Vreeland, K. Murakawa, Phys. Rev. 83, 229A.
S51RN — J. D. Ranade, Phil. Mag. 42, 279.
S51SI — W. v. Siemens, Naturwiss. 38, 455.
S51SU — S. Suwa, Phys. Rev. 83, 1258.
S51SW — S. Suwa, J. Phys. Soc. Japan 6, 231.
S51TF — F. S. Tomkins, M. Fred, W. F. Meggers, Phys. Rev. 84, 168.
S52BK — A. Bohr, J. Koch, E. Rasmussen, Ark. f. Fys. 4, 455.
S52KE — F. M. Kelly, Proc. Phys. Soc. A 65, 250.
S52MW — K. Murakawa, S. Suwa, Phys. Rev. 87, 1048.
S52RM — J. S. Ross, K. Murakawa, Phys. Rev. 83, 229A (1951); 85, 559 (1952).
S52ST — P. Brix, A. Steudel, Naturwiss. 38, 431 (1951); A. Steudel, Zeits. f. Phys. 132, 429 (1952).

E. F. KYULTS, V. V. KUNTS, V. G. HARTMAN

S52SU — S. Suwa, Phys. Rev. 86, 247.
S53BC — J. Blaise, H. Chantrell, J. phys. et rad. 14, 135.
S53BT — B. M. Brown, Phys. Rev. 87, 228A (1952); B. M. Brown, D. M. Tamboulian, Phys. Rev. 88, 1158 (1952). Correction: Phys. Rev. 91, 1580 (1953).
S53BY — F. Bitter, H. Plotkin, B. Richter, A. Teviotdale, J. E. R. Young, Phys. Rev. 91, 421.
S53FS — M. Fred, F. S. Tomkins, Phys. Rev. 89, 318.
S53FT — M. Fred, F. S. Tomkins, F. Barnes, Phys. Rev. 92, 1324.
S53KS — H. Kopfermann, A. Steudel, S. Wagner, W. Walcher, Nachr. Akad. Wiss. Göttingen, math.-phys. Kl. II a, Nr. 1, 1.
S53ME — H. Meyer, Helv. Phys. Acta 26, 811.
S53MT — K. G. Kessler, W. F. Meggers, Phys. Rev. 80, 905 (1950); Meet. Phys. Soc. New York (1950) 1, 3; Phys. Rev. 82, 341A (1951); Physica 17, 484 (1951); K. G. Kessler, R. E. Trees, Phys. Rev. 92, 303 (1953).
S53MU — K. Murakawa, J. Phys. Soc. Japan 8, 535.
S53MW — K. Murakawa, T. Kamei, Phys. Rev. 92, 325.
S53SE — W. v. Siemens, Ann. der Phys. 13, 136.
S53SI — W. v. Siemens, Ann. der Phys. 13, 158.
S53ST — B. Sprague, D. H. Tamboulian, Phys. Rev. 91, 476A; 92, 105.
S53SU — S. Suwa, J. Phys. Soc. Japan 8, 734.
S54CL — J. G. Conway, R. D. McLaughlin, Phys. Rev. 94, 498.
S54KK — F. M. Kelly, H. Kuhn, A. Pery, Proc. Phys. Soc. A 67, 450.
S54MS — K. Murakawa, S. Suwa, J. Phys. Soc. Japan 9, 93.
S54MW — K. Murakawa, Phys. Rev. 93, 1232.
S54MZ — K. Murakawa, S. Suwa, Zeits. f. Phys. 137, 575.
S54SN — K. L. Vander Sluis, J. R. McNally, J. Opt. Soc. Am. 44, 87.
S54VK — M. van den Berg, P. F. A. Klinkenberg, P. Reynault, Physica 20, 37.
S54VR — M. van den Berg, P. F. A. Klinkenberg, Physica 20, 461.
S54WO — E. C. Woodward, Phys. Rev. 93, 954A.
T49BE — G. J. Béné, P. M. Denis, R. C. Extermann, Helv. Phys. Acta 22, 606.
T49BI — F. Bitter, Phys. Rev. 76, 150.
T49CS — M. F. Crawford, A. L. Schawlow, Phys. Rev. 76, 1310.
T49FH — E. Feenberg, K. Hammack, Phys. Rev. 75, 1877.
T50AB — R. Avery, C. H. Blanchard, Phys. Rev. 78, 704.
T50BW — A. Bohr, V. Weisskopf, Phys. Rev. 77, 94.
T50FE — E. Feenberg, Phys. Rev. 77, 771.
T50HY — E. Hylleraas, S. Skowlem, Phys. Rev. 79, 117.
T50KS — P. Kusch, Phys. Rev. 78, 615.
T50NW — G. F. Newell, Phys. Rev. 77, 141 (1950); 78, 711 (1950).
T50NX — G. F. Newell, Phys. Rev. 80, 476.
T50RA — N. F. Ramsey, Phys. Rev. 78, 699.
T50RI — O. Riedel, Zeits. Naturforsch. 5a, 654.
T50RM — N. F. Ramsey, Phys. Rev. 79, 1010.
T50SR — R. Sternheimer, Phys. Rev. 80, 102.
T51AP — A. Abragam, M. H. L. Pryce, Proc. Roy. Soc. 206, 164.
T51ES — R. J. Elliott, K. W. H. Stevens, Proc. Phys. Soc. A 64, 205.
T51GA — J. W. Gardner, Phys. Rev. 82, 285.
T51GO — W. Gordy, J. Chem. Phys. 19, 792.
T51GS — M. Goldhaber, A. W. Sunyar, Phys. Rev. 83, 906.
T51MG — W. F. Meggers, J. Opt. Soc. Am. 41, 143.
T51MU — M. Mizushima, M. Umezawa, Phys. Rev. 83, 463.

T51NH — L. W. Nordheim, Rev. mod. Phys. 23, 322.
T51SR — R. Sternheimer, Phys. Rev. 84, 244; see the note to T52SR.
T51ST — A. L. Schawlow, C. H. Townes, Phys. Rev. 82, 268.
T52BB — H. A. Bethe, S. T. Butler, Phys. Rev. 85, 1045.
T52BE — G. J. Béné, J. phys. et rad. 13, 161.
T52BR — P. Brix, Zeits. f. Phys. 132, 579 (from measurements of hyperfine structure).
T52DA — J. P. Davidson, Phys. Rev. 85, 432.
T52ES — R. J. Elliott, K. W. H. Stevens, Proc. Phys. Soc. A 65, 370.
T52FL — B. H. Flowers, Phil. Mag. 43, 1330.
T52HC — A. Hitchcock, Phys. Rev. 87, 664.
T52KI — P. F. A. Klinkenberg, cited in Physica 18, 135; 18, 1235.
T52KL — P. F. A. Klinkenberg, Rev. mod. Phys. 24, 63.
T52KO — C. F. Koster, Phys. Rev. 86, 148.
T52KU — D. Kurath, Phys. Rev. 87, 528.
T52KW — D. Kurath, Phys. Rev. 88, 804.
T52MA — C. Marty, J. Prentki, C. R. Acad. Sci. 235, 654.
T52PI — D. Pfirsch, Zeits. f. Phys. 132, 409.
T52PY — M. H. L. Pryce, Proc. Phys. Soc. A 65, 773.
T52SR — R. Sternheimer, Phys. Rev. 86, 316. The work contains correction coefficients. The values given in the present table were obtained with these corrections taken into account.
T52WB — R. van Wageningen, J. de Boer, Physica 18, 369.
T53BA — A. Bassompierre, C. R. Acad. Sci. 237, 1224.
T53BX — P. Brix (on the basis of results by H. E. White, Phys. Rev. 34, 1397 (1929), method S); Phys. Rev. 89, 1245 (1953); A. Steudel, Zeits. f. Phys. 132, 429 (1952).
T53ES — R. J. Elliott, K. W. H. Stevens, Proc. Roy. Soc. A 219, 387.
T53HM — E. G. Harris, M. A. Melkanoff, Phys. Rev. 90, 585.
T53IN — D. R. Inglis, Rev. mod. Phys. 25, 390.
T53KP — R. W. King, D. C. Peaslee, Phys. Rev. 90, 1001.
T53KU — D. Kurath, Phys. Rev. 91, 1430.
T53MC — J. W. Du Mond, E. R. Cohen, Revs. mod. Phys. 25, 691.
T53MA — C. Marty, R. Nataf, J. Prentki, C. R. Acad. Sci. 237, 137.
T53SF — R. M. Sternheimer, H. M. Foley, Phys. Rev. 92, 1460.
T53SG — A. de Shalit, M. Goldhaber, Phys. Rev. 92, 1211.
T53SK — H. M. Schwartz, Phys. Rev. 89, 1293.
T53TR — R. E. Trees, Phys. Rev. 92, 308.
T53WA — I. A. Vaysman, DAN 88, 431.
T53WI — H. E. Walchli, Oak Ridge Nat. Lab. Report Nr. 1469 (1953); cited in Phil. Mag. 45, 329 (1954).
T54BD — A. R. Bodmer, Proc. Phys. Soc. 67 A, 622.
T54BR — D. M. Brink, Proc. Phys. Soc. 67 A, 757.
T54FL — B. H. Flowers, Phil. Mag. 45, 329.
T54HC — A. Hitchcock, Phil. Mag. 45, 385.
T54KC — N. N. Kolesnikov, Vestn. Mosk. Univ. 9, 63.
T54KP — R. W. King, D. C. Peaslee, Phys. Rev. 94, 705 A.
T54KS — R. W. King, D. C. Peaslee, Phys. Rev. 94, 1284.
T54MP — S. A. Moszkowski, D. C. Peaslee, Phys. Rev. 93, 455.
T54MT — S. A. Moszkowski, C. H. Townes, Phys. Rev. 93, 306.
T54RO — M. E. Rose, R. K. Osborn, Phys. Rev. 93, 1315.
T54SC — C. Schwartz, Phys. Rev. 94, 95.
T54SH — M. F. Scharff, Phys. Rev. 95, 1114.
W50CK — V. W. Cohen, W. S. Koski, T. Wentink, Jr., Phys. Rev. 77, 742A.
W50EH — J. R. Eshbach, R. E. Hillger, Phys. Rev. 80, 1106.

W50GM — S. Geschwind, H. Minden, C. H. Townes, Phys. Rev. 78, 174; 79, 226A.
W50GO — J. Sheridan, W. Gordy, Phys. Rev. 79, 224A.
W50GR — W. Gordy, H. Ring, A. B. Burg, Phys. Rev. 78, 512.
W50GS — J. Sheridan, W. Gordy, Phys. Rev. 79, 513.
W50JN — C. K. Jen, Phys. Rev. 78, 339A; C. K. Jen, cited in J. phys. et rad. 11, 41D.
W50SP — A. H. Sharbaugh, V. G. Thomas, B. S. Pritchard, Phys. Rev. 78, 64.
W50ST — A. H. Sharbaugh, B. S. Pritchard, V. G. Thomas, J. M. Mays, B. P. Dailey, Phys. Rev. 79, 189.
W50SW — D. F. Smith, M. Tidwell, D. K. P. Williams, Phys. Rev. 79, 1007.
W50WS — M. T. Weiss, M. W. P. Strandberg, R. B. Lawrance, C. C. Loomis, Phys. Rev. 78, 202.
W51CK — T. Wentink, Jr., W. S. Koski, V. W. Cohen, Phys. Rev. 81, 948.
W51GG — S. Geschwind, G. R. Gunther-Mohr, C. H. Townes, Phys. Rev. 81, 288; 82, 343A.
W51JG — C. M. Johnson, W. Gordy, R. Livingston, Phys. Rev. 83, 1249.
W51LS — C. C. Loomis, M. W. P. Strandberg, Phys. Rev. 81, 798.
W51MA — J. M. Mays, C. H. Townes, Phys. Rev. 81, 940.
W51MJ — S. L. Miller, C. H. Townes, Phys. Rev. 82, 454; 83, 209A.
W52EH — J. R. Eshbach, R. E. Hillger, Physica 17, 378 (1951); Phys. Rev. 85, 532 (1952).
W52GG — S. Geschwind, G. R. Gunther-Mohr, C. H. Townes, Phys. Rev. 83, 209A (1951); S. Geschwind, G. R. Gunther-Mohr, G. Silvey, Phys. Rev. 85, 474 (1952).
W52GT — D. A. Gilbert, Phys. Rev. 85, 716.
W52HS — W. A. Hardy, G. Silvey, C. H. Townes, Phys. Rev. 85, 494; 86, 608A.
W52JT — A. Javan, A. V. Grosse, Phys. Rev. 87, 227A.
W53GB — C. A. Burrus, W. Gordy, Phys. Rev. 92, 274.
W53HS — W. A. Hardy, G. Silvey, C. H. Townes, B. F. Burke, M. W. P. Strandberg, Phys. Rev. 92, 1953.
W53JT — A. Javan, G. Silvey, C. H. Townes, A. V. Grosse, Phys. Rev. 91, 222A.
W53LB — R. Livingston, B. M. Benjamin, J. T. Cox, W. Gordy, Phys. Rev. 92, 1271.
W53MT — S. L. Miller, C. H. Townes, Phys. Rev. 90, 537.
W53WT — R. W. White, C. H. Townes, Phys. Rev. 92, 1256.
W54AS — L. C. Aamodt, P. C. Fletcher, G. Silvey, C. H. Townes, Phys. Rev. 94, 789A.
W54CK — B. F. Burke, M. W. P. Strandberg, V. W. Cohen, W. S. Koski, Phys. Rev. 93, 193.
W54BT — G. R. Bird, C. H. Townes, Phys. Rev. 94, 1203.
W54GB — J. J. Gallagher, F. D. Bedard, C. M. Johnson, Phys. Rev. 93, 729.
W54KI — P. Kisliuk, J. Chem. Phys. 22, 86.
W54WT — T. C. Wang, C. H. Townes, Phys. Rev. 94, 767A.
X50AK — S. A. Al’tshuler, B. N. Kozyrev, S. P. Salikhov, DAN 71, 855.
X50BE — B. Bleaney, H. E. D. Scovil, Proc. Phys. Soc. A 63, 1369.
X50ES — T. S. England, E. E. Schneider, Nature 166, 437.
X51BD — B. Bleaney, H. E. D. Scovil, Proc. Phys. Soc. A 64, 204.
X51BE — B. Bleaney, Physica 17, 175.
X51BI — B. Bleaney, D. J. E. Ingram, Proc. Roy. Soc. A 205, 336.

X51BK — B. Bleaney, D. J. E. Ingram, Proc. Roy. Soc. A 208, 143.

X51BS — B. Bleaney, D. J. E. Ingram, H. E. D. Scovil, Proc. Phys. Soc. A 64, 601.

X51BW — B. Bleaney, K. D. Bowers, Proc. Phys. Soc. A 64, 1135.

X51BU — B. Bleaney, K. D. Bowers, D. J. E. Ingram, Proc. Phys. Soc. A 64, 758.

X51DK — C. F. Davis, A. F. Kip, R. Malvano, Atti. Accad. Naz. Lincei (R. C. Cl. Sci. Fis. Mat. Nat) 11, 77.

X52BA — B. Bleaney, H. E. D. Scovil, R. S. Trenam, Phil. Mag. 43, 995.

X52BE — B. Bleaney, H. E. D. Scovil, Phil. Mag. 43, 999.

X52BL — G. S. Bogle, H. E. D. Scovil, Proc. Phys. Soc. 65, 368.

X52BS — G. S. Bogle, H. J. Duffus, H. E. D. Scovil, Proc. Phys. Soc. A 65, 760.

X52BT — J. M. Baker, B. Bleaney, Proc. Phys. Soc. A 65, 952.

X52BW — K. D. Bowers, Proc. Phys. Soc. A 65, 860.

X52GO — J. H. E. Griffiths, J. Owen, Proc. Phys. Soc. A 65, 951.

X52KS — C. Kikuchi, M. H. Sirvetz, V. W. Cohen, Phys. Rev. 88, 142 (1952); 92, 109 (1953).

X53BB — J. M. Baker, B. Bleaney, K. D. Bowers, P. F. D. Shaw, R. S. Trenam, Proc. Phys. Soc. A 66, 305.

X53BT — B. Bleaney, K. D. Bowers, R. S. Trenam, Proc. Phys. Soc. A 66, 410.

X54BE — B. Bleaney, H. E. D. Scovil, R. S. Trenam, Proc. Roy. Soc. A 223, 15.

X54BL — B. Bleaney, P. M. Llewellyn, M. H. L. Pryce, G. R. Hall, Phil. Mag. 45, 773.

X54BP — B. Bleaney, P. M. Llewellyn, M. H. L. Pryce, Phil. Mag. 45, 991.

X54BR — B. Bleaney, P. M. Llewellyn, M. H. L. Pryce, Phil. Mag. 45, 992.

X54BT — R. S. Trenam, Proc. Phys. Soc. A 66, 414 (1953); B. Bleaney, R. S. Trenam, Proc. Roy. Soc. A 223, 1 (1954).

X54LZ — R. Livingston, H. Zeldes, E. H. Taylor, Phys. Rev. 94, 725.

X54UE — J. Uebersfeld, J. phys. et rad. 15, 126.

Z52JB — V. Jaccarino, B. Bederson, H. H. Stroke, Phys. Rev. 87, 676.

Submission history

[v1] 1955

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\(0^n\)	\(1^+\)	10,4 min	\(1/2\)	50MA, N50HA	\(-1,912\ 80 \pm 9\)	50MB, R50SR
\(1\mathrm{H}\)	1	99,99%	\(1/2\)	50MA	\(2,792\ 76 \pm 6\) corr.\(^*)\)	50MA, R50SR, R50TD, R51GA, R51BJ, (R51TS), R51TS, T53MC
\(1\mathrm{H}\)	2	0,01%	1	50MA, R50LV	\(0,857\ 354 \pm 9\) corr.	50MA, R50LV	\((2,738 \pm 14)\times 10^{-3}\)	50MA, T50NW, A52RK
\(1\mathrm{H}\)	\(3^+\)	12,4 yr	\(1/2\)	50MA	\(2,978\ 643 \pm 28\) corr.	50MA

Element	Mass number	Abundance or half-life	Spin	References	Magnetic moment	References	Quadrupole moment	References
\({}^{2}\mathrm{He}\)	3	\(1.3\cdot 10^{-4}\%\)	\(1/2\)	50MA, B50DR, S51FT, A53WH	\(-2.127\,414\) \(\pm 3\) corr.	50MA, S51FT
\({}^{2}\mathrm{He}\)	4	\(100\%\)	0	50MA
\({}^{2}\mathrm{He}\)	\(5^{+}\)	\(\ll 10^{-8}\ \mathrm{s}\)	\(3/2\)	T52DA	\(-1.59 \pm 9\)	T52DA
\({}^{3}\mathrm{Li}\)	\(5^{+}\)	\(\ll 10^{-8}\ \mathrm{s}\)	\(3/2\)	N52AL, T54KC
\({}^{3}\mathrm{Li}\)	6	\(7.4\%\)	1	50MA	\(0.821\,89\) \(\pm 4\) corr.	50MA	\((-)\,4.6\cdot 10^{-4}\)	50MA, R51SP, A53KU, T53IN, T54MT
\({}^{3}\mathrm{Li}\)	7	\(92.6\%\)	\(3/2\)	50MA	\(3.256\,33\) \(\pm 9\) corr.	50MA, R52LI )	\((<0)\)	50MA, T50AB, T53HM, A53KU, T53IN, T53SF
\({}^{3}\mathrm{Li}\)	\(8^{+}\)	\(0.83\ \mathrm{s}\)	(3)	T51GA, T52KW, N53CH

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(h)\)	Literature data	\(\mu\) nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{4}\mathrm{Be}\)	\(7+\)	53.6 d	\(1/2;\) \(3/2\)	T51MU, T52FL, T52DA, N52AL	\(-1.59 \pm 9\)	T50AB, T51MU, T52FL, T52DA	\(\approx Q(\mathrm{Li}^{7})\)	T50AB
\({}_{4}\mathrm{Be}\)	\(8+\)	\(< 2\cdot 10^{-14}\) s	\((0)\)	N52AL
\({}_{4}\mathrm{Be}\)	\(9\)	\(100\%\)	\(3/2\)	R51GC, R51HR, R51ST, R54WO	\(-1.17746\) \(\pm 9\) corr.	50MA, R51AV, R51SW	\(\approx \|0.02\|\)	R51HR, R53KN
\({}_{4}\mathrm{Be}\)	\(10+\)	\(2.7\cdot 10^{6}\) yr	\((0)\)	N52AL
\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)	\(\eta_{9}/\eta_{\mathrm{D}} = 0.915475 \pm 7\ \mathrm{R51SW}\)
\({}_{5}\mathrm{B}\)	\(9+\)	Very short	\(3/2\)	T51MU		T51MU
\({}_{5}\mathrm{B}\)	\(10\)	\(\approx 19.0\%\)	\(3\)	50MA, W50WS, W50GR	\(1.80066\) \(\pm 15\) corr.	50MA, R51TW, R53TW	\(0.0740 \pm 5\)	50MA, (T50SR, T52SR), W50GR, Q52DE, (Q53DE), A53WE
\({}_{5}\mathrm{B}\)	\(11\)	\(\approx 81.0\%\)	\(3/2\)	50MA, W50GR, N54BR	\(2.68853\) \(\pm 7\) corr.	50MA, R51SW, R52LI	\(0.0355 \pm 2\)	50MA, (T50SR, T52SR), W50GR, (T53BA), Q52DE, (Q53DE), A53WE
\({}_{5}\mathrm{B}\)	\(12+\)	22 ms	\(1\)	T51NH, T52KW
\(Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}\)	\(Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}\)	\(Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}\)	\(Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}\)	\(Q_{10}/Q_{11} = 2.084 \pm 2\ \mathrm{Q52DE}\)	\(\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}\)	\(\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}\)	\(\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}\)	\(\gamma_{10}/\gamma_{\mathrm{H}} = 0.107464 \pm 11\ \mathrm{R51TW,\ R53TW}\)

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\) nuclear magnetons	Literature data	\(Q\) \((e \cdot 10^{-24}\,\mathrm{cm}^2)\)	Literature data
\({}_{8}\mathrm{O}\)	\(15^{+}\)	118 s	\(\leqslant 5/2\)	N52AL
\({}_{8}\mathrm{O}\)	16	99.76%	0	50MA
\({}_{8}\mathrm{O}\)	17	0.04%	\(5/2\)	50MA, W51MJ, R51AU, W52GG, W53MT, N52BB	\(-1.8928 \pm 1.9\)	R51AU	\(-4 \cdot 10^{-3}\)	50MA, W52GG, W54BT
\({}_{8}\mathrm{O}\)	18	0.20%	0	50MA, W51MJ			\(< \|4 \cdot 10^{-3}\|\)	50MA
\({}_{8}\mathrm{O}\)	\(19^{+}\)	27 s	\((1/2; 3/2; 5/2)\)	T49FH, T52DA, T54FL	\(-0.73 \pm 8\)	T52DA *)
\({}_{8}\mathrm{O}\)				\(\nu_{17}/\nu_{\mathrm{D}} = 0.88313 \pm 4\) R51AU
\({}_{9}\mathrm{F}\)	\(17^{+}\)	70 s	\(3/2; 5/2\)	N52AL
\({}_{9}\mathrm{F}\)	\(18^{+}\)	112 min	1	T52BE, N53ST, T53KP, T54MP,	0.8	T49BE, T52BE	\(> 0\)	T54MT
\({}_{9}\mathrm{F}\)	19	100%	\(1/2\)	50MA	\(2.62895 \pm 10\) cor	50MA, R51SW**), R52LI
\({}_{9}\mathrm{F}\)	\(20^{+}\)	10.7 s	1	T49FH, T53KP N53FB, T54SC
\({}_{9}\mathrm{F}\)				\(\nu_{\mathrm{H}}/\nu_{19} = 1.062917 \pm 1\) R50GA, R51BD, R51MY, R51SW, R52LI *)

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(h)\)	Literature data	\(\mu\), nuclear magnetons	Literature data
				\(\nu_{\mathrm{Mn}^{55}}/\nu_{23}=0.9372\pm1\) R50PR, R51PY		\(\nu_{\mathrm{Co}^{59}}/\nu_{23}=0.89709\pm9\) R51PY
				\(\nu_{\mathrm{As}^{75}}/\nu_{23}=0.64745\pm15\) R51DW, R53WV		\(\nu_{\mathrm{Se}^{77}}/\nu_{23}=0.72193\pm2\) R52DW, R53WV
				\(\nu_{\mathrm{Cd}^{111}}/\nu_{23}=0.8016\pm1\) R50PY		\(\nu_{\mathrm{Cd}^{113}}/\nu_{23}=0.8386\pm1\) R50PY
				\(\nu_{\mathrm{In}^{113}}/\nu_{23}=0.82667\pm8\) R51PY		\(\nu_{\mathrm{In}^{115}}/\nu_{23}=0.82841\pm8\) R51PY
				\(\nu_{\mathrm{Sn}^{115}}/\nu_{23}=1.2362\pm1\) R50PY		\(\nu_{\mathrm{Sn}^{117}}/\nu_{23}=1.3468\pm1\) R50PY
				\(\nu_{\mathrm{Sn}^{119}}/\nu_{23}=1.4090\pm1\) R50PY		\(\nu_{\mathrm{Sb}^{121}}/\nu_{23}=0.90469\pm4\) R50CL, R50CK, R50PU, R51PY
				\(\nu_{\mathrm{Te}^{123}}/\nu_{23}=0.99085\pm3\) R51DV, R53DW		\(\nu_{\mathrm{Te}^{125}}/\nu_{23}=1.19457\pm4\) R51DV, R53DW
				\(\nu_{\mathrm{Xe}^{129}}/\nu_{23}=1.0457\pm1\) R50PU, R51PY		\(\nu_{\mathrm{Re}^{185}}/\nu_{23}=0.85114\pm9\) R51AY
				\(\nu_{\mathrm{Re}^{187}}/\nu_{23}=0.85987\pm9\) R51AY		\(\nu_{\mathrm{Pt}^{195}}/\nu_{23}=0.81273\pm8\) R51PY
				\(\nu_{\mathrm{Pb}^{207}}/\nu_{23}=0.7901\pm1\) R51PY
\({}^{12}\mathrm{Mg}\)	24	78.6%	(0)	50MA	\(\approx 0\)	50MA
\({}^{12}\mathrm{Mg}\)	25	10.1%	\(5/2\)	50MA, S50KS, N54EK	\(-0.85466\pm15\)	50MA, S50KS, R51AY
\({}^{12}\mathrm{Mg}\)	26	11.3%	(0)	50MA, N54EK	\(\approx 0\)	50MA
\({}^{12}\mathrm{Mg}\)	\(27+\)	9.5 m	\(1/2\)	T52DA, N54EK	\(-0.62\pm7\)	T52DA
				\(\nu_{25}/\nu_{\mathrm{N}^{14}}=0.84714\pm8\) R51AY

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TABLE OF NUCLEAR MOMENTS

Table of Nuclear Moments

TABLE OF NUCLEAR MOMENTS

Table of nuclear moments

CITED LITERATURE

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TABLE OF NUCLEAR MOMENTS

Element	Isotope	Half-life / abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
\({}_{6}\mathrm{C}\)	\(11^{+}\)	20.4 min	\(3/2\)	T49BE	\(-1.1\)	T49BE
\({}_{6}\mathrm{C}\)	12	98.9%	0	50MA, N54HR
\({}_{6}\mathrm{C}\)	13	1.1%	\(1/2\)	50MA, N52AL	\(0.702\,25 \pm 14\) cor	50MA
\({}_{6}\mathrm{C}\)	\(14^{+}\)	\(5.650 \cdot 10^{3}\) yr	0	50MA
\({}_{6}\mathrm{C}\)	\(15^{+}\)	2.4 s	\(5/2\)	T53IN, N54RH
\({}_{7}\mathrm{N}\)	\(12^{+}\)	12.75 ms	1	T51NH
\({}_{7}\mathrm{N}\)	\(13^{+}\)	10.1 min	\(1/2\)	N52AL
\({}_{7}\mathrm{N}\)	14	99.6%	1	50MA, W54GB, N54ST	\(0.403\,69 \pm 3\) cor	50MA, R50PR, R51PY, R53TW	0.01	50MA, (T52SR), W50GS, W54KI
\({}_{7}\mathrm{N}\)	15	0.4%	\(1/2\)	50MA, R54OG, N52GO	\(-0.283\,12 \pm 4\)	50MA, R50PR, R51PY
\({}_{7}\mathrm{N}\)	\(16^{+}\)	7.4 s	(2)	T49FH, T51NH, N53HP

Element	Mass number	Abundance or half-life	\(I\)
\({}_{10}\mathrm{Ne}\)	20	90,9%	(0)	50MA, A52WT	\(<12\cdot 10^{-4}\)	50MA, A52WT
\({}_{10}\mathrm{Ne}\)	21	0,3%	3/2	50MA, T51ST, T52BE, T52DA, N52MT	\(-0,73 \pm 8\)	50MA, T51ST, T52FL, T52BE, T52DA, T54SH	\(-0,195\)	T54SH
\({}_{10}\mathrm{Ne}\)	22	8,8%	(0)	50MA	\(\approx 0\)	50MA
\({}_{10}\mathrm{Ne}\)	\(23^{+}\)	40,2 s	(5/2)	N53HP
\({}_{11}\mathrm{Na}\)	\(22^{+}\)	2,60 y	3	50MA	\(1,745\ 82 \pm 22\ \mathrm{cor}\)	50MA
\({}_{11}\mathrm{Na}\)	23	100%	3/2	50MA, R51GC	\(2,217\ 54 \pm 10\ \mathrm{cor}\)	50MA, R52LI, R51SW	\(0,10 \pm 6\) \((-2,3)\)	S53MW ) T53IN *) D54SA T54MT, T54SH
\({}_{11}\mathrm{Na}\)	\(24^{+}\)	15,1 h	4	A51SB, A53SB, N54NY	\(1,688 \pm 5\)	A53SB
\({}_{11}\mathrm{Na}\)	\(25^{+}\)	58,2 s	3/2	A51SB, A53SB, N54NY

Element	Isotope	Abundance or half-life	Spin	References	Magnetic moment	References	Quadrupole moment	References
\(^{13}\mathrm{Al}\)	\(25+\)	7.3 s	\(3/2;\ 5/2\)	T51MU, N53GO		T51MU		50MA, (T50SR, T52SR), A53LE, T52KO
\(^{13}\mathrm{Al}\)	\(26+\)	109 y	5	T49BE, T52BE, T53KP, N54EK	3.0	T49BE
\(^{13}\mathrm{Al}\)	27	100%	\(5/2\)	50MA, R53PC, R54WO	\(3.641\,33 \pm 15\) cor	50MA, R51SV, S51SV, R52LI, R54WO	\(0.149 \pm 2\)	50MA, (T50SR, T52SR), A53LE, T52KO
\(^{13}\mathrm{Al}\)	\(28+\)	2.3 m	3	N54SH, N54EG, N54EK
\(^{13}\mathrm{Al}\)	\(29+\)	6.6 m	\(5/2\)	N54EK

Element	Isotope	Abundance or half-life	Spin	References	Magnetic moment	References	Quadrupole moment	References
\(^{14}\mathrm{Si}\)	28	92.2%	0	50MA, W50SP, R54OR	\((r < 0.05)\)	R54WG	\(\approx 0\)	50MA
\(^{14}\mathrm{Si}\)	29	4.7%	\(1/2\)	50MA, W50SP, R53WV, W53WT, R54OR, R54WG, N54EK	\(-0.554\,92 \pm 4\)	R51DV, R51HR, R53WV	\(< 1.1 \cdot 10^{-4}\)	50MA, W53WT
\(^{14}\mathrm{Si}\)	30	3.1%	0	50MA, W50SP, R54OR, N54EK		R54WG	\(\approx 0\)	50MA
\(^{14}\mathrm{Si}\)	\(31+\)	157 m	\(1/2;\ 3/2\)	N54EK

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I\) \((\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\,\mathrm{cm}^2)\)	Literature data
\({}_{15}\mathrm{P}\)	\(29^\dagger\)	4.5 s	\((1/2)\)	N54EK
\({}_{15}\mathrm{P}\)	\(30^\dagger\)	2.5 min	1	T52BE; T54MP, N54EL	0.65	T52BE	0	T54MT
\({}_{15}\mathrm{P}\)	31	100%	\(1/2\)	50MA	\(1.131\,65 \pm 7\) corr.	50MA, R51SW
\({}_{15}\mathrm{P}\)	\(32^\dagger\)	14.3 d	\((1;2)\)	T53SK, N54KB, T52BB, N54EG		T53SK
\({}_{15}\mathrm{P}\)	\(33^\dagger\)	25.0 d	\((3/2)\)	N54NJ
\({}_{15}\mathrm{P}\)	\(34^\dagger\)	12.7 s	\((1)\)	N54EK
		\(\gamma_{31}/\gamma_{\mathrm{H}} = 0.404\,804 \pm 10\) R52MY				\(\gamma_{31}/\gamma_{\mathrm{Li}^7} = 1.041\,82 \pm 5\) R51SW
\({}_{16}\mathrm{S}\)	\(31^\dagger\)	2.66 s	\(1/2\)	T52DA	\(-0.62 \pm 7\)	T52DA
\({}_{16}\mathrm{S}\)	32	95.00%	0	50MA			—
\({}_{16}\mathrm{S}\)	33	0.74%	\(3/2\)	50MA, W50EH, N54EK	\(0.642\,92 \pm 14\)	50MA, W50EH, W50JN, R51DR, W52EH, R53WV	\(-0.064\) corr.	50MA, (T52SR), Q53DH, W53GB, W54BT
\({}_{16}\mathrm{S}\)	34	4.24%	\((0)\)	50MA			\(<\lvert 2\cdot 10^{-3}\rvert\)	50MA
\({}_{16}\mathrm{S}\)	\(35^\dagger\)	87.1 d	\(3/2\)	50MA, W50CK, T51ST, W51CK	\((+)1.00 \pm 4^*)\)	T51ST, T52BE, W54CK, T52DA	0.045 corr.	50MA, (T52SR), W51CK, Q53DH, W53GB, W54BT
\({}_{16}\mathrm{S}\)	36	0.017%	\((0)\)	50MA			\(<0.01\)	50MA
		\(Q_{35}/Q_{36} = -0.695\) W51CK, (Q53DH)				\(\gamma_{33}/\gamma_{\mathrm{N}^{14}} = 1.061\,74 \pm 13\) R51DR, R53WV


\({}^{17}\mathrm{Cl}\)	\(33^{\dagger}\)	\(1,8\ \mathrm{s}\)	\((3/2;\ 5/2)\)	N54EK
\({}^{17}\mathrm{Cl}\)	\(34^{\dagger}\)	\(1,50\ \mathrm{s}\)	\(0\)	T52MA, T53KP, T54MP, N54EK			\(0\)	T54MT
\({}^{17}\mathrm{Cl}\)	\(35\)	\(75,39\%\)	\(3/2\)	50MA	\(0,821\ 80 \pm 5\ \text{sog}\)	50MA, R50PR, R51PY, R53TW, Q53TM, Q54TM	\(-0,084\ 31 \pm 2\ \text{sog}\)	50MA, T52KO, A51JK, (T51SR, T52SR)
\({}^{17}\mathrm{Cl}\)	\(36^{\dagger}\)	\(4,4\cdot 10^{5}\ \mathrm{yr}\)	\(2\)	50MA, W51JG, W52GT	\(0,9\)	T52KL	\(-0,0168 \pm 1\)	50MA, (T51SR, T52SR), W51JG, W52GT
\({}^{17}\mathrm{Cl}\)	\(37\)	\(24,61\%\)	\(3/2\)	50MA	\(0,684\ 10 \pm 5\ \text{sog}\)	50MA, R50PR, R51PY, R53TW	\(-0,066\ 35 \pm 2\ \text{sog}\)	50MA, T52KO, A51JK, (T51SR, T52SR)
\({}^{17}\mathrm{Cl}\)	\(38^{\dagger}\)	\(37,3\ \mathrm{min}\)	\((2)\)	T53KU, N50LA, T50FE, T52BB

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}^{18}\mathrm{Ar}\)	\(35^{+}\)	\(1.90\ \mathrm{s}\)	\((3/2)\)	T51MU	\(\approx 0\)	T51MU
\({}^{18}\mathrm{Ar}\)	\(36\)	\(0.34\%\)	\((0)\)	50MA		50MA, S53ME
\({}^{18}\mathrm{Ar}\)	\(37^{+}\)	\(35.0\ \mathrm{d}\)	\(3/2\)	T51MU, T52DA	\(0.98 \pm 7\)	T51MU, T52DA
\({}^{18}\mathrm{Ar}\)	\(38\)	\(0.06\%\)	\(0\)	T50FE	\(\approx 0\)	S53ME
\({}^{18}\mathrm{Ar}\)	\(39^{+}\)	\(265\ \mathrm{y}\)	\(7/2\)	N50BZ
\({}^{18}\mathrm{Ar}\)	\(40\)	\(99.60\%\)	\((0)\)	50MA	\(\approx 0\)	50MA, S53ME
\({}^{18}\mathrm{Ar}\)	\(41^{+}\)	\(110\ \mathrm{min}\)	\(5/2;\) \(7/2\)	T49FI, T52DA, N54EK	\(-1.17 \pm 12\)	T52DA
\({}^{19}\mathrm{K}\)	\(38^{+}\)	\(0.95\ \mathrm{s}\)	\(0\)	T53KP, T53KU, T54MP, N54EK	\(1.4\)	T52BE	\(>0\)	T54MT
\({}^{19}\mathrm{K}\)	\(39\)	\(93.08\%\)	\(3/2\)	50MA	\(0.390\,873 \pm 13\)	50MA, A52EB, R54BO	\((\approx -0.03)\)	49GH, T52WB T52PI
\({}^{19}\mathrm{K}\)	\(40^{+}\)	\(1.25\cdot 10^{9}\ \mathrm{y}\) \(0.01\%\)	\(4\)	50MA, N54EG	\(-1.298\,2\) \(\pm 4\ \mathrm{cor}\)	50MA A52EB
\({}^{19}\mathrm{K}\)	\(41\)	\(6.91\%\)	\(3/2\)	50MA	\(+0.214\,53 \pm 3\)	50MA, R54BO	\((\approx -0.02)\)	49GH, T52WB
\({}^{19}\mathrm{K}\)	\(42^{+}\)	\(12.5\ \mathrm{h}\)	\(2\)	A53SB, N54EK	\(-1.137 \pm 5\)	A53SB
\({}^{19}\mathrm{K}\)	\(43^{+}\)	\(22.0\ \mathrm{h}\)	\((3)\)	N54LT

Element	Isotope	Abundance or half-life	Spin	Method	Magnetic moment	References	Additional value	Additional references
\(^{20}\mathrm{Ca}\)	40	96.92%	(0)	50MA N54EK	\(\approx 0\)	50MA, R51GC
\(^{20}\mathrm{Ca}\)	41+	\(\left\{\begin{array}{l}<7\cdot 10^{-4}\%\\ 1.1\cdot 10^{5}\ \text{yr}\end{array}\right.\)	(5/2; 7/2)	N54EK
\(^{20}\mathrm{Ca}\)	42	0.64%	0	T50FE
\(^{20}\mathrm{Ca}\)	43	0.13%	7/2	R53JE, S54KK	\(-1.3152 \pm 2\)	R53JE, S54KK
\(^{20}\mathrm{Ca}\)	45+	164 d	5/2	T52DA	\(0.87 \pm 6\)	T52DA
\(^{20}\mathrm{Ca}\)	49+	2.5 h	3/2	T52DA	\(-0.85 \pm 9\)	T52DA
\(^{21}\mathrm{Sc}\)	43+	3.92 h	7/2	N54IM
\(^{21}\mathrm{Sc}\)	44+	3.92 h	(2; 3)	N54SD, T54HC, T54SC
\(^{21}\mathrm{Sc}\)	45	100%	7/2	50MA	\(4.75611 \pm 6\ \mathrm{cor}^{**)}\)	50MA, R50PU, R50SW, (T50RA), R51HU, R51PY	\((-0.31)\)	T52WB
\(^{21}\mathrm{Sc}\)	46+	84 d	4	N54KS, T52RB		R51SW
\(^{21}\mathrm{Sc}\)	47+	3.43 d	(7/2)	N53CB
\(^{21}\mathrm{Sc}\)	48+	43.7 h	\(>6\)	T52KU, T53KU, N52JW, N52RP, N53CG, N52JK

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\ \text{cm}^2)\)	Literature data
\({}_{21}\mathrm{Sc}\)		\(\gamma_{\mathrm{Mn}^{55}}/\gamma_{45}=1{,}020\)	\(28\pm 5\)	R51SW	\(\gamma_{\mathrm{Cu}^{63}}/\gamma_{45}=1{,}091\)	\(25\pm 6\) R51SW
\({}_{21}\mathrm{Sc}\)		\(\gamma_{\mathrm{Cu}^{65}}/\gamma_{45}=1{,}169\)	\(51\pm 6\)	R51SW	\(\gamma_{45}/\gamma_{\mathrm{Br}^{79}}=0{,}969\)	\(54\pm 6\) R50SW, R51SW
\({}_{21}\mathrm{Sc}\)		\(\gamma_{\mathrm{Br}^{81}}/\gamma_{45}=1{,}111\)	\(65\pm 6\)	R51SW	\(\gamma_{\mathrm{Nb}^{93}}/\gamma_{45}=1{,}006\)	\(13\pm 5\) R51SW
\({}_{21}\mathrm{Sc}\)		\(\gamma_{\mathrm{In}^{115}}/\gamma_{45}=0{,}901\)	\(877\pm 50\)	R52TB, R53TW
\({}_{22}\mathrm{Ti}\)	\(45^{+}\)	\(3{,}08\) h	\(7/2\)	T52DA	\(-1{,}17\pm 12\)	T52DA
\({}_{22}\mathrm{Ti}\)	47	\(7{,}75\%\)	\(5/2\)	R53JL, T53WI	\(-0{,}787\ 06\pm 10\)	R53JL
\({}_{22}\mathrm{Ti}\)	48	\(73{,}45\%\)	0	N54SB
\({}_{22}\mathrm{Ti}\)	49	\(5{,}51\%\)	\(7/2\)	R52JE *), R53JL, N54SB	\(-1{,}102\ 2\pm 2\)	R52JE *), R52ST R53JL	\((0{,}34)\)	T52WB
\({}_{22}\mathrm{Ti}\)	\(51^{+}\)	\(5{,}79\) min	\(3/2\)	T52DA	\(-0{,}85\pm 9\)	T52DA
\({}_{22}\mathrm{Ti}\)		\(\gamma_{47}/\gamma_{\mathrm{D}}=0{,}367\)	\(21\pm 6\)	R53JL	\(\gamma_{47}/\gamma_{\mathrm{Cr}^{53}}=0{,}574\)	\(93\pm 6\) R53JL
\({}_{22}\mathrm{Ti}\)		\(\gamma_{49}/\gamma_{\mathrm{H}}=0{,}056\)	\(38\pm 1\)	R52JE *)	\(\gamma_{49}/\gamma_{\mathrm{D}}=0{,}367\)	\(32\pm 6\) R53JL
\({}_{22}\mathrm{Ti}\)		\(\gamma_{49}/\gamma_{\mathrm{Cl}^{35}}=0{,}575\)	\(08\pm 6\)	R53JL
\({}_{23}\mathrm{V}\)	\(48^{+}\)	\(16{,}0\) d	\(4; 5\)	N53CG
\({}_{23}\mathrm{V}\)	\(49^{+}\)	635 d	\(7/2\)	N54NN, T54FL,
\({}_{23}\mathrm{V}\)	50	\(0{,}23\%\)	6	X52KS, X52BT, T52HC	\(3{,}347\) corr. **)	R52WL, R52WM
\({}_{23}\mathrm{V}\)	51	\(99{,}77\%\)	\(7/2\)	50MA, X51BE, X51BS	\(5{,}145\ 03\pm 23\) corr.	50MA, R51PY, R51SW, R52WM	\(0{,}3\pm 2\)	S53MW

Element	Isotope	Half-life / abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
	52+	3.75 min	(3)	N54KB, T52BB
		\(\nu_{50}/\nu_{51}=0.379\,074\pm17\) X52KS, X52BT, R52WM			\(\nu_{50}/\nu_D=0.649\,203\pm12\) R52WL, R52WM
		\(\nu_{50}/\nu_{\mathrm{Cr}^{53}}=1.017\,58\pm10\) R52WL			\(\nu_{50}/\nu_{\mathrm{Rb}^{85}}=1.032\,62\pm10\) R52WL
		\(\gamma_{51}/\gamma_{\mathrm H}=0.262\,65\) 50BE			\(\nu_{51}/\nu_{\mathrm{Na}^{23}}=0.993\,855\pm25\) R52WM
		\(\nu_{51}/\nu_{\mathrm{Sc}^{45}}=1.081\,56\pm5\) R51SW
\({}_{24}\mathrm{Cr}\)	49+	41.9 min	\(5/2\)	T52DA, N54NN	\(0.87\pm6\)	T52DA
\({}_{24}\mathrm{Cr}\)	51+	27.75 days	\(7/2\)	T52DA	\(-1.20\pm12\)	T52DA
\({}_{24}\mathrm{Cr}\)	53	9.55%	\(3/2\)	X51BW, X52BW, R53JS, R54HB	\(-0.473\,51\pm6\)	X51BE, X51BW, X52BW, R53AH, R53JS	\((-0.09)\)	T52WB
\({}_{24}\mathrm{Cr}\)	55+	3.52 min	\(3/2\)	T52DA	\(-0.66\pm9\)	T52DA
\({}_{24}\mathrm{Cr}\)		\(\nu_{53}/\nu_D=0.368\,20\pm3\) R53JS			\(\nu_{53}/\nu_{14}=0.782\,26\pm5\) R53AH
\({}_{25}\mathrm{Mn}\)	52+	6.0 days	5	N52GH, T54HC, T54SC			—
\({}_{25}\mathrm{Mn}\)	55	100%	\(5/2\)	50MA, X51BI, X51BE, X50AK, X50ES, W52JT, X54UE	\(3.467\,53\pm17\) corr.	50MA, R50PR, R51PY, R51SW	\(0.4\pm2\)	W53JT, T53TR, S53MW
\({}_{25}\mathrm{Mn}\)	56+	2.58 h	\(3\pm1\)	N54KB
\({}_{25}\mathrm{Mn}\)		\(\nu_{55}/\nu_{\mathrm H}=0.247\,86\pm12\) R50SC			\(\nu_{55}/\nu_{\mathrm{Na}^{23}}=0.937\,2\pm1\) R50PR, R51PY
\({}_{25}\mathrm{Mn}\)		\(\nu_{55}/\nu_{\mathrm{Sc}^{45}}=1.020\,28\pm5\) R51SW

\(Z\)	\(A\)	\(\rho\%\) or \(T_{1/2}\)	\(I\) (\(\hbar\))	Literature data	\(\mu\) nuclear magnetons	Literature data	\(Q\) \((e \cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{26}\mathrm{Fe}\)	\(53^{\dagger}\)	8.9 min	\(7/2\)	T52DA	\(-1.20 \pm 12\)	T52DA
\({}_{26}\mathrm{Fe}\)	\(55^{\dagger}\)	2.94 yr	\(3/2\)	T52DA	\(-0.85 \pm 9\)	T52DA
\({}_{26}\mathrm{Fe}\)	57	2.21%	\(\leq 5/2;\ \neq 1/2\)	T51ST, T52DA, T53WA, X54BT, N54KB	\(<0.05\)	50MA, T51ST, T52DA, X54BT	\((0.10)\)	T52WB
\({}_{26}\mathrm{Fe}\)	\(59^{\dagger}\)	45.1 d	\(3/2\)	T52DA	\(-0.10 \pm 9\)	T52DA	—	—
\({}_{27}\mathrm{Co}\)	\(55^{\dagger}\)	18.1 h	\(7/2\)	N54CM
\({}_{27}\mathrm{Co}\)	\(56^{\dagger}\)	80 d	(5)	N53MT
\({}_{27}\mathrm{Co}\)	\(57^{\dagger}\)	270 d	\(7/2\)	X53BB	\(\lvert 4.6 \pm 2\rvert\)	X53BB
\({}_{27}\mathrm{Co}\)	\(58^{\dagger}\)	72 d	2	N50SH, N52GA, N52DG	\(\lvert 3.5 \pm 3\rvert\)	N52GA, N52DG
\({}_{27}\mathrm{Co}\)	59	100%	\(7/2\)	50MA, X51BK, X51BE, R50PR, R51PY	\(4.639\,9 \pm 9\)	50MA, R50PR, R51PY
\({}_{27}\mathrm{Co}\)	\(60^{\dagger}\)	5.24 yr	\(5;4\)	N51DS, N52FN, N54KS	\(I=5;\ \mu=\lvert 3.5 \pm 5\rvert\)	N52BD, (N52DG), N52GT, N52GS, T52KI, N54BD	\(0.5 \pm 2\)	S53MW
\({}_{27}\mathrm{Co}\)	\(60^{\dagger}\)	5.24 yr	\(5;4\)	N51DS, N52FN, N54KS	\(I=4;\ \mu=3.5 \pm 5\ (3.2 \pm 5)\)	N54BD	\(0.5 \pm 2\)	S53MW

Element	Mass number	Half-life or abundance	Spin	References	Magnetic moment	References	Electric quadrupole moment	References
\({}_{28}\mathrm{Ni}\)	\(57+\)	\(36.4\) h	\(3/2\)	N51CM
\({}_{28}\mathrm{Ni}\)	\(59+\)	\(7.5\cdot 10^{4}\) yr	\(3/2\)	T52DA, N54ES	\(-0.66 \pm 9\)	T52DA
\({}_{28}\mathrm{Ni}\)	\(61\)	\(1.25\%\)	\(5/2\)	T51ST, T52DA, T53WA, N53SP	\(<0.25\)	50MA, S50KF, T51ST, T52DA
\({}_{29}\mathrm{Cu}\)	\(58+\)	\(7.9\) min or \(3.04\) s \(3.04\) s	\((1)\)	T54MP
\({}_{29}\mathrm{Cu}\)	\(60+\)	\(24.6\) min	\(2\)	N54NV
\({}_{29}\mathrm{Cu}\)	\(62+\)	\(10.1\) min	\(0;\ 1\)	T52MA, N54NW,
\({}_{29}\mathrm{Cu}\)	\(63\)	\(68.94\%\)	\(3/2\)	50MA, X51BE	\(2.226\,28 \pm 13\ \mathrm{cor}\)	50MA, R51SW	\(-0.157 \pm 31\)	50MA, (T51SR, T52SR), T51AP, Q51BE, X51BU, (T52KL), S53KS, X53BT
\({}_{29}\mathrm{Cu}\)	\(64+\)		\(1\)	A54LP, N54KB	\(\lvert 0.40 \pm 5\rvert\)	A54LP
\({}_{29}\mathrm{Cu}\)	\(65\)	\(31.1\%\)	\(3/2\)	50MA, X51BE	\(2.385\,94 \pm 13\ \mathrm{cor}\)	50MA, R51SW	\(-0.145 \pm 29\)	50MA, (T51SR, T52SR), T51AP, Q51BE, X51BU, (T52KL), X53BT
\({}_{29}\mathrm{Cu}\)	\(66+\)	\(5.08\) min	\((1)\)	T53MA, N54KB

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{30}\mathrm{Zn}\)	\(63^{+}\)	38.3 min	\(3/2\)	T52DA	\(-0.10 \pm 9\)	T52DA
\({}_{30}\mathrm{Zn}\)	64	48.89%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{30}\mathrm{Zn}\)	\(65^{+}\)	250 d	\(5/2\)	T52DA, N53PH, N54KB	\(-0.62 \pm 9^{*}\)	T52DA
\({}_{30}\mathrm{Zn}\)	66	27.81%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{30}\mathrm{Zn}\)	67	4.16%	\(5/2\)	50MA	\(0.873\,78 \pm 13\)	50MA, R52DV, R53WV
\({}_{30}\mathrm{Zn}\)	68	18.51%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{30}\mathrm{Zn}\)	\(69^{+}\)	57 min	\(1/2\)	T49FH, T51GS, T52DA, N53DD	0.48	T52DA
\({}_{30}\mathrm{Zn}\)		\(\gamma_{67}/\gamma_{\mathrm{N}^{14}} = 0.865\,80 \pm 1\) R52DV, R53WV
\({}_{31}\mathrm{Ga}\)	\(66^{+}\)	9.2 h	1	T53SK, N52MP		T53SK
\({}_{31}\mathrm{Ga}\)	\(67^{+}\)	3.26 d	\(3/2\)	N53KB
\({}_{31}\mathrm{Ga}\)	\(68^{+}\)	67 min	1	T53SK, N52MP		T53SK
\({}_{31}\mathrm{Ga}\)	69	60.2%	\(3/2\)	50MA	\(2.016\,7 \pm 11\) corr.	50MA	0.243 corr.	50MA, (T50SR, T52SR), T52KO
\({}_{31}\mathrm{Ga}\)	71	39.8%	\(3/2\)	50MA	\(2.561\,4 \pm 10\) corr.	50MA	0.152 corr.	50MA, (T50SR, T52SR), T52KO
\({}_{31}\mathrm{Ga}\)	\(73^{+}\)	4.9 h	\(3/2\)	N53HP
\({}_{31}\mathrm{Ga}\)		\((\gamma_{69}/\gamma_{71})_{Q}=1.586\,7 \pm 4\) Q53DM			\(\mu_{69}/\mu_{\mathrm{H}}\) see T50KS		\(\mu_{71}/\mu_{\mathrm{H}}\) see T50KS

Element	A	Half-life / abundance	I	References	μ	References	Q	References
\({}_{32}\mathrm{Ge}\)	\(67^{+}\)	20 min	3/2	T52DA	\(-0.62 \pm 9\)	T52DA	\(\lvert < 7 \cdot 10^{-3} \rvert\)	50MA, W51MA
\({}_{32}\mathrm{Ge}\)	70	20.52%	0	50MA, W50ST, W51MA
\({}_{32}\mathrm{Ge}\)	\(71^{+}\)	11 d	1/2	T49FH, T52DA, N53SV	\(0.48 \pm 7\)	T52DA
\({}_{32}\mathrm{Ge}\)	72	27.43%	0	50MA, W50ST, W51MA			\(\lvert < 7 \cdot 10^{-3} \rvert\)	50MA, W51MA
\({}_{32}\mathrm{Ge}\)	73	7.76%	9/2	50MA, W51MA	\(-0.876\,77 \pm 9\)	R53JL, R54AW	\(-0.22 \pm 10\) concord.	50MA, (T52SR) W51MA
\({}_{32}\mathrm{Ge}\)	74	36.54%	0	50MA, W50ST, W51MA			\(\lvert < 7 \cdot 10^{-3} \rvert\)	50MA, W51MA
\({}_{32}\mathrm{Ge}\)	\(75^{+}\)	80 min	(1/2)	N52SC
\({}_{32}\mathrm{Ge}\)	76	7.76%	0	50MA, W50ST, W51MA			\(\lvert < 7 \cdot 10^{-3} \rvert\)	50MA, W51MA
\({}_{32}\mathrm{Ge}\)	\(77^{+}\)	12 h	(7/2)	T52DA, N53HP	\(0.52 \pm 7\)	T52DA *)

Element	A	Half-life / abundance	I	References	μ	References	Q	References
\({}_{33}\mathrm{As}\)	\(72^{+}\)	25.8 h	2	T53SK		T53SK
\({}_{33}\mathrm{As}\)	\(73^{+}\)	76 d	(3/2; 5/2)	N53BB
\({}_{33}\mathrm{As}\)	75	100%	3/2	50MA, R52JE	\(1.438\,93\) \(\pm 8\) concord.	50MA, R51DW R52JE, Q52KB R53WV, R53TW	\(0.3 \pm 2\) concord.	50MA, (T52SR)

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e \cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{33}\mathrm{As}\)	\(76^{+}\)	\(26.8\ \mathrm{h}\)	\(2\)	N53HP
\({}_{33}\mathrm{As}\)	\(77^{+}\)	\(38.7\ \mathrm{h}\)	\(3/2\)	N52SA
\({}_{33}\mathrm{As}\)		\(\nu_{75}/\nu_{\mathrm H}=0.17129 \pm 3\)		R52JE, R53TW	\(\nu_{75}/\nu_{\mathrm D}=1.11569 \pm 5\)	R53TW	\(\nu_{75}/\nu_{\mathrm{Na}^{23}}=0.64745 \pm 15\)	R51DW, R53WV
\({}_{34}\mathrm{Se}\)	\(73^{+}\)	\(7.1\ \mathrm{h}\)	\(1/2\)	T52DA	\(0.48 \pm 7\)	T52DA
\({}_{34}\mathrm{Se}\)	\(74\)	\(0.87\%\)	\(0\)	50MA, W50GM			\(\lvert <2 \cdot 10^{-3} \rvert\)	W50GM
\({}_{34}\mathrm{Se}\)	\(75^{+}\)	\(127\ \mathrm{y}\)	\(5/2\)	N52SC, N54JI, W54AS	\(-1.61 \pm 14^{*)}\)	T52DA	\(0.9\)	W54AS
\({}_{34}\mathrm{Se}\)	\(76\)	\(9.02\%\)	\(0\)	50MA, W50GM	\(\approx 0\)	50MA	\(\lvert <2 \cdot 10^{-3} \rvert\)	50MA, W50GM
\({}_{34}\mathrm{Se}\)	\(77\)	\(7.58\%\)	\(1/2\)	50MA, W50GM, B51DJ, N51CH, B54DV	\(0.53326 \pm 5\)	R52DW, R53WV	\(\lvert <2 \cdot 10^{-3} \rvert\)	50MA, W50GM
\({}_{34}\mathrm{Se}\)	\(78\)	\(23.5\%\)	\(0\)	50MA, W50GM, B54DV, B51DJ	\(\approx 0\)	50MA	\(\lvert <2 \cdot 10^{-3} \rvert\)	50MA, W50GM
\({}_{34}\mathrm{Se}\)	\(79^{+}\)	\(<6.5 \cdot 10^{4}\ \mathrm{y}\)	\(7/2\)	W52HS, W53HS	\(-1.015 \pm 15\)	W53HS	\(0.7 \pm 1\)	W52HS, W53HS, W54BT
\({}_{34}\mathrm{Se}\)	\(80\)	\(49.82\%\)	\(0\)	50MA, W50GM, B54DV	\(\approx 0\)	50MA	\(\lvert <2 \cdot 10^{-3} \rvert\)	50MA, W50GM
\({}_{34}\mathrm{Se}\)	\(81^{+}\)	\(17.5\ \mathrm{min}\)	\(1/2\)	T51GS, N52GH
\({}_{34}\mathrm{Se}\)	\(82\)	\(9.19\%\)	\(0\)	50MA, W50GM	\(\approx 0\)	50MA	\(\lvert <2 \cdot 10^{-3} \rvert\)	W50GM
\({}_{34}\mathrm{Se}\)	\(83^{+}\)	\(25\ \mathrm{min}\)	\((7/2);\ 9/2\)	T49FN
\({}_{34}\mathrm{Se}\)		\(\nu_{77}/\nu_{\mathrm D}=1.24211 \pm 10\)		R53WA	\(\nu_{77}/\nu_{\mathrm{Na}^{23}}=0.72193 \pm 2\)	R52DW, R53WV

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\,\mathrm{cm}^2)\)	Literature data
\({}_{37}\mathrm{Rb}\)	\(87+\)	\(6.25\cdot 10^{10}\) y	\(3/2\)	50MA, N52CD	\(2.749\,37 \pm 19\) corr	50MA, R51SW	\((0.170)\)	49GH, T52WB T52PI
\({}_{37}\mathrm{Rb}\)	\(88+\)	\(17.8\)	\(2\)	N52TL
\({}_{37}\mathrm{Rb}\)				\(\mu_{87}/\mu_{85}=2.033\,390\,5\pm75\) R51AB, R51YS, A52OK			\(Q_{85}/Q_{87}=2.07\pm1\) E50HG
\({}_{37}\mathrm{Rb}\)				\(\nu_{\mathrm{H}}/\nu_{85}=10.357\,105\pm30\) R51YS, R52WL			\(\nu_{\mathrm{H}}/\nu_{87}=3.0561\,097\pm55\) R51YS, R51WL, R51WS
\({}_{37}\mathrm{Rb}\)				\(\nu_{85}/\nu_{\mathrm{Cl}^{35}}=0.985\,41\pm15\) R52WL			\(\nu_{87}/\nu_{\mathrm{Al}^{27}}=1.255\,29\pm6\) R51SW
\({}_{37}\mathrm{Rb}\)				\(\nu_{\mathrm{V}^{50}}/\nu_{85}=1.032\,62\pm10\) R52WL			\(\nu_{\mathrm{B}^{10}}/\nu_{85}=1.112\,82\pm5\) R53TW
\({}_{37}\mathrm{Rb}\)				\(\nu_{\mathrm{N}^{14}}/\nu_{85}=0.748\,37\pm4\) R53TW
\({}_{38}\mathrm{Sr}\)	\(85+\)	\(65\) d	\(9/2\)	N52SM
\({}_{38}\mathrm{Sr}\)	\(86\)	\(9.75\%\)	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{38}\mathrm{Sr}\)	\(87\)	\(6.96\%\)	\(9/2\)	50MA	\(-1.089\,2\pm15\)	50MA, R53JS	\(0.85\)	T52WB
\({}_{38}\mathrm{Sr}\)	\(88\)	\(82.7\%\)	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{38}\mathrm{Sr}\)	\(89+\)	\(54.5\) d	\(5/2\)	T49FH, T50FE, T52DA, N52GH	\(-0.58\pm11\)	T52DA
\({}_{38}\mathrm{Sr}\)	\(90+\)	\(19.9\) y	\(0\)	T50FE
\({}_{38}\mathrm{Sr}\)	\(91+\)	\(9.67\) h	\(5/2\)	T50FE, N53SP
\({}_{38}\mathrm{Sr}\)				\(\nu_{87}/\nu_{\mathrm{D}}=0.282\,32\pm3\) R53JS

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(t_i)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\,\mathrm{cm}^2)\)	Literature data
\({}_{41}\mathrm{Nb}\)	\(94^{\dagger}\)	\(2.2\cdot 10^4\) yr	\((6; 7)\)	N52GH
\({}_{41}\mathrm{Nb}\)	\(95^{\dagger}\)	35 d	\(9/2\)	T51GS, N51SP
\({}_{41}\mathrm{Nb}\)	\(97^{\dagger}\)	72.1 min	\(9/2\)	T51GS, N52GH
\({}_{41}\mathrm{Nb}\)		\(\nu_{93}/\nu_{\mathrm{B}^{11}}=0.761\,87\pm40\)	R50SH			\(\nu_{93}/\nu_{45}=1.006\,13\pm5\) R51SW
\({}_{42}\mathrm{Mo}\)	92	15.8%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{42}\mathrm{Mo}\)	\(93^{\dagger}\)	\(>2\) yr	\((7/2)\)	T52DA, N53KH	\(0.83\pm6\)	T52DA
\({}_{42}\mathrm{Mo}\)	94	9.04%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{42}\mathrm{Mo}\)	95	15.72%	\(5/2\)	50MA, S50AE, S50AO, S50MK, R51PY, S54WO, N51SP	\(-0.909\,8\pm2\)	R51PY, S54WO
\({}_{42}\mathrm{Mo}\)	96	16.53%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{42}\mathrm{Mo}\)	97	9.46%	\(5/2\)	50MA, S50AE, S50AO, R51PY, S54WO	\(-0.928\,9\pm2\)	R51PY, S54WO	\((0.50)\)	T52WB
\({}_{42}\mathrm{Mo}\)	98	23.78%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{42}\mathrm{Mo}\)	\(99^{\dagger}\)	67 h	\(1/2\)	N54CK
\({}_{42}\mathrm{Mo}\)	100	9.63%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{42}\mathrm{Mo}\)		\(\nu_{97}/\nu_{95}=1.021\,0\pm1\)	R51PY, S51MC, S54WO			\(\lvert Q_{97}/Q_{95}\rvert>1\) R51PY
\({}_{42}\mathrm{Mo}\)		\(\nu_{97}/\nu_{\mathrm{N}^{14}}=0.920\,8\pm1\)	R51PY

Element	Isotope	Half-life or abundance	Spin	References	Value	References	Value	References
\(^{43}\mathrm{Tc}\)	\(93^{+}\)	2.7 h	\((9/2)\)	N54LN
\(^{43}\mathrm{Tc}\)	\(94^{+}\)	52.5 min	\((3)\)	N50MP
\(^{43}\mathrm{Tc}\)	\(95^{+}\)	20 h	\((9/2)\)	T51GS, N50MP
\(^{43}\mathrm{Tc}\)	\(96^{+}\)	104 h	\((3; 5; 6); 7\)	N53EM
\(^{43}\mathrm{Tc}\)	\(97^{+}\)	\(>10^{4}\) yr	\(9/2\)	T51GS, N54BY
\(^{43}\mathrm{Tc}\)	\(99^{+}\)	\(2.12\cdot10^{5}\) yr	\(9/2\)	S53MT	\(5.6805 \pm 4\) cor	R52WA, S53MT, (T52KL)	\(0.34 \pm 34\) *)	S53MT
\(^{44}\mathrm{Ru}\)	\(95^{+}\)	1.65 h	\(5/2,\ 7/2\)	T52DA		T52DA
\(^{44}\mathrm{Ru}\)	99	12.8%	\(5/2\)	N52GH, X52GO, S53MU	\(<0\)	S53MU	\((-0.84)\)	T52WB
\(^{44}\mathrm{Ru}\)	101	16.98%	\(5/2\)	X52GO, S53MU	\(<0\)	S53MU
\(^{44}\mathrm{Ru}\)	\(103^{+}\)	39.8 d	\((5/2)\)	T49FH, N52CM
\(^{44}\mathrm{Ru}\)	\(105^{+}\)	4.4 h	\((1/2)\)	N52GH
\(^{44}\mathrm{Ru}\)		\(\mu_{101}/\mu_{99}=1.09\pm3\)	X52GO
\(^{45}\mathrm{Rh}\)	103	100%	\(1/2\)	50MA, S51KW	\(\approx -0.10\pm3\)	50MA, S51KW, T52BE
\(^{45}\mathrm{Rh}\)	\(104^{+}\)	42 s	1	N53JC
\(^{45}\mathrm{Rh}\)	\(105^{+}\)	36.5 h	\((7/2)\)	N52GH
\(^{45}\mathrm{Rh}\)	\(106^{+}\)	30 s	1	N52GH

\(Z\)	\(A\)	p% or \(T_{1/2}\)	\(I\) \((\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data
\({}_{46}\mathrm{Pd}\)	\(103^\dagger\)	15.5 d	\(5/2\)	N54RB
\({}_{46}\mathrm{Pd}\)	105	22.2%	\(5/2\)	S52ST, S53BC	\(-0.57 \pm 5\)	S52ST, S53BC
\({}_{46}\mathrm{Pd}\)	\(107^\dagger\)	\(7 \cdot 10^6\) y	\((5/2)\)	N52GH
\({}_{46}\mathrm{Pd}\)	\(109^\dagger\)	13.1 h	\((5/2)\)	N52GH
\({}_{46}\mathrm{Pd}\)	\(111^\dagger\)	26 min	\(5/2;\ (1/2)\)	N51GN
\({}_{47}\mathrm{Ag}\)	\(103^\dagger\)	66 min	\(1/2\)	N54HW
\({}_{47}\mathrm{Ag}\)	\(106^\dagger\)	24 min	1	N53BS
\({}_{47}\mathrm{Ag}\)	107	51.35%	\(1/2\)	50MA, S50CK	\(-0.113\ 014 \pm 4\)	50MA, S50CK, S51BK, A53LW, R54BO, R54JS
\({}_{47}\mathrm{Ag}\)	\(108^\dagger\)	2.44 min	1	N53PB
\({}_{47}\mathrm{Ag}\)	109	48.65%	\(1/2\)	50MA, S50CK	\(-0.129\ 924 \pm 4\)	50MA, S50CK, S51BK, A53LW, R54BO, R54JS
\({}_{47}\mathrm{Ag}\)	\(110^\dagger\)	24 s	\((1)\)	T51GS, N52GH
\({}_{47}\mathrm{Ag}\)	\(111^\dagger\)	181 h	\(1/2\)	N51GN, A54LP	\(\lvert 0.144 \pm 7 \rvert\)	A54LP
\({}_{47}\mathrm{Ag}\)	\(112^\dagger\)	3.2 h	2	N53NW
\({}_{47}\mathrm{Ag}\)	\(113^\dagger\)	5.3 h	\((1/2)\)	N52GH
\({}_{47}\mathrm{Ag}\)	\(115^\dagger\)	20 min	\((1/2)\)	N52GH
\({}_{47}\mathrm{Ag}\)	\(\gamma_{109}/\gamma_{107}\)	\(\begin{cases}=1.149\ 61 \pm 4\ \text{(in metal)}\\=1.149\ 62 \pm 4\ \text{(in } \mathrm{AgNO}_3 \text{ in } \mathrm{H}_2\mathrm{O}\text{)}\end{cases}\)				S51BK, R54JS, R54BO

\(Z\)	\(A\)	p% or \(T_{1/2}\)	\(I\) \((\hbar)\)	Literature data	\(\mu\) nuclear magnet.	Literature data	\(Q\) \((e \cdot 10^{-24}\,\text{cm}^2)\)	Literature data
\({}_{49}\mathrm{In}\)	\(113^{+}\)	\(4,23\%\) \((>10^{12}\ \text{yr})\)	\(9/2\)	50MA	\(5,522\ 2\) \(\pm 5\) corr.	50MA, R51PY, R53TW	\(1,181\) corr.	50MA, (T50SR, T52SR), T52KO
\({}_{49}\mathrm{In}\)	\(114^{+}\)	\(72\ \text{s}\)	\(1\)	N52GH
\({}_{49}\mathrm{In}\)	\(115^{+*}\)	\(95,77\%\) \((6 \cdot 10^{14}\ \text{yr})\)	\(9/2\)	50MA	\(5,533\ 9 \pm 4\)	50MA, R51PY, R52TB, R53TW,	\(1,198\) corr.	50MA, (T50SR, T52SR), T52KO
\({}_{49}\mathrm{In}\)	\(116^{+}\)	\(13\ \text{s}\)	\((1)\)	N52GH
\({}_{49}\mathrm{In}\)	\(117^{+}\)	\(1,95\ \text{h}\)	\((1/2)\)	N52GH
\({}_{49}\mathrm{In}\)				\(\mu_{115}/\mu_{113}=1,002\ 13 \pm 4\) corr. R51PY, R53TW \(\nu_{115}/\nu_{\mathrm{Sc}^{45}}=0,901\ 877 \pm 50\) R52TB, R53TW			\(Q_{115}/Q_{113}=1,014\ 6\) A50KM \(\nu_{113}/\nu_{\mathrm{Na}^{23}}=0,826\ 67 \pm 8\) R51PY \(\nu_{115}/\nu_{\mathrm{Na}^{23}}=0,828\ 41 \pm 8\) R51PY
\({}_{50}\mathrm{Sn}\)	\(111^{+}\)	\(35,0\ \text{min}\)	\(7/2;\) \(9/2;\) \(11/2\)	N51GN				.
\({}_{50}\mathrm{Sn}\)	\(115\)	\(0,34\%\)	\(1/2\)	50MA, R50PY	\(-0,913\ 4 \pm 2\)	50MA, R50PY
\({}_{50}\mathrm{Sn}\)	\(116\)	\(14,2\%\)	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{50}\mathrm{Sn}\)	\(117\)	\(7,57\%\)	\(1/2\)	50MA, R50PY	\(-0,995\ 1 \pm 2\)	50MA, R50PY
\({}_{50}\mathrm{Sn}\)	\(118\)	\(24,0\%\)	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{50}\mathrm{Sn}\)	\(119\)	\(8,58\%\)	\(1/2\)	50MA, R50PY	\(-1,041\ 1 \pm 2\)	50MA, R50PY
\({}_{50}\mathrm{Sn}\)	\(120\)	\(33,0\%\)	\((0)\)	50MA	\(\approx 0\)	50MA

A	Half-life or abundance	Spin	References
\(121^{+}\)	27,5 h	\(3/2\)	50ND **)
\(123^{+}\) ***)	126 d	\((11/2)\)	N52GH
\(123^{+}\) ***)	40,0 min	\(3/2\)	N52GH
\(125^{+}\)	9,8 min	\((11/2)\)	N52GH

Element	A	Half-life or abundance	Spin	References		References		References
\({}_{51}\mathrm{Sb}\)	\(117^{+}\)	2,8 h	\((5/2)\)	N52GH
	121	57,3%	\(5/2\)	50MA, W51LS	\(3,359\,5\) \(\pm 4\) cor	50MA, R50PU, R50CK, R50CL, R51PY, (T52KL)	\(-0,52 \pm 10\)	50MA, (T52SR), W51LS, S53ST, S54MW
	\(122^{+}\)	2,80 d	2	T52MA, N52GH
	123	42,8%	\(7/2\)	50MA, W51LS	\(2,547\,0\) \(\pm 3\) cor	50MA, R50CK, R50PU, R51PY, (T52KL)	\(-0,67 \pm 10\)	50MA, (T52SR), W51LS, S53ST, S54MW
	\(124^{+}\)	60 d	\((3;4)\)	T51GS, T53SK, N53MZ, N54LZ		T53SK
	\(125^{+}\)	2,7 y	\(7/2\)	N52GH

\(Z\)	\(A\)	\(p\%\) or \(t_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e\cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{52}\mathrm{Te}\)	\(121^{+}\)	17 d	\(1/2\)	N52GH
\({}_{52}\mathrm{Te}\)	123	0.87%	\(1/2\)	50MA, S50FW, N49HL	\(-0.731\ 88 \pm 4\)	R51DV; S52RM, S53WV
\({}_{52}\mathrm{Te}\)	125	6.99%	\(1/2\)	50MA, S50FW	\(-0.882\ 35 \pm 4\)	R51DV, S52RM, R53WV
\({}_{52}\mathrm{Te}\)	126	18.72%	(0)	50MA	\(\approx 0\)	50MA
\({}_{52}\mathrm{Te}\)	\(127^{+}\)	9.3 h	\((3/2)\)	T51GS, N52GH	0.8	T49BE
\({}_{52}\mathrm{Te}\)	128	31.79%	(0)	50MA	\(\approx 0\)	50MA
\({}_{52}\mathrm{Te}\)	\(129^{+}\)	72 min	\((3/2)\)	N52GH	0.8	T49BE
\({}_{52}\mathrm{Te}\)	130	34.49%	(0)	50MA	\(\approx 0\)	50MA
\({}_{52}\mathrm{Te}\)	\(131^{+}\)	24.8 min	\((3/2)\)	N53HP	0.8	T49BE
\({}_{52}\mathrm{Te}\)	\(133^{+}\)	\(\approx 2\) min	\((3/2)\)	N52PP
\({}_{52}\mathrm{Te}\)		\(\nu_{125}/\nu_{123}=1.205\ 60 \pm 7\)		S50FW, R51DV, S52RM, R53WV.
\({}_{52}\mathrm{Te}\)		\(\nu_{123}/\nu_{\mathrm{Na}^{23}}=0.990\ 85 \pm 3\)		R51DV, R53WV		\(\nu_{125}/\nu_{\mathrm{Na}^{23}}=1.194\ 57 \pm 4\) R51DV, R53WV
\({}_{53}\mathrm{I}\)	\(125^{+}\)	60 d	\((5/2;\ 7/2)\)	N52BS
\({}_{53}\mathrm{I}\)	\(126^{+}\)	13 d	2	N54PW
\({}_{53}\mathrm{I}\)	127*)	100%	\(5/2\)	50MA, A53JS	\(2.808\ 38 \pm 13\ \mathrm{cor}\)	50MA, R51WL, R51YS, R51SW	\(-0.75 \pm 2\ \mathrm{cor}^{**})\)	50MA, (T52SR) T51GO, Q52KE S54MZ

Isotope	Half-life or abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
\(129^{+}\)	\(1.72\cdot 10^{7}\) yr	\(7/2\)	50MA	\(2.617\ 3\pm3\) agree.	50MA, R51WL	\(-0.47\)	50MA, (T52SR), T51GO
\(130^{+}\)	12.6 h	6	N54CM
\(131^{+}\)	8.14 d	\(7/2\)	W53LB, N52BR			\(-0.412^{***}\)	W53LB
\(133^{+}\)	22.4 h	\((7/2)\)	N52GH

Element	Isotope	Half-life or abundance	Spin	References	Magnetic moment	References	Quadrupole moment	References
\({}_{54}\mathrm{Xe}\)	\(127^{+}\)	32 d	\(1/2\)	T51GS
\({}_{54}\mathrm{Xe}\)	129	26.44%	\(1/2\)	50MA, S50KR	\(-0.772\ 55\pm5\)	50MA, R50PU, R51PY, R54BS
\({}_{54}\mathrm{Xe}\)	131	21.18%	\(3/2\)	50MR, S50KR, N54SF	\(0.686\ 80\pm2\)	50MA, R54BS	\(-0.12\) agree.	50MA, S50KR, S52BK
\({}_{54}\mathrm{Xe}\)	132	26.89%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{54}\mathrm{Xe}\)	\(133^{+}\)	5.27 d	\(3/2,\ 9/2,\ 11/2\)	T51GS, N52BS
\({}_{54}\mathrm{Xe}\)	134	10.44%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{54}\mathrm{Xe}\)	\(135^{+}\)	9.15 h	\(3/2\)	T51GS, N52GH
\({}_{54}\mathrm{Xe}\)	136	8.87%	\((0)\)	50MA	\(\approx 0\)	50MA

Z	A	p% or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e \cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{55}\mathrm{Cs}\)	\(127+\)	6.1 h	\((5/2)\)	N53WP
\({}_{55}\mathrm{Cs}\)	\(129+\)	31 h	\((5/2)\)	N53WP
\({}_{55}\mathrm{Cs}\)	\(130+\)	30 min	1	N52SB
\({}_{55}\mathrm{Cs}\)	\(131+\)	9.6 d	\((5/2)\)	A53SB, N52GH	\(3.48 \pm 4\)	A53SB
\({}_{55}\mathrm{Cs}\)	133	100%	\((7/2)\)	50MA *)	\(2.578\,77 \pm 12\) cor	50MA *) R51SW	\(-0.003\)	50MA, D54AK
\({}_{55}\mathrm{Cs}\)	\(134+\)	2.3 yr	4	Z52JB, A53SB	\(2.96 \pm 1\)	Z52JB, A53SB
\({}_{55}\mathrm{Cs}\)	\(134^n\)	3.1 h	8	A54CG, A54GW	\(\lvert 1.10 \pm 1\rvert\)	A54CG, A54GW
\({}_{55}\mathrm{Cs}\)	\(135+\)	\(2.1 \cdot 10^6\) yr	\(7/2\)	50MA, N52GH, N54SF	\(2.727\,1 \pm 33\) cor	50MA
\({}_{55}\mathrm{Cs}\)	\(137+\)	33 yr	\(7/2\)	50MA, N49PM	\(2.839\,7 \pm 30\) cor	50MA	\(\ll 0.2\)	49GH

Z	A	p% or \(T_{1/2}\)	\(I(\hbar)\)	Literature data	\(\mu\), nuclear magnetons	Literature data	\(Q\) \((e \cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{56}\mathrm{Ba}\)	\(133+\)	\(\approx 10\) yr	\(1/2\)	T51GS, N52GH,
\({}_{56}\mathrm{Ba}\)	134	2.42%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{56}\mathrm{Ba}\)	135	6.59%	\(3/2\)	50MA, S50AR	\(0.834\,6 \pm 25\) cor	50MA	\((0.51)\)	T52WB
\({}_{56}\mathrm{Ba}\)	136	7.81%	\((0)\)	50MA	\(\approx 0\)	50MA
\({}_{56}\mathrm{Ba}\)	137	11.32%	\(3/2\)	50MA, S50AR	\(0.935\,1 \pm 27\) cor	50MA	\((0.51)\)	T52WB
\({}_{56}\mathrm{Ba}\)	138	71.66%	\((0)\)	50MA	\(\approx 0\)	50MA


\({}^{57}\mathrm{La}\)	\(135^{+}\)	19 h	\((5/2)\)	N53WP
\({}^{57}\mathrm{La}\)	\(138^{+}\)	\(2.0\cdot 10^{11}\) yr	5	N52MK
\({}^{57}\mathrm{La}\)	139	99.9%	\(7/2\)	50MA	\(2.77802 \pm 18\) corr.	50MA, R51SW	\(0.9 \pm 1\)	49GH, 50MA, S53MW
\({}^{57}\mathrm{La}\)	\(140^{+}\)	40.0 h	3	N53HP
\({}^{57}\mathrm{La}\)	\(141^{+}\)	3.6 h	\(5/2;\ 7/2\)	N51DL
\({}^{57}\mathrm{La}\)		\(\gamma_{139}/\gamma_D = 0.920\)	\(25 \pm 6\)	R51SW
\({}^{58}\mathrm{Ce}\)	\(141^{+}\)	33.1 d	\(7/2\)	N51DL
\({}^{58}\mathrm{Ce}\)	\(143^{+}\)	33 h	\((5/2;\ 7/2;\ 9/2)\)	N51KH
\({}^{59}\mathrm{Pr}\)	\(140^{+}\)	3.4 min	1	N52BR
\({}^{59}\mathrm{Pr}\)	141	100%	\(5/2\)	50MA, X51DK, X52BE	\(3.9 \pm 3\) corr.	50MA, R50WS, (R51WS) A53LH, T53BX, S54MS	\(-0.054\)	A53LH, S54MS
\({}^{59}\mathrm{Pr}\)	\(142^{+}\)	19.2 h	2	N54PL
\({}^{59}\mathrm{Pr}\)	\(143^{+}\)	13.6 d	\(7/2\)	N51KH
\({}^{59}\mathrm{Pr}\)	\(144^{+}\)	17.5 min	1; 0	N52AK, N52PC,
\({}^{59}\mathrm{Pr}\)	\(146^{+}\)	24.4 min	3	N54BK

\(Z\)	\(A\)	\(p\%\) or \(T_{1/2}\)	\(I(h)\)	Literature data	\(\mu\) nuclear magn.	Literature data	\(Q\) \((e\cdot 10^{-24}\ \mathrm{cm}^2)\)	Literature data
\({}_{60}\mathrm{Nd}\)	142	27,09%	0	X50BE
\({}_{60}\mathrm{Nd}\)	143	12,14%	7/2	S51MU, X51BE, X50BE	\(-1,0 \pm 2\) cor	S51MU, (T52KL), T51ES, (T53ES), X54BE	\(\lvert 1\rvert\)	X52BA, T52WB, T51ES, (T53ES), X54BE
\({}_{60}\mathrm{Nd}\)	144	23,83%	0	X50BE
\({}_{60}\mathrm{Nd}\)	145	8,29%	7/2	S51MU, X51BE, X50BE	\(-0,65 \pm 9\) cor	S51MU, (T52KL), T51ES, (T53ES), X54BE	\(\lvert 1\rvert\)	X52BA, T51ES, (T53ES), X54KL
\({}_{60}\mathrm{Nd}\)	146	17,26%	0	X50BE
\({}_{60}\mathrm{Nd}\)	148	5,74%	0	X50BE
\({}_{60}\mathrm{Nd}\)	150	\(>2\cdot 10^{15}\) yr 5,63%	0	X50BE