Abstract Generated abstract
This paper develops an abstract notion of Lyapunov norm on a linear set, defined by order-valued homogeneity and ultrametric-type subadditivity conditions. It establishes basic properties of such norms in finite-dimensional subspaces, including the existence of a specially adapted basis whose linear combinations have norm equal to the greatest norm among the active basis elements. The paper further describes the classification of these bases via step matrices, the induced decomposition of a finite-dimensional space into nested hyperplane differences, and invariants under automorphisms preserving the Lyapunov norm. Examples connect the framework to Lyapunov characteristic numbers and related refinements used for solutions of homogeneous linear differential equations.
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Yu. S. Bogdanov
LYAPUNOV NORMS IN LINEAR SPACES
(Presented by Academician V. I. Smirnov on 6 X 1956)
MATHEMATICS
1°. Notation. Let us denote: \(A\) — a linear set, \(a\) — elements of \(A\); \(T\) — an automorphism of \(A\); \(B\) — an \(n\)-dimensional subspace of \(A\); \(b\) — elements of \(B\); \(\beta \equiv (b^1, b^2, \ldots, b^n)\) — a basis of \(B\); \(\Delta\) — an ordered set; \(\lambda\) — a mapping of \(A\) into \(\Delta\); \(c\) — a real number; \(C \equiv (c_j^i)\) — an \(n\)-dimensional matrix \((i\) — column number, \(j\) — row number\()\).
2°. Definition of a Lyapunov norm. We shall say that \(\lambda\) normizes \(A\) in the sense of Lyapunov if, for any \(a, a', c\):
1) \(\lambda(ca) \preceq \lambda(a)\);
2) \(\lambda(a+a') \preceq \max\{\lambda a,\lambda a'\}\).
The element \(\lambda a \in \Delta\) will be called the Lyapunov norm \(\lambda\) (or the \(\lambda\)-norm) of the element \(a \in A\).
3°. Properties of the Lyapunov norm. From the definition of the Lyapunov norm it follows:
a) \(c \ne 0 \to \lambda(ca)=\lambda a\);
b) \(\lambda a \succeq \lambda0\);
c) \(\lambda(c_1a^1+c_2a^2+\cdots+c_ma^m)=\preceq \max(\lambda a^1,\lambda a^2,\ldots,\lambda a^m)\);
d) \(c \ne 0,\ \lambda a \succ \lambda a^i\ (i=1,2,\ldots,m)\to \lambda(ca+c_1a^1+\cdots+c_ma^m)=\lambda a\);
e) \(\lambda a^i \ne \lambda a^j,\ i\ne j,\ a^i\ne0\ (i,j=1,2,\ldots,m)\to a^1,a^2,\ldots,a^m\) are linearly independent.
4°. The Lyapunov norm in a finite-dimensional linear space. Any \(m\) \((m>n)\) elements of \(B\) are linearly dependent, and therefore (see 3°, e)) the set \(\{\lambda b\}\), where \(b\) is any nonzero element of \(B\), has no more than \(n\) pairwise distinct elements.
5°. Definition of a \(\lambda\)-basis. A basis \(\beta\) of the set \(B\) will be called a \(\lambda\)-basis if every linear combination of the elements of \(\beta\) has a \(\lambda\)-norm equal to the greatest of the \(\lambda\)-norms of those elements of \(\beta\) which enter into the combination with coefficients different from 0.
6°. Existence of a \(\lambda\)-basis. Let \(\beta\) be a basis of \(B\). Then there exists a triangular matrix \(C\) with unit diagonal elements such that \(\beta_1=\beta_2C\) is a \(\lambda\)-basis of \(B\). The proof of the statement just made is carried out in the same way as the proof of Lyapunov’s theorem on the existence of a triangular matrix \(C\) transforming a given fundamental system of solutions of a system of homogeneous linear differential equations into a normal system of solutions \((^1)\).
7°. Properties of a \(\lambda\)-basis. Here and in the remaining paragraphs let \(\beta_1\) denote a \(\lambda\)-basis of \(B\); \(\beta_2\) a basis of \(B\), with any basis assumed to be written so that \(\lambda b_i^j \preceq \lambda b_i^l\), if \(j<l\) \((i,j=1,2,\ldots,n)\). Then:
a) \(0\ne b\in B\to \lambda b\in\{\lambda b_1^1,\lambda b_1^2,\ldots,\lambda b_1^n\}\);
b) \(\lambda b\preceq \lambda b_1^i\to b=c_1b_1^1+c_2b_1^2+\cdots+c_{i-1}b_1^{i-1};\)
c) in order that the basis \(\beta_2\) be a \(\lambda\)-basis of \(B\), it is necessary and sufficient that
\(\lambda b_2^i=\lambda b_1^i,\ i=1,2,\ldots,n\).
8°. The number of elements of a basis with one and the same \(\lambda\)-norm. Let \(k\) denote the number of mutually distinct values \(\lambda b_1^i\) \((i=1,2,\ldots,n)\). Suppose that these values are \(\delta_1,\delta_2,\ldots,\delta_k\), with \(\delta_i\succ \delta_j\) for \(i<j\). Suppose further that \(n_i\) is the greatest possible number of linearly independent elements of \(B\) with Lyapunov norm not exceeding \(\delta_i\). Denote by \(N_i(\beta_2)\) the number of elements of \(\beta_2\) with \(\lambda\)-norm \(\delta_i\). Then:
a) \(N_1(\beta_2)+N_2(\beta_2)+\cdots+N_k(\beta_2)=n\);
b) \(n_k=n,\ n_i<n_j\), if \(i<j\);
c) \(N_1(\beta_2)+N_2(\beta_2)+\cdots+N_i(\beta_2)\leq n_i\);
d) \(N_1(\beta_1)=n_1,\ N_i(\beta_1)=n_i-n_{i-1}\ (i=2,3,\ldots,k)\).
9°. Step matrices. A matrix \(C\equiv(c_j^i)\) will be called \(m_l;\,r\)-step if \(c_j^i=0\) for \(i\leq m_l<j\) for any \(l=1,2,\ldots,r;\ i,j=1,2,\ldots,n\) \((m_r=n)\). A triangular matrix is, evidently, \(l;\,n\)-step. All nonsingular \(m_l;\,r\)-step matrices (for fixed \(m_l\)) form a group with respect to multiplication in the usual sense for matrices.
10°. Transformation of a \(\lambda\)-basis. The basis \(\beta_2\), like any other system of \(n\) elements of \(B\), can be represented in the form \(\beta_2=\beta_1 C\), where \(C\) is a real matrix. The basis \(\beta_2\) will be a \(\lambda\)-basis if and only if \(C\) is an \(n_i;\,k\)-step nonsingular matrix. This can be proved by the same arguments by which the validity of the corresponding proposition is established for a normal system of solutions \((^2)\).
11°. The sets \(M_i\). Denote by \(M_i\) the set of all elements of \(B\) with \(\lambda\)-norm \(\delta_i\), where \(0\) is not included in \(M_1\), even if \(\lambda 0=\delta_1\). In addition, put \(M_0\equiv0\). Then:
a) \(M_i\cap M_j\) for \(i\ne j\);
b) \(M_0\cup M_1\cup\cdots\cup M_k=B\).
12°. The structure of \(M_i\). Each \(M_i\) is an \(n_i\)-dimensional hyperplane with the \(n_{i-1}\)-dimensional hyperplane removed. Indeed,
\[
M_0\cup M_1\cup\cdots\cup M_i=\bigcup \left(c_1 b_1^1+c_2 b_1^2+\cdots+c_{n_i}b_1^{n_i}\right)
\]
(the last sum is taken over all \(c_1,c_2,\ldots,c_{n_i}\in(-\infty,\infty)\)). The converse assertion is also true: if \(B\) is represented as the sum of hyperplanes \(P_0\equiv0;\ P_1,P_2,\ldots,P_m\), each of which strictly contains the preceding ones, then one can indicate a Lyapunov norm \(\lambda\) such that the decomposition of the space \(B\) into the sets \(M_1,M_2,\ldots,M_k\) effected by it has the property: \(k=m;\ M_i=P_i-P_{i-1}\ (i=1,2,\ldots,k)\).
13°. \(\lambda\)-similar transformations of \(A\). An automorphism \(T\) of the linear set \(A\): \(TA=A\), will be called a \(\lambda\)-similar transformation if
\[
\lambda a \preceq \max\{\lambda Ta,\lambda T^{-1}a\}.
\]
In order that \(T\) be a \(\lambda\)-similar transformation, it is necessary and sufficient that
\[
\lambda a=\lambda Ta=\lambda T^{-1}a
\]
(\(a\), as always, is any element of \(A\)).
14°. Invariants of \(\lambda\)-similar transformations. Under an automorphism \(T\) of the linear set \(A\), an \(n\)-dimensional linear subset \(B\subset A\) is transformed into an \(n\)-dimensional linear subset \(\widetilde B\subset A\). It is not difficult to show (based, for example, on 7°, c)) that if \(T\) is a \(\lambda\)-similar transformation, then the \(\lambda\)-basis \(\beta_1\) of the linear subset \(B\) under \(T\) passes into the \(\lambda\)-basis \(\widetilde\beta_1\) of the linear subset \(\widetilde B\), and moreover
\(\lambda_1 b_1^i=\lambda\widetilde b_1^i\ (i=1,2,\ldots,n)\). Thus the numbers \(n_i\) (see 8°) are invariants of all \(\lambda\)-similar transformations.
15°. Examples. The first example of a Lyapunov norm on the set of solutions of all possible systems of homogeneous linear differential equations specified for \(t \geqslant t_0\) is the Lyapunov characteristic number \((^3)\), taken with the opposite sign. As a second example one may point to the aggregate (characteristic exponent, type of solution) considered by L. Markus \((^4)\). In this case the second \([\lambda'']\)-norm refines the first \(\{\lambda'\}\), i.e.,
\[
\lambda'' a \supseteq \lambda'' a' \to \lambda' a \supseteq \lambda' a', \qquad
\lambda'' a \subseteq \lambda'' a' \to \lambda' a = \lambda' a' .
\]
Leningrad Branch
of the V. A. Steklov Mathematical Institute
Academy of Sciences of the USSR
Received
3 X 1956
REFERENCES
\(^{1}\) A. M. Lyapunov, The General Problem of the Stability of Motion, Moscow—Leningrad, 1950, pp. 48–50.
\(^{2}\) Yu. S. Bogdanov, DAN, 57, No. 3, 215 (1947).
\(^{3}\) A. M. Lyapunov, DAN, 57, No. 3, 39 (1947).
\(^{4}\) L. Markus, Math. Zs., 62, 310 (1955).