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Article

Distribution of Eigenvalues and Upper Bounds of the Spread of Interval Matrices

College of Mathematics, Physics and Data Science, Chongqing University of Science and Technology, Chongqing 401331, China
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Mathematics 2023, 11(19), 4032; https://doi.org/10.3390/math11194032
Submission received: 17 August 2023 / Revised: 14 September 2023 / Accepted: 20 September 2023 / Published: 22 September 2023
(This article belongs to the Special Issue Advances in Numerical Linear Algebra and Its Applications)

Abstract

:
The distribution of eigenvalues and the upper bounds for the spread of interval matrices are significant in various fields of mathematics and applied sciences, including linear algebra, numerical analysis, control theory, and combinatorial optimization. We present the distribution of eigenvalues within interval matrices and determine upper bounds for their spread using Geršgorin’s theorem. Specifically, through an equality for the variance of a discrete random variable, we derive upper bounds for the spread of symmetric interval matrices. Finally, we give three numerical examples to illustrate the effectiveness of our results.
MSC:
15A18; 05B20; 34L15

1. Introduction

The distribution of eigenvalues of complex matrices is a topic widely researched by some researchers (see Refs. [1,2]). However, in practical problems, matrix elements are often obtained through measurements and computations, which can produce perturbations due to round-off errors and measurement inaccuracies. Consequently, we cannot precisely determine the elements of a matrix. Instead, we can only establish upper and lower bounds for the intervals within which these elements are constrained. As a result, the eigenvalues of real interval matrices become uncertain due to the inherent uncertainties in the matrix elements. This uncertainty complicates the task of locating and estimating the eigenvalues of interval matrices. Recently, a growing number of researchers have begun to study the eigenvalues of interval matrices (see Refs. [3,4,5,6,7,8,9,10,11]).
Throughout this paper, t r ( A ) denotes the trace of matrix A; λ i ( A ) ( i = 1 , 2 , , n ) denotes the eigenvalues of the matrix; R e λ i ( A ) and I m λ i ( A ) stand for the real part and the imaginary part of λ i ( A ) , respectively; · F denotes a Frobenius norm, i.e., for a given n × n matrix A, A F 2 = i , j = 1 n | a i j | 2 ; and S n [ a , b ] denotes the set of n × n real symmetric matrices whose entries are in the interval [ a , b ] .
Let A I be a set of real matrices defined by [12]:
A I = A = ( a i j ) | a i j [ p i j , q i j ] , i , j = 1 , 2 , , n .
Let A A I , P = ( p i j ) , Q = ( q i j ) ( i , j = 1 , 2 , , n ) be real matrices; then, P A Q .
In 1956, Mirsky conducted the first study on the spread of a matrix in [13], denoted by
s ( A ) = max i , j | λ i ( A ) λ j ( A ) | , i , j = 1 , 2 , , n ,
and then, he obtained some meaningful inequalities of the spread of a matrix for normal and hermitian matrices (see Ref. [14]). The spread of an interval matrix is denoted by
s ( A I ) = max i , j | λ i ( A I ) λ j ( A I ) | , i , j = 1 , 2 , .
The real spread and the imaginary spread of an interval matrix are defined by
s R ( A I ) = max i , j | R e λ i ( A I ) R e λ j ( A I ) | , i , j = 1 , 2 , ,
s I ( A I ) = max i , j | I m λ i ( A I ) I m λ j ( A I ) | , i , j = 1 , 2 , .
Many researchers have studied the spread of matrices (see Refs. [1,15,16,17]). However, only a few of them were interested in the spread of interval matrices. In [11], upper bounds of the spread of real symmetric interval matrices were established; it has been shown that if A S n [ a , a ] with n 2 and a > 0 , then
s ( A ) 2 n a if n is even , 2 n 2 1 a if n is odd .
In this article, we focus on the distribution of the eigenvalues and upper bounds for the spread of interval matrices. In Section 2, we present the distribution for the eigenvalues of interval matrices based on Geršgorin’s theorem. In Section 3, we obtain some upper bounds of the spread of interval matrices and establish upper bounds for the spread of real symmetric interval matrices. In Section 4, we provide three numerical examples to illustrate the effectiveness of our results.

2. Distribution of the Eigenvalues of Interval Matrices

In this section, we present a theorem concerning the distribution of eigenvalues of interval matrices. To begin, we introduce the following lemma, which is Geršgorin’s theorem.
Lemma 1.
([18], Theorem 6.1.1). Let A = ( a i j ) be an n × n complex matrix; every eigenvalue λ i ( A ) , i = 1 , 2 , , n , must lie in at least one of n closed discs:
G ( A ) = λ ( A ) C | | λ ( A ) a i i | j = 1 j i n | a i j | , i = 1 , 2 , , n .
Based on Lemma 1, we obtain the distribution of eigenvalues of interval matrices using Geršgorin’s theorem.
Theorem 1.
Let A I = A = ( a i j ) | a i j [ p i j , q i j ] , i , j = 1 , 2 , , n be an n × n interval matrix and λ ( A I ) = λ i ( A ) | A A I , i = 1 , 2 , , n be the set of eigenvalues of A I :
G ( A I ) = λ C | | λ min p i i | max R i λ C | | λ max q i i | max R i
λ C | min p i i R e λ max q i i , | I m λ | max R i
where R i = j = 1 j i n max | p i j | , | q i j | , i , j = 1 , 2 , , n .
Then, λ ( A I ) G ( A I ) .
Proof. 
Applying the Geršgorin disc theorem, for any A = ( a i j ) A I , i , j = 1 , 2 , , n , every λ i ( A ) , i = 1 , 2 , , n must lie in at least one of n closed discs, i.e.,
| λ a i i | j = 1 j i n | a i j | R i , i = 1 , 2 , , n .
As a i i ( i = 1 , 2 , , n ) locates on the x axis, so we can obtain n small discs centered at a i i ( p i i a i i q i i ) and with radius R i . There is an annulus runway which is symmetric with respect to the x axis containing all the n small discs. We can express the annulus runway as follows:
λ C | | λ p i i | R i λ C | | λ q i i | R i
λ C | | p i i R e λ q i i , | I m λ | R i .
The significance of the above formula is shown in Figure 1.
For an n × n interval matrix A I , there are numerous annulus runways like Figure 1, containing all the eigenvalues of interval matrix A I , so we can use a single big annulus runway containing all the small annulus runways. We can express the big annulus runway as follows:
G ( A I ) = λ C | | λ min p i i | max R i λ C | | λ max q i i | max R i
λ C | min p i i R e λ max q i i , | I m λ | max R i .
The significance of the above formula is shown in Figure 2.
Thus, λ ( A I ) G ( A I ) , and the proof is completed. □
If all the elements of an interval matrix belong to the same interval, then an application of Theorem 1 can be seen in the following result.
Corollary 1.
Let A I = A = ( a i j ) | a i j [ a , b ] , i , j = 1 , 2 , , n be an n × n interval matrix and λ ( A I ) = λ i ( A ) | A A I , i = 1 , 2 , , n be the set of eigenvalues of A I :
G ( A I ) = λ C | | λ a | max R i λ C | | λ b | max R i
λ C | | a R e λ b , | I m λ | max R i
where R i = j = 1 j i n max | a | , | b | , max | a | , | b | is the maximum of | a i j | ( i j ) , i , j = 1 , 2 , , n .
Then, λ ( A I ) G ( A I ) .

3. The Spread of Interval Matrices

In this section, we give some upper bounds of the spread of general interval matrices and real symmetric interval matrices.
Based on Theorem 1, we have our first result for upper bounds of the spread of general interval matrices.
Theorem 2.
Let A I be an n × n interval matrix and the set of eigenvalues of A I : λ ( A I ) = λ i ( A ) | A A I , i = 1 , 2 , , n . Then,
s ( A I ) max q i i min p i i + 2 max R i , i = 1 , 2 , , n ,
s R ( A I ) max q i i min p i i + 2 max R i , i = 1 , 2 , , n ,
s I ( A I ) 2 max R i , i = 1 , 2 , , n .
Proof. 
In Theorem 1, we bind all eigenvalues of a given interval matrix in a single big annulus runway in the complex plane; then, the spread of s ( A I ) , s R ( A I ) must not exceed the major axis max q i i min p i i + 2 max R i in the annulus runway, that is
s ( A I ) max q i i min p i i + 2 max R i , i = 1 , 2 , , n ,
s R ( A I ) max q i i min p i i + 2 max R i , i = 1 , 2 , , n ,
s I ( A I ) must not exceed the minor axis 2 max R i in the annulus runway, that is
s I ( A I ) 2 max R i , i = 1 , 2 , , n .
The proof is completed. □
In order to obtain a better upper bound for the spread of interval matrices, we introduce a lemma from reference [13].
Lemma 2.
Let z 1 , z 2 , , z n be any complex numbers, and write
s = max i , j | z i z j | ;
then,
1 2 n s 2 1 i < j n | z i z j | 2 ,
with equality if and only if z 1 , z 2 , , z n satisfy condition φ.
Remark 1.
If n complex numbers z 1 , z 2 , , z n are such that n 2 among them are equal to each other and to the arithmetic mean of the remaining two, we shall say that the n numbers satisfy condition φ.
Based on inequality (2) in Lemma 2, we have another result about the upper bound for the spread of interval matrices.
Theorem 3.
Let A I be an n × n interval matrix and λ ( A I ) = λ i ( A ) | A A I , i = 1 , 2 , , n be the set of eigenvalues of A I ; then,
s ( A I ) 2 i , j = 1 n max | p i j | 2 , | q i j | 2 2 n m i n ( i = 1 n p i i ) 2 , ( i = 1 n q i i ) 2 1 2
Proof. 
According to inequality (2), for any matrix A A I , we can obtain
1 2 n [ s ( A ) ] 2 1 i < j n | λ i λ j | 2
for the eigenvalues λ 1 , λ 2 , , λ n of matrix A. By Lagrange’s identity, it follows that
1 i < j n | λ i λ j | 2 = n i = 1 n | λ i | 2 | i = 1 n λ i | 2 = n i = 1 n | λ i | 2 | t r A | 2 ;
thus,
1 2 n [ s ( A ) ] 2 n i = 1 n | λ i | 2 | t r A | 2 ,
and then,
s ( A ) ( 2 i = 1 n | λ i | 2 2 n | t r A | 2 ) 1 2 .
By the following inequality in [19],
i = 1 n | λ i | 2 A F 2 ;
then, we have
i = 1 n | λ i | 2 A F 2 = i , j = 1 n | a i j | 2 i , j = 1 n max | p i j | 2 , | q i j | 2 ,
| t r ( A ) | 2 m i n ( i = 1 n p i i ) 2 , ( i = 1 n q i i ) 2 ,
Apply inequalities (4) and (5) to (3), and we can obtain the following conclusion:
s ( A ) 2 i , j = 1 n max | p i j | 2 , | q i j | 2 2 n m i n ( i = 1 n p i i ) 2 , ( i = 1 n q i i ) 2 1 2 .
The above inequality holds for any matrix A A I . The proof is completed. □
Remark 2.
The upper bound of spread of Theorem 3 is more accurate than the result of Theorem 2.
Next, we will consider a special type of interval matrices whose entries are in the interval [ a , b ] . The following lemma about an equality for the variance of a discrete random variable is necessary.
Lemma 3.
([20], Lemma 1). Let x i be discrete random variables, P ( x = x i ) = p i , i = 1 , 2 , , n , and b = max i x i , a = min i x i , c = i = 1 n p i x i ; then,
V a r ( x ) = ( b c ) ( c a ) i = 1 n p i ( b x i ) ( x i a ) .
Based on inequality (3) and Lemma 3, we have the following theorem.
Theorem 4.
Let A = ( a i j ) S n [ a , b ] and n 2 , a < b ; then,
s ( A ) 2 ( n 2 n ) max a 2 , b 2 + n ( b a ) 2 2 i f n i s e v e n , 2 ( n 2 n ) max a 2 , b 2 + ( n 2 1 ) ( b a ) 2 2 n i f n i s o d d .
Proof. 
By inequality (3) and i = 1 n | λ i | 2 A F 2 , we have
s ( A ) 2 A F 2 2 n ( t r A ) 2 1 2 ,
Since the elements of A locate in the interval [ a , b ] , s ( A ) cannot attain the maximum until 2 A F 2 2 n ( t r A ) 2 1 2 attains the maximum. Without loss of generality, we have the following inequality:
s ( A ) 2 A F 2 2 n ( t r A ) 2 1 2 = 2 i , j = 1 n ( a i j ) 2 ( i = 1 n a i i ) 2 n 1 2 = 2 i , j = 1 j i n ( a i j ) 2 + i = 1 n ( a i i ) 2 ( i = 1 n a i i ) 2 n 1 2 .
So taking max | a | , | b | as the maximum of | a i j | ( i j ) , we obtain
max i , j = 1 j i n ( a i j ) 2 = ( n 2 n ) max a 2 , b 2 .
By the variance formula, then we have
1 n i = 1 n ( a i i ) 2 ( i = 1 n a i i ) 2 n = 1 n i = 1 n a i i i = 1 n a i i n 2 = V a r ( a i i ) ,
Combining (7) with Lemma 3, then
V a r ( a i i ) = ( b i = 1 n a i i n ) ( i = 1 n a i i n a ) i = 1 n 1 n ( b a i i ) ( a i i a ) ,
V a r ( a i i ) cannot achieve the maximum until ( b i = 1 n a i i / n ) ( i = 1 n a i i / n a ) attains the maximum and i = 1 n ( b a i i ) ( a i i a ) / n attains the minimum simultaneously.
If n is even, let ( b a i i ) ( a i i a ) = 0 ( ( b a i i ) ( a i i a ) 0 ) , that is a i i = b or a i i = a , i = 1 , 2 , , n . Now, we can consider ( b i = 1 n a i i / n ) ( i = 1 n a i i / n a ) as a function f ( i = 1 n a i i / n ) , and V a r ( a i i ) can achieve the maximum as i = 1 n a i i / n = ( a + b ) / 2 and a i i = b or a i i = a . Let 1 < m < n , a 11 = a , a 22 = a , , a m m = a , a m + 1 , m + 1 = b , , a n n = b ; then, ( m a + ( n m ) b ) / n = ( a + b ) / 2 , solving the equation m = n 2 , so we conclude that
max V a r ( a i i ) = ( b a ) 2 4 .
Considering (7), we have
i = 1 n a i i 2 ( i = 1 n a i i ) 2 n n ( b a ) 2 4 ,
Combining (6) with (8), we have
s ( A ) 2 ( n 2 n ) max a 2 , b 2 + n ( b a ) 2 2 .
If n is odd, let ( b a i i ) ( a i i a ) = 0 , that is a i i = b or a i i = a ( i = 1 , 2 , , n ) . Similar to n being even, m = ( n 1 ) / 2 , so we conclude that ( b i = 1 n a i i / n ) ( i = 1 n a i i / n a ) ( n 2 1 ) ( b a ) 2 4 n 2 , and then,
V a r ( a i i ) ( n 2 1 ) ( b a ) 2 4 n 2 ,
i = 1 n a i i 2 ( i = 1 n a i i ) 2 n ( n 2 1 ) ( b a ) 2 4 n ,
Combining (6) with (9), we have
s ( A ) 2 ( n 2 n ) max a 2 , b 2 + ( n 2 1 ) ( b a ) 2 2 n .
The proof is completed. □
Corollary 2.
Let A = ( a i j ) S n [ a , a ] and n 2 , a > 0 ; then,
s ( A ) 2 n a i f n i s e v e n , 2 n 3 2 n a i f n i s o d d .
Remark 3.
If n is even, the conclusion in Corollary 2 is the same as inequality (1), but we have provided a more concise proof.

4. Numerical Example

In this section, we will give several examples to illustrate the effectiveness of our results.
Example 1.
A I = [ 1 , 2 ] [ 0.5 , 1 ] [ 2 , 1 ] [ 3 , 1 ] [ 1 , 1 ] [ 0 , 1.5 ] [ 2.5 , 0.5 ] [ 0.5 , 1 ] [ 1 , 2 ] .
In interval matrix A I , we have min p i i = 1 , max q i i = 2 , max R i = 4.5 .
Choose a matrix A A I ,
A = 2 1 2 3 1 1.5 2.5 1 2 .
The eigenvalues of A are
λ 1 ( A ) = 4.1910 , λ 2 ( A ) = 0.5955 + 1.0662 i , λ 3 ( A ) = 0.5955 1.0662 i , ( i 2 = 1 ) ,
so we obtain
s ( A ) = 4.9029 .
From Theorem 1, we can obtain the following region:
G ( A I ) = λ C | | λ ( 1 ) | 4.5 λ C | | λ 2 | 4.5
λ C | 1 R e λ 2 , | I m λ | 4.5 .
Clearly, we can obtain λ i ( A ) G ( A I ) , i = 1 , 2 , 3 .
From Theorem 2, we have
s ( A I ) 9 , s R ( A I ) 9 , s I ( A I ) 6 .
From Theorem 3, we have
s ( A I ) 7.8952 ,
which provides a more precise estimation for the spread of interval matrices than Theorem 2.
Example 2.
Choose a matrix B S 3 ( 1 , 4 ) ,
B = 1 4 1 4 1 4 1 4 4 .
The eigenvalues of B are λ 1 ( B ) = 3.7163 , λ 2 ( B ) = 1.4680 , λ 3 ( B ) = 8.2483 ; then, we have
s ( B ) = 11.9646 .
From Corollary 1, we obtain the following region:
G ( S 3 [ 1 , 4 ] ) = λ C | | λ 1 | 8 λ C | | λ 4 | 8
λ C | 1 R e λ 4 , | I m λ | 8
Clearly, we can obtain λ i ( B ) G ( S 3 [ 1 , 4 ] ) , i = 1 , 2 , 3 .
From Theorem 2, we have
s ( S 3 [ 1 , 4 ] ) 19 , s R ( S 3 [ 1 , 4 ] ) 19 , s I ( S 3 [ 1 , 4 ] ) 16 .
From Theorem 3, we have
s ( S 3 [ 1 , 4 ] ) 16.7928 .
From Theorem 4, we have
s ( S 3 [ 1 , 4 ] ) 14.2828 ,
and the upper bounds of the spread is more precise than Theorems 2 and 3.
Example 3.
Choose a matrix C S 3 [ 2 , 2 ] and D S 4 [ 2 , 2 ] ,
C = 2 2 2 2 2 2 2 2 2 ,
D = 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 .
The eigenvalues of C are λ 1 ( C ) = 4 , λ 2 ( C ) = 2 , λ 3 ( C ) = 4 ; then, we have
s ( C ) = 8 ,
and the eigenvalues of D are
λ 1 ( D ) = 5.2263 , λ 2 ( D ) = 2.1648 , λ 3 ( D ) = 2.1648 , λ 4 ( D ) = 5.2263
Then,
s ( D ) = 10.4526 .
From Corollary 2, we have
s ( S 3 [ 2 , 2 ] ) 8.3266 , s ( S 4 [ 2 , 2 ] ) 11.3137 ,

5. Conclusions

We present the distribution of eigenvalues of interval matrices and establish upper bounds for their spread. Theorem 1 provide the distribution of eigenvalues of interval matrices. Theorems 2 and 3 both offer upper bounds for the spread of general interval matrices. Notably, the upper bound provided by Theorem 4 exhibits higher accuracy compared with that of Theorems 2 and 3. Theorem 4 introduces upper bounds for the spread of symmetric interval matrices, and we obtain the same inequality as (1) when n is even based on a simple proof.

Author Contributions

This work was carried out in collaboration between the authors. P.L. designed the study and guided the research. W.L. performed the analysis and wrote the first draft of the manuscript. P.L. and W.L. managed the analysis of the study. All authors have read and agreed to the published version of the manuscript.

Funding

This research was supported by the Science and Technology Research Program of Chongqing Municipal Education Commission (grant No. KJQN201901546 and No. KJQN201901518) and the Science and Technology Research Program of Chongqing Municipal Education Commission (grant No. KJQN202101536).

Institutional Review Board Statement

We certify that this manuscript is original and has not been published and will not be submitted elsewhere for publication while being considered by Mathematics. And, the study is not split up into several parts to increase the number of submissions and submitted to various journals or to one journal over time.

Data Availability Statement

Data sharing not applicable.

Acknowledgments

All authors are thankful to the honorable reviewers for their valuable suggestions and comments, which improved the paper.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. An annulus runway that contains all the small discs.
Figure 1. An annulus runway that contains all the small discs.
Mathematics 11 04032 g001
Figure 2. A single big annulus runway that contains the small annulus runways.
Figure 2. A single big annulus runway that contains the small annulus runways.
Mathematics 11 04032 g002
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Liao, W.; Long, P. Distribution of Eigenvalues and Upper Bounds of the Spread of Interval Matrices. Mathematics 2023, 11, 4032. https://doi.org/10.3390/math11194032

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Liao W, Long P. Distribution of Eigenvalues and Upper Bounds of the Spread of Interval Matrices. Mathematics. 2023; 11(19):4032. https://doi.org/10.3390/math11194032

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Liao, Wenshi, and Pujun Long. 2023. "Distribution of Eigenvalues and Upper Bounds of the Spread of Interval Matrices" Mathematics 11, no. 19: 4032. https://doi.org/10.3390/math11194032

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