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(1)

Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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ON THE HÖLDER CONTINUITY OF MATRIX

FUNCTIONS FOR NORMAL MATRICES

THOMAS P. WIHLER Mathematics Institute University of Bern

Sidlerstrasse 5, CH-3012 Bern Switzerland.

EMail:[email protected]

Received: 28 October, 2009

Accepted: 08 December, 2009

Communicated by: F. Zhang

2000 AMS Sub. Class.: 15A45, 15A60.

Key words: Matrix functions, stability bounds, Hölder continuity.

Abstract: In this note, we shall investigate the Hölder continuity of matrix functions ap-plied to normal matrices provided that the underlying scalar function is Hölder continuous. Furthermore, a few examples will be given.

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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Contents

1 Introduction 3

2 Proof of Theorem 1.1 6

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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1.

Introduction

We consider a scalar functionf :DCon a (possibly unbounded) subsetDof the

complex planeC. In this note, we shall be particularly interested in the case wheref

is Hölder continuous with exponentαonD, that is, there exists a constantα (0,1]

such that the quantity

(1.1) [f]α,D := sup

x,y∈D x6=y

|f(x)f(y)|

|xy|α

is bounded. We note that Hölder continuous functions are indeed continuous. More-over, they are Lipschitz continuous ifα = 1; cf., e.g., [4].

Let us extend this concept to functions of matrices. To this end, consider

Mnnormal×n (C) = ACn×n :AHA=AAH ,

the set of all normal matrices with complex entries. Here, for a matrixA= [aij]ni,j=1,

we use the notationAH = [a

ji]ni,j=1 to denote the conjugate transpose ofA. By the

spectral theorem normal matrices are unitarily diagonalizable, i.e., for each X

Mnnormal×n (C) there exists a unitary n × n-matrix U, UHU = U UH = 1 =

diag (1,1, . . . ,1), such that

UHXU = diag (λ1, λ2, . . . , λn),

where the setσ(X) ={λi}in=1is the spectrum ofX. For any functionf : D→C,

withσ(X)D, we can then define a corresponding matrix function “value” by

f(X) = Udiag (f(λ1), f(λ2), . . . , f(λn))UH;

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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We can now easily widen the definition (1.1) of Hölder continuity for a scalar functionf :D Cto its associated matrix functionf applied to normal matrices:

Given a subsetDMn×n

normal(C), then we say that the matrix functionf : D→C

n×n

is Hölder continuous with exponentα(0,1]onDif

(1.2) [f]α,D:= sup X,Y∈D

X6=Y

kf(X)f(Y)kF

kX YkαF

is bounded. Here, for a matrixX = [xij]ni,j=1 ∈ Cn

×n we define kXk

F to be the

Frobenius norm ofX given by

kXk2F = trace XHX =

n

X

i,j=1 |xij|

2

, X = (xij)ni,j=1 ∈M

n×n

(C).

Evidently, for the definition (1.2) to make sense, it is necessary to assume that the scalar functionf associated with the matrix functionf is well-defined on the spectra of all matricesX D, i.e.,

(1.3) [

X∈D

σ(X)D.

The goal of this note is to address the following question: Provided that a scalar functionf is Hölder continuous, what can be said about the Hölder continuity of the corresponding matrix functionf? The following theorem provides the answer:

Theorem 1.1. Let the scalar function f : D Cbe Hölder continuous with ex-ponentα (0,1], and D Mn×n

normal(C)satisfy (1.3). Then, the associated matrix

functionf : DCn×nis Hölder continuous with exponentαand

(1.4) [f]α,D≤n

1−α

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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holds true. In particular, the bound

(1.5) kf(X)f(Y)kF [f]α,Dn

1−α

2 kX−Ykα

F,

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

2.

Proof of Theorem

1.1

We shall check the inequality (1.5). From this (1.4) follows immediately. Consider two matrices X,Y D. Since they are normal we can find two unitary

matri-cesV,W Mn×n(C)which diagonalizeX andY, respectively, i.e., VHXV =DX= diag (λ1, λ2, . . . , λn),

WHY W =DY = diag (µ1, µ2, . . . , µn),

where{λi}ni=1 and {µi}ni=1 are the eigenvalues ofX andY, respectively. Now we

need to use the fact that the Frobenius norm is unitarily invariant. This means that for any matrixX Cn×nand any two unitary matricesR,U Cn×nthere holds

kRXUk2F =kXk2F.

Therefore, it follows that

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

In the same way, noting that

f(X) = Vf(DX)VH, f(Y) =Wf(DY)WH,

Employing the Hölder continuity off, i.e.,

|f(x)f(y)| ≤[f]α,D|x−y|α, x, y ∈D,

it follows that

(2.2) kf(X)f(Y)k2F [f]2

In the present situation this yields

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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Therefore, using the identity (2.1), there holds

kf(X)f(Y)kF [f]α,DkX −YkαF n

X

i,j=1

W

HV

i,j

2!

1−α

2

.

Then, recalling again thatk·kF is unitarily invariant, yields

n

X

i,j=1

W

HV

i,j

2!

1−α

2

= WHV

1−α

F =k1k

1−α

F =n

1−α

2 ,

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

We shall look at a few examples which fit in the framework of the previous analy-sis. Here, we consider the special case that all matrices are real and symmetric. In particular, they are normal and have only real eigenvalues.

Let us first study some functionsf : DR, whereDRis an interval, which

are continuously differentiable with bounded derivative onD. Then, by the mean value theorem, we have

[f]1,D = sup

i.e., such functions are Lipschitz continuous.

Trigonometric Functions:

Let m N. Then, the functions t 7→ sinm(t) and t

7→ cosm(t) are Lipschitz

continuous onR, with constant

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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Thence, we immediately obtain the bounds

ksinm(X)sinm(Y)kF √m

m1

m

m−1

kXYkF

kcosm(X)

−cosm(Y)

kF ≤

m

m1

m

m−1

kXYkF

for any real symmetricn×n-matricesX,Y. We note that

lim

m→∞

m1

m

m−1

=e−12,

and henceLm ∼√mwithm → ∞.

Gaussian Function:

For fixedm >0, the Gaussian functionf :t 7→exp(mt2

)is Lipschitz continuous onRwith constant[f]1,R =2mexp(1

2). Consequently, we have for the matrix

exponential that

exp(−mX

2

)exp(mY2)

F ≤

2me−12 kX −Yk

F,

for any real symmetricn×n-matricesX,Y.

We shall now consider some functions which are less smooth than in the previous examples. In particular, they are not differentiable at0.

Absolute Value Function:

Due to the triangle inequality

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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the absolute value functionf : t7→ |t|is Lipschitz continuous with constant[f]1,R= 1, and hence

(3.1) k|X||Y|kF ≤ kXYkF,

for any real symmetricn ×n-matrices X,Y. We note that, for general matrices, there is an additional factor of√2on the right hand side of (3.1), whereas for sym-metric matrices the factor 1 is optimal; see [1] and the references therein.

p-th Root of Positive Semi-Definite Matrices:

Finally, let us consider the p-th root (p > 1) of a real symmetric positive semi-definite matrix. The spectrum of such matrices belongs to the non-negative real axesD =R+ ={x R :x 0}. Here, we notice that the functionf : t 7→t1p is

Hölder continuous onDwith exponentα = 1

p and[f]p1,D = 1. Hence, Theorem1.1

applies. In particular, the inequality

(3.2)

X

1

p −Y

1

p

p

F ≤

np−21 kX−Yk

F

holds for any real symmetric positive-semidefiniten×n-matricesX,Y. We note that the estimate (3.2) is sharp. Indeed, there holds equality ifX is chosen to be the identity matrix, andY is the zero matrix.

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Hölder Continuity of Matrix Functions

Thomas P. Wihler

vol. 10, iss. 4, art. 91, 2009

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References

[1] H. ARAKI AND S. YAMAGAMI, An inequality for Hilbert-Schmidt norm,

Comm. Math. Phys., 81(1) (1981), 89–96.

[2] R. BHATIA, Matrix Analysis, Volume 169 of Graduate Texts in Mathematics, Springer-Verlag New York, 2007.

[3] Z. CHEN AND Z. HUAN, On the continuity of the mth root of a continuous nonnegative definite matrix-valued function, J. Math. Anal. Appl., 209 (1997), 60–66.

[4] D. GILBARGANDN.S. TRUDINGER, Elliptic partial differential equations of

second order, Classics in Mathematics, Springer-Verlag Berlin, 2001 (Reprint of

the 1998 edition).

[5] G.H. GOLUB AND C.F. VAN LOAN, Matrix Computations, Johns Hopkins

University Press, 3rd edition, 1996.

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