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(1)

MAURO NACINOVICH

Abstract. We consider Hermitian symmetric matrices H under the stan- dard action a

Ha of the complex linear group.

Rank and signature give a complete set of discrete invariants for a single Hermitian symmetric matrix.

For a pair (H

1

, H

2

) of Hermitian symmetric matrices, a complete set of invariants consists of the rank r, defined as the complement of the dimension of the intersection of their two kernels; of a set of minimal indices, that are positive integers that appear only when no linear com- bination aH

1

+ bH

2

has rank r; and by some relative eigenvalues, with multiplicities, of H

2

with respect to H

1

, that can be real, complex or in- finity (they are points of the complex projective line). This description is related to a canonical biorthogonal decomposition. The case of larger sets of linearly independent Hermitian matrices is an open question in algebra.

The linear groups act naturally on the space of matrices. We shall con- sider in the following the question of finding canonical forms for pairs of general and of Hermitian matrices. The use of a large group in the first case, and the special structure of the Hermitian matrices in the second, allow to reduce part of the discussion to the Jordan form of endomorphisms. How- ever, an extra feature appears, which is related to the Hilbert resolutions of polynomial modules, when we deal with singular pencils.

I used canonical forms for pairs of Hermitian matrices in the study of a class or real submanifolds of complex manifolds (see [4]).

We give two di fferent proofs of the main Theorem 2.8. The first utilize the canonical form for pencils of linear maps of [2], that we rehearse in §1.

In §4 we give an independent direct proof of Theorem 2.8, which allows to better understand the geometrical significance.

1. Pencils of linear maps

Denote by M m×n (C) the space of complex m × n matrices. The group G m,n (C) = GL m (C) × GL n (C) acts on M m×n (C) by

M m×n (C) × GL m,n (C) 3 (A, (α, β)) −→ αAβ −1 ∈ M m×n (C).

Canonical forms, through the associated invariants, are a tool to discuss the congruence of the subsets of M m×n (C) under the action of G m,n (C).

1

(2)

Remark 1.1. The only invariant of a single matrix A ∈ M m×n (C) is its rank.

A matrix A of rank r is congruent to

I r 0 r×(n−r)

0 (m−r)×r 0 (m−r)×(n−r)

! .

The next natural question, that we shall discuss in the following, is to find a canonical form for a pair of linearly independent linear maps. To describe the result, we shall essentially follow [2].

Since canonical forms for matrices correspond to canonical forms of their transposes, we can and we shall assume, in the following, that m ≤ n.

A pencil of complex matrices is a linear plane 1

hA 0 , A 1 i = {k 0 A 0 + k 1 A 1 | k 0 , k 1 ∈ C} ⊂ M m×n (C), where A 1 and A 2 are linearly independent matrices.

The pair A 0 , A 1 can be conveniently associated to the first degree poly- nomial A 0 + λA 1 ∈ M m×n (C)[λ], or to the corresponding affine line

{A(λ) = A 0 + λA 1 | λ ∈ C} ⊂ M m×n (C).

Definition 1.2. Let A 0 , A 1 ∈ M m×n (C) be complex m×n matrices, with m ≤ n.

We say that the pencil hA 0 , A 1 i is nondegenerate if

(1.1) ker A 0 ∩ ker A 1 = 0, Im A 0 + Im A 1 = C m .

Remark 1.3. By Grassmann intersection formula, a necessary condition for hA 0 , A 1 i ⊂ M m×n (C) being nondegenerate, is that n ≤ 2m.

We can always reduce the study of a pencil of complex matrices to the non degenerate case. We have indeed

Proposition 1.4. Let hA 0 , A 1 i ⊂ M m×n (C) be a degenerate pencil.

If k = dim ker A 0 ∩ ker A 1 > 0, ` = m − dim(Im A 0 + Im A 1 ), then we can find α ∈ GL(m, C), β ∈ GL(n, C) and A 0 0 , A 0 1 ∈ M (m−`)×(n−k) (C) such that hA 0 0 , A 0 1 i is nondegenerate and

(1.2) α(A 0 + λA 1 )β = 0 `×k 0 `×(n−k) 0 (m−`)`×k A 0 0 + λA 0 1

! .

Definition 1.5. Let A 0 , A 1 ∈ M m×n (C). The rank of the pencil hA 0 , A 1 i is (1.3) rankhA 0 , A 1 i = sup a ,b∈C rank(k 0 A 0 + k 1 A 1 ).

If either m , n, or rankhA 0 , A 1 i < n the pencil hA 0 , A 1 i is called singular.

If rank hA 0 , A 1 i < n, we say that the pencil hA 0 , A 1 i is singular for columns.

If rank hA 0 , A 1 i < m, we say that the pencil hA 0 , A 1 i is singular for rows.

If m = n and rankhA 0 , A 1 i = n the pencil hA 0 , A 1 i is called regular.

Remark 1.6. The rank of the pencil hA 0 , A 1 i is the generic rank of A(λ) = A 0 +λA 1 . This means that the set of λ ∈ C for which rank A(λ) < rankhA 0 , A 1 i is finite.

1 We may consider the pencil as a line in the projective space PM

m×n

(C) ' CP

mn−1

.

(3)

Example 1.7. Let A 0 =

 

 

 

 

0 0 0 0 0 1 1 0 0

 

 

 

 

, A 1 =

 

 

 

 

0 0 1 0 0 0 0 1 0

 

 

 

  .

Then

A(λ)

 

 

 

  z 1

z 2

z 3

 

 

 

 

=

 

 

 

  λz 3

z 3

z 1 + λz 2

 

 

 

  . Thus hA 0 , A 1 i is nondegenerate, but

Im A(λ) = {z ∈ C 3 | λz 2 = z 1 }

has dimension 2 for all λ ∈ C. Therefore rank hA 0 , A 1 i = 2, and the pencil is singular.

1.1. Regular pencils.

Proposition 1.8. Assume that m = n and that the pencil hA 0 , A 1 i is regular.

Then we can find α, β ∈ GL(n, C) such that

(1.4) α(A 0 + λA 1 ) =

 

 

 

 

 

 

 

 J 1 (λ)

J 2 (λ) ...

J s (λ)

 

 

 

 

 

 

 

 where the matrices J h (λ) have either the form

(1.5) J λ r

h

h

(λ) =

 

 

 

 

 

 

 

 

 

 

λ + λ h 1 λ + λ h 1

... ...

λ + λ h 1 λ + λ h

 

 

 

 

 

 

 

 

 

 

∈ H r

h

×r

h

(C),

with λ h ∈ C, or

(1.6) J r

h

(λ) =

 

 

 

 

 

 

 

 

 

  0 λ

0 λ

... ...

0 λ

0

 

 

 

 

 

 

 

 

 

 

∈ H r

h

×r

h

(C).

Proof. By the assumption, we can fix a λ 0 ∈ C for which B = A(λ 0 ) = A 0 + λ 0 A 1 is invertible.

Then L 0 = A 0 B −1 and L 1 = A 1 B −1 are matrices corresponding to com- muting endomorphisms. Indeed, L 0 = I n − λ 0 L 1 .

Consider the decomposition

(1.7) C n = W 0 ⊕ W 1 , with W 0 = [

h∈N ker L h 1 , W 1 = \

h∈N

L h 1 (C n ).

(4)

Then L 1 is invertible on W 1 and nilpotent on W 0 . We claim that L 0 is invert- ible on W 0 .

Indeed, since [L 0 , L 1 ] = L 0 L 1 − L 1 L 0 = 0, we have L 0 (W 0 ) ⊂ W 0 . If L 0 and L 1 were both nilpotent on W 0 , then ker L 0 ∩ ker L 1 ∩ W 0 , 0 by Engel’s theorem. But this implies that ker A 0 ∩ ker A 1 , 0, contradicting the assumption that hA 0 , A 1 i is regular.

Consider

B 0 = A 1 A −1 0 | W

0

: W 0

L

−10

−−→ W 0 −→ W L

1

0 ∈ End C (W 0 ), B 1 = A 0 A −1 1 | W

1

: W 1 L

−1

−−→ W

1

0 −→ W L

0

0 ∈ End C (W 1 ).

We note that B 0 is nilpotent. We can find a basis e 1 , . . . , e q of W 0 and a basis e q +1 , . . . , e n of W 1 in which the matrices of B 0 and B 1 are in Jordan form. Then A 0 e 1 , . . . , A 0 e q , A 1 e q +1 , . . . , A 1 e n is also a basis of C n and, in these bases, the matrices A(λ) have the desired form.  Definition 1.9. The string

1 , r 1 ), . . . , (λ s

0

, r s

0

), (∞, r s

0

+1 ), . . . , (∞, r s )

| {z }

r−r

0

 ,

where λ 1 , . . . , λ 0 s are the eigenvalues of B 1 , repeated with their multiplicity, r 1 , . . . , r s

0

the size of their Jordan blocks, and r s

0

+1 , . . . , r s the size of the Jordan blocks of B 0 , is said to be associated to the pair (A 0 , A 1 ).

1.2. Singular pencils. We turn now to the case of a singular pencil. Recall that we assumed m ≤ n.

Lemma 1.10. If the pencil hA 0 , A 1 i is singular for columns, then there is some non zero polynomial

z(λ) = z 0 + z 1 λ + · · · + z d λ d ∈ C d [λ]

such that

(1.8) (A 0 − λA 1 )z(λ) = 0.

Proof. Let C(λ) be the field of complex rational function of one variable.

By the assumption, A 0 − λA 1 defines a matrix in M m×n (C(λ)) having rank r less than n. Then dim C(λ) ker(A 0 − λA 1 ) = n − r > 0 and there exists Z(λ) ∈ [C(λ)] n \{0} such that (A 0 − λA 1 )Z(λ) = 0. We can write Z(λ) = (1/ f (λ))z(λ) with f (λ) ∈ C[λ] \ {0} and z(λ) ∈ C n [λ] \ {0}. Clearly z(λ) solves (1.8).  Remark 1.11. We note that (1.8) is equivalent to

(1.9)

 

 

 

 

A 0 z 0 = 0,

A 0 z j = A 1 z j−1 , for 1 ≤ j ≤ d,

0 = A 1 z d .

(5)

Equation (1.9) can be rewritten as

(1.10)

 

 

 

 

 

 

 

 

 

 

 

 

−A 0

A 1 −A 0

A 1 −A 0 ... ...

A 1 −A 0 A 1

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 z 0

z 1

z 2

...

z d−1

z d

 

 

 

 

 

 

 

 

 

 

 

 

= 0.

Consider the sequence of matrices

M 0 = −A 0 A 1

!

, M 1 =

 

 

 

 

−A 0 A 1 −A 0

A 1

 

 

 

 

, . . . , M d =

 

 

 

 

 

 

 

 

 

 

 

 

−A 0 A 1 −A 0

A 1 −A 0 ... ...

A 1 −A 0 A 1

 

 

 

 

 

 

 

 

 

 

 

 

 where M d is a matrix with m(d + 2) rows and n(d + 1) columns. Then a necessary and su fficient condition to find a non zero solution z(λ) of (1.8) of degree d is that the rank of M d be less than n(d + 1).

Definition 1.12. We denote by Z(A 0 , A 1 ) ⊂ C n [λ] the set of polynomial solutions of (1.8).

Lemma 1.13. The set Z(A 0 , A 1 ) is a C[λ]-module. This means that p 1 (λ)z 1 (λ) + p 2 (λ)z 2 (λ) ∈ Z(A 0 , A 1 ),

∀z 1 (λ), z 2 (λ) ∈ Z(A 0 , A 1 ) and p 1 (λ), p 2 (λ) ∈ C[λ].

Theorem 1.14. Let hA 0 , A 1 i be a nondegenerate singular pencil in M m×n (C) and let d be the smallest degree of a non zero polynomial in Z(A 0 , A 1 ). We have:

(1) If z(λ) = z 0 + · · · + λ d z d ∈ Z(A 0 , A 1 ) has minimal degree, then z 0 , . . . , z d are linearly independent,

A 0 z 1 , . . . , A 0 z d are linearly independent.

(2) We can find α ∈ GL(m, C), β ∈ GL(n, C) such that (1.11) α(A 0 + λA 1 )β = N d (λ)

A 0 0 + λA 1 0

!

where A 0 0 , A 0 1 ∈ M (m−d)×(n−d−1) (C) and

(1.12) N d (λ) =

 

 

 

 

 

 

 

 λ 1

λ 1 ... ...

λ 1

 

 

 

 

 

 

 

∈ M (d +1) (C).

(6)

Proof. Let z(λ) = z 0 + z 1 λ + · · · + z d λ d ∈ Z(A 0 , A 1 ) be a non zero solution of (1.8), with minimal degree. Note that d ≥ 1 because hA 0 , A 1 i is nonde- generate, and that z 0 , 0, because otherwise ζ(λ) = z 1 + z 2 λ + · · · + z d λ d−1 would be an element of Z(A 0 , A 1 ), with degree d−1 < d.

We divide the proof in several steps.

Step 1. A 0 z 1 , . . . , A 0 z d are linearly independent in C n . We first show that A 0 z 1 , 0. Otherwise,

0 = A 0 z 1 = A 1 z 0 =⇒ 0 , z 0 ∈ ker A 0 ∩ ker A 1 contradicts the assumption that hA 0 , A 1 i is nondegenerate.

Assume, by contradiction, that A 0 z 1 , . . . , A 0 z d are linearly dependent. Then there is a smallest h ≥ 2 for which A 0 z h is linearly dependent from {A 0 z i | 1 ≤ i < h}. Let

A 0 z h = a 1 A 0 z 1 + · · · + a h−1 A 0 z h−1 . This equation yields

A 1 z h−1 = a 1 A 1 z 0 + · · · + a h−1 A 1 z h−2 . Hence, setting

z h−1 = z h−1 − a 1 z 0 − · · · − a h−1 z h−2 we obtain

A 1 z h−1 = 0, A 0 z h−1 = A 1 (z h−2 − a 2 z 0 − · · · − a h−1 z h−3 ) = A 1 z h−2 , with

z h−2 = z h−2 − a 2 z 0 − · · · − a h−1 z h−3 . Let us define the chain

 

 

z 0 = z 0 ,

z h− j = z h− j − a j z 0 − a j +1 z 1 − . . . − a h−1 z h− j−1 for 1 ≤ j < h.

Then

 

 

 

 

A 0 z 0 = 0,

A 0 z j = A 1 z j−1 , for 1 ≤ j ≤ h − 1, 0 = A 1 z h−1 .

Indeed we already know that the first and the last equalities hold. For 2 ≤ j < h we obtain

A 0 z h− j = A 0 (z h− j − a j z 0 − a j +1 z 1 − . . . − a h−1 z h− j−1 )

= A 1 z h− j−1 − a j +1 A 1 z 0 − . . . − a h−1 A 1 z h− j−2

= A 1 z h− j−2 .

Hence z (λ) = z 0 + z 1 λ + · · · + z h−1 λ h−1 ∈ Z(A 0 , A 1 ), yielding a contradic- tion, because h−1 < d.

Step 2. z 0 , z 1 , . . . , z d are linearly independent.

Indeed, if a 0 z 0 + a 1 z 1 + · · · + a d z d = 0, we obtain a 1 A 0 z 1 + · · · a d A 0 z d = 0.

Hence a 1 = 0, . . ., a d = 0 by Step 1. Then a 0 z 0 = 0 implies that also a 0 = 0,

because z 0 , 0.

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Step 3. If

V =hz 0 , . . . , z d i ⊂ C n ,

W =hA 0 z 1 , . . . , A 0 z d i = hA 1 z 0 , . . . , A 1 z d−1 i ⊂ C m , we have A(λ)(V) = W for all λ ∈ C.

Choosing a new basis of C n in which the first d +1 vectors are z 0 , z 1 , . . . , z d , and a basis of C m in which the first vectors are A 0 z 1 , . . . , A 0 z d , we can as- sume that the matrices A 0 and A 1 have the form

A 0 = J d C 0

0 B 0

!

, A 1 = K d C 1

0 B 1

!

where J d = (δ i, j−1 ) 1≤i≤d,1≤ j≤d +1 , K d = (δ i, j ) 1≤i≤d,1≤ j≤d +1 ∈ M (d +1) (C) are the matrices

J d =

 

 

 

 

 

 

 

 

 

 

0 1 0 · · · 0 0 0 0 1 · · · 0 0 ... ... ... ... ... ...

0 0 0 · · · 1 0 0 0 0 · · · 0 1

 

 

 

 

 

 

 

 

 

 

, K d =

 

 

 

 

 

 

 

 

 

 

1 0 0 · · · 0 0 0 1 0 · · · 0 0 0 0 1 · · · 0 0 ... ... ... ... ... ...

0 0 0 · · · 1 0

 

 

 

 

 

 

 

 

 

  and C 0 , C 1 ∈ M (n−d−1) (C), B 0 , B 1 ∈ M (m−d)×(n−d−1) (C). Set

L(λ) = J d + λK d , C(λ) = C 0 + λC 1 , B(λ) = B 0 + λB 1 . Step 4. We conclude now the proof of the theorem.

To this aim we show that we can find matrices X ∈ M (d +1)×(m−d−1) (C) and Y ∈ M d× (n−d) (C) such that

I Y 0 I

! L(λ) C(λ) 0 B(λ)

! I −X

0 I

!

= L(λ) 0 0 B(λ)

! . This equation is equivalent to

(1.13)

 

 

L(λ)X = C(λ) + YB(λ),

X ∈ M (d +1)×(m−d−1) (C), Y ∈ M d× (n−d) (C).

Write

X =

 

 

 

 

  X 1

...

X d +1

 

 

 

 

 

, with X j ∈ M 1×(m−d−1) .

Then

L(λ)X =

 

 

 

 

  X 2

...

X d +1

 

 

 

 

  + λ

 

 

 

 

  X 1

...

X d−1

 

 

 

 

  .

Thus

U + λV =

 

 

 

 

  U 1

...

U d−1

 

 

 

 

  + λ

 

 

 

 

  V 1

...

V d−1

 

 

 

 

 

∈ L(λ)M (d +1)×(n−d−1)

(8)

if and only if

 

 

 

 

  U 1

...

U d−2

 

 

 

 

 

=

 

 

 

 

  V 2

...

V d−1

 

 

 

 

  .

Since

 

 

 

 

  U 1

...

U d−2

 

 

 

 

 

= K d−1

 

 

 

 

  U 1

...

U d−1

 

 

 

 

 

= K d−1 U,

 

 

 

 

  V 2

...

V d−1

 

 

 

 

 

= J d−1

 

 

 

 

  V 1

...

V d−1

 

 

 

 

 

= J d−1 V ,

this equation can be rewritten by

(K d−2 , −J d−1 ) U V

!

= 0.

Hence (1.13) admits a solution (X, Y) if and only if the equation 2 (1.14) J d−1 C 1 − K d−1 C 0 = K d−1 Y B 0 − J d−1 Y B 1 , Y ∈ M d×n−d

is solvable. Let us write

Y =

 

 

 

 

  y 1

...

y d

 

 

 

 

  with y j being an (n−d) row matrix. Then

K d−1 Y =

 

 

 

 

  y 1

...

y d−1

 

 

 

 

 

, J d−1 Y =

 

 

 

 

  y 2

...

y d

 

 

 

 

  ,

and the right hand side of (1.14) becomes

 

 

 

 

 

 

 

y 1 B 0 − y 2 B 1

y 2 B 0 − y 3 B 1

...

y d−1 B 0 − y d B 1

 

 

 

 

 

 

 

 .

This can also be written as

(1.15) (y 1 , y 2 , y 3 , . . . , y d−1 , y d )

 

 

 

 

 

 

 

 

 

 

 

 

 B 0

−B 1 B 0

−B 1 B 0 ... ...

−B 1 B 0

−B 1

 

 

 

 

 

 

 

 

 

 

 

 

 .

By the assumption that d is the minimal degree of a polynomial in Z(A 0 , A 1 ), the matrix M d−1 (B 0 , −B 1 ) in (1.15) has rank ≥ d(n − d − 1). Thus (1.14), and hence equation (1.13) is solvable for every C 0 , C 1 ∈ M d×(n−d−1) (C). This

completes the proof. 

2 We have K

d−1

J

d

= J

d−1

K

d

= (0

(d−1)×1

, I

d−1

, 0

(d−1)×1

) ∈ M

(d−1)×d+1

(C).

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Example 1.15. Consider the singular pencil of 1.7. We obtain

(A 0 − λA 1 )(λ)(z 0 + λz 1 ) = 0 with z 0 =

 

 

 

  0 1 0

 

 

 

 

, z 1 =

 

 

 

  1 0 0

 

 

 

  .

Taking in the domain the basis

 

 

 

  0 1 0

 

 

 

  ,

 

 

 

  1 0 0

 

 

 

  ,

 

 

 

  0 0 1

 

 

 

  ,

and in the codomain the basis

 

 

 

  0 0 1

 

 

 

  ,

 

 

 

  1 0 0

 

 

 

  ,

 

 

 

  0 1 0

 

 

 

  we obtain, in the new basis, the matrix

 

 

 

 

λ 1 0 0 0 λ 0 0 1

 

 

 

  .

Using Theorem 1.14, we obtain

Theorem 1.16. The C[λ] module N(A 0 , A 1 ) is free.

Proof. The statement means that there exists a set of generators z 1 (λ), . . . , z p (λ) ∈ N(A 0 , A 1 )

such that every element of N(A 0 , A 1 ) can be expressed in a unique way as a linear combination, with coe fficients in C[λ], of z 1 (λ), . . . , z p (λ). It can be obtained after reducing, by applying several times Theorem 1.14, to the case where

A(λ) =

 

 

 

 

 

 

 

 

 

  N d

1

(λ)

N d

2

(λ) ...

N d

p

(λ) B(λ)

 

 

 

 

 

 

 

 

 

 

with B(λ) nonsingular for columns. 

Definition 1.17 (minimal indices for columns). If hA 0 , A 1 i is a nondegener- ate singular pencil, the degrees

d 1 = deg z 1 (λ) ≤ d 2 = deg z 2 (λ) ≤ · · · d p = deg z p (λ).

of the elements z 1 (λ), . . . , z p (λ) of a basis of the free module N(A 0 , A 1 ), with P p

i =1 deg z i (λ) minimal are called the minimal indices for columns of

hA 0 , A 1 i.

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Definition 1.18 (minimal indices for rows). If hA t 0 , A t 1 i is a nondegenerate singular pencil, the degrees

d 1 0 = deg u 1 (λ) ≤ d 0 2 = deg u 2 (λ) ≤ · · · d q 0 = deg u q (λ).

of the elements u 1 (λ), . . . , u q (λ) of a basis of the free module N(A t 0 , A t 1 ), with P q

i =1 deg u i (λ) minimal are called the minimal indices for rows of hA 0 , A 1 i.

1.3. Canonical form of a pencil of linear maps. Let A 0 , A 1 ∈ M m×n (C) be linearly independent matrices. By Proposition 1.4, the orbit of A(λ) by G m,n (C) contains a matrix of the form

(1.16) 0 `×k 0 `×(n−k)

0 (m−`)×` A 0 (λ)

!

with A 0 (λ) = A 0 0 +λA 0 1 , and A 0 0 , A 0 1 ∈ M (m−`)×(n−k) and hA 0 0 , A 00 1 i nondegenerate.

Definition 1.19. The minimal indices for columns (respectively. for rows) of hA 0 0 , A 0 1 i are called the minimal indices for columns (respectively. for rows) of the pencil hA 0 , A 1 i.

Using Theorem 1.16 and Proposition 1.8 to decompose A 0 (λ), we con- clude that the orbit of A(λ) by G m,n (C) contains a matrix of the form

(1.17)

 

 

 

 

 

 

 0

B(λ) C(λ)

D(λ)

 

 

 

 

 

 

 ,

where 0 ∈ H `×k (C), with ` + dim(Im A 0 + Im A 1 ), k = dim(ker A 0 ∩ ker A 1 ), and B(λ), C(λ), D(λ) nondegenerate and, respectively, of the form

B(λ) =

 

 

 

 

  N d

1

(λ)

...

N d

p

(λ)

 

 

 

 

  ,

C(λ) =

 

 

 

 

 

  N d t

0

1

(λ) ...

N d t

0 q

(λ)

 

 

 

 

 

  ,

D(λ) =

 

 

 

 

  J 1 (λ)

...

J r (λ)

 

 

 

 

  ,

where (d 1 , . . . , d p ) are the minimal indices for columns, (d 0 1 , . . . , d 0 q ) the min- imal indices for rows, and the J h (λ) are described by (1.5) and (1.6).

Definition 1.20. The polynomials (λ − λ h ) r

h

, for J h (λ) of the form (1.5),

and the rational functions λ −r

h

for J h (λ) of the form (1.6), are called the

invariant factors of A(λ).

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Theorem 1.21 (Kronecker [3]). The integers k = dim(ker A 0 ∩ ker A 1 ), ` = dim(Im A 0 +Im A 1 ), the minimal indices for columns and for rows of hA 0 , A 1 i and the invariant factors of the pair (A 0 , A 1 ) are uniquely determined and characterize the orbit of A(λ) by GL m,n (C).

For the complete proof we refer to [2].

2. Pencils of Hermitian matrices

Let H n denote the space of n×n Hermitian symmetric matrices:

(2.1) H n = {H ∈ M n×n (C) | H = H},

where, for H = (h i, j ) 1≤i, j≤n the matrix H = (h i, j ) 1≤i, j≤n has entries h i, j = ¯h j,i . The set H n is an n 2 -dimensional real linear space of complex matrices.

The group GL n (C) acts on H n by

H n × GL n (C) 3 (H, α) −→ αHα ∈ H n .

Denote by Gr k (H n ) the Grassmannian of k-dimensional subspaces of H n

and by O k (H n ) the space of orbits of Gr k (H n ) for the action of GL n (C).

Given a k-tuple (H 1 , . . . , H k ) of linearly independent Hermitian symmet- ric forms, we denote by F =< H 1 , . . . , H k > the subspace of H n that they generate, and by [F] ∈ O k (H n ) the orbit of F.

More generally, we shall use the notation H(V) for the space of Hermitian symmetric forms on a finite dimensional complex linear space V and G C (V) for the group of linear automorphisms of V.

Definition 2.1. A linear subspace F ⊂ H n is called nondegenerate if (2.2) ∀v ∈ C n \ {0} ∃H ∈ F such that Hv , 0.

The subspace F is called regular if F contains a nondegenerate form H, and singular if all forms H ∈ F are degenerate.

Remark 2.2. Regular F’s are nondegenerate, but a nondegenerate F can be singular if dim R F ≥ 2.

Remark 2.3. For every H ∈ H n we can find α ∈ GL n (C) such that

(2.3) αHα =

 

 

 

  I p

−I q

0 (n−p−q)×(n−p−q)

 

 

 

  ,

where p + q is the rank of H and (p, q) its signature.

Other canonical forms for a Hermitian matrix use the matrices

J d =

 

 

 

 

· 1

·

·

1

 

 

 

 

∈ M d×d (C).

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A matrix H of signature (p, q), with dim ker H = k and ν = min(p, q), h = p + q − 2ν is equivalent to the matrix

±

 

 

 

 

 

 

J ν

I h

I ν

0

 

 

 

 

 

 

if h > 1, ± J p +q

0

!

if 0 ≤ h ≤ 1.

Note that, for h = 0, the two matrices with the plus and minus sign are equivalent.

Remark 2.4. If H 1 , H 2 ∈ H n and H 1 is positive definite, i.e. if v H 1 v > 0 for all v ∈ C n \ {0}, then there is α ∈ GL n (C) such that

αH 2 α =

 

 

 

 

 

 

 

 λ 1

λ 2

...

λ n

 

 

 

 

 

 

 

, with λ i ∈ R, αH 1 α = I n .

The real numbers λ 1 , . . . , λ n are the eigenvalues of H 2 with respect to H 1 , and in fact are the eigenvalues of the endomorphism H 1 −1 H 2 . Indeed, from (α ) −1 H 1 −1 α −1 = I n , we obtain that

 

 

 

 

 

 

 

 λ 1

λ 2 ...

λ n

 

 

 

 

 

 

 

= αH 2 α = (α ) −1 H 1 −1 α −1 αH 2 α = (α ) −1 (H 1 −1 H 2 .

The general case of a pair (H 1 , H 2 ) of Hermitian symmetric matrices is actually more complicated when no matrix in F = hH 1 , H 2 i R is positive definite.

The discussion relates to that for a pencil of linear maps by the following Theorem 2.5. Let (H 1 , H 2 ) and (K 1 , K 2 ) be two pairs of linearly indepen- dent Hermitian symmetric matrices in H n , and set H(λ) = H 2 + λH 1 , K(λ) = K 2 − λK 1 . Then the following are equivalent:

(1) ∃α, β ∈ GL n (C) such that αH(λ)β = K(λ);

(2) ∃α ∈ GL n (C) such that α H(λ)α = K(λ).

Proof. Clearly (2) ⇒ (1). Assume vice versa that there exist α, β ∈ GL n (C) such that

αH(λ)β = K(λ).

Since K 1 , K 2 are Hermitian symmetric, we also have β H(λ)α = K(λ).

With γ = α −1 β ∈ GL n (C), we obtain that γH(λ) = H(λ)γ . From this equality, it follows that

f (γ)H(λ) = H(λ) f (γ ), ∀ f ∈ C[λ].

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If we take f with real coe fficients, we have f (γ ) = [ f (γ)] . Take f ∈ R[λ]

with f (γ) ∈ GL n (C). Then we have

f (γ)H(λ)[ f (γ )] −1 = H(λ) and therefore

K(λ) = α f (γ)H(λ)[ f (γ )] −1 β.

We want to prove that f can be chosen in such a way that α f (γ) = [ f (γ )] −1 β = β [ f (γ)] −1 , i.e.

[ f (γ)] 2 = α −1 β = γ.

This is always possible, because γ ∈ GL n (C).  This Theorem reduces the classification of the pencils of Hermitian sym- metric forms to the results for pencils of linear maps, after recognizing the pairs of (H 1 , H 2 ) corresponding to canonical forms of H(λ) = H 2 + λH 1 . Indeed we have

Corollary 2.6. Two pairs of Hermitian forms (H 1 , H 2 ) and (K 1 , K 2 ) are equivalent if and only if they have the same invariant factors and minimal indices.

Remark 2.7. Note that for a pair of Hermitian matrices (H 1 , H 2 ) the rank for rows and the rank for columns coincide.

We have the following (see [1], [5]):

Theorem 2.8. Let H 1 , H 2 ∈ H n and assume that F = hH 1 , H 2 i R is a two- dimensional nondegenerate linear subspace of H n .

Then there is a direct sum decomposition:

(2.4) C n = V 1 ⊕ V 2 ⊕ · · · ⊕ V m

having the following properties:

(i) V i is orthogonal to V j for every 1 ≤ i , j ≤ m and every H ∈ F (biorthogonality);

(ii) for each i = 1, . . . , m the subspace V i is not a direct sum of two nontrivial subspaces that are orthogonal with respect to all the forms H ∈ F (indecomposability).

For each i = 1, . . . , m we can find a basis of V i such that, the restrictions of H 1 and H 2 to V i has one of the following forms:

(I) [H 1 | V

i

] = 

 

 

 

 

 

 

 

 

 

1

·

·

· 1

 

 

 

 

 

 

 

 

 

, [H 2 | V

i

] = 

 

 

 

 

 

 

 

 

 

γ

· 1

· ·

· · γ 1

 

 

 

 

 

 

 

 

  ,

which are e-square matrices for some positive integer e, where γ is a real

number and  = ±1;

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(II) [H 1 | V

i

] =

 

 

 

 

 

 

 

 

 

 

 0 E

· 1

·

· 1

· 1

·

· 1

0 E

 

 

 

 

 

 

 

 

 

 

, [H 2 | V

i

] =

 

 

 

 

 

 

 

 

 

 

  0 E

· 1 Γ

· · Γ 1 · · Γ ¯

· · · 1

¯ · · Γ 1

0 E

 

 

 

 

 

 

 

 

 

 

  ,

which are 2E-square matrices for a positive integer E, and where Γ is a complex number with Im Γ > 0;

(III) [H 1 | V

i

] = 

 

 

 

 

 

 

 

 

 

0

· 1

· ·

· · 0 1

 

 

 

 

 

 

 

 

 

, [H 2 | V

i

] = 

 

 

 

 

 

 

 

 

 

1

·

·

· 1

 

 

 

 

 

 

 

 

  ,

which are e-square matrices for a positive integer e;

(IV) [H 1 | V

i

] =

 

 

 

 

 

 

 

 

 

  0 d +1

1 ...

1 0 ··· 0

1 0

... ...

1 0

0 d

 

 

 

 

 

 

 

 

 

 

, [H 2 | V

i

] =

 

 

 

 

 

 

 

 

 

  0 d +1

0 ··· 0 1 ...

1 0 1 ... ...

0 1

0 d

 

 

 

 

 

 

 

 

 

  ,

which are (2d +1)-square matrices of odd size 2d+1 for a positive integer d.

The decomposition (2.4) is essentially unique: by this we mean that the number and the dimensions of the subspaces involved and also the kind of the blocks and the parameters involved are uniquely determined.

Definition 2.9. Let the basis (H 1 , H 2 ) of F be fixed.

A basis of C n , subordinated to a biorthogonal decomposition (2.4) and for which the matrices corresponding to H 1 and H 2 are block diagonal with blocks of the types (I), (II), (III) and (IV) described in the theorem, will be called canonical for the pair (H 1 , H 2 ).

The parameters  = ±1 appearing in the blocks of type (I) and (III) are called sign or inertial signature.

The parameters γ ∈ R appearing in the blocks of type (I), Γ and ¯Γ ap- pearing in the blocks of type (II), and ∞ if there are blocks of type (III), are called roots or eigenvalues of the pair (H 1 , H 2 ). The set Σ(H 1 , H 2 ) ⊂ CP 1 of all roots (including ∞ if there are blocks of type (III)), is called the spectrum of (H 1 , H 2 ).

The integers d characterizing the blocks of type (IV) are called the mini- mal indices of F. Note that they are independent of the choice of the basis (H 1 , H 2 ).

A block of type (III) for the basis (H 1 , H 2 ) becomes a block of type (I)

for the basis (H 2 , H 1 ). Accordingly, we shall distinguish only three types

of subspaces in the decomposition (2.4): a subspace V i will be called of the

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real type if it corresponds to blocks of the types (I) or (III); of the com- plex type if it corresponds to a block of type (II); of the singular type if it corresponds to a block of type (IV).

Proof. We note that the minimal indices for rows and columns of (H 1 , H 2 ) coincide, and that also roots and multiplicities of (H 1 , H 2 ) are invariant by conjugation. Then we can construct a Hermitian pair with the correct data

using blocks of the types I, II, III, IV,. 

3. The string of data

Having fixed a basis (H 1 , H 2 ) of F, by the preceding theorem we can have, in a canonical basis, a block decomposition of the matrices represent- ing the two forms into blocks of the types (I), (II), (III), (IV). We shall as- sociate to (H 1 , H 2 ) a string of data to describe the di fferent blocks; namely:

(1) we shall list the minimal indices in increasing order:

(3.1) d 1 < d 2 < · · · < d s

and denote by m i , for 1 ≤ i ≤ s, the number of singular subspaces of dimension 2d i + 1 of the decomposition (2.4);

(2) we shall list all eigenvalues Γ 1 , . . . , Γ L in Σ(H 1 , H 2 ) with Im Γ I > 0 for 1 ≤ I ≤ L, together with their complex conjugated, and we shall order the sizes 2E I,J of the blocks in which appear the parameters Γ I , ¯Γ I in decreasing order:

(3.2) E I,1 > E I,2 > · · · > E I,S

I

and denote by M I,J the number of blocks of size 2E I,J (for 1 ≤ I ≤ L, 1 ≤ J ≤ S I );

(3) finally we list all distinct eigenvalues γ 1 , . . . , γ ` ∈ R∪{∞} in Σ(H 1 , H 2 );

for each γ i , 1 ≤ i ≤ `, we list in decreasing order the sizes (3.3) e i,1 > e i,2 > · · · > e i,s

i

of the corresponding blocks of type (I) or (III) with parameter γ i

and denote by m + i, j , m i, j the number of those with  = 1,  = −1 respectively; we set m i, j for the sum m + i, j + m i, j .

We organize these informations, that describe all the invariants of the pair of Hermitian forms (H 1 , H 2 ), into its string of data:

(3.4) ∆(H 1 , H 2 ) =

 

 

 

 

 

 

 

 

 

 

 

 

 

 

d 1 , m 1 , . . . , d s , m s

Γ 1 , ¯Γ 1 , M 1,1 , . . . , M 1,S

1

. . .

Γ L , ¯Γ L , M L,1 , . . . , M L,S

L

γ 1 , e 1,1 , m + 1,1 , m 1,1 , . . . , e 1,s

1

, m + 1,s

1

, m 1,s . . .

1

γ ` , e `,1 , m + `,1 , m `,1 , . . . , e `,s

`

, m + `,s

`

, m `,s

`

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(16)

3.1. The e ffect of a change of basis in F. We consider the way in which the string of data changes if we change the basis of F. If (H 1 0 , H 2 0 ) is another basis, there is a matrix B = a b

c d

!

in GL 2 (R) such that

(3.5)

 

 

H 1 0 = aH 1 + bH 2 , H 2 0 = cH 1 + dH 2 .

The canonical form relative to (H 1 0 , H 0 2 ) has blocks of the same type (only those of type (I) and (III) can be changed one into the other), corresponding to a same biorthogonal decomposition (2.4). The string of data ∆(H 1 0 , H 2 0 ) is obtained from ∆(H 1 , H 2 ) by keeping all the integral parameters fixed, but changing the spectrum: Σ(H 1 0 , H 2 0 ) is obtained from Σ(H 1 , H 2 ) by letting

(3.6) −1 0

0 1

!

t B −1 −1 0

0 1

!

= d c b a

!

act as a real linear fractional transformation. This indeed trivially follows from

(3.7) H 2 0 − λ 0 H 1 0 = (d − λ 0 b)H 2 − (λ 0 a − c)H 1 ,

showing that the eigenvalues λ of the pair (H 1 , H 2 ) and λ 0 of (H 0 1 , H 2 0 ) are related by:

(3.8) λ = λ 0 a − c

d − λ 0 b , λ 0 = d λ + c b λ + a .

The inertial signatures remain the same or change to their opposite.

4. A direct proof of Theorem 2.8 It is convenient to introduce the notation:

V 0 = {w ∈ C n | w v = 0},

V = [H 1 (V)] 0 = {w ∈ C n | v H 1 w = 0, ∀v ∈ V}, V = [H 2 (V)] 0 = {w ∈ C n | v H 2 w = 0, ∀v ∈ V},

V y = V ∩ V = {w ∈ C n | v H 1 w = 0, v H 2 w = 0, ∀v ∈ V}.

4.1. The subspace N. Subspaces of the singular type appear in the decom- position (2.4) if and only if F is singular. We have indeed:

Proposition 4.1. Equation

(4.1) H(λ)z(λ) = (H 2 − λH 1 )z(λ) = 0, z(λ) = z 0 +λz 1 +· · ·+z d λ d ∈ C n [λ]

admits a non trivial solution if and only if hH 1 , H 2 i is singular.

(17)

Proof. The rank of hH 1 , H 2 i equals the rank of (H 2 − λH 1 ), considered as a matrix with coe fficients in the field C(λ) of rational functions. The equation

H(λ)z(λ) = (H 2 − λH 1 )z(λ), z (λ) ∈ [C(λ)] n has a non trivial solution if and only if

dim C(λ) ker H(λ) = n − rank C(λ) H(λ) > 0.

By chasing denominators, from any non tivial element of ker H(λ) in [C(λ)] n we obtain non trivial solutions of (4.1). This proves the proposition.  Remark 4.2. Equation (4.1) is equivalent to

(4.2)

 

 

 

 

H 2 z 0 = 0,

H 2 z j = H 1 z j−1 for 1 ≤ j ≤ m, 0 = H 1 z d ,

that can also be written as

(4.3)

 

 

 

 

 

 

 

 

 

 

 

 

−H 2

H 1 −H 2 H 1 −H 2

... ...

H 1 −H 2 H 1

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 z 0

z 1

z 2

...

z d−1

z d

 

 

 

 

 

 

 

 

 

 

 

 

= 0

where the left hand side is a matrix M d with n(d + 2) rows and and (d+1)n columns. Thus, the necessary and su fficient condition for the existence of a non trivial solution is that rank C M d < n(d+1).

Lemma 4.3. Let

z(λ) = z 0 + λz 1 + · · · + λ m z d ∈ C n [λ]

solve equation (4.1). Then the linear subspace hz 0 , z 1 , . . . , z d i generated by the coe fficients of z(λ) is totally isotropic for both H 1 and H 2 and hence for all H ∈ F = hH 1 , H 2 i.

Proof. We define z i for all i ∈ Z, by setting z i = 0 for i < 0 and i > d. Then (4.2) can be rewritten as

H 1 e i = H 2 e i +1 , ∀i ∈ Z.

Then we have

e i H 1 e j = e i H 2 e j +1 = e i−1 H 1 e j +1 = · · · = e i + j−d H 1 e d = 0, e i H 2 e j = e i−1 H 1 e j = e i−1 H 2 e j +1 = · · · = e 0 H 2 e i + j−d = 0,

for all i, j = 0, . . . , d. 

Definition 4.4. The set Z(H 1 , H 2 ) ⊂ C n [λ] of solutions of (4.1) is a module over the ring C[λ] of complex polynomials in one indeterminate.

Let N be the linear subspace of C n generated by the coe fficients of the

polynomials in Z(H 1 , H 2 ).

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Corollary 4.5. The subspace N is totally isotropic for all Hermitian matri- ces H ∈ F = hH 1 , H 2 i.

Proof. Let z 0 (λ), z 00 (λ) ∈ Z(H 1 , H 2 ). If z 0 has degree d 0 , we can consider the polynomial z 000 (λ) = z 0 (λ) + λ d

0

+1 z 00 (λ). It is still contained in Z(H 1 , H 2 ) and therefore the vector space generated by the coe fficients of z 0 (λ) and of z 00 (λ), being equal to the vector space generated by the coe fficients of z 000 (λ), is totally isotropic for all H ∈ F by Lemma 4.3.  Lemma 4.6. Let hH 1 , H 2 i be a nondegenerate singular pencil of Hermitian matrices and let

z(λ) = z 0 + λz 1 + · · · + λ d z d ∈ Z(H 1 , H 2 ) be a non trivial solution of (4.1) having minimal degree. Then

z 0 , z 1 , . . . , z d , H 2 z 1 , . . . , H 2 z d

are linearly independent.

Proof. Step 1. H 2 z 1 , . . . , H 2 z d are linearly independent in C n . We first show that H 2 z 1 , 0. Otherwise,

0 = H 2 z 1 = H 1 z 0 =⇒ 0 , z 0 ∈ ker H 2 ∩ ker H 1

contradicts the assumption that F is nondegenerate.

Assume, by contradiction, that H 2 z 1 , . . . , H 2 z d are linearly dependent.

Then there is a smallest integer h, with 2 ≤ h ≤ d, for which H 2 z h is linearly dependent from {H 2 z i | 1 ≤ i < h}. Let

H 2 z h = a 1 H 2 z 1 + · · · + a h−1 H 2 z h−1 . This equation yields

H 1 z h−1 = a 1 H 1 z 0 + · · · + a h−1 H 1 z h−2 . Hence, setting

z 0 h−1 = z h−1 − a 1 z 0 − · · · − a h−1 z h−2

we obtain

H 1 z 0 h−1 = 0, H 2 z 0 h−1 = H 1 (z h−2 − a 2 z 0 − · · · − a h−1 z h−3 ) = H 1 z 0 h−2 , with

z 0 h−2 = z h−2 − a 2 z 0 − · · · − a h−1 z h−3 . Let us define the chain

 

 

z 0 0 = z 0 ,

z 0 h− j = z h− j − a j z 0 − a j +1 z 1 − . . . − a h−1 z h− j−1 , for 1 ≤ j < h.

Then

 

 

 

 

H 2 z 0 0 = 0,

H 2 z 0 j = H 1 z 0 j−1 , for 1 ≤ j ≤ h − 1,

0 = H 1 z 0 h−1 .

Riferimenti

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