Добавил:
Upload Опубликованный материал нарушает ваши авторские права? Сообщите нам.
Вуз: Предмет: Файл:

0387986995Basic TheoryC

.pdf
Скачиваний:
23
Добавлен:
10.06.2015
Размер:
11.75 Mб
Скачать
are (01(x), 02(x), ... , On(x)) and (ti1(x),

418

XIII. SINGULARITIES OF THE SECOND KIND

Observation XIII-3-2. In order to prove that Oj (x)

0 (j = 1, 2,... , n) as

x -+ oo in Do(Nh'), use the fact that, for each positive integer k, the functions

4j (x) (j = 1, 2, ... , n) also satisfy the integral equations

 

Oj(x(k))exp

.(xr+1 _ (xok))r+1)I

 

1r+1

 

 

 

 

 

 

-JAI

 

+ f tTRj(t, i (t)) exp [r

(tr+l - xr+1) I dt

 

J

(XIII.3.2) uj(x) =

Ljc

 

 

 

(j E G1 U G2),

 

 

 

 

 

[r+i(tr+1

_xr+1)ldt

I

trR1(t,, (t))exp

 

 

JJ

 

UVG1UG2)

in the domain Do(Nk). Here, u(x) denotes the Cn-valued function whose entries are

(u1(x),u2(x),... ,un(x)). Note that we can assume Do(Nk) C Do(Nh') without loss of generality.

Upon applying successive approximations similar to those of §XII-3 together with Lemma XIII-2-6 to (XIII.3.2), it can be proved that (XIII.3.2) has a solution u,(x) = 0., (x) (j = 1,2,... ,n) such that IiP, (x) I < CkIxI-k U = 1,2,... ,n) in

Do(Nk), where Ck is a suitable positive number. Also, using Lemma XIII-2-6 and (XIII.2.13), it can be shown that ¢j (x) = ikj (x) (j = 1,2,... , n) in VO(Nk), since

Oj (x) - j (x) = j tr [RR (t, fi(t)) - Rj(t,,(t))I exp Ir +

1(tr+1 _ xr+1)l dt,

J

where j = 1, 2,... , n, and ¢(x) and tG(x) denote en-valued functions whose entries ,11 (x)), respectively. Thus, we

conclude that 0, (x) 0 (j = 1, 2,... , n) as x -' oo in Do(Nh,).

Now, let us return to Observation XIII-2-2. If we set pj(x) = Oj(x) + zj(x), the solution v , = pj(x) (j = 1, 2, ... , n) of (XIII.1.1) satisfies all of the requirements of

Theorem XIII-1-2. 0

Remark XIII-3-3. Let Ax, y', µ, e) be a Cn-valued function of a variable (x,

e)

E C x Cn x Cn x C such that

(a) the entries of f are bounded and holomorphic in a domain

Do = { (x, b, µ, e) : IxI > Ro, Iu-1 < do, lµl < p o, IeI < Eo, I arg EI < po},

where R0, 60, µo, co, and po are some positive constants,

(b) f admits a uniform asymptotic expansion in Do

r/x, a/, e) ti

+0

as e - 0,

Ehfh(x, . p)

s/

 

 

 

h=0

 

where coefficients fh (x, y, i) are single-valued, bounded, and holomorphic in the domain

Ao = {(x, 9, #) : IxI > Ro, I vi < 6o, Iµl < po},

3. PROOF OF THEOREM XIII-1-2

419

(c) if f (x, y, µ', e) = fo (x, #,c) + A(x, µ, e)y + O(I y12), then

fo(oo,µ',e) = 0

and

detA(oo,0,0) 0 0.

Let )q, A2, ... , )1n be n eigenvalues of A(oo, 0', 0) and set wf = arg A, (j _

1, 2, ... , n). Note that the w, are not unique. Set also S(pl, p2) _ {x : Pi < argx < p2}. Let a and r be two non-negative integers. Assume that the sector

S(pl, p2) is contained in the sector

32 - min{wj} + apo < (r+ 1)argx < 32 - max{wj} - apo

f o r a suitable choice of {wj : j = 1, 2, ... , n}.

Under these assumptions, we can prove the following theorem in a way similar to the proof of Theorem XIII-1-2.

Theorem XIII-3-4. The system e° fy = x"f (x,

c) has two solutions

¢(x, 91, e) and i (x, µ, e) such that

(i) these two solutions are bounded and holomorphic in the domain

So = {(x, 9, e) : Ix1 > N, x E S(p1, p2), 1141 < ul, 0 < IEI < e1,1 arg el < p0},

if p1 and E1 are sufficiently small,

(ii) the solution ¢(x, µ, e) admits an uniform asymptotic expansion

+oo

as x -. oo

F, x-k&(µ, e)

k=1

 

in So, where coefficients &(µ,e) are bounded, holomorphic, and admit uniform asymptotic expansions in powers of a as c -+ 0 in the domain {(µ, e)

Iµ1 < {31, 0 < lei < el, I argel < po},

(iii) the solution 1'(x, N, e) admits an uniform asymptotic expansion:

+oo

 

(x, , e) ' ehWh(x, µ)

as f -4 0

h=0

 

in So, where coefficients >Gh(x,#) are bounded, holomorphic, and admit uni- form asymptotic expansions in powers of x'1 as x - oo in the domain

{(x,µ') : Ixf > N, x E S(p1,p2), Jill < p1}.

FLrther more, there exist functions tc(x, µ, e) for t = 0,1, ... such that

(a) these functions ¢'c satisfy conditions (i) and (is) given above,

(b)

h=0

A complete proof of Theorem XIII-3-4 is found in [Si7J and (Si101.

420

XIII. SINGULARITIES OF THE SECOND KIND

Remark XIII-3-5. In the proof of Theorem XHI-1-2, we used the assumption that the matrix Ao on the right-hand side of (XIII.1.10) is invertible (cf. Assumption

III of §XIII-1). Without such an assumption, we can prove the following theorem.

Theorem XIII-3-6. Let F(x, yo, yr, ... , yn) be a nonzero polynomial in yo, yl,

,

 

00

 

yn whose coefficients are convergent power series in x'1, and let p(x) =

an,x-°`

E C[(x-1)) be a formal solution/ of the differential equation

M--0

 

 

 

(XIII.3.3)

F(x,y,Ly,..., fn)=0.

 

 

\arg

Then, for any given direction

x = 0, there exist two positive numbers 6 and a

and a function 0(x) such that

 

(i) ¢(x) is holomorphic in the sector S = {x E C:0< [xj <6, (arg x - 0[ < a},

(ii) 0(x) admits the formal solution p(x) as its asymptotic expansion as x

o0

in S,

(iii) 0(x) satisfies differential equation (XIII.3.3) in S.

The main idea of the proof is similar to the proof of Theorem XIII-1-2. However, we need the thorough knowledge of the structure of solutions of a linear system

xd = A(x)y that we shall explain in §XIII-6. Also, it is more difficult to define

the paths of integration (cf. [I] and (RS11). A complete proof of Theorem XIII-3-6 is found in [RS1). See, also, §XIII-8.

XIII-4. A block-diagonalization theorem

Consider a system of linear differential equations

(XIIi.4.1)

dg

= x' A(x}y,

 

dx

 

where r is a positive integer, y" E C', and A(x) is an n x n matrix. The entries of

A(x) are holomorphic with respect to a complex variable x in a sector

(XIII.4.2)

jxl > No,

f argx[ < ao,

where No and ao are positive numbers. Assume that the matrix A(x) admits an asymptotic expansion in the sense of Poincare

 

00

(X1II.4.3)

A(x) E x'"A

&'=o

as x - oo in sector (XIII.4.2), where coefficients A are constant n x n matrices.

Suppose also that Ao = A(oo) has a distinct eigenvalues A1, A2, ... , J1t with mul-

tiplicities n1, n2, ... , nt, respectively (nl + n2 +

+ nt = n). Without loss of

generality, assume that Ao is in a block-diagonal form:

()UII.4.4)

AO = diag [Al, A2, ... , At) ,

 

4. A BLOCK-DIAGONALIZATION THEOREM

421

where Aj are of x n, matrices in the form

 

 

(XIII.4.5)

A,

=A,In, +Nj

(j=1,2,...,1).

 

Here, A , is a lower-triangular nilpotent n, x n, matrix. The main result of this section is the following theorem (cf. (Si7J).

Theorem XIII-4-1. Under the assumption (XIIL4.3) and (XIII.4.4), there exists an n x n matrix P(x) whose entries are holomorphic in a sector

(XIII.4.6)

IxI > N1,

I argxj < al,

where Ni 1 and a1 are sufficiently small positive numbers, such that

(i) P(x) admits an asymptotic expansion

 

 

00

 

(XIII.4.7)

P(x)

Ex-"p-

(Pp = In),

 

 

"=0

 

as x -' oo in sector (X111.4.6), where coefficients P" are constant n x n matrices,

(ii) the transformation

(XIII.4.8)

y = P(x)zi

reduces system (X111.4.1) to

(XIII.4.9)

di = x, B(x)i,

where B(x) is in a block-diagonal form

(XIII.4.10)

B(x) = diag [BI (x), B2(x),... , Bt(x)J .

Hen, B,(x) an n, x n. matrices and admit asymptotic expanswns

 

00

(XIII.4.11)

B, (x) ^-- E xBj"

 

"=o

as x oo in (XIII.4.6), where coefficients B,, are constant n) x n) matrices.

Proof.

From (XIII.4.1), (XIII.4.8), and (XIII.4.9), we derive the equation

(XIII.4.12)

dP = xr(A(x)P - PB(x)]

 

that determines the matrices P(x) and B(x). Set

 

(XIII.4.13)

A(x) = Ao + E(x),

B(x) = A0 + F(x),

P(x) = In + Q(x).

422

XIII. SINGULARITIES OF THE SECOND KIND

Then, E(x) = O(x-1), F(x) = O(x'1), and Q(x) = O(x-1). Furthermore,

(XIII.4.12) becomes

(XIII.4.14)

dQ = x''[AoQ - QAo + E - F + EQ - QF].

 

dx

Write each of three matrices E(x), F(x), and Q(x) in a block-matrix form according to that of Ao in (XIII.4.4), i.e.,

(XIII.4.15)

F(x) = diag]Fl,F2,... ,Ft],

 

E11

E12 ...

Ell

Q11 Q12 ... Qlt

E21

E22 ...

E2t

 

E(x) _

 

 

Q(x) =

Ell E 2

Eu

Q11 Q2t

.

Qtt

 

where EJk and QJk are nJ X nk matrices and F, are nJ x nJ matrices. Set

(XIII.4.16)

QJJ = 0 (j = 1,2,... ,t).

From (XIII.4.4), (XIII.4.14), (XIII.4.15), and (XIII.4.16), it follows that

(XIII.4.17)

F,=EJJ+FEJhQh,

(j=1,2,...,t)

 

h#J

 

and

 

 

(XIII.4.18)

dQjk = x' [43Qik - QJkAk + EJk +

EJhQhk - QJkAk] (j j4 k).

 

 

h*k

Substituting (XIII.4.17) into (XIrII.4.18), a system of nonlinear differential equations

dQJk

 

EJhQhk

 

= x' LAJQJk - QJkAk +

 

dx

 

h*k

 

{

 

 

(XIII.4.19)

 

 

 

- QJk (Ekk +

EkhQhk) + EJkJ

(j # k)

 

h*k

 

 

is obtained. Since it is assumed that .11i ... , Al are distinct eigenvalues of Ao and that A0 is in the block-diagonal form (XIII.4.5), upon applying Theorem XIII-1-2

to (XIII.4.19) we can construct a desired holomorphic solution Qjk(x) of (XIII.4.19)

00

which admit an asymptotic expansion Qjk(x) > x "Qjk" (j, k = 1, 2,... , 3; j

"=1

k), where Qjk" are constant nj by nk matrices. Defining Fj by (XIII.4.17) and then

B(x) by (XIII.4.13), the proof of Theorem XIII-4-1 is completed. 0

Theorem XIII-4-1 concerns the behavior of solutions of system (XIII.4.1) near x = oo. Since it is useful to give a similar result concerning behavior of solutions near x = 0, we consider, hereafter in this section, a system of differential equations

(XIII.4.20)

xa+1 dY = A(x)y,

4. A BLOCK-DIAGONALIZATION THEOREM

423

where d is a positive integer and the entries of n x n matrix A(x) are holomorphic in a neighborhood of x = 0. Also, assume that A(0) is in a block-diagonal form

()III.4.21)

A(0) = diag[A11,,,

+N2,...

+JVt],

where a1, ... , .1t are distinct eigenvalues of A(0) with multiplicities n1, n2, ... , nt, respectively (n1 + n2 + + nt = n), and, for each j, .W is a lower-triangular and nilpotent nj x nj matrix.

Comparing the present situation with that of Theorem XIII-4-1, we notice the following two differences:

(a)singularity is at x = 0 in the present situation, while singularity is at x = 00 in Theorem XIII-4-1,

(b)The power series expansion of A(x) is convergent in the present situation, while A(x) in Theorem XIII-4-1 admits only an asymptotic expansion in a sector containing the direction arg x = 0.

We can change any singularity at x = 0 to a singularity at x = oo by changing the independent variable x by x1. Also, any direction argx = 8 can be changed

to the direction arg x = 0 by rotating the independent variable x. Furthermore, the asymptotic expansion P of Po(x) and the expansion b of Be are formal power

series satisfying the equation xd+i dP = AP - PB. This implies that two matrices

P and b are independent of P. Hence, using Corollary XIII-1-3, the following result is obtained.

Theorem XIII-4-2. Let A(x) be an n x n matrix whose entries are holomorphic in a neighborhood of x = 0. Also, let d be a positive integer. Assume that the matrix A(0) is in block-diagonal form (XIII.4.21), where al, ... , at are distinct eigenvalues of A(0) with multiplicities n1, n2, ... , nt, respectively (n1 + n2 +, + nt = n), and for each j, JVj is a lower-triangular and nilpotent n, x nj matrix. Fix a real number

0 so that (a, - Xk)e-utO V EP for j 96 k. Then, there exists two positive numbers be and ee and an n x n matrix Pe(x) such that

(a) the entries of Po(x) are holomorphic and admit asymptotic expansions in pow-

ers of x as x - 0 in the sector Se =

Ix: 0 < IxI < be, I arg x - 01 <

+ to },

00

(b) if >2 xmP,,, is the asymptotic expansion of Pe(x), then this expansion is

m=0

independent of 8 and Po = I,,,

(c) the transformation PB(x)u" changes system (XIIL4.20) to a system

(XIII.4.22)

xd+1

= Be(x)u,

where the matrix Be(x) is in a block-diagonal form

(XIII.4.23)

Be(x) = diag (B1e(x), B2e(x), ... , Bte(x)]

For each,, Bje is an n, xn2 matrix which admits also an asymptotic expansion in x as x--i0 in So.

The main claims of this theorem are

424 XIII. SINGULARITIES OF THE SECOND KIND

(i) the asymptotic expansion of Pe(x) is independent of 0,

(ii) the opening of the sector So is larger than

k.

Proof of Theorem XIII-4-2 is left to the reader as an exercises.

Remark XIII-4-3. Using Theorem XIII-3-4, we can generalize Theorem XIII-

4-1 to the system e°dx = xr'A(x, µ, e)y", where r and o are non-negative integers,

y" E C^, and A(x, µ', e) is an n x n matrix with the entries that are bounded and holomorphic with respect to the variable (x, µ, e) E C x C'° x C in a domain

Do = {(x, µ, e) : 1x1 > N, Iµ1 < µo, 0 < 1e1 < eo, 0 < 1 arg e1 < po}. Also, assume

00

that A admits a uniform asymptotic expansion A(x, µ, e) - > ehAh(x, µ) in Do

h=0

as a -+ 0, where coefficients Ah (X, µ) are bounded and holomorphic in the domain

{(x,µ) : 1x1 > N, 1µ1 < µo}. A complete proof of this result is found in [Si7] and

[Hs2].

XIII-5. Cyclic vectors (A lemma of P. Deligne)

In the study of singularities, a single n-th-order differential equation is, in many cases, easier to treat than a system of differential equations. In this section, we explain equivalence between a system of linear differential equations and a single n-th-order linear differential equation.

Let us denote by 1C the field of fractions of the ring C[(x]] of formal power series in x, i.e.,

I

p E C[Ix]J, 9 E C[Ix]j, 9 34 0}

K=

9:

Also, denote by V the set of all row vectors (cl(x), c2(x), ... , c,,(x)), where the entries are in the field K. The set V is an n-dimensional vector space over the

field 1C.

Define a linear differential operator C : V - V by G[vl = by + 7l(x) (v' E V ), where b = x d and S2(x) is an n x n matrix whose entries are in the field 1C. We

first prove the following lemma.

Lemma XIII-5-1 (P. Deligne [Del]). There exists an element iio E V such that

{v"o, Gv"o, G2v"o, ... , G"-lvo} is a basis for V as a vector space over IC.

Proof.

For each nonzero element v of V, denote by µ(v'' the largest integer t such that

{ii, Cii, C2v, ... ,.CeV) is linearly independent over K. In two steps, we shall derive

a contradiction from the assumption that max{µ(v') : v' E V} < n - 1.

v A,06 A
v A DU A

5. CYCLIC VECTORS

425

Step 1. First, we introduce a criterion for linear dependence of a set of elements of V. Consider a set {i11, ... vm } C V, where m is a positive integer not greater than n = dim, V. Let 6j = (c31,c12,... ,Cin) (j = 1,2,... ,m). Set .7 = {(jl,... ,jm)

1 < it < j2 < . < jm < n}, and introduce a linear order .7 -' { 1, 2,... , (M-)) in the set J. Let us now define a map

V ={(v1,V2,...,Vm): 61 EV (j=l,...,m)} -+ (.) m Id.)

(VI, ... , Vm) --+ V1 A v2 A ... A vm, where

1,AV2A ... A vm

 

f

cI31

Cj32 ...

clim

 

 

 

 

 

 

 

 

 

 

 

det

:

: :

(jl,... ,jm) E .7

 

 

C-i 1

Cmj2

C-3-

 

 

It is easy to verify the following properties of V1 A v"2 A

A v,,,:

 

 

Vk_1 A

 

1m_1 A Um

(1)

=

 

Vk_1 A

Vm_1 A v"m

 

+

 

v'k_1 A

 

Vm_1 A Vm,

 

V1 A ... A Vk_1 A (a Vk) A vk+I A ... A Vm_1 A Vm

(2)

=

 

6k_1 A irk

 

A vm),

 

 

 

for all aEIC,

 

 

 

 

(3)

VIA.-.A irk A ...A...AVjA ... A Vm

 

= -(11A...A iY A

 

A Vm),

 

 

(4) a sety{ {6j, 62,... , Vm } E V is linearly dependent if and only if v'1 AV2 A A 17m =

6 in K('^).

Step 2. Fix an element Vo of V such that µ(6o) = max{p(V) : v" E V} < n-1. Since p(VO) < n-1, another element w of V can be chosen so that {VO, Cv"o, CZi3o, ... , CnOv', w"} is linearly independent, where no = max{µ(v") : v E V}. Set v' = vo+Ax"'O E V, where A E C and m is an integer. Then, Cwt = Cw"o + C'(Ax-ti) = Crvo +

Axm(C + m)tw. Since {V, Cv", ... , Cn0+1V} is linearly dependent, it follows that A CnOv' A C"O+I V = 6 for all A E C and all integers in. Note that

A C"OiYA C"°+16 is a polynomial in A. Since this polynomial is iden- tically zero, each coefficients must be zero. For example, the constant term of this polynomial is i6o A CVO A ... A 00+I V"o. This is zero since {iio, Ciio..... G"0+Iuo} is linearly dependent. Compute the coefficient of the linear term in A of the polynomial. Then,

w A C60 A ... A Cna+1v'o + v'Y A ... A 00 Vo A (C +

m)n0,+1ti

 

no

+ 1:60A...ACi-IVoA (C+m)lw A CJ+'A A...ACnb+Ii = 0

J=1

426

XIII. SINGULARITIES OF THE SECOND KIND

identically for all integers m. The left-hand side of this identity is a polynomial in in of degree no + I. Hence, each coefficient of this polynomial must be zero. In particular, computing the coefficient of mn0+1, we obtain vOAGvOA . A GnbtloAw' =

0. This is a contradiction, since {vo, Gvo, ... , L"Ovo, w} is linearly independent.

This completes the proof of Lemma XIII-5-1.

Definition XIII-5-2. An element vo E V is called a cyclic vector of G if {6o, Lu0,

L2v'o, ... , Ln-1%) is a basis for V as a vector space over X.

Observation XI II-5-3. Let uo be a cyclic vector of Land let P(x) be the n x n ma-

 

Uo

trix whose row vectors are {vo,G'o,... ,L' 'io}, i.e., P(x) =

Gvo

. Then,

 

Gn-lvo

nv"o

 

L21 yo

 

o

 

=and, hence, setting A(x) = L[P(x)]P(x)-1 = bP(x)P(x)-l +

P(x)f2(x)P(x)-1, we obtain

0

1

0

0 ..

0

0

0

1

0 ...

0

A

 

 

0 ...

 

0

0

0

1

ap

al

a2

a3 ...

an-1

with the entries a, E C. Thus, we proved the following theorem, which is the main result of this section.

Theorem XIII-5-4. The system of differential equations

 

y1

(XIII.5.1)

by' = fl(x)y", where g _

 

Y.

becomes

 

(XIII.5.2)

bu" = A(x)u,

if y is changed by u = P(x)y". System (XIll.5.2) is equivalent to the n-th-order differential equation

 

bnq -

n-1

(XHI.5.3)

arbrq = 0, where q = yl.

1=o

5. CYCLIC VECTORS

427

Example XIII-5-5.

(1) Let us consider the system

 

 

 

 

 

 

 

y1

 

 

(a)

 

by" = 0,

 

where

y =

 

 

 

 

 

 

 

 

 

yn

 

 

The transformation

 

 

 

 

 

 

 

 

(T)

 

 

u = diag[l, X'... , xn-11y

 

 

changes system (a) to

 

 

 

 

 

 

 

 

(E)

 

 

bu = diag[0,1,... ,n - 1]u.

 

 

Further, the transformation

 

 

 

 

 

 

 

 

 

 

 

1

 

 

 

 

 

 

 

 

 

2

 

 

 

 

(r)

 

--

 

 

22

 

U

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

2n-1

 

 

 

 

changes (E) to the form

 

 

 

 

 

 

 

 

 

 

0

1

0

0

0

 

 

 

 

 

0

0

1

0

0

 

 

 

 

 

 

 

 

 

w,

 

 

 

 

 

0

0

0

0

1

 

 

 

 

 

ao

a1

a2

a3 ...

an-1

 

 

 

 

 

 

 

 

where ao, a,,.. . , an-1 are integers. Hence, the transformation

 

 

 

1

1

1

...

 

1

 

 

 

 

0

1

2

..

n- 1

 

 

 

w" =

0

1

2 2

...

(n - 1)2

diag [1, x,...

,x°-1

y

 

 

 

 

 

 

 

 

0

1

2n-1

...

(n -

1)n-1

 

 

 

 

 

 

 

 

 

 

 

changes (a) to (E'). This implies that vo = (1, x,

x2'. .. xn-1) is a cyclic vector in

this case.

 

 

 

 

 

 

 

 

 

(II) Next, consider the system

 

 

 

 

 

 

(b)

 

 

 

 

by = Ay,

 

 

 

where A is a constant diagonal n x n matrix. Choose a transformation similar to

(T) of (a) to change system (b) to

(E") oiZ = A'u