0387986995Basic TheoryC
.pdf380 XII. ASYMPTOTIC SOLUTIONS IN A PARAMETER
To show (iii), from (XII.2.11), (XII.3.3), and Lemma XII-2-4, we obtain
Iu-(h+l)(x,E)-u-(h)(x,E)I :5c8 sup Iiz(h)(t,E)-tL(h-1)(t,E)I tED(6)
in (XII.3.5) for h = 1 , 2, 3, .... Hence, the sequence (u -1 h ) (x, E) : h = 0,1, 2, ... } is convergent to (x, f) uniformly in (XII.3.5). Furthermore, uj = Oj (x, e) (j = 1, 2,... , n) satisfy system (XII.2.14). Thus, the proof of Theorem XII-1-2 is completed. 0
XII-4. A block-diagonalization theorem
Consider a system of linear differential equations
(XII.4.1) |
E° fy = A(x, E)y, |
where a is a positive integer, y E C", and A(x, c) is an n x n matrix. The entries of A(x, E) are holomorphic with respect to a complex variable x and a complex parameter c in a domain
(XII.4.2) lxi < ao, 0 < IEI < po, I argEl < no,
where bo, po, and ao are positive numbers. Assume that the matrix A(x, e) admits a uniform asymptotic expansion in the sense of Poincar6,
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(XII.4.3) |
A(x, e) E E"A, (x), |
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V=o |
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in domain (XII.4.2) as c --# 0 in the sector |
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(XII.4.4) |
0< IEI < po, |
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ao, |
where the entries of coefficients |
are holomorphic with respect to x in the |
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domain |
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(XII.4.5) |
Ixl < do. |
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Suppose that Ao(O) has a distinct eigenvalues A1, A2i ... , At with multiplicities
n1, n2i ... , nt, respectively (n1 + n2 + - - |
+ ne = n). Without loss of general- |
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ity, assume that Ao(0) is in a block-diagonal form |
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(XII.4.6) |
Ao(0) = diag [Al, A21 ... , At] , |
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where Aj are n, x n, matrices in the form |
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(XII.4.7) |
Aj =A,I",+N, |
(j=1,2,...,t). |
Here, I,, is the nj x n, identity matrix and Yj is an n, x nj lower-triangular nilpotent matrix. The main result of this section is the following theorem.
4. A BLOCK-DIAGONALIZATION THEOREM |
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Theorem XII-4-1 ([Si7]). Under assumptions (X11.4.8) and (X11.4.6), then exists an n x n matrix P(x, e) such that
(i) the entries of P(x, e) are holomorphic with respect to (x, e) in a domain
(XII.4.8) |
Ix j < 6, 0< kkI < p, l argeI < a, |
where 6, p, and a are positive numbers such that 0 < 5 < 60, 0 < p < po and
0<or <ao,
(ii) P(x, e) admits a uniform asymptotic expansion
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(XII.4.9) |
etPP(x) |
(P0(0) = I,,) |
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V=0 |
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in domain (XII.4.8) as e - 0 in the sector |
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(XII.4.10) |
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0< IkI < p, |
argel < a, |
where the entries of coefficients P,(x) are holomorphic with respect to x in the domain
(XII.4.11) |
fix, < 6, |
(iii) the transformation |
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(XII.4.12) |
y" = P(x, e)zi |
reduces system (X11.4.1) to a system |
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(XII.4.13) |
e° d = B(x, e)z |
with the coefficient matrix B(x, e) in a block-diagonal form |
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(XII.4.14) |
B(x, e) = diag[Bj (x, e), B2(x, e), ... , B,(x, e)], |
where B , (x, e) is an n, x n, matrix (j = 1, 2, ... , e),
(iv) the matrix B, (x, e) admits a uniform asymptotic expansion
(XII.4.15) |
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Bj (x, e) ^- 001: |
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in sector (XII.4.10), where the entries of coef- |
ficients |
are holomorphic with respect to x in domain (X11.4.11). |
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382 XII. ASYMPTOTIC SOLUTIONS IN A PARAMETER
Remark XII-4-2.
(a) Set
(XII.4.16) diag [B1v(x), B2 ,(x), ... , Bl,(x)] -
Then, the coefficient matrix B(x, e) of system (XII.4.13) admits a uniform
0
asymptotic expansion B(x, e)
'=a
(b)When a fundamental matrix solution Z(x, e) of (XII.4.13) is known, a fundamental matrix solution Y(x, e) of (XII.4.1) is given by Y(x, e) = P(x, e)Z(x, e).
(c)In the case when the matrix Ao(O) has n distinct eigenvalues, by Theorem
XII-4-1, we can diagonalize system (XII.4.1).
(d)In the case when eigenvalues of the matrix Ao(O) are not completely distinct, the point x = 0 is, in general, a so-called transition point. In order to study
behavior of solutions in the neighborhood of a transition point, we need a much deeper analysis of solutions of system (XII.4.1). For these informations, see, for example, [Wash], [Was2], and [Si12].
Proof of Theorem XII-4-1.
We prove this theorem in two steps. The proof is similar to that of Theorem
VII-3-1.
Step 1. We show that there exist a positive number 6 (< oo) and an n x n matrix Po(x) such that
(i)the entries of Po(x) and Po(x)-1 are holomorphic in the domain {x : JxI < b} and Po(0) = In,
(ii)the matrix Co(x) = Po(x)-1Ao(x)Po(x) is in a block-diagonal form
(XIL4.17) Co(x) = diag [Col)(x),Co2)(x),... ,C(c)(x)]
where Ca) (x) is an n, x nj matrix such that
Co)(0) = Aj=a,ln,+Arj |
(J=1,2,...,e). |
In fact, two matrices Po(x) and Co(x) must be determined by the equation
(XII.4.18) |
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Ao(x)Po(x) - Po(x)Co(x) = 0. |
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Set |
4(11)(x) |
4(12)(x) |
4(13)(x) ... |
40(2) |
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AA(x) ... |
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2 1) |
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Aou) (x) |
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Ao |
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o2) |
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Ao(x) |
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Aat1)(x) |
Aotz}(x) |
Ao)(x) |
Ao r)(x) |
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nd |
Poll)(x) |
Po12)(x) |
Po's)(x) |
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Pol() (x) |
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Pa21)(x) |
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Po2)(x) |
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Po2'(x) |
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Po(x) = |
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o |
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Poti)(x) |
P ' (x) |
Po )(x) |
Poti) (x) 1 |
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384 |
XII. ASYMPTOTIC SOLUTIONS IN A PARAMETER |
and
B(x, e) = diag [b(') (X, E), b(2) (X, E), . . . , B(') (x, E)] ,
where A(jk) (x) and P(Jk) (x) are nj x nk matrices and BJ (x, c) is an nj x nJ matrix
(j, k = 1,... , e). Furthermore, set
(XII.4.25) |
P(JJ)(x,E) = 0 |
(j = 1,2,... |
Then, equation (XII.4.23) becomes
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B(.)(x, f) = A(Jj)(x,E) + Ey: A(Jh)(x,E)P(hJ)(x,e)
(XII.4.26)
h=1
(j = 1,2,...,t)
and
(XII.4.27)
EodP(jk)(x,E) |
= A(J)(x)P(Jk)(x,E) |
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P(Jk)(x,E)A(k)(x) + A(jk)(x,E) |
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+ E E A(jh)(x f)P(hk)(x,E) |
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P(jk)(x,f)P(k)(x,E) |
(i |
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1hjAk |
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Combining (XII.4.26) and (XII.4.27), we obtain |
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Eo dP(J c) (x, E) |
4J) |
x P(Jk) x E - P(Jk) x, e A(k) x + A(Jk) x, E |
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- Ep(Jk)(x, E)A(kk) |
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+ E |
L.:A(Jh)(x, E)P(hk)(x, E) |
(x, E) |
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h=1 |
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- (2P(Jk) (x, c) |
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A(kh) (x, E)P(hk) (x, E) |
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h=1
Replacing P(jk)(x,E) by an nJ x nk matrix X(Jk), we derive a system of nonlinear differential equations
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o dX (2k) |
= A |
(J) ( |
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X (jk) |
(k) (X) |
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- X (jk) A x+ A(Jk) x E), |
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dx |
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(XII.4.28) |
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+ E E A(Jh)(x, C)X(hk) - EX (Jk)A(kk)(x, f) |
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- E2X(jk) FA(kh)(x,e)X(hk) |
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Consider the entries of X (jk) |
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altogether to form |
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a system of nonlinear differential equations. Upon applying Theorem XII-1-2, we
5. GEVREY ASYMPTOTIC SOLUTIONS IN A PARAMETER |
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construct an analytic solution of this nonlinear system in a domain (XII.4.8) admitting an asymptotic expansion in e as described in Theorem XII-4-1. This completes the proof of Theorem Xll-4-1. 0
XII-5. Gevrey asymptotic solutions in a parameter
In this section, using Theorems XI-2-3 and the proof of Theorem XII-1-2, we construct Gevrey asymptotic solutions of a system of differential equations
(XII.5.1) |
= Ax, y, E), |
Ea dx |
where x is a complex variable, y E Cn, E is a complex parameter, a is a positive integer, and Ax, if, e) is a Ca-valued function of (x, y', f). Define three domains by
A(So) = {x E C : IxI < bo}.
(XII.5.2)
S(ro, no) = {E E , arg E < ao, 0 < H < ro}.
Also, define two matrices A(x, E) and Ao(x) by
(XII.5.3) |
A(x, e) |
89
Oyn (x, 0, f)
8y1(x,E)
and
(XII.5.4) |
Ao(x) = limo A(x,e), |
respectively.
We first prove the following lemma.
Lemma XII-5-1. Assume that
(i)Ax, y", e) is holomorphic with respect to (x, f, c) in a domain A(bo) x Q(po) x S(ro, no), where 6o, po, ro, and no are positive numbers,
(ii)f (x, y", c) is bounded on A(60) x i2(po) x S(ro, no),
(iii)the matrix Ao(x) defined by (XII. 5.4) exists as e - 0 in S(ro, no) uniformly in x E A(6o) and Ao(0) is invertible,
(iv)f (x, 0, e) is flat of Gevrey order -r as e -+ 0 in S(ro, no) uniformly in x E
A(60), where r is a non-negative number.
Then, there exist three positive numbers b, r, and or such that system (XIL5.1) has a solution O(x, e) which is holomorphic in (x, t) E A(6) x S(r, a) and that (x, c) is flat of Gevrey order -r as e -' 0 in S(r,a) uniformly in x E L1(6).
386 XII. ASYMPTOTIC SOLUTIONS IN A PARAMETER
Proof.
Note first that
(XII.5.5) I exp1- k1I = expJ-cJfJ-'cos(k(arge))]
for any positive numbers c and k. Note next that assumptions (i) and (iv) imply th in the case when r = 0, Ax, 0, e) is identically equal to 0 for (t, f) E A(b) x S(r, a).
Hence, in this case, 0 is a solution of (XII.5.1). In the case when r > 0, it holds that
(XII.5.6) |
If(x,o,e)I < h |
exp[-2cIEl-k1 |
for some positive numbers K and c if (x, e) E A(b) x S(r, a) for sufficiently small positive numbers 6, r, and a and if
k
(XII.5.7)
(cf. Theorem X1-3-2). Therefore, (XII.5.5) and (XII.5.6) imply that
(XII.S.8) |
I exp[ce-k] I If (x, O, E)I = if (x, o, e)I expf clkl-k cos(k(arg e))] |
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for (x, e) E A(6) x S(r, a). Note also that |
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(XII.5.9) |
cos(k(arge)) > cos(ka) > 0 for f E S(r,a) if ka < 2. |
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Let us change l/ in (XII.5.1) by |
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(XII.5.10) |
Ii = exp(-ce-'16. |
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Then, (XII.5.1) is reduced to |
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(XII.5.11) |
el" = exp[m-kJf(x,eXP[-ce-k]u,e). |
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Set |
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f (x+ FJ, e) = f (x, 0, e) + A(x, e)il + E yPfp(x, e). |
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JpI>2 |
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Then,
exp[cE-k1f(x, eXp[-cE-k]u, e)
= eXPfce-kJf (x, 0, e) + A(x, e)U + |
explc(1 - lpl)E-k]ul fp(x, e)' |
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ip1>2 |
Using a method similar to the proof of Theorem XII-1-2, we construct a bounded solution u = tlr(x, e) of (XII.5.11). Therefore, system (XII.5.1) has a solution of the form y" _ ¢(x,e) = expl-ce-k]y,(x,e). This completes the proof of Lemma
XII.5.1.
The main result of this section is the following theorem, which was originally conjectured by J: P. Ramis.
5. GEVREY ASYMPTOTIC SOLUTIONS IN A PARAMETER |
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Theorem XII-5-2. Assume that
(i)f (x, y', e) is holomorphic in (x, y, e) on a domain 0(6o) x f2(po) x S(ro, ao), where bo, po, ro, and ao are positive numbers,
(ii)f (x, y, e) admits an asymptotic expansion F(x, y, e) of Cevmy orders as a --+ 0 in S(ro, ao) uniformly in (x, y-) E A(bo) x f2(po), where s is a non-negative
number,
(iii)the matrix Ao(x) given by (XIL5.4) is invertible on 0(bo),
(iv)it holds that
(XII.5.12) |
lim f (x, 0, e) = 0 |
on 0(bo). |
Then, |
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(1) (XIL5.1) has a unique formal solution |
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(X1.5.13) |
Plx, e) _ |
eep'e(x) |
c-
with coefficients p"t(x) which are holomorphic on A(bo),
(2)there exist three positive numbers 6, r, and a such that (XII. 5.1) has an actual solution ¢(x, e) which is holomorphic in (x, e) E A(5) x S(r, a) and that ¢(x, e) admits the formal solution P(x, e) as its asymptotic expansion of Gevrey order
max { 1, s } as e - 0 in S(r, a) uniformly in x E L1(b).
a
J11
Proof.
If a positive number & is sufficiently small, for every real number 6, there exists a C"-valued function fe(x,y,e) such that
(a)fe(x, y', e) is holomorphic in (x, y", e) on a domain A(60) x f2(po) x Se(ro, &), where
(XIL5.14) Se(ro,&) = {e: jarge - 61 < &, 0 < fej < ro},
(b)fe(x, y, e) admits an asymptotic expansion F(x, y e) of Gevrey order s as e - 0 in Se(ro, &) uniformly in (x, y) E 0(bo) x f2(po), where s is the non- negative number given in Theorem XII.5.2.
Such a function fe(x, y, e) exists if & is sufficiently small (cf. Corollary XI-2-5). In particular, set
(XII.5.15) |
fo(x, b, e) = f (x, v, e) |
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Let y = & (x, e) be a solution of the system |
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(XII.5.16) |
e° |
= fe(x, y, e) |
such that &(x, e) is holomorphic and bounded in (x, e) E i (b1) x Seri, al) for suitable positive numbers 61, r1, and al. Using Theorem XII-1-2, it can be shown that such a solution of (XII.5.16) exists.
