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1.
2.
(C, ). , . 0<<1. 1) - ( k ), k =a k , (C, ), . 2) , , (C, ) ; k = =¦a k ¦.  相似文献   

3.
The model problem -i y'+q(x)y= y, y(-1)=y(1)=0 is associated with the Orr-Sommerfeld operator well-known in hydrodynamics. Here is the spectral parameter, is the small parameter which is proportional to the viscosity of the liquid and to the reciprocal of the Reynolds number, and q(x) is the velocity of the stationary flow of the liquid in the channel |x| 1. We study the behavior of the spectrum of the corresponding model operator as to 0 with linear, quadratic, and monotonic analytic functions. We show that the sets of accumulation points of the spectra (the limit spectral graphs) of the model and corresponding Orr-Sommerfeld operators coincide just as the main terms of the eigenvalue counting functions along the curves of the graphs do.  相似文献   

4.
The series 1 n r–1 J n (n)J n (n) (r 0, 0 < 1) arise in studying the emission and absorption of radiation by a charged particle on a Kepler orbit. For the first few even,r, the sums are obtained in closed form, and for oddr they are given in terms of a certain definite integral. The integral is expressed as a power series in for ||<1, and, near =1, an asymptotic expansion in powers of (1–2)1/2 may be obtained.
Résumé La série 1 n r–1 J n (n)J n (n) (r 0, 0 < 1) se trouve par l'émission et l'absorption du rayonnement d'une particule chargée sur l'orbite Keplerien. Pour les plus petites valuers paires der, les sommes s'obtienment en forme compacte, et pour les valuers impaires, elles se déterminent d'après une intégrale definie. Pour ||<1, cette intégrale se développe dans une série de puissances de , et dans le voisinage de =1, on obtient une série asymptotique et puissances de (1–2)1/2.
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5.
Q (.. , L). Q . P(Sr(2)) — 2 (S r(2) (r — ). , M(P(S r(m=sup{t(·)t(·)1:t P(S r(2)),t 0}. , /4+(1)M(P(S r(2)))/r 215/17+(1)(r+). (Q), Q L.  相似文献   

6.
Converse theorems for multidimensional Kantorovich operators   总被引:4,自引:0,他引:4  
L p [0, l]. . . - .

Supported by National Science Foundation, Zhejiang Provincial Science Foundation of China, and Alexander von Humboldt Foundation of Germany.  相似文献   

7.
Summary We consider low temperature limits of Gibbs states of the ferromagnetic nearest-neighbour Ising Hamiltonian in the positive orthant of the lattice d ,d=1, 2,..., under a negative boundary condition and a small positive external fieldh that decreases linearly with the temperatureT. It is shown that positive and negative spins are separated by a staircase-shaped random boundary. Its explicit distribution is computed in the case that the ratio =h/T exceeds some positive 0. For < 0, our results do not rule out infinite negative areas.  相似文献   

8.
[0,1], - H .

This paper was written during the author's scholarship at the State University of Odessa in the USSR.  相似文献   

9.
10.
, , . , . Lip

The authors are indebted to Professor R. Bojanic for his valuable remarks and suggestions, especially for the simplification of the proof of Theorem 4.  相似文献   

11.
, . . Q k [0,2],k=1,2, — . F(x, y)L(T), T=[0, 2]2, G(x, y)L(T) , G(x,y)=F(x,y) Q=Q 1 ×Q 2 - .  相似文献   

12.
This paper deals with positive solutions of degenerate and strongly coupled quasi-linear parabolic system not in divergence form: ut=vp(u+au), vt=uq (v+bv) with null Dirichlet boundary condition and positive initial condition, where p, q, a and b are all positive constants, and p, q 1. The local existence of positive classical solution is proved. Moreover, it will be proved that: (i) When min {a, b} 1 then there exists global positive classical solution, and all positive classical solutions can not blow up in finite time in the meaning of maximum norm (we can not prove the uniqueness result in general); (ii) When min {a, b} > 1, there is no global positive classical solution (we can not still prove the uniqueness result), if in addition the initial datum (u0v0) satisfies u0 + au0 0, v0+bv0 0 in , then the positive classical solution is unique and blows up in finite time, where 1 is the first eigenvalue of – in with homogeneous Dirichlet boundary condition.This project was supported by PRC grant NSFC 19831060 and 333 Project of JiangSu Province.  相似文献   

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14.
n- (n1) fL p ([–, ] n ),=1 = (L C) . , , f([–, ] n ).  相似文献   

15.
The article discusses a probability model of the spread of an epidemic in which the elimination of sick persons (through death, immunity, or isolation) is taken into account. The authors find a limit distribution for the magnitude of the epidemic,v, on the assumption that n, where n is the original number of susceptible persons, and , where and are the coefficient of infection and the coefficient of elimination, respectively.Translated from Matematicheskie Zametki, Vol. 3, No. 2, pp. 179–185, February, 1968.  相似文献   

16.
(r k ) - , +1 –1 1/2. =( i ) , 0< 1 p ... n ... . (a i )M. (a i ) . , [2], .  相似文献   

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18.
Ercan  Z.  Onal  S. 《Positivity》2004,8(2):123-126
We introduce weak quasinilpotence for operators. Then, by substituting Markushevich basis and weak quasinilpotence at a nonzero vector for Schauder basis and quasinilpotence at a nonzero vector, respectively, we answer a question on the invariant subspaces of positive operators in [3].  相似文献   

19.
(0; 0, 1) , {x k <x k * <x k+1} k=1 n–1 {x k k=1 n }., I, , n (x)=P n (, ) (x)–n- , =, n3 . , x 0=+1 x n+1= –1. II .

To the memory of Paul Erds

The research was supported by the Hungarian National Foundation for Scientific Research under Grant # T 914 244.  相似文献   

20.
M. . , . , p () (). , , .  相似文献   

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