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1.
Let be one of the N 2-dimensional bicovariant first-order differential calculi on the quantum groups O q (N) or Sp q (N), where q is not a root of unity. We show that the second antisymmetrizer exterior algebra s is the quotient of the universal exterior algebra u by the principal ideal generated by . Here denotes the unique up to scalars bi-invariant 1-form. Moreover, is central in u and u is an inner differential calculus.  相似文献   

2.
We give the algebraic characteristics of the range of the system Cp, C2p, ..., cnp f() ( fixed, 0<¦¦<1, n1, P=1, 2, ...) on certain subclasses Cm,p, of the class C of functions, regular in the circle ¦z¦<1 and satisfying in it the condition Re f(z)>0. As an application one finds the range of f() on the subclasses C m,p, (n) of functions from Cm,p, with prescribed coefficients cp c2p, ..., cnp.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 100, pp. 17–25, 1980.  相似文献   

3.
In this paper we study initial value problems likeu t–R¦u¦m+uq=0 in n× +, u(·,0+)=uo(·) in N, whereR > 0, 0 <q < 1,m 1, andu o is a positive uniformly continuous function verifying –R¦u o¦m+u 0 q 0 in N . We show the existence of the minimum nonnegative continuous viscosity solutionu, as well as the existence of the function t(·) defined byu(x, t) > 0 if 0<t<t (x) andu(x, t)=0 ift t (x). Regularity, extinction rate, and asymptotic behavior of t(x) are also studied. Moreover, form=1 we obtain the representation formulau(x, t)=max{([(u o(x – t))1–q (1–q)t]+)1/(1–q): ¦¦R}, (x, t) + N+1 .Partially supported by the DGICYT No. 86/0405 project.  相似文献   

4.
Summary Let X={X(t), t N} be a centred Gaussian random field with covariance X(t)X(s)=r(t–s) continuous on N×N and r(0)=1. Let (t,s)=((X(t)–X(s)) 2)1/2; (t,s) is a pseudometric on N. Assume X is -separable. Let D 1 be the unit cube in N and for 0<k, D k= {xN: k –1 xD1}, Z(k)=sup{X(t),tD k}. If X is sample continuous and ¦r(t)¦ =o(1/log¦t¦) as ¦t¦8 then Z(k)-(2Nlogk) 1/20 as k a.s.  相似文献   

5.
Let A be a partition of the segment [0, 1] into a countable number of disjoint subsets of positive measure, let tL1(0,1), let Nt be the smallest rearrangement-invariant order ideal vector lattice in L1(0,1), containing t. In the paper one investigates the properties of the image E(Nt¦A) of the averaging operator with respect to A. In particular, one elucidates under what conditions there exists a function g, gL1(0,1), such that E(Nt¦A)Ng. One formulates a generalization of the known Hardy-Littlewood inequality, namely Theorem E(tA)QE(t*A*), where is the Hardy-Littlewood preorder, t* and A* are the decreasing rearrangements of the function ¦t¦ and (in a special sense) of the partition A, while Q is an absolute constant, 1Q25. One formulates the problem of the smallest value of Q.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 149, pp. 137–141, 1986.  相似文献   

6.
By the M.Riesz Convexity Theorem, an operator T on the space of simple integrable functions into the measurable functions (on some measure space) which has continuous extensions to Lp() and Lq() , where 1 p q , also has continuous exten — sions to all Lr () , p r q . It is shown that, whenever (Tp) and (Tq) are o-dimensional (in particular, countable) then the spectra (Tr) (p r q) are pairwise identical. For q = , only w*-continuous extensions are considered. An example due to Dayanithy shows that the conclusion fails in general.  相似文献   

7.
Summary We prove the existence of nontrivial solutions for nonlinear equations of the type Lu=g(x, u) + ¦u¦¯p–2u, ¯ p > 2, where L is a continuous self- adjoint linear operator in a Hilbert space H and ug(x, u) is a lower order perturbation of ¦u¦¯p–1. We assume that ¯p is the critical exponent in the sense that the embedding H Lp, If is compact for 1p<¯p and is continuous (not necessarily compact) for p=¯p. From this result we deduce, for example, that utt -u- u=¦u¦2/Nu, u L2(SN×S1) has at least one pair (–u, u) of solutions nonconstant with respect to t, provided that is sufficiently close to some eigenvalue of tt–.Work supported by M.P.I. Italy (fondi 40%, 60%) and by G.N.A.F.A. of C.N.R.  相似文献   

8.
A vibrating plate is here taken to satisfy the model equation:u tt + 2u = 0 (where 2u:= (u); = Laplacian) with boundary conditions of the form:u v = 0 and(u) v = = control. Thus, the state is the pair [u, u t] and controllability means existence of on := (0,T transfering any[u, u t]0 to any[u, u t]T. The formulation is given by eigenfunction expansion and duality. The substantive results apply to a rectangular plate. For largeT one has such controllability with = O(T –1/2). More surprising is that (based on a harmonic analysis estimate [11]) one has controllability for arbitrarily short times (in contrast to the wave equation:u tt = u) with log = O(T –1) asT0. Some related results on minimum time control are also included.This research was partially supported under the grant AFOSR-82-0271.  相似文献   

9.
The paper deals with the Cauchy problem for a complete second-order differential equation with unbounded operator coefficientsu+A(t)u+B(t)u=f, u(0)=u0, u(0)=u 1 . By using the commutant method, we construct a coercive solution of this problem in Holder space in the case where the operatorB is as strong as the operator A2.Translated from Ukrainskii Matematicheskii Zhurnal, Vol. 45, No. 10, pp. 1449–1454, October, 1993.  相似文献   

10.
Let be a bounded domain in n (n3) having a smooth boundary, let be an essentially bounded real-valued function defined on × h, and let be a continuous real-valued function defined on a given subset Y of Y h. In this paper, the existence of strong solutions u W 2,p (, h) W o 1,p (n/2<p<+) to the implicit elliptic equation (–u)=(x,u), with u=(u1, u2, ..., uh) and u=(u 1, u 2, ..., u h), is established. The abstract framework where the problem is placed is that of set-valued analysis.  相似文献   

11.
Conditions are found under which for an entire function f represented by a Dirichlet series with finite Ritt order on some sequence (xk), 0 < xk , as k one has ¦f(xk)¦=Mt((1 + 0(1) xk), Mf(x)=sup {¦ f (z) ¦:Re z x}.Translated from Ukrainskii Matematicheskii Zhurnal, Vol. 43, No. 2, pp. 265–269, February, 1991.  相似文献   

12.
Strict upper bounds are determined for ¦s(z)¦, ¦Re s(z)¦, and ¦Im s(z) ¦ in the class of functions s(z)=a nzn+an+1zn+1+... (n1) regular in ¦z¦<1 and satisfying the condition ¦u (1) –u (2) ¦K¦ 1- 2¦, where U()=Re s (ei ), K>0, and 1 and 2 are arbitrary real numbers. These bounds are used in the determination of radii of convexity and close-to-convexity of certain integral representations.Translated from Matematicheskie Zametki, Vol. 7, No. 5, pp. 581–592, May, 1970.The author wishes to thank L. A. Aksent'ev for his guidance in this work.  相似文献   

13.
We study the regularity of the minimizer u for the functional F (u,f)=|u|2 + |u–f{2 over all maps uH 1(, S 2). We prove that for some suitable functions f every minimizer u is smooth in if 0 and for the same functions f, u has singularities when is large enough.
Résumé On étudie la régularité des minimiseurs u du problème de minimisation minueH 1(,S2)(|u|2 + |u–f{2. On montre que pour certaines fonctions f, u est régulière lorsque 0 et pour les mêmes f, si est assez grand, alors u possède des singularités.
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14.
Denote by q an affine plane of order q. In the desarguesian case q=AG(2,q), q 5(q= ph, p prime), we prove that the smallest cardinality of a blocking set is 2q–1. In any arbitrary affine plane q (desarguesian or not) with q5, for any integer k with 2q–1 k(q–1)2, we construct a blocking set S with ¦S¦=k. For an irreducible blocking set S of q we determine the upper bound S [qq]+1. We prove that if q contains a blocking set S which is irreducible with its complementary blocking set, then necessarily q=AG(2, 4) and S is uniquely determined. Finally we introduce techniques to obtain blocking sets in AG(2, q) and in PG(2, q).Research partially supported by G.N.S.A.G.A. (CNR)  相似文献   

15.
We establish conditions under which the relation M(x, F) (x, F) m(x, F) holds except for a small set, as ¦x¦ + for an entire function F(z) of several complex variables z (p2) represented by a Dirichlet series, where M(x, F) = sup{¦F(x+iy¦: y p}, m(x, F) = inf{¦F(x+iy)¦: y p} (x, F) being the maximal term of the Dirichlet series, and x p.Translated fromMatematichni Metodi ta Fiziko-Mekhanichni Polya, Vol. 40, No. 4, 1997, pp. 21–25.  相似文献   

16.
Summary The Cahn-Hilliard model for phase separation in a binary alloy leads to the equations (I) ut=w, (II) w= (u)– u with an associated energy functional F(u)=f [(u)+ +¦u¦2/2] dx. In this paper we discuss the existence theory for initial bounday value problems arising from modifications to the Cahn-Hilliard model due to the addition of the non-differentiable term ¦u¦dx to the energy F(u).  相似文献   

17.
In this paper we study the question of uniqueness for an inverse problem, arising in the (thermal) linear and/or non-linear potential theory. The overdetermined problem we shall study is represented by(div(|u| p–2u)–D t u+)u=0where supp()R n ×(0,), 1<p<, L and {t=} is bounded for >0.The problem has applications in shape-recognition in underground water/oil recovery, subject to shape-change during time intervals. The particular case u0, D t u0, and p=2, is an example of the well-known Stefan.  相似文献   

18.
Summary The sum a n X n of a weighted series of a sequence {X n } of identically distributed (not necessarily independent) random variables (r.v.s.) is a.s. absolutely convergent if for some in 0<1, ¦a n ¦ < and E¦X n ¦ < ; if a n =z n for some ¦z¦<1 then it suffices that E(log¦X n ¦)+<. Examples show that these sufficient conditions are not necessary. For mutually independent {X n } necessary conditions can be given: the a.s. absolute convergence of X n z n (all ¦z¦<1) then implies E(log¦X n ¦)+ < , while if the X n are non-negative stable r.v.s. of index , ¦a n X n ¦< if and only if ¦a n ¦ < .  相似文献   

19.
We consider the linear program min{cx: Axb} and the associated exponential penalty functionf r(x) = cx + rexp[(A ix – bi)/r]. Forr close to 0, the unconstrained minimizerx(r) off r admits an asymptotic expansion of the formx(r) = x * + rd* + (r) wherex * is a particular optimal solution of the linear program and the error term(r) has an exponentially fast decay. Using duality theory we exhibit an associated dual trajectory(r) which converges exponentially fast to a particular dual optimal solution. These results are completed by an asymptotic analysis whenr tends to : the primal trajectory has an asymptotic ray and the dual trajectory converges to an interior dual feasible solution.Corresponding author. Both authors partially supported by FONDECYT.  相似文献   

20.
For a solution u of –u=u(1–|u|2) on the whole plane, |u|<1 holds everywhere unless u=ei for some ; the derivatives of order k have moduli a constant M kdepending only on k. For a solution u on an open set 2, the moduli of u and its derivatives have upper bounds depending only on the distance to 2\ therefore the set of solutions on a given is compact in C() for the topology of uniform convergence on compact subsets of . For a solution u such that |u|<1, 1–|u| satisfies an estimation similar to the classical Harnack inequality for positive harmonic functions.Finally, if is bounded and |u| has a lim supm at each boundary point, the |u|m in if m1, but if m<1 then |u| admits only a majorant S m with values in ]m, 1[ and sufficient conditions are given for lim S m =0 or S m =O(m) as m0.
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