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1.
Let A 1,…,Am be nxn hermitian matrices. Definine

W(A 1,…,Am )={(xA1x ?,…xAmx ?):x?C n ,xx ?=1}. We will show that every point in the convex hull of W(A 1,…,Am ) can be represented as a convex combination of not more than k(m,n) points in W(A 1,…,Am ) where k(m,n)=min{n,[√m]+δ n 2 m+1}.  相似文献   

2.
Let V be an n-dimentional unitary space with inner product (·,·) and S the set {xV:(x, x)=1}. For any A∈Hom(V, V) and q∈C with ∣q∣?1, we define
W(A:q)={(Ax, y):x, y∈S, (x, y)=q}
. If q=1, then W(A:q) is just the classical numerical range {(Ax, x):xS}, the convexity of which is well known. Another generalization of the numerical range is the C-numerical range, which is defined to be the set
WC(A)={tr(CU1AU):U unitary}
where C∈Hom(V, V). In this note, we prove that W(A:q) is always convex and that WC(A) is convex for all A if rank C=1 or n=2.  相似文献   

3.
For 0<q<1, the q-numerical range is defined on the algebra Mn of all n×n complex matrices by
Wq(A)={xAy:x,yCn,∥x∥=∥y∥=1,〈y,x〉=q}.  相似文献   

4.
5.
We consider the acoustic propagator A=−∇·c2∇ in the strip Ω={(x, z)∈ℝ2∣0<z<H} with finite width H>0. The celerity c depends for large ∣x∣ only on the variable z and describes the stratification of Ω: it is assumed to be in L(Ω), bounded from below by cmin>0, such that there exists M>0 with c(x, z)=c1(z) if x< −M and c(x, z)=c2(z) if x>M. We look at the propagator A as a ‘perturbation’ of the free propagators Aj in Ω associated to the velocities cj, j=1, 2, and implement a ‘perturbative’ method, adapting ideas of Majda and Vainberg. The spectrum of A is defined in section 2, a limiting absorption principle is proved in section 3 outside of a countable set Γ(A). The points of Γ(A) can only accumulate at the left of the thresholds of the free propagators. The needed material about Aj, j=1, 2, and some technical estimates for A are given in Appendix. © 1998 B. G. Teubner Stuttgart—John Wiley & Sons, Ltd.  相似文献   

6.
Let p(n) denote the smallest prime factor of an integer n>1 and let p(1)=∞. We study the asymptotic behavior of the sum M(x,y)=Σ1≤nx,p(n)>yμ(n) and use this to estimate the size of A(x)=max|f|≤12≤n<xμ(n)f(p(n))|, where μ(n) is the Moebius function. Applications of bounds for A(x), M(x,y) and similar quantities are discussed.  相似文献   

7.
Given an m×n matrix M over E=GF(qt) and an ordered basis A={z1,…,zt} for field E over K=GF(q), expand each entry of M into a t×1 vector of coordinates of this entry relative to A to obtain an mt×n matrix M1 with entries from the field K. Let r=rank(M) and r1=rank(M1). We show that r?r1?min{rt,n}, and we determine the number b(m,n,r,r1,q,t) of m×n matrices M of rank r over GF(qt) with associated mt×n matrix M1 of rank r1 over GF (q).  相似文献   

8.
9.
A new class of bilinear relative equilibria of identical point vortices in which the vortices are constrained to be on two perpendicular lines, conveniently taken to be the x- and y-axes of a Cartesian coordinate system, is introduced and studied. In the general problem we have m vortices on the y-axis and n on the x-axis. We define generating polynomials q(z) and p(z), respectively, for each set of vortices. A second-order, linear ODE for p(z) given q(z) is derived. Several results relating the general solution of the ODE to relative equilibrium configurations are established. Our strongest result, obtained using Sturm’s comparison theorem, is that if p(z) satisfies the ODE for a given q(z) with its imaginary zeros symmetric relative to the x-axis, then it must have at least n?m+2 simple, real zeros. For m=2 this provides a complete characterization of all zeros, and we study this case in some detail. In particular, we show that, given q(z)=z 2+η 2, where η is real, there is a unique p(z) of degree n, and a unique value of η 2=A n , such that the zeros of q(z) and p(z) form a relative equilibrium of n+2 point vortices. We show that $A_{n} \approx\frac{2}{3}n + \frac{1}{2}$ , as n→∞, where the coefficient of n is determined analytically, the next-order term numerically. The paper includes extensive numerical documentation on this family of relative equilibria.  相似文献   

10.
Let A be an n × n matrix; write A = H+iK, where i2=—1 and H and K are Hermitian. Let f(x,y,z) = det(zI?xH?yK). We first show that a pair of matrices over an algebraically closed field, which satisfy quadratic polynomials, can be put into block, upper triangular form, with diagonal blocks of size 1×1 or 2×2, via a simultaneous similarity. This is used to prove that if f(x,y,z) = [g(x,y,z)]n2, where g has degree 2, then for some unitary matrix U, the matrix U1AU is the direct sum of n2 copies of a 2×2 matrix A1, where A1 is determined, up to unitary similarity, by the polynomial g(x,y,z). We use the connection between f(x,y,z) and the numerical range of A to investigate the case where f(x,y,z) has the form (z?αax? βy)r[g(x,y,z)]s, where g(x,y,z) is irreducible of degree 2.  相似文献   

11.
12.
Let k and n be positive integers such that kn. Let Sn (F) denote the space of all n×n symmetric matrices over the field F with char F≠2. A subspace L of Sn (F) is said to be a k-subspace if rank Ak for every A?L.

Now suppose that k is even, and write k=2r. We say a k∥-subspace of Sn (F) is decomposable if there exists in Fn a subspace W of dimension n?r such that xtAx=0 for every x?W A?L.

We show here, under some mild assumptions on k n and F, that every k∥-subspace of Sn (F) of sufficiently large dimension must be decomposable. This is an analogue of a result obtained by Atkinson and Lloyd for corresponding subspaces of Fm,n .  相似文献   

13.
Let F(z)=∑ n=1 A(n)q n denote the unique weight 6 normalized cuspidal eigenform on Γ0(4). We prove that A(p)≡0,2,−1(mod 11) when p≠11 is a prime. We then use this congruence to give an application to the number of representations of an integer by quadratic form of level 4.   相似文献   

14.
For a continuous linear operator A on a Hilbert space X and unit vectors x and y, an investigation of the set W[x,y]={z1Az:z1z=1 and z?span{x,y}} reveals several new results about W(A), the numerical range of A. W[x,y] is an elliptical disk (possibly degenerate), and several conditions are given which imply that W[x,y] is a line segment. In particular if x is a reducing eigenvector of A, then W[x,y] is a line segment. A unit vector is called interior (boundary) if x1Ax is in the interior (boundary) of W(A). It is shown that interior reducing eigenvectorsare orthogonal to all boundary vectors and that boundary eigenvectors are orthogonal to all other boundary vectors y [except possibly when y1Ay is interior to a line segment in the boundary of W(A) through the given eigenvalue].  相似文献   

15.
For a fixed prime q, let eq(n) denote the order of q in the prime factorization of n!. For two fixed integers m?2 and r with 0?r?m−1, let A(x;m,q,r) denote the numbers of positive integers n?x for which . In this paper we shall prove a sharp asymptotic formula of A(x;m,q,r).  相似文献   

16.
Let Ω and Π be two finitely connected hyperbolic domains in the complex plane \Bbb C{\Bbb C} and let R(z, Ω) denote the hyperbolic radius of Ω at z and R(w, Π) the hyperbolic radius of Π at w. We consider functions f that are analytic in Ω and such that all values f(z) lie in the domain Π. This set of analytic functions is denoted by A(Ω, Π). We prove among other things that the quantities Cn(W,P) := supf ? A(W,P)supz ? W\frac|f(n)(z)| R(f(z),P)n! (R(z,W))nC_n(\Omega,\Pi)\,:=\,\sup_{f\in A(\Omega,\Pi)}\sup_{z\in \Omega}\frac{\vert f^{(n)}(z)\vert\,R(f(z),\Pi)}{n!\,(R(z,\Omega))^n} are finite for all n ? \Bbb N{n \in {\Bbb N}} if and only if ∂Ω and ∂Π do not contain isolated points.  相似文献   

17.
Let U be a class of subsets of a finite set X. Elements of U are called blocks. Let υ, t, λ and k be nonnegative integers such that υ?k?t?0. A pair (X, U) is called a (υ, k, λ) t-design, denoted by Sλ(t, k, υ), if (1) |X| = υ, (2) every t-subset of X is contained in exactly λ blocks and (3) for every block A in U, |A| = k. A Möbius plane M is an S1(3, q+1, q2+1) where q is a positive integer. Let ∞ be a fixed point in M. If ∞ is deleted from M, together with all the blocks containing ∞, then we obtain a point-residual design M*. It can be easily checked that M* is an Sq(2, q+1, q2). Any Sq(2, q+1, q2) is called a pseudo-point-residual design of order q, abbreviated by PPRD(q). Let A and B be two blocks in a PPRD(q)M*. A and B are said to be tangent to each other at z if and only if AB={z}. M* is said to have the Tangency Property if for any block A in M*, and points x and y such that x?A and y?A, there exists at most one block containing y and tangent to A at x. This paper proves that any PPRD(q)M* is uniquely embeddable into a Möbius plane if and only if M* satisfies the Tangency Property.  相似文献   

18.
Let Fn be a binary form with integral coefficients of degree n?2, let d denote the greatest common divisor of all non-zero coefficients of Fn, and let h?2 be an integer. We prove that if d=1 then the Thue equation (T) Fn(x,y)=h has relatively few solutions: if A is a subset of the set T(Fn,h) of all solutions to (T), with r:=card(A)?n+1, then
(#)
h divides the numberΔ(A):=1?k<l?rδ(ξk,ξl),
where ξk=〈xk,yk〉∈A, 1?k?r, and δ(ξk,ξl)=xkylxlyk. As a corollary we obtain that if h is a prime number then, under weak assumptions on Fn, there is a partition of T(Fn,h) into at most n subsets maximal with respect to condition (#).  相似文献   

19.
Let a, b, c be relatively prime positive integers such that a p  + b q  = c r for fixed integers p, q, r ≥ 2. Terai conjectured that the equation a x  + b y  = c z in positive integers has only the solution (x, y, z) = (p, q, r) except for specific cases. In this paper, we consider the case q = r = 2 and give some results related to exceptional cases.  相似文献   

20.
We consider an Abel equation (*)y’=p(x)y 2 +q(x)y 3 withp(x), q(x) polynomials inx. A center condition for (*) (closely related to the classical center condition for polynomial vector fields on the plane) is thaty 0=y(0)≡y(1) for any solutiony(x) of (*). We introduce a parametric version of this condition: an equation (**)y’=p(x)y 2 +εq(x)y 3 p, q as above, ℂ, is said to have a parametric center, if for any ε and for any solutiony(ε,x) of (**),y(ε,0)≡y(ε,1). We show that the parametric center condition implies vanishing of all the momentsm k (1), wherem k (x)=∫ 0 x pk (t)q(t)(dt),P(x)=∫ 0 x p(t)dt. We investigate the structure of zeroes ofm k (x) and on this base prove in some special cases a composition conjecture, stated in [10], for a parametric center problem. The research of the first and the third author was supported by the Israel Science Foundation, Grant No. 101/95-1 and by the Minerva Foundation.  相似文献   

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