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1.
Summary We consider the one dimensional nearest neighbors asymmetric simple exclusion process with ratesq andp for left and right jumps respectively;q<p. Ferrari et al. (1991) have shown that if the initial measure isv , , a product measure with densities and to the left and right of the origin respectively, <, then there exists a (microscopic) shock for the system. A shock is a random positionX t such that the system as seen from this position at timet has asymptotic product distributions with densities and to the left and right of the origin respectively, uniformly int. We compute the diffusion coefficient of the shockD=lim t t –1(E(X t )2–(EX t )2) and findD=(p–q)()–1((1–)+(1)) as conjectured by Spohn (1991). We show that in the scale the position ofX t is determined by the initial distribution of particles in a region of length proportional tot. We prove that the distribution of the process at the average position of the shock converges to a fair mixture of the product measures with densities and . This is the so called dynamical phase transition. Under shock initial conditions we show how the density fluctuation fields depend on the initial configuration.  相似文献   

2.
Summary Given two pointsx, yS 1 randomly chosen independently by a mixing absolutely continuous invariant measure of a piecewise expanding and smooth mapf of the circle, we consider for each >0 the point process obtained by recording the timesn>0 such that |f n (x)–f n (y)|. With the further assumption that the density of is bounded away from zero, we show that when tends to zero the above point process scaled by –1 converges in law to a marked Poisson point process with constant parameter measure. This parameter measure is given explicity by an average on the rate of expansion off.Partially supported by FAPESP grant number 90/3918-5  相似文献   

3.
Stoll's construction [7] of Lévy Brownian motion l on d as a white noise integral is used to obtain an action functional I(x) defined for the surfaces x of l. This provides a Cameron-Martin formula for translation of Lévy measure , and also a large deviation principle for scaled Lévy measures . Proofs follow the lines of [2], where nonstandard techniques were used to give natural proofs of the corresponding results for Wiener measure.The research for this paper was supported partly by a grant from the SERC.  相似文献   

4.
5.
Summary The result linking shift-coupling to time-average total variation convergence and to the invariant -field is extended to continuous time and an analogous result established linking -couplings to smooth total variation convergence and to a smooth tail -field. Shift- and -coupling inequalities are presented.  相似文献   

6.
n (D) — ,s n (D), v (v=1, 2, ...,s/2) — . m={0x 0<x 1<...<x 2m–1<2,x 2m =x 0+2} , x j +1–x j <(4s max v )–1,j=0, 1, ..., 2m –1, ( ) 2- - n,m 2m , m . , L q - (1q) W ( n )={f 2 :f (n–1)AC 2 , n (D)f 1} 2- - (s n f), m . , - - n,m .

The author expresses his gratitude to Yu. N. Subbotin for a useful discussion on the results of this paper.  相似文献   

7.
Let be a fixed point free group given by the presentation where and are relative prime numbers, t = /s and s = gcd( – 1,), and is the order of modulo . We prove that if (1) = 2, and (2) is embeddable into the multiplicative group of some skew field, then is circular. This means that there is some additive group N on which acts fixed point freely, and |((a)+b)((c)+d)| 2 whenever a,b,c,d N, a0c, are such that (a)+b(c)+d.  相似文献   

8.
Summary We investigate classes of conditioned super-Brownian motions, namely H-transformsP H with non-negative finitely-based space-time harmonic functionsH(t, ). We prove thatH H is the unique solution of a martingale problem with interaction and is a weak limit of a sequence of rescaled interacting branching Brownian motions. We identify the limit behaviour of H-transforms with functionsH(t, )=h(t, (1)) depending only on the total mass (1). Using the Palm measures of the super-Brownian motion we describe for an additive spacetime harmonic functionH(t, )=h(t, x) (dx) theH-transformP H as a conditioned super-Brownian motion in which an immortal particle moves like an h-transform of Brownian motion.  相似文献   

9.
Summary We consider increasing processes {X(t)t0} of classL, that is, increasing self-similar processes with inswpendent increments. Leth(t) be an increasing positive function on (0,) withh(0+)=0 andh()=. By virtue of the zero-one laws, there existsc (resp.C) [0,] such that lim inf (resp. lim sup)X(t)/h(t)=c (resp.C) a.s. both ast tends to 0 and ast tends to . We decide a necessary and sufficient condition for the existence ofh(t) withc orC=1 and explicitly constructh(t) in caseh(t) exists withc orC=1. Moreover, we give a criterion to classify functionsh(t) withc (orC)=0 andh(t) withc (orC)= in caseh(t) does not exist withc (orC)=1.  相似文献   

10.
Some dimension results for super-Brownian motion   总被引:4,自引:0,他引:4  
Summary The Dawson-Watanabe super-Brownian motion has been intensively studied in the last few years. In particular, there has been much work concerning the Hausdorff dimension of certain remarkable sets related to super-Brownian motion. We contribute to this study in the following way. Let (Y t)t0 be a super-Brownian motion on d (d2) andH be a Borel subset of d . We determine the Hausdorff Dimension of {t0; SuppY tHØ}, improving and generalizing a result of Krone. We also obtain a new proof of a result of Tribe which gives, whend4, the Hausdorff dimension of SuppY t as a function of the dimension ofB.  相似文献   

11.
Z d — k=(k 1, ...,k d) k j,d1.d- (8), . . a k s m= a k s, >0 N, min (m 1,...,m d)N, ¦s ms¦. , , >0 N, min (m 1,...,m d)N min (n 1,...,n d)N, ¦s ms n. . , (8) , >0 N, max (b 1,...,b d) N, mZ d , m1, ¦s(b, m)¦ where   相似文献   

12.
Let be a ball in N, centered at zero, and letu be a minimizer of the nonconvex functional over one of the classesC M := {w W loc 1, () 0 w(x) M in,w concave} orE M := {w W loc 1,2 () 0 w(x) M in,w 0 inL()}of admissible functions. Thenu is not radial and not unique. Therefore one can further reduce the resistance of Newton's rotational body of minimal resistance through symmetry breaking.  相似文献   

13.
. (R) fg(y)h(x–y) dx dy f ^ (x)g ^ (y)h ^ (x–y)dx dy (f,g0) —:f×gf ^ ×g ^(f,g 0) f^ g^ f g -, X — . , - f 1f 2 , f 1 ^ ×gf 2×g 0g. .  相似文献   

14.
, (t) >0 E(–, +),E<, , ¦f(t(t) xE, f(t)=0 (–, +).  相似文献   

15.
16.
Summary Let be a natural exponential family on and (V, ) be its variance function. Here, is the mean domain of andV, defined on , is the variance of . A problem of increasing interest in the literature is the following: Given an open interval and a functionV defined on , is the pair (V, ) a variance function of some natural exponential family? Here, we consider the case whereV is a polynomial. We develop a complex-analytic approach to this problem and provide necessary conditions for (V, ) to be such a variance function. These conditions are also sufficient for the class of third degree polynomials and certain subclasses of polynomials of higher degree.  相似文献   

17.
18.
Summary We say that the discD()R 2, of radius , located around the origin isp-covered in timeT by a Wiener processW(·) if for anyzD() there exists a 0tT such thatW(t) is a point of the disc of radiusp, located aroundz. The supremum of those 's (0) is studied for which,D() isp-covered inT.  相似文献   

19.
We construct a probability measure giving a mathematical realization of Polyakov's heuristic measure for bosonic strings in space-time dimensions 3d13, having as world sheet compact Riemann surfaces of arbitrary genus. The measure involves the path space measures for scalar fields with exponential interaction on and a measure on Teichmüller space.Deceased 24 January 1988  相似文献   

20.
, . , L p (2) p>1 . , C(T3), - , . - .

This work was completed while the first named author was a visiting professor at Indiana University, Bloomington, Indiana; and the second named author was a visiting professor at Ohio State University, Columbus, Ohio, U.S.A.  相似文献   

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