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1.
We show that Toda lattices with the Cartan matrices A n , B n , C n , and D n are Liouville-type systems. For these systems of equations, we obtain explicit formulas for the invariants and generalized Laplace invariants. We show how they can be used to construct conservation laws (x and y integrals) and higher symmetries.  相似文献   

2.
We describe W-geometry of two-dimensional Toda systems associated with the Lie algebra C n . __________ Translated from Fundamental’naya i Prikladnaya Matematika (Fundamental and Applied Mathematics), Vol. 11, No. 1, Geometry, 2005.  相似文献   

3.
We present an explicit formula for integrals of the open two-dimensional Toda lattice of type An. This formula is applicable for various reductions of this lattice. As an illustration, we find integrals of the G2 Toda lattice. We also reveal a connection between the open An Toda and Shabat-Yamilov lattices.  相似文献   

4.
We establish, using a new approach, the integrability of a particular case in the Kozlov-Treshchev classification of Birkhoff integrable Hamiltonian systems. The technique used is a modification of the so called quadratic Lax pair for D n Toda lattice combined with a method used by M. Ranada in proving the integrability of the Sklyanin case.   相似文献   

5.
Let (B n) be the order complex of the Boolean algebra and let B(n, k) be the part of (B n) where all chains have a gap at most k between each set. We give an action of the symmetric group S l on the l-chains that gives B(n, k) a Hodge structure and decomposes the homology under the action of the Eulerian idempontents. The S n action on the chains induces an action on the Hodge pieces and we derive a generating function for the cycle indicator of the Hodge pieces. The Euler characteristic is given as a corollary.We then exploit the connection between chains and tabloids to give various special cases of the homology. Also an upper bound is obtained using spectral sequence methods.Finally we present some data on the homology of B(n, k).  相似文献   

6.
We consider the heat equation u t = Lu where L is a second-order difference operator in a discrete variable n. The fundamental solution has an expansion in terms of the Bessel functions of imaginary argument. The coefficients α k (n, m) in this expansion are analogs of Hadamard’s coefficients for the (continuous) Schr?dinger operator. We derive an explicit formula for α k in terms of the wave and the adjoint wave functions of the Toda lattice hierarchy. As a first application of this result, we prove that the values of these coefficients on the diagonals n = m and n = m + 1 define a hierarchy of differential-difference equations which is equivalent to the Toda lattice hierarchy. Using this fact and the correspondence between commutative rings of difference operators and algebraic curves we show that the fundamental solution can be summed up, giving a finite formula involving only two Bessel functions with polynomial coefficients in the time variable t, if and only if the operator L belongs to the family of bispectral operators constructed in [18].  相似文献   

7.
Under the constraint determined by a relation (a n ,b n )T={f(?)} n between the reflectionless potentials and the eigenfunctions of the general discrete Schrödinger eigenvalue problem, the Lax pair of the Toda lattice is nonlinearized to be a finite-dimensional difference system and a nonlinear evolution equation, while the solution varietyN of the former is an invariant set of S-flows determined by the latter, and the constants of the motion for the algebraic system are presented.f maps the solution of the algebraic system into the solution of a certain stationary Toda equation. Similar results concerning the Langmuir lattice are given, and a relation between the two difference systems, which are the spatial parts of the nonlinearized Lax pairs of the Toda lattice and Langmuir lattice, is discussed.  相似文献   

8.
Lattice chains and Delannoy paths represent two different ways to progress through a lattice. We use elementary combinatorial arguments to derive new expressions for the number of chains and the number of Delannoy paths in a lattice of arbitrary finite dimension. Specifically, fix nonnegative integers n1,…,nd, and let L denote the lattice of points (a1,…,ad)∈Zd that satisfy 0≤aini for 1≤id. We prove that the number of chains in L is given by where . We also show that the number of Delannoy paths in L equals Setting ni=n (for all i) in these expressions yields a new proof of a recent result of Duchi and Sulanke [9] relating the total number of chains to the central Delannoy numbers. We also give a novel derivation of the generating functions for these numbers in arbitrary dimension.  相似文献   

9.
We consider the heat equation u t = Lu where L is a second-order difference operator in a discrete variable n. The fundamental solution has an expansion in terms of the Bessel functions of imaginary argument. The coefficients α k (n, m) in this expansion are analogs of Hadamard’s coefficients for the (continuous) Schr?dinger operator. We derive an explicit formula for α k in terms of the wave and the adjoint wave functions of the Toda lattice hierarchy. As a first application of this result, we prove that the values of these coefficients on the diagonals n = m and n = m + 1 define a hierarchy of differential-difference equations which is equivalent to the Toda lattice hierarchy. Using this fact and the correspondence between commutative rings of difference operators and algebraic curves we show that the fundamental solution can be summed up, giving a finite formula involving only two Bessel functions with polynomial coefficients in the time variable t, if and only if the operator L belongs to the family of bispectral operators constructed in [18].   相似文献   

10.
We have studied recently solvability and semi‐cycles of eight systems of difference equations of the following form: where a ∈ [0, + ), the sequences pn, qn, rn, sn are some of the sequences xn and yn, with positive initial values x?j,y?j, j = 1,2, in detail. This paper is devoted to the study of the other eight systems of the form. We show that these systems are also solvable in closed form and describe semi‐cycles of their solutions complementing our previous results on such systems of difference equations.  相似文献   

11.
We present the third in the series of papers describing Poisson properties of planar directed networks in the disk or in the annulus. In this paper we concentrate on special networks N u,v in the disk that correspond to the choice of a pair (u, v) of Coxeter elements in the symmetric group S n and the corresponding networks Nu,v°N_{u,v}^\circ in the annulus. Boundary measurements for N u,v represent elements of the Coxeter double Bruhat cell G u,v ⊂GL n . The Cartan subgroup H acts on G u,v by conjugation. The standard Poisson structure on the space of weights of N u,v induces a Poisson structure on G u,v , and hence on the quotient G u,v /H, which makes the latter into the phase space for an appropriate Coxeter–Toda lattice. The boundary measurement for Nu,v°N_{u,v}^\circ is a rational function that coincides up to a non-zero factor with the Weyl function for the boundary measurement for N u,v . The corresponding Poisson bracket on the space of weights of Nu,v°N_{u,v}^\circ induces a Poisson bracket on the certain space Rn {\mathcal{R}_n} of rational functions, which appeared previously in the context of Toda flows.  相似文献   

12.
Li  David Linnan  Shahriari  Shahriar 《Order》2001,18(3):247-267
Let 2 [n] denote the poset of all subsets of [n]={1,2,...,n} ordered by inclusion. Following Gutterman and Shahriari (Order 14, 1998, 321–325) we consider a game G n (a,b,c). This is a game for two players. First, Player I constructs a independent maximal chains in 2 [n]. Player II will extend the collection to a+b independent maximal chains by finding another b independent maximal chains in 2 [n]. Finally, Player I will attempt to extend the collection further to a+b+c such chains. The last Player who is able to complete her move wins. In this paper, we complete the analysis of G n (a,b,c) by considering its most difficult instance: when c=2 and a+b+2=n. We prove, the rather surprising result, that, for n7, Player I wins G n (a,na–2,2) if and only if a3. As a consequence we get results about extending collections of independent maximal chains, and about cutsets (collections of subsets that intersect every maximal chain) of minimum possible width (the size of largest anti-chain).  相似文献   

13.
We consider a system of equations describing stimulated combination scattering of light. We show that solutions of this system are expressed in terms of two solutions of the sine-Gordon equation that are related to each other by a Bäcklund transformation. We also show that this system is integrable and admits a Zakharov-Shabat pair. In the general case, the system of equations for the Bäcklund transformation of periodic A n (1) Toda chains is also shown to be integrable and to have a Zakharov-Shabat pair.  相似文献   

14.
We give necessary and sufficient conditions for the sum of subspaces H 1,…, H n , n ≥ 2, of a Hilbert space H to be a subspace and present various properties of the n-tuples of subspaces with closed sum.  相似文献   

15.
16.

This paper considers extremal systems of points on the unit sphere S rR r+1, related problems of numerical integration and geometrical properties of extremal systems. Extremal systems are systems of d n =dim P n points, where P n is the space of spherical polynomials of degree at most n, which maximize the determinant of an interpolation matrix. Extremal systems for S 2 of degrees up to 191 (36,864 points) provide well distributed points, and are found to yield interpolatory cubature rules with positive weights. We consider the worst case cubature error in a certain Hilbert space and its relation to a generalized discrepancy. We also consider geometrical properties such as the minimal geodesic distance between points and the mesh norm. The known theoretical properties fall well short of those suggested by the numerical experiments.

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17.
As in [A. Sarychev, Controlling multiparticle system on the line. I, J. Differential Equations 246 (12) (2009) 4772-4790] we consider classical system of interacting particles P1,…,Pn on the line with only neighboring particles involved in interaction. On the contrast to [A. Sarychev, Controlling multiparticle system on the line. I, J. Differential Equations 246 (12) (2009) 4772-4790] now periodic boundary conditions are imposed onto the system, i.e. P1 and Pn are considered neighboring. Periodic Toda lattice would be a typical example. We study possibility to control periodic multiparticle systems by means of forces applied to just few of its particles; mainly we study system controlled by single force. The free dynamics of multiparticle systems in periodic and nonperiodic case differ substantially. We see that also the controlled periodic multiparticle system does not mimic its nonperiodic counterpart.Main result established is global controllability by means of single controlling force of the multiparticle system with a generic potential of interaction. We study the nongeneric potentials for which controllability and accessibility properties may lack. Results are formulated and proven in Sections 2, 3.  相似文献   

18.
A real number x is computable iff it is the limit of an effectively converging computable sequence of rational numbers, and x is left (right) computable iff it is the supremum (infimum) of a computable sequence of rational numbers. By applying the operations “sup” and “inf” alternately n times to computable (multiple) sequences of rational numbers we introduce a non‐collapsing hierarchy {Σn, Πn, Δn : n ∈ ℕ} of real numbers. We characterize the classes Σ2, Π2 and Δ2 in various ways and give several interesting examples.  相似文献   

19.
20.
We prove an isoperimetric inequality for wreath products of Markov chains with variable fibers. We use isoperimetric inequalities for wreath products to estimate the return probability of random walks on infinite groups and graphs, drift of random loops, the expected value E(exp(−tR n )), where R n is the number of distinct sites, visited up to the moment n, and, more generally, (where L z,n is the number of visits of z up to the moment n and F(x, y) is some non-negative function).  相似文献   

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