闲逛
发表于 2025-3-26 23:25:00
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ALLEY
发表于 2025-3-27 02:51:51
Neurobiology of Decision-Makingd ... It is proved that the characteristic polynomial of any C-invariant (1, 1) tensor .. is a perfect square; therefore, its eigenvalues have even multiplicities. Any .-invariant metric .. is indefinite and has signature σ ≤ ..
好色
发表于 2025-3-27 05:59:18
Neurobiology of Decision-Makingstruction of .-matrices in terms of any generalized inverse of ad(.). For generic . a generalized inverse (and indeed the Moore-Penrose inverse) is explicitly constructed. The .-matrices are in general momentum dependent and dynamical. We apply our construction to the elliptic Calogero-Moser-Sutherl
avenge
发表于 2025-3-27 10:27:38
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Aids209
发表于 2025-3-27 16:21:18
The Springer Series on Human Exceptionality, . ≥ 1, and the anisotropy parameter Δ ∈ ℝ. The Heisenberg spin chain corresponds to Δ = 1. We show the completeness of the Bethe ansatz eigenstates, and give an explicit Plancherel decomposition of ..(Δ) for all N and Δ. We observe a critical spectral phenomenon in the anisotropy regime |Δ | < 1.
共栖
发表于 2025-3-27 21:18:37
Cindy Van Rooy,John Song,Con Stoughding to Baxter’s argument for commuting transfer matrices, the trace of the .-operator gives a commutative difference system. We show that for our .-operator this approach gives the elliptic Macdonald-type operators, actually equivalent to Ruijsenaars’s operators. The calculation of the trace uses a
珐琅
发表于 2025-3-27 23:15:33
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过分
发表于 2025-3-28 04:54:33
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语言学
发表于 2025-3-28 06:52:08
https://doi.org/10.1007/b111152ecial inverse problem for linear operators with elliptic coefficients. Hamiltonian theory of such systems is developed with the help of universal symplectic structure proposed by D. H. Phong and the author. Canonically conjugated variables for spin generalizations of the elliptic CM and RS systems a
压倒性胜利
发表于 2025-3-28 10:53:44
https://doi.org/10.1007/b111152aars—Schneider (RS) models. This paper is devoted to recent advances in the combinatorial theory of these functions. The emphasis is put on the creation operators that allow us to construct the excited state wave functions of the CS and RS models from their ground state wave functions.