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Parallel lanczos algorithm on a CRAY-T3D combining PVM and SHMEM routines

机译:结合PVM和SHMEM例程的CRAY-T3D并行Lanczos算法

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The metal insulator transition (MIT) of cubic tungsten bronzes Na spb x WO sub 3 has been studied in detail as a function of composition x and temperature [6]. One theoretical approach to address the question of the origin of the MIT in the Na sub x WO sub 3 bronzes incorporating electron interaction and correlated disorder is a two-dimensional Anderson-Mott-Hubbard (AMH) model [7]. The resulting Hamiltonian matrix H has to be solved in an unrestricted Hartree-Fock (UHF) approach, t.m. independently for electrons in teh two spin states alhha and beta. At each step of an UHF iteration the matrix H has to be diagonalized. Only conduction band (CB) states are taken into account, t.m. approximately 3
机译:立方钨青铜Na spb x WO sub 3的金属绝缘体转变(MIT)已作为成分x和温度的函数进行了详细研究[6]。解决Nasub x WO sub 3青铜器中电子结合和相关无序的MIT起源问题的一种理论方法是二维Anderson-Mott-Hubbard(AMH)模型[7]。最终的哈密顿矩阵H必须以无限制Hartree-Fock(UHF)方法t.m求解。对于两个自旋态的电子分别为Alhha和Beta。在UHF迭代的每个步骤中,矩阵H必须对角线化。仅考虑导带(CB)状态t.m.约3

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