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In a regular grid (gij) that obeys the cubic symmetry, the Fermi surface is represented as Fgij = ∑n exp [- (E gij (n) - EF) 2 /2 σ2], where E gij (n) are all electronic eigenvalues and σ=35 meV is the integration window. The density of spanning vectors is Dhkl = ∑ gij [Fgij F (g+h,j+k,j+l) mod], where the sum runs over the same cubic grid with indices modulo the size of the unit cell in the reciprocal space.
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In a regular grid (gij) that obeys the cubic symmetry, the Fermi surface is represented as Fgij = ∑n exp [- (E gij (n) - EF) 2 /2 σ2], where E gij (n) are all electronic eigenvalues and σ=35 meV is the integration window. The density of spanning vectors is Dhkl = ∑ gij [Fgij F (g+h,j+k,j+l) mod], where the sum runs over the same cubic grid with indices modulo the size of the unit cell in the reciprocal space.
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See EPAPS Document No. E-PRBMDO-78-R11826 for the visualization of the contributions to the spanning density for selected momentum transfers. For more information on EPAPS, see
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