Program PHONON v.4.1.1 starts ... Today is 18Dec2009 at 18:21:45 Ultrasoft (Vanderbilt) Pseudopotentials bravais-lattice index = 2 lattice parameter (a_0) = 10.2000 a.u. unit-cell volume = 265.3020 (a.u.)^3 number of atoms/cell = 2 number of atomic types = 1 kinetic-energy cut-off = 18.0000 Ry charge density cut-off = 72.0000 Ry convergence threshold = 1.0E-14 beta = 0.7000 number of iterations used = 4 Exchange-correlation = SLA PZ NOGX NOGC (1100) celldm(1)= 10.20000 celldm(2)= 0.00000 celldm(3)= 0.00000 celldm(4)= 0.00000 celldm(5)= 0.00000 celldm(6)= 0.00000 crystal axes: (cart. coord. in units of a_0) a(1) = ( -0.5000 0.0000 0.5000 ) a(2) = ( 0.0000 0.5000 0.5000 ) a(3) = ( -0.5000 0.5000 0.0000 ) reciprocal axes: (cart. coord. in units 2 pi/a_0) b(1) = ( -1.0000 -1.0000 1.0000 ) b(2) = ( 1.0000 1.0000 1.0000 ) b(3) = ( -1.0000 1.0000 -1.0000 ) Atoms inside the unit cell: Cartesian axes site n. atom mass positions (a_0 units) 1 Si 28.0800 tau( 1) = ( 0.00000 0.00000 0.00000 ) 2 Si 28.0800 tau( 2) = ( 0.25000 0.25000 0.25000 ) Computing dynamical matrix for q = ( 0.0000000 0.0000000 0.0000000 ) 49 Sym.Ops. (with q -> -q+G ) G cutoff = 189.7462 ( 2733 G-vectors) FFT grid: ( 20, 20, 20) number of k points= 10 cart. coord. in units 2pi/a_0 k( 1) = ( 0.1250000 0.1250000 0.1250000), wk = 0.0625000 k( 2) = ( 0.1250000 0.1250000 0.3750000), wk = 0.1875000 k( 3) = ( 0.1250000 0.1250000 0.6250000), wk = 0.1875000 k( 4) = ( 0.1250000 0.1250000 0.8750000), wk = 0.1875000 k( 5) = ( 0.1250000 0.3750000 0.3750000), wk = 0.1875000 k( 6) = ( 0.1250000 0.3750000 0.6250000), wk = 0.3750000 k( 7) = ( 0.1250000 0.3750000 0.8750000), wk = 0.3750000 k( 8) = ( 0.1250000 0.6250000 0.6250000), wk = 0.1875000 k( 9) = ( 0.3750000 0.3750000 0.3750000), wk = 0.0625000 k( 10) = ( 0.3750000 0.3750000 0.6250000), wk = 0.1875000 PseudoPot. # 1 for Si read from file Si.vbc.UPF Pseudo is Norm-conserving, Zval = 4.0 Generated by new atomic code, or converted to UPF format Using radial grid of 431 points, 2 beta functions with: l(1) = 0 l(2) = 1 Electric field: Dielectric constant Born effective charges Atomic displacements: There are 2 irreducible representations Representation 1 3 modes -T_1u G_15 G_4- To be done Representation 2 3 modes -T_2g G_25' G_5+ To be done