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TOMBO Ver.2 Manual

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4.8 WaveF_HOMO-1.cube, WaveF_HOMO-1.grd,<br />

WaveF_HOMO-1.vasp, and so on 46<br />

Microsoft EXCEL to draw the energy band diagram as a line graph.<br />

band_0001.out is the result of energy eigenvalues (at sequential k points) in the 1 st band;<br />

band_0002.out is the result of energy eigenvalues (at sequential k points) in the 2 nd band;<br />

band_0003.out is the result of energy eigenvalues (at sequential k points) in the 3 rd band;<br />

... ...<br />

4.8 WaveF_HOMO-1.cube, WaveF_HOMO-1.grd,<br />

WaveF_HOMO-1.vasp, and so on<br />

If “W” is assigned in iApp of INPUT.inp, wave output files are generated for all wave<br />

functions between Llevel and Ulevel assigned in INPUT.inp. Files with an extension “cube”<br />

is for GaussView, files with an extension “grd” is for Materials Studio, and files with an<br />

extension “vasp” is for VESTA.<br />

4.9 GWA.out<br />

"GWA.out" file saves the GW calculation results.<br />

In a GW cluster calculation, GWA.out looks like Table 4.1.<br />

In a GW crystal calculation, please find the sentence The Result of q-point sum in<br />

GWA.out file. Information above this sentence is for intermediate calculations and not the<br />

final result. The final result is below this sentence, and looks like Table 4.2 for rutile TiO 2 .<br />

Note: Loopk_k = n (n=1, 2, ...)<br />

n means n th k point, corresponding to KPOINT.inp file.<br />

Note: level with * symbol<br />

It means this level is the highest occupied level, and level *+1 is the lowest empty level.<br />

Note: exc(LDA) is the LDA exchange-correlation potential, Vxc<br />

LDA , in [eV].<br />

Note: eps(LDA) is LDA eigenvalue in [eV].<br />

Note: xg(Fock) is exchange part of self-energy, Σ x , in [eV].<br />

Note: slf(GWA) is correlation part of self-energy, Σ x , in [eV].<br />

Note: QP(GWA) is quasi-particle energy εn,k 0 in [eV].<br />

∫<br />

εn,k 0 = εLDA n,k +<br />

drdr ′ ψ LDA<br />

n,k<br />

∗<br />

(r)[Σ(r,r ′ ;ε LDA<br />

n,k<br />

LDA<br />

) −Vxc<br />

δ(r − r ′ )]ψn,k LDA (r′ ) (4.1)

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