Lucia Reining - TDDFT.org

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Comparison in“Transition” spaceΦ(n1,n2;r)≡ψ (r)ψ* (r)n1 n2FBSE(n1n2)(n3n4)=−∫drdr'Φ(n1,n3;r)W(r',r)Φ * (n2,n4;r')F<strong>TDDFT</strong>(n1n2)(n3n4)= ∫ drdr'Φ(n1,n2;r)fxc(r,r')Φ * (n3,n4;r')
Comparison in“Transition” spaceΦ(n1,n2;r)≡ψ (r)ψ* (r)n1 n2FBSE(n1n2)(n3n4)=−∫drdr'v,v’c,c’Φ(n1,n3;r)W(r',r)Φ * (n2,n4;r')F<strong>TDDFT</strong>(n1n2)(n3n4)= ∫ drdr'Φ(n1,n2;r)fxc(r,r')Φ * (n3,n4;r')v,c v’,c’
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How to describe………………
Page 5 and 6:
What is a spectrum?
Page 7 and 8:
hνWhat is a spectrum?
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hνWhat is a spectrum?
Page 12 and 13:
…but also:Perturbation -- Respons
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Perturbation -- ResponseResponse =>
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Perturbation -- ResponseResponse =>
Page 18 and 19:
V ind = (δV H /δρ + δV xc /δρ
Page 20 and 21: ρ ind = χ V extχ = χ 0 + χ 0 (
Page 22 and 23: 1b) TDDFT in practicei) Finite syst
Page 24 and 25: EELS : v is dominantOlevano and Rei
Page 26 and 27: Absorption: no long range in RPA.An
Page 28 and 29: So which potential in the “real w
Page 30 and 31: So which potential ?cv
Page 32 and 33: Koopman’s theorem(e.g. Hartee Foc
Page 34 and 35: Hartree :Hartree - Fock :Beyond :ρ
Page 36 and 37: From ∂ρ/∂tto:∂/∂t G =…
Page 38 and 39: Σ = i ∫GWΓW = v + ∫v P WP = -
Page 40 and 41: Σ = i ∫GWΓW = v + ∫v P WP = -
Page 42 and 43: E c -E v (minimum, eV)DFT-KSΣ=iGWE
Page 44 and 45: Γ = δΣ = i ∫GWΓW = v + ∫v P
Page 46 and 47: χ = P 0 + P 0 (v-W) χδV H /δρ
Page 48 and 49: χ = P 0 + P 0 (v-W) χδV H /δρ
Page 50 and 51: Absorption ?cv
Page 52 and 53: Absorption ?cVariation of potential
Page 54: (H el + H hole + H el-hole ) A λ =
Page 59 and 60: BSE and TDDFT: different worlds, sa
Page 67 and 68: TDLDA
Page 69: BSE and TDDFT: different worlds, sa
Page 73 and 74: Reining, Olevano, Rubio, Onida (PRL
Page 76 and 77: Botti, Vast, Reining, Olevano, Andr
Page 78 and 79: •The lack of a long range term in
Page 80 and 81: BSE and TDDFT: merge!TDDFT:χ = χ
Page 82 and 83: BSE and TDDFT: merge!TDDFT:χ = χ
Page 84 and 85: BSE and TDDFT:”Mapping theory”T
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Page 92 and 93: All of us:•Potentially efficient
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Lucia Reining - TDDFT.org

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