The Generalized Coherent State ansatz: Application to quantum electron-vibrational dynamics

The Generalized Coherent State ansatz: Application to quantum electron-vibrational dynamics

Accepted Manuscript The Generalized Coherent State Ansatz: Application to Quantum Electron-Vibrational Dynamics Raffaele Borrelli, Maxim F. Gelin PII:...

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Accepted Manuscript The Generalized Coherent State Ansatz: Application to Quantum Electron-Vibrational Dynamics Raffaele Borrelli, Maxim F. Gelin PII: DOI: Reference:

S0301-0104(16)30271-3 http://dx.doi.org/10.1016/j.chemphys.2016.05.013 CHEMPH 9557

To appear in:

Chemical Physics

Please cite this article as: R. Borrelli, M.F. Gelin, The Generalized Coherent State Ansatz: Application to Quantum Electron-Vibrational Dynamics, Chemical Physics (2016), doi: http://dx.doi.org/10.1016/j.chemphys.2016.05.013

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i o ω 2 2 (pli + qli2 ) + gqli + ωki (rlK + s2lK ) 2 l,i,K X p + (ωqli + g) 2(ki + 1)(rlK+1i rlK + slK+1i slK )

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l +

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+

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l,i,K

V = 2J Re{ O!" (".6F7 6F"3 N,

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X

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(k1 , ..., kd ),

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7."

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1.0

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0.8

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!"#$% &' ()*#+,-!). )/ -0% !.!-!,+ %+%1-$).!1 2-,-% ,2 , /#.1-!). )/ -!3% !. , 3)+%1#+,$ $!." 4!-0 && %+%1-$).!1 2-,-%25 60% *,$,3%-%$2 )/ -0% 3)7%+ ,$% J = 100 13−1 8 ω = 1000 13−1 9 ,: g = 0.2ω8 ;: g = ω5 60% .#3;%$ )/ ;,-0 3)7%2 !2 N = 119 -0% 3,?@& ,.7 =>?@A5 B,20@7)--%7 +!.% C −·: %<1!-,-!). +%D%+2 )/ -0% N %+%1-$).!1 2-,-%2 c = 0 CB&:9 7,20%7 +!.% C@ @: c = 19 /#++ +!.% CE: c = 29 C×: F>6BG $%2#+-5 !

1.0

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45698

+3)% :!&-!; ,/&*2 (!" )3(!)*)3%$'&(0 )+ (!" .$/&/ +,*-(&)*/ K, αl ; :" !$<"

i o g 2 H= m + ω(|αmi | + ki ) + √ (¯ αmi + αmi ) |CmK | 2 miK X g p + [ωαmi + √ ] ki + 1C¯mK+1i CmK 2 miK X g p + [ω α ¯ mi + √ ] ki C¯mK−1i CmK 2 miK X +J C¯lK CmJ hK, αl |J, αm i + #6-6. X nh

2



456=8

lmKJ

>?'&((&*2 "$-! ?$3$%"("3 &*() &(/ 3"$' $*1 &%$2&*$30 -)%?)*"*(; (!" #$%&'@ ()*&$* -$* ." 3":3&(("* &* (!" +)3% H = H◦ + V

456A8

o i 2 2 )/2 + ωki + gqmi (rmK m + ω(p2mi + qmi + s2mK )

456B8

:&(! H◦ = +

X nh

miK

X

p (ωqmi + g) 2(ki + 1)(rmK+1i rmK + smK+1i smK )

X

ωpmi

miK

+

miK

V=J

X

lmKJ

p

2(ki + 1)(rmK+1i smK − smK+1i rmK )

C¯lK CmJ hK, αl |J, αm i = 2J

− (rlK smJ

X Xh (rlK rmJ + slK smJ ) Re hK, αl |J, αm i JK m>l

i − slK rmJ ) Im hK, αl |J, αm i

7B

456C8

!" #$%"&'()* hK, αl |J, αmi ('" +,-.)"/ $0-1"'*2 %!(% +($ 1" "3()0(%"4 15 0*#$& %!" '"+0''"$+" '")(%#,$* 4"*+'#1"4 #$ (.."$4#/ 67 !" +()+0)(%#,$ ,8 %!" 4"'#3(%#3"* ,8 %!" 9(-#)%,$ 80$+%#,$ :#%! '"*."+% %, (rlK , slK , qli, pli) 8,)),:* 8',- *%($4('4 4#;"'"$%#(%#,$ '0)"* io n Xh ω (p2li + qli2 ) + gqli + ωki slK ∂slK H = 2 l + 2 i Xp + 2(ki + 1)[(ωqli + gli )slK+1i − ωpli rlK+1i ]

<=7>(?

i

+

Xp i

2ki [(ωqli + g)slK−1i + ωpli rlK−1i ] + ∂slK V

io n Xh ω (p2li + qli2 ) + gqli + ωki rlK ∂rlK H = 2 l + 2 i Xp + 2(ki + 1)[(ωqli + g)rlK+1i + ωpli slK+1i ]

<=7>1?

i

+

Xp i

∂pli H = ωpli

2ki [(ωqli + g)rlK−1i − ωpli slK−1i ] + ∂rlK V

X

2 (rlK + s2lK ) +

K

∂qli H = (ωqli + g)

X p ω 2(ki + 1)(rlK slK+1i − rlK+1i slK ) + ∂pli V K

X K

2 (rlK

<=7>+?

X p + s2lK ) + ω 2(ki + 1)(rlK+1i rlK + slK+1i slK ) + ∂qli V. K

<=7>4?

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hK, αl |J, αm i = K D(−αl )D(αm ) J

DE

<=7C?

!" #$%!& '(# )%*!$ +,- !" +,. /' *0) %! X Vln (rlK rnJ + slK snJ )× ∂qni V = 2 lKJ

r hr j + 1 i ji pni i RehK, αl |J+1i , αn i− RehK, αl |J−1i , αn i+ ImhK, αl |J, αn i 2 2 2 X −2 Vln (rlK snJ − slK rnJ )× lKJ

r hr j + 1 i ji pni i ImhK, αl |J+1i , αn i− ImhK, αl |J−1i , αn i− RehK, αl |J, αn i 2 2 2 12,34 !"

∂pni V = −2

X

Vln (rlK rnJ + slK snJ )×

lKJ

r hr j + 1 i ji qni i ImhK, αl |J+1i , αn i+ ImhK, αl |J−1i , αn i+ ImhK, αl |J, αn i 2 2 2 X +2 Vln (rlK snJ − slK rnJ )× lKJ

r i hr j + 1 ji qni i RehK, αl |J+1i , αn i+ RehK, αl |J−1i , αn i+ RehK, αl |J, αn i 2 2 2 12,564

!!"#$%& '( )*+#,-.'/#$/# %#0"1*+23 78' *!'9"%:'!$%*! ; <= !>?9@*!"*! %!)'&= ;$ hK, αl |J, αm i > ! 0' >*:9 A#)'" 0B ='>#=='!>' C*=:#; ',DE.F EGF EEH I!"''" /' J=$) *0$'=K' )8 )



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1@,M4

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