sfb 450 seminary: wave packet dynamics & relaxation jan. 21, 2003 arthur hotzel, fu...
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Liouville representation: L = Liouville tensor, R = relaxation tensor (4th order tensors). relaxation of an harmonic oscillator:. SFB 450 seminary: wave packet dynamics & relaxation Jan. 21, 2003 Arthur Hotzel, FU Berlin. - PowerPoint PPT PresentationTRANSCRIPT
SFB 450 seminary: wave packet dynamics & relaxationJan. 21, 2003 Arthur Hotzel, FU Berlin
density matrix representation, relaxation: energy dissipation and pure dephasing
Liouville representation:
L = Liouville tensor, R = relaxation tensor (4th order tensors)
RHiL
dtd ,
Redfield theory I: relaxation due to "random" perturbation
relaxation rates given by spectral densities of the autocorrelation function of the perturbation needs ad-hoc correction for finite temperature
Redfield theory II: relaxation due to coupling to bath which is in thermal equilibrium
gives correct temperature dependence
202
2
22
22qqm
qH
relaxation of an harmonic oscillator:
"random" variation of equilibrium position q0 ~ perturbation q: energy dissipation by 1-quantum stepsno pure dephasing (diagonal elements of perturbation vanish)
"random" variation of eigenfrequency ~ perturbation q2: energy relaxation by 2-quantum stepspure dephasing
Coupled harmonic oscillators:Excited state intramolecular proton transfer (ESIPT)SFB 450 seminary, Jan. 21, 2003 Arthur Hotzel, FU Berlin
enol/enol
keto/enol enol/keto
2,5-bis(2-benzoxazolyl)-hydroquinone (BBXHQ)
proton transfer in the first excited state (singlet), enol (A) keto (B)
high-frequency proton oscillation around equilibrium positions A, B (coordinate q)
proton site-site distance modulated by low-frequency scaffold mode (coordinate Q)
q(proton coordinate)
Q(scaffo ld coord.)
ener
gy
enolketo
enolketo
Dynamics without dissipation second Born-Oppenheimer approximation:
pure enol(A)/keto(B) eigenstates:electrons: proton,: scaffold,:
),,(),()(),,( rqQqQQrqQ
consider only first electronically excited enol and keto singlet states
total Hamiltonian:pure enol/keto Hamiltonian:
EH
rqQWHH
0
0 ),,(
enol-keto coupling:
),,(),,(),,(),(
),(),(),()(
)()()(
*'
3.'
.'
*''
..''
..''
*''''''
rqQrqQWrqQrdqQW
qQqQWqQdqQW
QQWQdQW
nel
elelpr
elpr
and
with
meV517:),(),( ..,
.' elel
enolketoel WqQWqQW
assume electronic coupling independent of nuclear coordinates:
Proton wave functions
furthermore, consider only proton vibrational ground states ( = ' = 0):
)()()(
),(),()(
,*
,'.
,0,,0',''
,0*,0
QFCPRQQdQWWW
qQqQdqQFCPR
enolketoel
enolketo
enolketo
factor CondonFrankprotonic
protonic Frank-Condon factor FCPR depends strongly on scaffold coordinate Q:
FCPR(Q) = 0.006 at left-hand classical turning point of scaffold vibrational
ground state (enol)
FCPR(Q) = 0.081 at right-hand classical turning point of scaffold vibrational
ground state (enol)q
(proton coordinate)
Q(scaffo ld coord.)
ener
gy
enolketo
enolketo
Scaffold vibrational states
Effective scaffold potentials are harmonic potentials with vibrational energy ħ = 14.6 meV, reduced mass M = 47.8 amu (proton vibrational energy ħ = 335 meV).
enol keto basis transformation:
enolketoFCSC ,*
,','
Keto and enol scaffold equilibrium positions are shifted by 0.077 Å with respect to each other.
,3,2,1,0',
4.4321''2
1
ityexothermicmeV:keto
:enol
E
E
Eigenenergies of scaffold vibrational states without enol-keto coupling:
Enol-keto coupling
enolketo
el
FCSC
QFQFFFCSCWW
MQ
,*
,','
,'2.
,' 210
03003020
02010010
2
express Q in terms of creation/annihilation operators of vibrational scaffold states(enol basis):
)()()( ,*
,'.
,0,,0','' QFCPRQQdQWWW enolketoel
enolketo
approximate FCPR(Q) by parabola:
2210)( QFQFFQFCPR
Total Hamiltonian in the enol/keto basis
,,,α,,,α
W
WH
†
,,,α,,,α
210'210
4.4321'
21
',
,'
210'210
states, keto states, enol
meV
states, keto states, enol
Eigenstates of H (considering enol/keto states = 0, ..., 9, ' = 0, ..., 9):
Initial state: Excitation from molecular ground state with delta pulse; scaffold ground state equilibrium position shifted by 0.077 Å with respect to electronically excited enol state.
Q[Å]
ener
gy [a
mu
Å2 p
s-2]
initi
al s
tate
(eno
l bas
is)
pure
eno
l sta
tes
pure
ket
o st
ates
initi
al s
tate
(ene
rgy
bas
is)
H e
igen
stat
es
Wavefunction dynamics without dissipation
transfer back into enol/keto basis
diagonalize H: eigenvalues Hk, eigenvectors k
express initial state in terms of eigenstates of H
kk
ktHi
exp
propagate for time t:
blue: projection onto enol basisred: projection onto keto basis
elapsed time [oscillation periods = 0.283 ps]energy
(reduced enol/keto Hamiltonian)[amu Å2 ps-2]
Q[Å]
Dissipation We consider random perturbation of the form (in enol/keto basis):
,,,α
,,,α
G
,,,α,,,α
210'
210
03003020
02010010
0
003003020
02010010
~
210210
states, keto
states, enol
states, enol states, enol
Random perturbation proportional to scaffold elongation from equilibrium (Q - Q0) in the enol and keto states.
Relaxation tensor
Make basis transformation to eigensystem of H:
We assume short correlation time c of random correlation:
r lr
rjlrik
r kr
rkirjl
lj
iklj
ki
ikljijkl
ji
c
kTHHGG
kTHHGG
kTHHGG
kTHHGGfR
H
jiHH
exp1exp1
exp1exp1
,1
2
:) of basis reigenvecto (in tensor relaxation
const.onperturbati random of function ationautocorrel ofdensity spectral
GG ~
We take f = 200 ps
Wavepacket dynamics with dissipation
= density matrix in eigenvector basis of H
L = Liouville tensor
kl
klijklijji
klklijkl
ij RHHi
Ldtd
22n treat as -dimensional vector (n = 10 = number of included scaffold vibrational states in the enol- and keto electronic states)
22 22 nn treat L as -matrix
diagonalize L: eigenvalues Lk, eigenvectors k
express initial state (t = 0) in terms of eigenstates of L
kkk tL exp propagate for time t:
transfer back into eigenvector basis of H and then into enol/keto basis
blue: projection onto enol basisred: projection onto keto basis
energy(reduced enol/keto Hamiltonian)
[amu Å2 ps-2]elapsed time [oscillation periods = 0.283 ps]
Q[Å]