1) again: dephasing and energy relaxation with redfield theory

13
1) Again: Dephasing and Energy Relaxation with Redfield Theory 2) Compare with: Kubo Lineshape Theory h Q 0 (1- )( - ) H Q 0 2 Q = F 0 0 o 1965+ 1957

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1) Again: Dephasing and Energy Relaxation with Redfield Theory. 1965+. 2) Compare with: Kubo Lineshape Theory. 1957. Bloch Model :. Redfield Model :. 2. Pollard, Friesner JCP 100 (1994) 5054, Oxtoby, Rice, CPL 42 (1976) 1. 2. Spatial Coherence. IR-Spectrum. - PowerPoint PPT Presentation

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Page 1: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

1) Again: Dephasing and Energy Relaxation with Redfield Theory

2) Compare with: Kubo Lineshape Theory

h Q0 (1- ) ( - )H Q0

2

Q = F0

0

o

1965+

1957

Page 2: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

d dt/ = - i -

n

n

m

m mm

nn

mm

nm

(t+dt)

mm

nn

mm

nm

(t)

Page 3: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

n

n

m

m mm

nn

mm

nm

(t+dt)

mm

nn

mm

nm

(t)Rn m n m

=1/ T2

mm mmR =1/ T1

Bloch Model:

Page 4: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

n

n

m

m mm

nn

mm

nm

(t+dt)

mm

nn

mm

nm

(t)

Redfield Model:

Rn m n m

mm mmR

Rn mk l

Rm mnn

Rn m n m

mm mmR

Rn mk l

Rm mnn

Page 5: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

Q = F0

Q F (t) Q F (0)

o

Q H (t) Q H (0)2

Rn m n m

mm mmR

Rn mk l

Rm mnn

2

Pollard, Friesner JCP 100 (1994) 5054,Oxtoby, Rice, CPL 42 (1976) 1

Page 6: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

0 2 4 6 8 10 12-0.75

-0.5

-0.25

0

0.25

0.5

0.75

1

25 50 75 100 125 150 175 200

0

0.1

0.2

0.3

0.4

25 50 75 100 125 150 175 200

0

0.5

1

1.5

2

2.5

3

IR-Spectrum

0 2 4 6 8 10 12-1

-0.5

0

0.5

1

Spatial Coherence

Page 7: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

0 2 4 6 8 10 12

0

0.1

0.2

0.3

0.4

0.5

0 2 4 6 8 10 12

0

0.5

1

1.5

2

2.5

3

0 2 4 6 8 10 12

0

0.2

0.4

0.6

0.8

0 2 4 6 8 10 12

0

0.5

1

1.5

2

2.5

3

Level Populations

Energy above zero-level

Page 8: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

H H(t) (o)2 2 2Q.Q

JG( )

F F2 Q.Q (t) (0)

JF( )

Page 9: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

m

m+1

m-1

m-2

m+2

1h

2 (m+1) e JF( )0

- h 0

1h

2 m JF( )0

12h

2

- h 2012h

2 (m+1)(m+2) e JG( )2 0

12h

212h

2 m(m-2) JG( )2 0

Rm mnn

Page 10: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

m

14h

2

{

Rn mnm

n

1h

2 { (m+n) + (n+m+2) e }

JF( )0

- h 0

11h

2 (m-n) J2 G( )0

JG( )20

[(n+1)(n+2) +(m+1)(m+2)] e + + n (n-1) m (m-1)

- h 20 {

Pure dephasing:

Population-induced:

Page 11: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

JG( )

S Dpectral ensity

10 fs time

c

modulation strength

modulation speed

2) Compare with Kubo Lineshape Theory - totally classical !

h Q0 (1- ) ( - )H Q0

2

0 o

H H(t) (o)2 2 2Q.Q (t) (o) A C Futo orrelation unction

Page 12: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

Q

(t)

10 fs time

c

modulation strength

modulation speed

d dt (t) (t)Q/ = i Q

Q = Q exp{i } exp{i d } (t) t0 0

tintegrate:

Q Q = Q exp{i } exp{i d } (t) (0) t02

0

tautocorrelate:

(t) (o)

exp{ d (t )

M( ) }0

t

cumulant expansion:

=M ( )t

Page 13: 1)   Again:         Dephasing and Energy Relaxation  with Redfield Theory

(t) (o)

exp{ d (t )

M( ) }0

t

=M ( )t

Q

(t)

10 fs time

c

modulation strength

modulation speed

e xp { i M ( ) + d d

M ( ) }

0

t

0

t

0

general:

Kubo

=0,fast M(t)