elastic and inelastic electron-phonon scattering in...
TRANSCRIPT
![Page 1: Elastic and Inelastic Electron-Phonon Scattering in ...th.fhi-berlin.mpg.de/th/meetings/vc2012/presentations/2012-11-09_C… · O. V. Prezhdo J. Chem. Phys. 124 201104 (2006) problems](https://reader033.vdocuments.mx/reader033/viewer/2022052006/601ab54e94e2517c8643cc7c/html5/thumbnails/1.jpg)
CECAM
Nov 7-9, 2012
Oleg Prezhdo
U. Rochester
Elastic and Inelastic Electron-Phonon
Scattering in Quantum Dots
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Electron-Phonon
Dynamics in QDs
Elastic
Luminescence linewidths
Coherences between single and
multiple excitons, etc.
Semiclassical corrections to
quantum-classical simulations
Inelastic
Charge cooling
Phonon-assisted Auger processes
Electron transfer from QD to TiO2
Photochemistry on QD surface
(e.g. water splitting)
We study these processes in other nanoscale materials as well
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Outline
Nonadiabatic Molecular Dynamics with TDDFT
• Quantum-classical approximations
• Decoherence & zero-point energy corrections
Quantum Dots
• Electron-Phonon Relaxation & Phonon Bottleneck
• Multiple Exciton Generation and Recombination
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Nonadiabatic Molecular Dynamics
electrons treated quantum-mechanically
nuclei treated classically
e e
e e
e
e
Nonadiabatic MD: Coupling
between potential surfaces
opens channels for system to
change electronic states.
transition allowed
weak coupling strong coupling
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Time-Domain DFT for
Nonadiabatic Molecular Dynamics
p
p xx2
)( SDNvqp txtxtx ,,, 21
Electron density derives from Kohn-Sham orbitals
H tRDFT functional depends on nuclear evolution
txH
t
txi p
p,
,
2,1pVariational principle gives
Ricci R
Orbitals are expanded in adiabatic KS basis
xtctx pp ,
tRxtRtRxtRxH ;;;
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Time-Domain DFT
in Many-Body Kohn-Sham Basis C. Craig, W. Duncan, O. V. Prezhdo Phys. Rev. Lett. 95, 163001 (2005)
non-zero only if different in one orbital
Need to define states to hop between
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1. KS excitations close to LR/TDDFT (in contrast to HF and CIS)
2. Typically, no bond-breaking, conformational changes, etc.
3. Many-electron systems, single excitation is a small perturbation
4. Averaging over many initial conditions and pathways
Why KS Representation Works S. Fischer, B. Habenicht, A. Madrid, W. Duncan,
O. V. Prezhdo, J. Chem. Phys. 134, 024102 (2011)
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Silicon Quantum Dot S. Fischer, B. Habenicht, A. Madrid, W. Duncan,
O. V. Prezhdo, J. Chem. Phys. 134, 024102 (2011)
KS and LR
agree
better for
PW91
(pure DFT)
than
B3LYP
(hybrid)
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Silicon Quantum Dot S. Fischer, B. Habenicht, A. Madrid, W. Duncan,
O. V. Prezhdo, J. Chem. Phys. 134, 024102 (2011)
KS and LR
agree
better for
PW91
(pure DFT)
than
B3LYP
(hybrid)
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Silicon Quantum Dot S. Fischer, B. Habenicht, A. Madrid, W. Duncan,
O. V. Prezhdo, J. Chem. Phys. 134, 024102 (2011)
W. H. Miller, T. F. George,
J. Chem. Phys. 56, 5637 (1972)
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Theoretical Questions
our group is interested in
How to couple quantum and classical dynamics?
quantum influence on classical trajectory
Can one do better than classical mechanics for nuclear motion?
zero-point motion, tunneling, branching, loss of coherence
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Quantum-Classical Lie Bracket O. V. Prezhdo, V. V. Kisil Phys. Rev. A 56 162 (1997)
O. V. Prezhdo J. Chem. Phys. 124 201104 (2006)
problems with Jacobi identity:
Practical solution: derive everything quantum mechanically,
take classical limit at the end
quantum commutator + classical Poisson bracket
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Ehrenfest (mean-field)
Total energy of
electrons and nuclei
0dt
dEtotis conserved
RxHxTrRVRM
E xtot ;2
2
time-dependent Hellmann-Feynman theorem gives Newton equation
quantum force
RxHxTrVRM RxR ;
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Bohmian Quant.-Class. Mechanics
/),(),(),( txiSetxtx gives Newton eq.
)(
)(
2)(
22
x
x
mxQ x
)()( xQxVxm r
with non-local quantum potential
Q(x)
),()( RxVRVRM xRRR )(RQdrop
)(),()( xQRxVxVxm xRxx
Quantum (x) – Classical (R)
Advantage
Branching
C. Brooksby, O. V. Prezhdo Phys. Rev. Lett. 86, 3215 (2001); ibid 90, 118902 (2003)
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Bohmian Quant.-Class. Mechanics
Q(x)
),()( RxVRVRM xRRR
Advantage: correlation between quantum and
classical particles (branching)
C. Brooksby, O. V. Prezhdo Phys. Rev. Lett. 86, 3215 (2001); ibid 90, 118902 (2003)
),()()( RxVxTrRVRM xRxRR
– Bohmian
– Ehrenfest
In practice, Bohmian trajectories are obtained from Schrodinger eq.
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Highly simplified representation of O2 interacting with Pt
J. Strömquist, S. Gao, J.Chem.Phys. 106, 5751 (1997); D.S. Sholl, J.C. Tully, J.Chem.Phys. 109, 7702 (1998)
Q)B(q
c)b(qc)2b(q
q
22
Q
qQqqQq
AeQ)(q,V
)2ea(e(q)V
2
QMΩ(Q)V
Q)(q,V(Q)V(q)VTTQ)H(q,
Bohmian Quant.-Class.
Brooksby, Prezhdo Phys. Rev. Lett. 86, 3215 (2001)
- - - Ehrenfest
––– Bohmian
o o exact
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a.k.a., quantum-master equation
with time-dependent transition rates:
- non-perturbative
- correct short time dynamics
Trajectory branching: Tully, JCP 93, 1061 (1990);
Detailed balance / thermal equilibrium (due to hop rejection): Parahdekar, Tully JCP 122, 094102 (2005)
Surface Hopping
Within TDDFT: Craig, Duncan, Prezhdo PRL 95, 163001 (2005)
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Schrodinger Cat and Decoherence
| B >0
cat
alive
dead
atom
System - radioactive atom; Bath - cat
In Nanomaterials
System - electrons, spins; Bath - phonons
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Franck-Condon Factor
and Decoherence
Bath (vibrational) wave
functions diverge
B2
B1 B2
2
E1 – E2
= e i E 1 – E 2 t/h B1 t B2 t dt
| B >0
This affects evolution of (electronic) system
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Decoherence and Surface Hopping
hopping probability
11 12
21 22
11 12 B2 B1
21 B1 B2 22
P12 ~ 12
Reduced density matrix: = B S–B B
12 0 on decoherence
time scale
O. V. Prezhdo, P. J. Rossky, Phys. Rev. Lett. 81, 5294 (1998)
O. V. Prezhdo, Phys. Rev. Lett. 85, 4413 (2000)
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Decoherence and Surface Hopping
hopping probability
11 12
21 22
11 12 B2 B1
21 B1 B2 22
P12 ~ 12
Reduced density matrix: = B S–B B
12 0 on decoherence
time scale
0.1
2+ 0.1
2< 0.1 + 0.1
2Decoherence makes transitions less likely
P12 = T12
2+ T12
2+ ...With decoherence:
P12 = T12 + T12+ ...
2
Without decoherence
Quantum Zeno Effect
O. V. Prezhdo, P. J. Rossky, Phys. Rev. Lett. 81, 5294 (1998)
O. V. Prezhdo, Phys. Rev. Lett. 85, 4413 (2000)
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Stochastic Mean-Field (SMF)
dWLdtLLdtiHd
2
Stochastic Schrodinger equation
in place of regular SE in Ehrenfest
L – system-bath interaction
– decoherence rate
Advantages
1. Includes decoherence
2. Gives branching
3. Infinitesimal velocity rescaling,
(but every time-step)
O. V. Prezhdo J. Chem. Phys. 111, 8366 (1999); Phys. Rev. Lett. 85, 4413 (2000)
Ehrenfest/MF
SH
SMF
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Decoherence Induced
Surface Hopping (DISH)
Evolve in an adiabatic state.
Hop when a decoherence event occurs.
Rescale velocity as before in SH.
Advantages
1. Includes decoherence
2. Gives branching
3. Nuclear evolution in pure states
4. Gives detailed balance / thermal equilibrium
H. Jaeger, S. Fisher, O. V. Prezhdo J. Chem. Phys. 137, 22A545 (2012)
DISH
SMF
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Evaluating Decoherence Times
Optical response function
DE
, eV
2nd order cumulant approximation
in (6,4) CNT
Kamisaka, Kilina, Yamashita, Prezhdo, Nano Lett. 6, 2295 (2006)
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Evaluating Decoherence Times
Optical response function
DE
, eV
in (6,4) CNT
Gaussian approximation
| B >0
thermal de Broglie width
2nd order cumulant approximation
Kamisaka, Kilina, Yamashita, Prezhdo, Nano Lett. 6, 2295 (2006)
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but and
the infinite hierarchy is
terminated by a closure
q2
q q
q3
3 q2
q 2 q3
d q2
dtpq qp 2 pq s
Quantized Hamilton Dynamics O. V. Prezhdo, Y. V. Pereverzev J. Chem. Phys. 113, 6557 (2000)
O. V. Prezhdo Theor. Chem. Acc. 116, 206 (2006)
V = q 2
2 + q 3
3
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Harmonic Oscillator in Mapped QHD-2
hbar
mass hbar
mass
QHD-2 takes care of
zero-point-energy
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Metastable Cubic Potential in Mapped QHD-2
hbar
mass hbar
mass
QHD-2
gives
tunneling
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Double-Slit Potential in Mapped QHD-2
potential seen by
a narrow wavepacket
V q1
2V
2q s
2
potential seen by
a wide wavepacket
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QMF-2 equations require no new quantum calculation !
C. Brooksby, O. V. Prezhdo,
Chem. Phys. Lett., 346 463 (2001)
Quantized Ehrenfest
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Highly simplified representation of O2 interacting with Pt
J. Strömquist, S. Gao, J.Chem.Phys. 106, 5751 (1997); D.S. Sholl, J.C. Tully, J.Chem.Phys. 109, 7702 (1998)
Q)B(q
c)b(qc)2b(q
q
22
Q
qQqqQq
AeQ)(q,V
)2ea(e(q)V
2
QMΩ(Q)V
Q)(q,V(Q)V(q)VTTQ)H(q,
C. Brooksby, O. V. Prezhdo,
Chem. Phys. Lett., 346 463 (2001)
Quantized Ehrenfest
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Energy Transfer (Tunneling)
and Dephasing
Spin-Boson/Marcus Model
aSSagωS
2
1aaΩH z
Jaynes-Cummings Model
- same curvatures
- no displacement
- resonance (rotating wave) approx.
D.S. Kilin, Yu.V. Pereverzev, O.V. Prezhdo, J. Chem. Phys., 120 11209 (2004)
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ENERGY TRANSFER
(TUNNELING):
spin oscillation
DEPHASING:
wave-packet splits
spin stops oscillating
Quantum Result
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Evolution of <Sz> by QHD
aSSaα
aSSaβ
zS2
1aaγ
1n
z
nn
z
nn
nn
γSg
βγgdtγSd
αγδdtβγd
βγδdtαγd
n=0,1,2…
βγ,αγ,γS,β,α,S zz - 6 variables
2
z
2
zz
2
z γS2γSγγS2γS closure:
2γ,γ are constants of motion, linear system of ODE
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tg
tg
tSz 22
2
00
2
12
1
00
2
cos12
1cos1
2
1
2
1
Multiple transfer events
Dephasing envelope
D.S. Kilin, Yu.V. Pereverzev, O.V. Prezhdo, J. Chem. Phys., 120 11209 (2004)
Evolution of <Sz> by QHD
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State-Specific Dynamics a.k.a. multi-configuration mean-field
closure:
– as before
D.S. Kilin, Yu.V. Pereverzev, O.V. Prezhdo, J. Chem. Phys., 120 11209 (2004)
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Surface hopping is needed to describe inelastic scattering
Kohn-Sham representation works well for surface hopping in
nanoscale materials
Decoherence (elastic scattering) is fast in condensed phases
Stochastic Mean-Field (SMF) and Decoherence Induced Surface
Hopping (DISH) “derive” a SH algorithm from decoherence
Quantized Hamilton Dynamics (QHD) provides models for zero-
point energy and decoherence
Summary for TDDFT / NAMD
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Electron-Phonon Dynamics in QDs
rates of carrier cooling
mechanisms for carrier
multiplication
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Excitons in QDs: 2005 Shaller, Klimov PRL 92 186601 (2004); Ellingson, Beard, Johnson,
Yu, Micic, Nozik, Shabaev, Efros, Nano Lett. 5 865 (2005)
Biexciton creation yield Exciton to biexciton time
under 0.25ps
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Schaller, Pietryga, Goupalov, Petruska, Ivanov, Klimov
Phys. Rev. Lett. 95 196401 (2005)
Electron-Phonon Relaxation
No phonon bottleneck.
Times are similar to
biexciton creation times
Larger dots relax more slowly ?!
Excitons in QDs: 2005
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Nair, Bawendi Phys. Rev. B 76 081304(R) (2007)
Original multiplication
experiments could not be
reproduced by other groups.
Experimental conditions
and data interpretation
are very important.
Excitons in QDs: 2007
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Efficiency estimates are
significantly lowered
Observed
Ideal
Bulk
Excitons in QDs: 2008 McGuire, Joo, Pietryga, Schaller, Klimov
Acc. Chem. Res. 41 1810 (2008)
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Electron-phonon bottleneck found for electrons
in CdSe QDs, in the absence of holes
Excitons in QDs: 2008
Pandey, Guyot-Sionnest, Science 322 929 (2008)
(shell thickness)
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Excitons in PbSe QDs: 2010 Zhu group, Science 328 1543 (2010); Parkinson group, Science 330
63 (2010); Nozik group, Science 334 1530 (2011)
absorbed photon–to–current efficiency 50 fs injection time
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Structural Relaxation PbSe QDs
Relaxed,
T=0 K
Bulk,
T=0 K Heated,
T=300 K
136 atoms Pb68
Se68 d=1.4nm 32 atoms Pb
16Se
16 d=1.0nm
Bulk,
T=0 K
Relaxed,
T=0 K
Heated,
T=300 K
states mix
(LUMO+1) (LUMO+2) (LUMO+3) (LUMO) (LUMO+1) (LUMO+2) (LUMO+3) (LUMO)
Kilina, Kilin, Prezhdo, ACS Nano, 3, 93 (2009)
Kilina, Craig, Kilin, Prezhdo, J. Phys. Chem. C 111 4871 (2007)
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Absorption Spectra of PbSe QDs
Pb68
Se68
Energy, eV
oscillator strength
Pb16
Se16
Energy, eV
oscillator strength
Kilina, Kilin, Prezhdo, ACS Nano, 3, 93 (2009)
Kilina, Craig, Kilin, Prezhdo, J. Phys. Chem. C 111 4871 (2007)
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Pop
ula
tion
of
4 s
tate
s n
ear
to
thre
shold
hole states (VB)
electron states (CB)
Time, fs
Comparison of Relaxation, PbSe
Sub-picosecond times
agree with experiment e.g. Gdor et al.
ACS Nano 6, 3269 (2012)
Similar relaxation times
for electrons and holes
Larger dot relaxes more slowly
due to weaker
electron-phonon coupling
Kilina, Kilin, Prezhdo, ACS Nano, 3, 93 (2009)
Kilina, Craig, Kilin, Prezhdo, J. Phys. Chem. C 111 4871 (2007)
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Phonon Bottleneck for 1P
Electron in CdSe Quantum Dots
1P–1S electron states show big gap
Relaxation time ~ 1ns
Pandey, Guyot-Sionnest, Science 322 929 (2008)
Kilina, Kilin, Prezhdo,
ACS Nano, 3, 93 (2009)
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Phonon Bottleneck for 1P
Electron in CdSe Quantum Dots
Relaxation time ~ 1ns
Pandey, Guyot-Sionnest, Science 322 929 (2008)
Neukirch, Kilina, Kilin, Prezhdo,
in preparation
Simulation shows bottleneck
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Electrons relax much faster than holes ! (despite nearly symmetric DOS)
Enhanced Energy Losses
due to Ligands
Ge Si
Si DOS
Kim, Madrid, Prezhdo, Dalton Trans., 45, 10069 (2009)
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Low frequency modes
are active for both
electrons and holes
However,
high frequency
(ligand)
modes are active
only for electrons
Enhanced Energy Losses due to
Ligands: Active Phonon Modes Kim, Madrid, Prezhdo, Dalton Trans., 45, 10069 (2009)
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Phonon-Assisted Auger Processes
Eg = 2.1 eV
SE & DE DOS
cross at 5.8 eV
25 VB and 24 CB orbitals
98,101 states =
ground+600SE+97,500DE
(9,623,806,201
matrix elements)
Kim, Prezhdo, Nano Lett., 11, 1845 (2011)
Kim, Prezhdo, ACS Nano, 6, 1239 (2012)
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ME Generation
Gaussian + Exponential
Rates increase
with energy
Phonon-assisted
Auger at energies
less than 2Eg
Kim, Prezhdo, Nano Lett., 11, 1845 (2011)
Kim, Prezhdo, ACS Nano, 6, 1239 (2012)
Auger processes are slower than electron-phonon relaxation,
multiple excitons are created while interacting with light
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ME Recombination
Robel et al. PRL 102 177404 (2009)
MEG
MEG
MER
MER
Si29H24
sub-10ps for small QDs
rate theories give much longer times
experiment
Kim, Prezhdo, Nano Lett., 11, 1845 (2011)
Kim, Prezhdo, ACS Nano, 6, 1239 (2012)
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Electron-Phonon
Dynamics in QDs
Inelastic scattering on 10-100fs timescale (luminescence, single &
multiple exciton coherences)
Electron-phonon relaxation on a picosecond timescale
Phonon bottleneck in special cases
Phonon-assisted Auger processes are predicted
Phonons drive adiabatic and nonadiabatic electron transfer
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Quantum dots
Chem. Phys. Lett. – Frontier 460 1 (2008)
Acc. Chem. Res 42 2005 (2009)
Chem. Science 2 400 (2011)
Selected Publications
Surface hopping within TDDFT
Phys. Rev. Lett. 95, 163001 (2005) /original implementation/
Phys. Rev. Lett. 100, 197402 (2008) /decoherence corrected/
J. Am. Chem. Soc., 134, 15648 (2012) /spin-orbit interactions/
Decoherence based surface hopping/
J. Chem. Phys. 111, 8366 (1999) /stochastic mean-field/
Phys. Rev. Lett. 85, 4413 (2000) /anti-Zeno effect/
J. Chem. Phys. 137, 22A545 (2012) /decoherence induced SH/
Quantized Hamilton dynamics
J. Chem. Phys. 113, 6557 (2000)
Theor. Chem. Acc. 116, 206 (2006)
Quantum-classical Lie bracket
Phys. Rev. A 56 162 (1997)
J. Chem. Phys. 124 201104 (2006)
Bohmian quantum-classical dynamics
Phys. Rev. Lett. 86, 3215 (2001)
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Group Picture
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Group Picture
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Questions Arising
in our Research
− When is classical description of phonons valid?
− What quantum corrections are needed and when
(zero point energy, decoherence)?
− Are there alternatives to surface hopping;
can one “derive” surface hopping?
− Surface hopping requires states, can we use DFT?
− Can we model light-matter interactions separate
from electron-phonon dynamics?
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Pure-Dephasing: Luminescence,
ME Generation & ME Fission
T=300K/100K
Luminescence – 50meV linewidth, agree with exp.
ME Generation – rapid 10fs dephasing
ME Fission – 100fs
Phonon-induced pure-dephasing times, fs
Madrid, Hyeon-Deuk, Prezhdo, ACS Nano 3 2487 (2009)
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More Realistic Ligands:
Electronic Structure Kilina, Velizhanin, Ivanov, Prezhdo, Tretiak ACS Nano, 6, 6515 (2012)
Ligands start contributing
at energies of 2.5-3Eg
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Ligand Contribution to
Electron-Phonon Relaxation Kilina, Velizhanin, Ivanov, Prezhdo, Tretiak ACS Nano, 6, 6515 (2012)
Ligands contributes up to 10nm QDs
bulk
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Electron Transfer from QDs to TiO2
Parkinson group, Science 330 63 (2010)
absorbed photon–to–current efficiency 50 fs injection time
Zhu group, Science 328 1543 (2010)
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• 10 fs time; mostly adiabatic ET
strong donor-acceptor coupling
• ET is driven by high frequency
polar phonons
Long, Prezhdo J. Am. Chem. Soc.133 19240 (2011)
e- transfer from QDs to TiO2
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Hartree-Fock Band Structure
1. Small dots represent large dot DOS
2. Huge one-electron gap
3. Symmetric vs. asymmetric DOS
4. Secondary gaps in PbSe DOS
Fischer, Isborn, Prezhdo, Chem. Science, 2, 400 (2011)
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Spectra and Multiple Excitons
PbSe
CdSe
spectra (SAC-CI calculations) fraction of multiple excitons
1. Sharp onset of multiple excitons
2. Above threshold: double excitons in PbSe;
single, double and superpositions in CdSe
CdSe spectra agree
with experiment
JACS 128, 629 (2006)
Fischer, Isborn, Prezhdo, Chem. Science, 2, 400 (2011)
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Direct Mechanism: Si Clusters
spectra fraction of multiple excitons
1. Complete and fairly sharp transition
2. Si is more similar to PbSe than CdSe
due to symmetric band structure
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Universal Optical Response
in Si Clusters
Classical Mie theory matches ab initio
calculations on very small clusters,
independent of bonding configuration
Idrobo et al. PRB 79 125322 (2009)
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Defects Introduce
New Transitions
ideal QDs anion cation dopant
dangling bonds
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Calculations for Charged PbSe Dots
Conduction band
transitions
overwhelm MEs
Much higher
ME threshold
Fischer, Isborn, Prezhdo, Chem. Science, 2, 400 (2011)