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New Approaches for Quantum Dissipative Dynamics and Spectroscopy of Condense-Phase Molecular Systems

Department of Chemistry & Center for Quantum �Science and Technology, National Taiwan University

Physics Division, National Center for Theoretical Sciences

QFort Workshop, NCKU, Tainan

April 16, 2024

Yuan-Chung Cheng*yuanchung@ntu.edu.tw

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Molecular Modeling of Excitonic Dynamics

Research in the Cheng group concerns molecular simulations and quantum dynamic calculations for excitonic phenomena in molecular systems

Dynamics of light harvesting

LHCII, 42 Chls

Exciton/charge dynamics in molecular materials

Singlet fission

Donor/acceptor polymer

2D spectroscopy

Modeling EET using quantum noises

Characterization of gate errors on IBM-Q

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Generic Model for Condensed-Phase Quantum Dynamics

J

Spectral density:

System

Bath

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Generic Model for Condensed-Phase Quantum Dynamics

J

Spectral density:

System

Bath

Electronic Hamiltonian

Spectral density function:�coarse-grained system-bath �interactions

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Strategy for Excitonic System Modeling

J

Spectral density:

System

Bath

Exciton Hamiltonian�Quantum chemistry �+ electrostatic �embedding model

Spectral fitting & MD simulations

Spectral density function

Dynamical theory

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Conventional Theories for Condensed-Phase Quantum Dynamics

J

Spectral density:

System

Bath

Forster theory: weak electronic coupling, incoherent dynamics

Redfield theory: weak system-bath coupling, coherent dynamics

HEOM/QUAPI/…: non-perturbative methods, numerically exact

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Conventional Methods Inadequate for Coherent EET in Photosynthesis

Conventional Förster theory or Redfield equation do not adequately describe photosynthetic EET dynamics – new theories suitable for the intermediate regime are needed.

Comparative study with exact calculations based on the reduced hierarchy equation approach on a model chlorophyll dimer (Ishizaki &Fleming, JCP 2009).

exact

full Redfield

secular Redfield

Forster

Redfield

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Theories for Dissipative Quantum Dynamics

We develop perturbative methods to provide accurate descriptions of quantum dynamics in various parameter regimes:�

  • Small-Polaron Quantum Master Equation (SP-QME): based on a small-polaron basis for quantum excitations
  • Pure-Dephasing Reference System (PDRS) theory: based on a pure-dephasing electronic basis for excitons and electrons (e.g. coherent modified-Redfield theory)
  • Schrodinger-Langevin Equation: based on a separation of frictional effects and fluctuations around the mean – specifically suitable for coupled electronic/nuclear wavepacket dynamics

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Simulating Quantum Dynamics & Spectra

  • Full quantum dynamics
    • Ultrafast & non-Markovian dynamics
    • General form of system-bath interactions
    • Coherence transfer dynamics
    • Dynamics in τ and t periods
    • Two-exciton states
  • Explicit treatment of laser fields
    • Pulse-overlap effects, pulse profiles
    • Avoids rotating-wave approximation

🡪 Single consistent theory for signals and dynamics �going beyond response function formalism

http://quantum.ch.ntu.edu.tw/ycclab/QDAS.html

Quantum Dynamics

Nonlinear Optical

Spectral Signals

Model: He + Ω(ω)

Generalized

dynamical

theory

Light-matterinteractions

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Theories for Dissipative Quantum Dynamics

We develop perturbative methods to provide accurate descriptions of quantum dynamics in various parameter regimes:�

  • Small-Polaron Quantum Master Equation (SP-QME): based on a small-polaron basis for quantum excitations
  • Pure-Dephasing Reference System (PDRS) theory: based on a pure-dephasing electronic basis for excitons and electrons (e.g. coherent modified-Redfield theory)
  • Schrodinger-Langevin Equation: based on a separation of frictional effects and fluctuations around the mean – specifically suitable for coupled electronic/nuclear wavepacket dynamics

Accurate quantum dynamics via 2nd-order perturbative quantum master equation

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Pure Dephasing Reference System (PDRS)

11

Electronic reference basis

 

unitary transformation

U

Diagonal He

 

 

General basis:

 

Site basis

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PDRS Dynamics via 2nd-order Perturbations

12

Diagonal part of Hsb included in the zero-th order Hamiltonian, treated exactly (pure dephasing)

Off-diagonal part of Hsb and Hs treated in the 2nd-order quantum master equation framework

Perturbation

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PDRS Quantum Master Equation

Naturally leads to one FT-term caused by excitonic coupling, one mRT-term by electron-phonon coupling, and cross-terms

13

(Förster theory)

(modified Redfield theory)

Mix perturbation by an intermediate reference system

 

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Variational Polaron Reference System

  • To find an appropriate PDRS basis, we must treat electron-phonon coupling properly
  • variational polaron transformation

14

Site basis (f=0)

(Förster, Redfield)

Displaced basis �(0<f<1)

(variational polaron)

 

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Pure Dephasing Variational Polaron Reference System (PDVPRS)

  •  

15

 

artifact of variational small polaronic ansatz

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PDVPRS vs QUAPI Dynamics

  •  

16

 

 

 

PDVPRS-QME, �CMRT, FT, QUAPI

 

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Dynamics at the Intermediate Regime

  •  

17

PDVPRS-QME, �CMRT, FT, QUAPI

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Theories for Dissipative Quantum Dynamics

We develop perturbative methods to provide accurate descriptions of quantum dynamics in various parameter regimes:�

  • Small-Polaron Quantum Master Equation (SP-QME): based on a small-polaron basis for quantum excitations
  • Pure-Dephasing Reference System (PDRS) theory: based on a pure-dephasing electronic basis for excitons and electrons (e.g. coherent modified-Redfield theory)
  • Schrodinger-Langevin Equation: based on a separation of frictional effects and fluctuations around the mean – specifically suitable for coupled electronic/nuclear wavepacket dynamics

Simulate nonlinear spectra of strongly coupled electronic-vibrational systems

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Two-dimensional Spectroscopy: Four-wave Mixing

Es(τ, Τ, ωt) ~

spectrometer

sample

local

oscillator (LO)

1

2

3

Es(ωτ, Τ, ωt)

Fourier

transform

along τ

1

2

3

4 (LO)

coh.

time

pop.

time

echo

time

T

t

signal

τ

12050

12550

12050

12550

ωτ (input)

ωt (output)

(cm-1)

Energy transfer

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Rich Information Content in a 2D Spectrum

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Theoretical Simulation of 2DES Spectra

The method with explicit treatment on vibrational relaxation dynamics is still underdeveloped

QSLE

Approach

Wong and Cheng JCP 2021

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The Quantum Schrodinger-Langevin Equation Approach

An efficient, novel method for coupled vibronic dynamics and 2D spectroscopy in a dissipative environment

 

Dissipative dynamics + Light-matter interactions

M. T. Wong & Y.-C. Cheng, J. Chem. Phys., 154, 154107 (2021)

 

 

pulse overlap, realistic pulse shape, multiple pathways,… automatically included

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The Quantum Langevin Equation Approach

An efficient, novel method for coupled vibronic dynamics and 2D spectroscopy in a dissipative environment

 

M. T. Wong & Y.-C. Cheng, J. Chem. Phys., 154, 154107 (2021)

  • Friction operator (quantum Schrodinger-Langevin equation)�����Explicit treatment of vibrational relaxation dynamics in each mode on each individual electronic potential energy surface

 

Drag force

Random force

Dissipative dynamics + Light-matter interactions

Separates friction and fluctuation, unlike stochastic approaches

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The Quantum Langevin Equation Approach

An efficient, novel method for coupled vibronic dynamics and 2D spectroscopy in a dissipative environment

 

M. T. Wong & Y.-C. Cheng, J. Chem. Phys., 154, 154107 (2021)

  • Explicit external fields in dynamical simulations�Phase-matching

    • Photon-echo �signals

 

 

 

 

 

 

 

Dissipative dynamics + Light-matter interactions

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The Quantum Langevin Equation Approach

An efficient, novel method for coupled vibronic dynamics and 2D spectroscopy in a dissipative environment

M. T. Wong & Y.-C. Cheng, J. Chem. Phys., 154, 154107 (2021)

  • Combinations of auxiliary wavefunctions

 

 

 

 

 

 

 

 

 

 

10 auxiliary wavefunctions

 

2D spectra

 

Dissipative dynamics + Light-matter interactions

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Vibrational Relaxation in 2DES Signals

Simple model simulation to demonstrate the capability of the QLE approach

Displaced-oscillator model

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Vibrational Relaxation in 2DES Signals

  • Separation of ground-state vs. excited-state coherences:�beating in diagonal peaks 🡪 GS�beating in off-diagonal peaks 🡪 ES

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Spectroscopy of Tagged Hydronium Ions

X=Ar or N2

SLE simulated IR Spectra

Ar-tagged:�Fermi resonance

N2-tagged:�No Fermi resonance

Collaboration with Jer-Lai Kuo & Asuka Fujii

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SLE 2DIR Simulations & Fermi Resonance

Ar-tagged

N2-tagged

Strong coupling leads to square peak pattern for Fermi resonance systems

With Fermi resonance

Without Fermi resonance

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Vibronic Effects in Conical-Intersection (CI) Systems

Dissipative CI dynamics with QME based methods

Solvent effects on CI geometry and mixed quantum-classical methods

Malhado et al., J. Chem. Phys., 137, 22A543 (2012)

Chen et al. Faraday Discuss., 194, 61 (2016)

Irregular intensity distribution for CI model (left)

Excited-state absorption due to CI dynamics

Duan et al., J. Phys. Chem. Lett., 7, 382−386 (2016)

Theoretical studies of 2DES spectra for CI systems

Krčmář et al., J. Chem. Phys., 143, 074308 (2015)

Also Cederbaum/Domcke/Dassia Egorova/Fleming/Mexim Gelin/Yarkony/Artur Izmaylov/David Jonas/ …

Decisive evidence for CI dynamics for molecular systems in condensed-phase remains elusive (Berry phase effect).

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Probing Vibronic Dynamics via 2DEV Spectroscopy

No vibronic coupling

Franck-Condon coupling

Herzberg–Teller coupling

Fleming and coworkers, J. Chem. Phys. 155, 054201 (2021).

2DEV beat maps

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Probing Vibronic Dynamics via 2DEV Spectroscopy

No vibronic coupling

Franck-Condon coupling

Herzberg–Teller coupling

Fleming and coworkers, J. Chem. Phys. 155, 054201 (2021).

2DEV beat maps

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Three-state Two-mode Model

 

 

 

Tuning mode 𝜔𝑡 = 1536 cm−1

Coupling mode 𝜔𝑐 = 1317 cm−1

(model pyrazine system)

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Three-state Two-mode Model

 

 

 

Elucidate CI dynamics and 2D spectra by comparative studies

Two vibronic coupling models

 

Basis states:

Excited-state label (i=1,2)

Coupling mode quanta (nc=1,2,…)

Tuning mode quanta (nt=1,2,…)

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Possible CI Signatures in 2DEV Spectra

2DEV 🡪 electronic excitation (first two pulses), IR probe (last two pulses)

CI

AvC

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2DEV Beat Maps?

CI

AvC

Black curves: 2DEV @ T=0

Color map: beat amplitudes

  • Most peaks exhibit significantly beating signals
  • CI & AvC show very difficult beat patterns

We found it difficult to understand these differences!�

How do we interpret these 2DEV results?

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Interpretation of 2DEV Spectra

2DEV 🡪 electronic excitation (first two pulses), IR probe (last two pulses)

Probe IR signals from the eigenstate selected by optical excitation frequency

2DEV probes nonadiabatic nuclear dynamics on the excited-state potential energy surface after optical excitation 🡪 seeking information at a giving excitation frequency to elucidate CI dynamics?

We should focus on IR signals probed at a given visible excitation frequency!

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CI vs. AvC Dynamics in 2DEV Spectra

Simulated spectra show distinctive difference for the CI system

Probe IR signals from the eigenstate selected by optical excittaion frequency

CI

AvC

 

 

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CI vs. AvC Dynamics in 2DEV Spectra

Ground-state IR

Additional signals sensitive to the transitions between eigenstates strongly affected by CI

Not too different from the two peaks in the ground state IR

CI

AvC

 

 

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CI vs. AvC Dynamics in 2DEV Spectra

Ground-state IR

CI

AvC

FT

Fourier transform along T

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2DEV Signal Beating Frequency Map

CI

AvC

signal

No signal

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2DEV Signal Beating Frequency Map

CI

The signal is from a special coherence transfer pathway that should be unique to CI dynamics

 

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Spectral Dynamics in 2DEV Signals

  • Effectively focusing on anharmonic effects in the potential energy surfaces and linear form of the couplings
  • No true “degenerate CI point (seam)” in quantized energy levels
  • Spectral evolution in T 🡪 detailed vibronic wavepacket dynamics and features of the potential surfaces
  • Genuine spectral signitures of geometric phase effects

CI

AvC

FT

Spectral-evolution based analysis

🡪 provide a less ambiguous way to identify characteristic beating frequencies

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Concluding Remarks

  • A novel quantum Langevin equation approach for dissipative dynamics and 2D spectra simulations with emphasis on vibrational relaxation effects is proposed and developed
  • The QLE approach was applied to investigate 2DES spectra of vibrational relaxation dynamics in a displaced-oscillator mode to demonstrate its capability to describe and capture complete vibrational dynamics in the model
  • 2DES as well as 2DEV spectra for a model CI system were simulated by the QLE approach to search for spectral signatures of CI dynamics
  • We proposed that 2DEV signals probed at a given optical excitation frequencies provide relevant representation of CI dynamics, and showed clearly distinct features in the CI model compared to a avoided crossing model for a representative system

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Acknowledgements

Funding: NCTS/NTU/CoS/CQSE

QSLE/2DEV: Man Tou Wong (黃文滔)

PDVPRS-QME: Pin-Ze Huang (黃品澤)�2DIR: Jun-Hao Yu (尤俊皓)

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Thank You!!