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Nonadiabatic Dynamics

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... section for the reactive channel of F HD HF D ... The time-independent calculations were carried out on Capecchi and Werner (CW) diabatic PESs ... – PowerPoint PPT presentation

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Title: Nonadiabatic Dynamics


1
Nonadiabatic Dynamics
  • Ke-Li Han
  • State Key Laboratory of Molecular Reaction
    Dynamics, Dalian Institute of Chemical Physics,
    Chinese Academy of Sciences

2
Outline
  • Theoretical studies Nonadiabatic Quantum
    dynamics of F(2P3/2,2P1/2)HD, Cl(2P3/2,
    2P1/2)H2, O(3P,1D)H2 using time-dependent
    wavepacket method
  • Experimental studies Direct measurement of the
    conversion time from the Sn(n2,3,4) to the S1
    states of Chlorophyll a by using femtosecond
    laser in solution

3
The spin-orbit effect for nonadiabatic F(2P3/2,
2P1/2) H2 /DH reaction
  • Since Lee and coworkers work in 1985, the
    reaction FH2 has been as a case example of
    textbook for molecular reaction dynamics
  • Recently Kopin Liu and coworkers have found that
    a resonant peak appears in the integral cross
    section for the reactive channel of FHD?HFD
    experimentally
  • Skodje and coworkers have done the quantum
    scattering calculations on Stark and Werner (SW)
    PES.

4
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5
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6
Alexander, Stark, and Werner fitted new coupled
PESs (named as ASW PESs) published in J. Chem.
Phys. 113 (2000) 11084.
7
Research approach
  • Improvement of the three-dimensional
    time-dependent wavepacket method
  • Develop an extended split operator
    scheme(XSOS) to propagate the quantum wavepacket
  • A Fortran code embodied the XSOS

8
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9
Basis Function
Kk?s
10
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11
Probabilities calculated on the two PESs and six
PESs for the reaction of F(2P1/2) with H2 (vj0)
as a function of the translation energy for
J0.5. the dotted line is for the
time-independent result(Ref.24).
12
TDWP nonadiabatic calculation for the FHD
reaction on ASW surfaces
13
TDWP nonadiabatic calculation for the FHD
reaction on ASW surface
14
Modified ASW potential energy surfaces (MASW PESs)
  • The barrier height of ASW potential energy
    surfaces is lowered by 0.016eV for the lowest
    barrier at the bent configuration and lowered by
    0.015eV for the collinear with the scale external
    correlation technique, developed by Truhlar and
    coworkers

15
FHD?HFD
16
FHD?DFH
17
Cl(2P3/2)?Cl(2P1/2)H2
18
????
19
????
The time-independent calculations were carried
out on Capecchi and Werner (CW) diabatic PESs
20
We have re-fitted the diabatic coupled surfaces
for ClH2, named as Xie and Han (XH) PESs
21
The integral cross sections for the reaction ClH2
22
Conclusions
  • The calculated cross sections on modified ASW
    PESs are much closer to experimental results than
    those on ASW PESs for FHD
  • The calculated cross sections of the SO excited
    state on XH PESs are much higher than those on CW
    PESs for ClH2. We are confirming those results.

23
Time-dependent wavepacket study of the
intersystem crossing effects in O(3P,1D)H2
reaction
  • An exact quantum scattering calculation

24
About O(3P,1D)H2 reaction
  • Prolific dynamics information
  • Most investigated reaction system
  • Research interests
  • single PES problems
  • abstraction/insertion mechanism et al.
  • multi-PES problems
  • role of excited surface
  • role of spin-orbit induced transition

25
Why do this quantum calculation?
  • Intersystem crossing is important in many
    reaction systems such as enzymatic reaction,
    surface induced collision and dissociation et al.
  • Very few theoretical work, no quantum study so
    far
  • Schatz and coworkers TSH method
  • Challenges are daunting difficult to perform
    exact quantum scattering calculation for such
    issue.

26
Challenges
  • Too many electronic states coupled in the
    intersystem crossing
  • A feasible quantum dynamics method to treat this
    multi-surface problem
  • The deep singlet state potential well about 7.9
    eV in the reaction system

27
A schematic profile of singlet-triplet crossing
in O(3P,1D)H2 reaction
Schatz and coworkers
28
Results of the quantum calculations (1)
Cross section with wavepacket initially in 3P2
state
29
Results of the quantum calculations (2)
Cross section with wavepacket initially in 3P2
state
30
Results of the quantum calculations (3)
Cross section with wavepacket initially in 3P1
state
31
Results of the quantum calculations (4)
Cross section with wavepacket initially in 3P1
state
32
Results of the quantum calculations (5)
Cross section with wavepacket initially in 3P0
state
33
Results of the quantum calculations (6)
Cross section with wavepacket initially in 3P0
state
34
Results of the quantum calculations (7)
Cross section with wavepacket initially in 1D2
state
35
Results of the quantum calculations (8)
Cross section with wavepacket initially in 1D2
state
36
A comparison between the previous TSH study and
the present quantum study (1)
37
A comparison between the previous TSH study and
the present quantum study (2)
38
Conclusion remark
  • The spin-orbit coupling between triplet states of
    different symmetry, such as 3A and 3A, plays a
    significant role in the singlet-triplet crossing
    process.
  • A branch ratio of product OH spin state ?3/2 to
    ?1/2 is calculated to be around 2.75 1 at high
    collision energy, which is in rough agreement
    with the measured OH ratio of 21 in the reaction
    of O(3P2,1,0) with hydrocarbon.

39
Nonadiabatic quantum dynamics studies of other
systems
  • Nonadiabatic Dynamics of Energy Transfer Process
    electronic quenching process O(1D)
    N2(X1Sg) ?O(3P) N2(X1Sg)
  • Nonadiabatic Dynamics of Charge Transfer
    DH2?DH2
  • Nonadiabatic Photodissociation H2O, CH3I

40
Collaborators
  • Ting-Xian Xie
  • Yan Zhang
  • Tian-Shu Chu
  • Xin Zhang
  • John Zhang
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