As discussed in Section 9.9, optimization of minimum-energy crossing points (MECPs) along conical seams, followed by optimization of minimum-energy pathways that connect these MECPs to other points of interest on ground- and excited-state potential energy surfaces, affords an appealing one-dimensional picture of photochemical reactivity that is analogous to the “reactant transition state product” picture of ground-state chemistry. Just as the ground-state reaction is not obligated to proceed exactly through the transition-state geometry, however, an excited-state reaction need not proceed precisely through the MECP and the particulars of nuclear kinetic energy can lead to deviations. This is arguably more of an issue for excited-state reactions, where the existence of multiple conical intersections can easily lead to multiple potential reaction mechanisms. AIMD potentially offers a way to sample over the available mechanisms in order to deduce which ones are important in an automated way, but must be extended in the photochemical case to reactions that involve more than one Born-Oppenheimer potential energy surface.
The most widely-used trajectory-based method for nonadiabatic simulations is
Tully’s “fewest-switches” surface-hopping (FSSH) algorithm.
1207
J. Chem. Phys.
(1990),
93,
pp. 1061.
Link
In this approach, classical
trajectories are propagated on a single potential energy surface, but can
undergo “hops” to a different potential surface in regions of near-degeneracy
between surfaces. The probability of these stochastic hops is governed by the
magnitude of the nonadiabatic coupling [Eq. (9.48)].
Considering the ensemble average of a swarm of trajectories then provides
information about, e.g., branching ratios for photochemical reactions.
The FSSH algorithm, based on the AIMD code, is available in Q-Chem for any
electronic structure method where analytic derivative couplings are available,
which at present means CIS, TDDFT, and their spin-flip analogues (see
Section 9.9.1). The nuclear dynamics component of the
simulation is specified just as in an AIMD calculation. Artificial decoherence
can be added to the calculation at additional cost according to the augmented
FSSH (AFSSH) method,
1158
J. Chem. Phys.
(2011),
134,
pp. 024105.
Link
,
1161
J. Phys. Chem. A
(2011),
114,
pp. 12083.
Link
,
657
J. Chem. Phys.
(2012),
137,
pp. 22A513.
Link
which
enforces stochastic wave function collapse at a rate proportional to the
difference in forces between the trajectory on the active surface and position
moments propagated the other surfaces. At every time step, the component of
the wave function on each active surface is printed to the output file. These
amplitudes, as well as the position and momentum moments (if AFSSH is
requested), is also printed to a text file called SurfaceHopper located
in the $QC/AIMD sub-directory of the job’s scratch directory.
In order to request a FSSH calculation, only a few additional $rem variables must be added to those necessary for an excited-state AIMD simulation. At present, FSSH calculations can only be performed using Born-Oppenheimer molecular dynamics (BOMD) method. Furthermore, the optimized velocity Verlet (OVV) integration method is not supported for FSSH calculations.
FSSH_LOWESTSURFACE
FSSH_LOWESTSURFACE
Specifies the lowest-energy state considered in a surface hopping calculation.
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
Only states and above are considered in a FSSH calculation.
RECOMMENDATION:
None
FSSH_NSURFACES
FSSH_NSURFACES
Specifies the number of states considered in a surface hopping calculation.
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
states are considered in the surface hopping calculation.
RECOMMENDATION:
Any states which may come close in energy to the active surface should
be included in the surface hopping calculation.
FSSH_INITIALSURFACE
FSSH_INITIALSURFACE
Specifies the initial state in a surface hopping calculation.
TYPE:
INTEGER
DEFAULT:
None
OPTIONS:
An integer between FSSH_LOWESTSURFACE and FSSH_LOWESTSURFACE
FSSH_NSURFACES .
RECOMMENDATION:
None
AFSSH
AFSSH
Adds decoherence approximation to surface hopping calculation.
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
0
Traditional surface hopping, no decoherence.
1
Use augmented fewest-switches surface hopping (AFSSH).
RECOMMENDATION:
AFSSH will increase the cost of the calculation, but may improve accuracy
for some systems. See Refs.
1158
J. Chem. Phys.
(2011),
134,
pp. 024105.
Link
,
1161
J. Phys. Chem. A
(2011),
114,
pp. 12083.
Link
,
657
J. Chem. Phys.
(2012),
137,
pp. 22A513.
Link
for more detail.
AIMD_SHORT_TIME_STEP
AIMD_SHORT_TIME_STEP
Specifies a shorter electronic time step for FSSH calculations.
TYPE:
INTEGER
DEFAULT:
TIME_STEP
OPTIONS:
Specify an electronic time step duration of /AIMD_TIME_STEP_CONVERSION
a.u. If is less than the nuclear time step variable TIME_STEP, the
electronic wave function will be integrated multiple times per nuclear time step,
using a linear interpolation of nuclear quantities such as the energy gradient and
derivative coupling. Note that must divide TIME_STEP evenly.
RECOMMENDATION:
Make AIMD_SHORT_TIME_STEP as large as possible while keeping the trace of
the density matrix close to unity during long simulations. Note that while specifying an
appropriate duration for the electronic time step is essential for maintaining accurate
wave function time evolution, the electronic-only time steps employ linear interpolation
to estimate important quantities. Consequently, a short electronic time step is not a
substitute for a reasonable nuclear time step.
FSSH_CONTINUE
FSSH_CONTINUE
Restart a FSSH calculation from a previous run, using the file 396.0. When this is enabled,
the initial conditions of the surface hopping calculation will be set, including the correct
wave function amplitudes, initial surface, and position/momentum moments (if AFSSH) from the
final step of some prior calculation.
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
Start fresh calculation.
Restart from previous run.
RECOMMENDATION:
None
Example 9.39 FSSH simulation. Note that analytic derivative couplings must be requested via CALC_NAC, but it is unnecessary to include a $derivative_coupling section. The same is true for SET_STATE_DERIV, which will be set to the initial active surface automatically. Finally, one must be careful to choose a small enough time step for systems that have energetic access to a region of large derivative coupling, hence the choice for AIMD_TIME_STEP_CONVERSION and TIME_STEP.
$molecule 0 1 C -1.620294 0.348677 -0.008838 C -0.399206 -0.437493 -0.012535 C -0.105193 -1.296810 -1.081340 H -0.789110 -1.374693 -1.905080 C 1.069016 -2.045054 -1.072304 H 1.292495 -2.701157 -1.889686 C 1.956240 -1.940324 0.002842 H 2.859680 -2.517019 0.008420 C 1.666259 -1.084065 1.071007 H 2.348104 -1.005765 1.894140 C 0.495542 -0.335701 1.065497 H 0.253287 0.325843 1.871866 O -1.931045 1.124872 0.911738 H -2.269528 0.227813 -0.865645 $end $rem JOBTYPE aimd EXCHANGE hf BASIS 3-21g CIS_N_ROOTS 3 SYMMETRY off SYM_IGNORE true CIS_SINGLETS false CIS_TRIPLETS true PROJ_TRANSROT true FSSH_LOWESTSURFACE 1 FSSH_NSURFACES 3 ! hop between T1 and T2 FSSH_INITIALSURFACE 1 ! start on T1 AFSSH 0 ! no decoherence CALC_NAC true AIMD_STEPS 50 ! Typically more would be used TIME_STEP 14 AIMD_SHORT_TIME_STEP 2 AIMD_TIME_STEP_CONVERSION 1 ! Do not alter time_step duration AIMD_PRINT 1 AIMD_INIT_VELOC thermal AIMD_TEMP 300 # K AIMD_INTEGRATION vverlet FOCK_EXTRAP_ORDER 6 FOCK_EXTRAP_POINTS 12 $end