Chapter 13: ab initio MD Flashcards
1
Q
Effect on Nuclei Outside BO Approximation
A
- nuclei move in response to electron cloud
2
Q
Hellman-Feynman Theorem
A
gives force on nucleus I
3
Q
ab initio MD General Approach
A
- Solve SE
- Get groundstate wavefunction
- Calculate HF and electrostatic forces
- Perform MD step with forces on ions
4
Q
Ehrenfest MD
A
solve EOM for electronic and nuclear subsystems separately for each timestep
-
Advantages:
- can capture non-adiabatic effects
-
Disadvantages:
- ∆tE very small (10-3 - 10-5 fs)
- might miss important chemical reactions
5
Q
Born-Oppenheimer MD
A
similar to Ehrenfest MD, but use TISE
-
Advantages:
- electron motion treated implicitly → ∆tBO = 102 ∆tE
- electron wavefunction changes because electrons are dragged along with nucleus
6
Q
Car-Parrinello MD
A
avoid QM calculation at each timestep by treating both subsystems classically
- define Lagrangian
- fictituous mass µ
- time dependence in Λ
-
Advantages:
- if µ is tuned correctly, can get exact results without QM calculation
- ∆tCP approx. 10 ps
-
Disadvantages:
- bad initial nuclear configuration → potentially miss global minimum
7
Q
Quantum Mechanics/Molecular Mechanics
A
split system into two parts
- quantum part
- classical part
8
Q
QMMM Hamiltonians
A