Chapter 12: Quantum Calculations Flashcards

1
Q

Hamiltonian under Born-Oppenheimer Approximation

A
  • can separate and decouple nuclear and electronic wavefunctions
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2
Q

Hartree Method

(Assumptions)

A
  • non-interacting electrons
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3
Q

Hartree Wavefunction

A
  • Drawbacks:
    • not antisymmetric → no exchange
    • only include Coulomb correlation
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4
Q

Hartree Single Particle Equation

A
  • gives energy and orbital for electron i
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5
Q

Hartree-Fock Wavefunction

A
  • uses Slater determinant to form wavefunction
    • includes Pauli Principle exchange
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6
Q

Hartree-Fock Single Particle Equation

A
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7
Q

Hartree-Fock Approximations

A
  • Born-Oppenheimer
  • Coulomb correlation only
  • non-relativistic
  • attainable phase space is constrained by single Slater determinant
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8
Q

Post-HF Methods

A
  • mostly aim to increase correlation
  • may try to increase phase space
  • e.g. Coupled-Cluster Method
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9
Q

Coupled-Cluster Method

A
  • can look at excited states
  • good for chemical reactions with small molecules
  • increases correlation
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10
Q

Hartree-Fock Limit

A
  • HF groundstate prediction be bounded by below and is an overestimate for true groudstate
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11
Q

Density Functional Theory

A

Reduces 3N-dimensional wavefunction to 3-dimensional wavefunction using density n(r )

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12
Q

Hohenberg-Kohn Theorems

A
  1. There exists a one-to-one mapping between groundstates density and groundstate wavefunction for non-degenerate groundstates
  2. Groundstate density minimizes total energy.
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13
Q

Kohn-Sham Equation

A
  • ε<em>i</em>, φi are for fictitious particle i
  • however, densities match nDFT(r ) = nexact(r )
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14
Q

Exchange-Correlation Functional

A
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15
Q

Local Density Approximation

A
  • local functional
  • uses homogeneous electron gas exchange-correlation
  • fails for vdW forces and metallic systems
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16
Q

Generalized Gradient Apprixmation

A
  • semi-local functional
  • also depends on gradient of density
17
Q

DFT Short-Comings

A
  • overbinding → underestimates bandgap
  • can only predict trends for excited states → TDDFT better for excited states
18
Q

Time-Dependent DFT

A
  • rewrite KS equations in time-dependent manner using quantum mechanical action A[n]
  • need new functionals because (non-)locality can occur in space and time
19
Q

Pseudo-Potentials

A

Used to neglect core electrons and avoid singularities

  • functional specific
20
Q

DFT Algorithm

A
  1. Initial guess of density
  2. Evaluate potential
  3. Solve KS equation
  4. Get new density
  5. Test for self-consistency