Computational Materials Theory and Methods

Computational
Materials
 Theory and
Methods
Alexey V. Akimov 
University at Buffalo, SUNY
1
Lecture 3: 
Quantum Mechanics
Basics of the Molecular Orbital Theory
Basis set expansion
 
=
 
Basis functions
:
Atomic orbitals, plane-
waves, etc.
 
Orbitals
:
Molecular, crystal, etc.
 
In general
Atomic orbitals
 
Just for the radial component of wavefunction
 
Energy of electron in H atom
4
Atomic orbitals
https://bse.pnl.gov/bse/portal
Where to get
Potential problems
 
Dissociation
 
Basis set superposition error
 
Linear dependence
Pulay forces
5
Plane waves (PW)
Real
 space unit cell
 
Reciprocal
 space unit cell
 
k-point vector
(crystal momentum
vector)
 
Band (“orbital”) index
 
Reciprocal space
grid points
 
Real space
coordinate
 
The bigger the size in real space, the smaller its counterpart in the reciprocal
6
Plane waves (PW)
In DFT, many properties are given by:
k-points convergence
 
pw convergence
 
Kinetic energy of free electrons
7
Basis set comparisons
 
Atomic basis
 
PW basis
 
Doesn’t depend on the unit cell size
Good for finite systems (clusters/molecules)
Analytic integrals
All-electron
Basis set superposition error
Not systematically controllable
Linear dependence for large sets
Pulay forces
8
 
=
Schrodinger equation
 
Variational principle
 
Diabatic 
Hamiltonian
(non-interacting basis)
 
Adiabatic
 
Hamiltonian
(interacting basis)
9
Hierarchy of wavefunctions
Primitive mathematical basis
 
Solution to the mean-filed SE
 (1-electron functions)
 
Account for anti-symmetry
(exchange/fermionic statistics)
 
Account for correlation,
proper spin symmetry
10
Constructing the Hamiltonian
(in the AO basis)
Fock (mean-filed) Hamiltonian
 
Core Hamiltonian
 
Coulomb and Exchange Hamiltonian
 
(depends on charge/spin density)
 
(does not depend on charge/spin density)
 
Molecular integrals
 
Density matrix
 
(depends on the solution of SE)
11
Dealing with the complexity of SE
Scaling
considerations
 
Approximations
 
Keep only the core part
 
Replace the core with
a special formula
(TB- or extended Hückel)
One-shot solution
 
Semiempirical methods:
Simplify the 2-electron 4-center
integrals, neglect some
(CNDO, INDO, MNDO, etc. PMn)
Need self-consistent solution
 
Akimov, A. V.; Prezhdo, O. V. 
Chem. Rev.
 
2015
, 
115
, 5797–5890.
12
Extended Hückel theory (EHT)
Hoffmann, R. 
J. Chem. Phys.
 
1963
, 
39
, 1397–1412.
 
Simple math, efficient
Clear meaning of parameters
Consider it a Tight-Binding
General-purpose (analog of UFF)
No SCF required: 1-shot
 
Akimov, A. V.; Prezhdo, 
J. Math. Chem.
 
2015
, 
53
, 528–550.
 
Fancier schemes: SC-EHT
Charge-dependent VSIP
13
Self-consistent field (SCF)
 
Done
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This content delves into Quantum Mechanics Basics and Molecular Orbital Theory, discussing concepts like Atomic Orbitals, Basis Sets, and Wavefunction Components. It covers topics such as Slater-type Orbitals, Gaussian-type Orbitals, and Plane Waves in reciprocal and real space, focusing on their significance in computational materials theory and methods.

  • Quantum Mechanics
  • Atomic Orbitals
  • Basis Sets
  • Molecular Orbital Theory
  • Computational Materials

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  1. Computational Materials Theory and Methods Lecture 3: Quantum Mechanics Alexey V. Akimov University at Buffalo, SUNY 1

  2. Basics of the Molecular Orbital Theory ???? ??= ????,? Basis set expansion ?=1 ??? Orbitals: Molecular, crystal, etc. ??? ???? ???? = Basis functions: Atomic orbitals, plane- waves, etc. ???? ??? In general

  3. Atomic orbitals Slater-type orbitals (STO): ??,?,?,??,?,? = ?????,? ?? 1? ?? Gaussian-type orbitals (GTO): ??,?,?,??,?,? = ??????????? ??2 where ??+ ??+ ??= ? STO-2G: ????= ?1????1+ ?2????2 Energy of electron in H atom Energy [hartree] 3/4 3/4 2?2 ? Basis set 2?1 ? ? ?2?2 ? ?1?2 ????2= ????1= STO-3G -0.49491 ?? ?? ?? ?? STO-2G STO-4G -0.49848 1s (C) 0.151623 0.678914 0.851819 0.430129 STO-5G -0.49951 2s (C) 0.0974545 0.963782 0.384244 0.0494718 STO-6G -0.49983 2p (C) 0.0974545 0.61282 0.384244 0.511541 Exact -0.5 Just for the radial component of wavefunction

  4. Atomic orbitals Potential problems Where to get Basis set superposition error https://bse.pnl.gov/bse/portal Dissociation Linear dependence Pulay forces 4

  5. Plane waves (PW) Reciprocal space unit cell Real space unit cell The bigger the size in real space, the smaller its counterpart in the reciprocal Unit cell volume = ? (? ?) Real space coordinate 1 ??? ??(?+?)? ??,?(?) = k-point vector (crystal momentum vector) ? Reciprocal space grid points Band ( orbital ) index 5

  6. Plane waves (PW) pw convergence k-points convergence Kinetic energy of free electrons In DFT, many properties are given by: ? + ?2 2 ? = ???? ????= ? ???? ???? ? ? 6

  7. Basis set comparisons Atomic basis PW basis Depends on the unit cell size, not the number of atoms Good for periodic systems Doesn t depend on the unit cell size Good for finite systems (clusters/molecules) Analytic integrals Massive linear algebra All-electron Needs a pseudopotential Basis set superposition error No BSSE Not systematically controllable Systematically controllable via k-points and ???? Linear dependence for large sets No problems with linear dependence Pulay forces No Pulay forces 7

  8. Schrodinger equation ? ? ?? = ?? ??| ? |????,?= ?? |????,??? ,? = 1,2, ? ?=1 ?=1 Variational principle ? ? ? ? ? = ???? ??? Diabatic Hamiltonian (non-interacting basis) Adiabatic Hamiltonian (interacting basis) 8

  9. Hierarchy of wavefunctions AO or PW (??) Primitive mathematical basis MO or Crystal orbitals: Solution to the mean-filed SE (1-electron functions) ??= ????,? ? Slater determinants: ??= ??? ??? Account for anti-symmetry (exchange/fermionic statistics) Account for correlation, proper spin symmetry Configuration interaction (CI), SAC-CI, MR-CI: ??= ????? 9

  10. Constructing the Hamiltonian (in the AO basis) Fock (mean-filed) Hamiltonian ???,?= ???+ ???,? Core Hamiltonian Coulomb and Exchange Hamiltonian (does not depend on charge/spin density) (depends on charge/spin density) ???,?= ????? ?? ???,??? ?? ?? ? = ???? Density matrix Molecular integrals (depends on the solution of SE) 10

  11. Dealing with the complexity of SE Approximations Scaling considerations Keep only the core part Solution of the eigenvalue problem: ?(???? 3) Replace the core with a special formula (TB- or extended H ckel) One-shot solution Construction of the integrals: ?(???? 4) Semiempirical methods: Simplify the 2-electron 4-center integrals, neglect some (CNDO, INDO, MNDO, etc. PMn) Need self-consistent solution Akimov, A. V.; Prezhdo, O. V. Chem. Rev.2015, 115, 5797 5890. 11

  12. Extended Hckel theory (EHT) Simple math, efficient Clear meaning of parameters Consider it a Tight-Binding General-purpose (analog of UFF) No SCF required: 1-shot Hoffmann, R. J. Chem. Phys.1963, 39, 1397 1412. ??= ?1?1exp ??? + ?2?2exp ??? ???= ???? ???=??? Fancier schemes: SC-EHT Charge-dependent VSIP ???(???+ ???) 2 0 ??? ??= ?? Energy ??= VSIPa ?? Akimov, A. V.; Prezhdo, J. Math. Chem.2015, 53, 528 550. 12

  13. Self-consistent field (SCF) Guess density matrix, ?0 Core Hamiltonian, ? Overlap matrix, ? Pre-compute integrals in AO basis Construct the Fock matrix ??= ? + ?(??) Density matrix, ?? Solve the eigenvalue problem: ????= ????? Update density matrix: ??+1= ?????? ? Compute the total energy : ??= ?? (??+ ??)?? Check the convergence: ?? 1 ?? < ????? ?? 1 ?? < ??? Done 13

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