The ZORA equation is the zeroth order regular approximation to the Dirac equation. The relativistic and non-relativistic Kohn-Sham DFT equations can be written as:
[ T + VKS] φi = εi φi
The potential VKS is the local Kohn-Sham potential, see also the Kohn-Sham MO model. T is the kinetic energy operator, which is different for each relativistic method:
TDirac = σ⋅p c2/(2c2 + εi - VKS) σ⋅p
TZORA = σ⋅p c2/(2c2 - VKS) σ⋅p
TNR = p2/2
TDirac is the energy dependent Dirac kinetic energy operator, TZORA is the ZORA kinetic energy operator, and TNR is the non-relativistic kinetic energy operator.
The scaled ZORA spinor energy εiscaled is:
εiscaled = εiZORA / < φi | σ⋅p c2/(2c2 - VKS)2 σ⋅p | φi >
The scaled ZORA spinor energies are exactly equal to the Dirac energies for hydrogen like systems,
where VKS = -Z/r.
A magnetic field can be included by minimal substitution for a negatively charge particle:
p → Π = p + A/c
The ZORA kinetic energy can be split in a scalar relativistic part TSR and a spin-orbit coupling TSO term:
TZORA = TSR + TSO = p⋅ c2/(2c2 - VKS) p + c2/(2c2 - VKS)2 σ⋅ (∇ VKS × p )
ADF User Documentation: relativistic effects
ADF-GUI: model Hamiltonians
Examples: relativistic effects
References: ZORA
Related: ZORA, spin-orbit coupling




