In: Chemistry
The Hohenberg-Kohn theorems show a one-to-one mapping between the density and the molecular Hamiltonian. What information is contained in the Hamiltonian and, conceptually, how can this information be extracted from the density?
The Hohenberg-Kohn Theorems
The Hohenberg-Kohn theorems relate to any system consisting of
electrons moving under the influence of an external potential
. Stated simply they are as
follows:
Theorem 1.
The external potential , and hence the total energy, is a
unique functional of the electron density
.
The energy functional alluded to in the first Hohenberg-Kohn
theorem can be written in terms of the external potential
in the following way,
![]() |
(1.28) |
where is an unknown, but otherwise universal
functional of the electron density
only. Correspondingly, a Hamiltonian
for the system can be written such that the electron wavefunction
that minimises the expectation value
gives the groundstate energy (1.30) (assuming a non-degenerate
groundstate),
![]() |
(1.29) |
The Hamiltonian can be written as,
![]() |
(1.30) |
where is the electronic Hamiltonian
consisting of a kinetic energy operator
and an interaction operator
,
![]() |
(1.31) |
The electron operator is the same for all
-electron systems, so
is completely defined by the
number of electrons
, and the external potential
.
The proof of the first theorem is remarkably simple and proceeds
by reductio ad absurdum. Let there be two different
external potentials, and
, that give rise to the same density
. The associated Hamiltonians,
and
, will therefore have different
groundstate wavefunctions,
and
, that each yield
. Using the variational principle [19],
together with (1.31) yields,
![]() |
![]() |
![]() |
(1.32) |
![]() |
![]() |
(1.33) |
where and
are the groundstate energies of
and
respectively. It is at this point that
the Hohenberg-Kohn theorems, and therefore DFT, apply rigorously to
the groundstate only. An equivalent expression for (1.34) holds
when the subscripts are interchanged. Therefore adding the
interchanged inequality to (1.35) leads to the result:
![]() |
(1.34) |
which is a contradiction, and as a result the groundstate
density uniquely determines the external potential , to within an additive constant.
Stated simply, the electrons determine the positions of the nuclei
in a system, and also all groundstate electronic properties,
because as mentioned earlier,
and
completely define
.
Theorem 2.
The groundstate energy can be obtained variationally: the
density that minimises the total energy is the exact groundstate
density.
The proof of the second theorem is also straightforward: as just
shown, determines
,
and
determine
and therefore
. This ultimately means
is a functional of
, and so the expectation value of
is also a functional of
, i.e.
![]() |
(1.35) |
A density that is the ground-state of some external potential is
known as -representable. Following from this, a
-representable energy functional
can be defined in which the external
potential
is unrelated to another density
,
![]() |
(1.36) |
and the variational principle asserts,
![]() |
(1.37) |
where is the wavefunction associated with
the correct groundstate
. This leads to,
![]() |
(1.38) |
and so the variational principle of the second Hohenberg-Kohn theorem is obtained,
![]() |
(1.39) |