Density-functional theory: Difference between revisions

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This is a set of theories in statistical mechanics that profit from the
This is a set of theories in statistical mechanics that profit from the
fact that the free energy of a system can be cast as a functional of
fact that the [[Helmholtz energy function]] of a system can be cast as a functional of
the density. That is, the density (in its usual sense of particles
the density. That is, the density (in its usual sense of particles
per volume), which is a funtion of the position in inhomogeneous systems,
per volume), which is a function of the position in inhomogeneous systems,
uniquely defines the free energy. By minimizing this free energy one
uniquely defines the Helmholtz energy. By minimizing this Helmholtz energy one
arrives at the true free energy of the system and the equilibrium
arrives at the true Helmholtz energy of the system and the equilibrium
densify function. The situation
density function. The situation
parallels the better known electronic density functional theory,
parallels the better known electronic density functional theory,
in which the energy of a quantum system is shown to be a functional
in which the energy of a quantum system is shown to be a functional
of the electronic density (theorems by Hohenberg, Kohn, Sham, and Mermin.)
of the electronic density (see the theorems by [[Hohenberg-Kohn-Mermin theorems |Hohenberg, Kohn, Sham, and Mermin]]).


Starting from this fact, approximations are usually made in order
Starting from this fact, approximations are usually made in order
Line 15: Line 15:
In a local density theory the
In a local density theory the
in which the dependence is local, as exemplified by the (exact)
in which the dependence is local, as exemplified by the (exact)
free energy of an ideal system:
Helmholtz energy of an ideal system:


<math>F_{id}=kT\int dr \rho(r) [\log \rho(r) -1 -U(r)],</math>
<math>F_{id}=kT\int dr \rho(r) [\log \rho(r) -1 -U(r)],</math>


where <math>U(r)</math> is an external potential. It is an easy exercise
where <math>U(r)</math> is an external potential. It is an easy exercise
to show that Boltzmann's barometric law follows from minimization.
to show that [[Boltzmann's barometric law]] follows from minimization.
 
An example of a weighed density theory would be the
An example of a weighed density theory would be the
(also exact) excess free energy for a system
(also exact) excess free energy for a system
of 1D hard rods:
of [[hard rods | 1-dimensional hard rods]]:


<math>F_{ex}=-kT\int dz \rho(z) \log [1-t(z)],</math>
<math>F_{ex}=-kT\int dz \rho(z) \log [1-t(z)],</math>

Revision as of 12:31, 9 October 2007

This is a set of theories in statistical mechanics that profit from the fact that the Helmholtz energy function of a system can be cast as a functional of the density. That is, the density (in its usual sense of particles per volume), which is a function of the position in inhomogeneous systems, uniquely defines the Helmholtz energy. By minimizing this Helmholtz energy one arrives at the true Helmholtz energy of the system and the equilibrium density function. The situation parallels the better known electronic density functional theory, in which the energy of a quantum system is shown to be a functional of the electronic density (see the theorems by Hohenberg, Kohn, Sham, and Mermin).

Starting from this fact, approximations are usually made in order to approach the true functional of a given system. An important division is made between local and weighed theories. In a local density theory the in which the dependence is local, as exemplified by the (exact) Helmholtz energy of an ideal system:

where is an external potential. It is an easy exercise to show that Boltzmann's barometric law follows from minimization. An example of a weighed density theory would be the (also exact) excess free energy for a system of 1-dimensional hard rods:

where , precisely an average of the density over the length of the hard rods, . "Excess" means "over ideal", i.e., it is the total that is to be minimized.

See also

Interesting reading

  1. Robert Evans "Density Functionals in the Theory of Nonuniform Fluids", in "Fundamentals of Inhomogeneous Fluids" (ed. D. Henderson). Marcel Dekker.
  2. Robert G. Parr "Density Functional Theory", Annual Review of Physical Chemistry 34 pp. 631-656 (1983)
  3. C. Ebner, H. R. Krishnamurthy and Rahul Pandit "Density-functional theory for classical fluids and solids", Physical Review A 43 pp. 4355 - 4364 (1991)