Density-functional theory: Difference between revisions

From SklogWiki
Jump to navigation Jump to search
(New page: *Classical DFT *Quantum DFT)
 
m (→‎Interesting reading: Added book ISBn)
 
(22 intermediate revisions by 3 users not shown)
Line 1: Line 1:
*[[Classical DFT]]
'''Density-functional theory''' is a set of theories in [[statistical mechanics]] that profit from the
*[[Quantum DFT]]
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-Mermin theorems |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:
 
:<math>A_{id}=k_BT\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
to show that [[Boltzmann's barometric law]] follows from minimization.
An example of a weighed density theory would be the
(also exact) excess  Helmholtz energy for a system
of [[1-dimensional hard rods]]:
 
:<math>A_{ex}=-k_BT\int dz \rho(z) \log [1-t(z)],</math>
 
where <math>t(z)=\int_{z-\sigma}^z dy \rho(y)</math>,
precisely an average of the density over the length of
the hard rods, <math>\sigma</math>. "Excess" means "over
ideal", i.e., it is the total <math>A=A_{id}+A_{ex}</math>
that is to be minimized.
==See also==
*[[van der Waals' density gradient theory]]
*[[Ebner-Saam-Stroud]]
*[[Fundamental-measure theory]]
*[[Hohenberg-Kohn-Mermin theorems]]
*[[Quantum density-functional theory]]
*[[Ramakrishnan-Youssouff]]
*[[Weighted density approximation]]
**[[Kierlik and Rosinberg's weighted density approximation]]
**[[Tarazona's weighted density approximation]]
*[[Dynamical density-functional theory]]
*[[Perdew-Burke-Ernzerhof functional]]
*[[Becke-Lee-Yang-Parr functional]] (BLYP)
 
==Interesting reading==
*Robert Evans "Density Functionals in the Theory of Nonuniform Fluids", Chapter 3 pp. 85-176 in "Fundamentals of Inhomogeneous Fluids" (editor: Douglas Henderson) Marcel Dekker (1992) ISBN 978-0824787110
*[http://dx.doi.org/10.1146/annurev.pc.34.100183.003215 Robert G. Parr "Density Functional Theory",  Annual Review of Physical Chemistry '''34''' pp. 631-656 (1983)]
*[http://dx.doi.org/10.1103/PhysRevA.43.4355 C. Ebner, H. R. Krishnamurthy and Rahul Pandit "Density-functional theory for classical fluids and solids", Physical Review A '''43''' pp. 4355 - 4364 (1991)]
*[http://dx.doi.org/10.1002/aic.10713 Jianzhoung Wu "Density-functional theory for chemical engineering: from capillarity to soft materials", AIChE Journal '''52''' pp. 1169 - 1193 (2005)]
[[category: Density-functional theory]]

Latest revision as of 15:57, 14 June 2010

Density-functional theory 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 Helmholtz 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[edit]

Interesting reading[edit]