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 | 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 | per volume), which is a function of the position in inhomogeneous systems, | ||
uniquely defines the | uniquely defines the Helmholtz energy. By minimizing this Helmholtz energy one | ||
arrives at the true | arrives at the true Helmholtz energy of the system and the equilibrium | ||
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) | ||
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 | 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 11:31, 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
- Dynamical density-functional theory
- Ebner-Saam-Stroud
- Fundamental-measure theory
- Hohenberg-Kohn-Mermin theorems
- Quantum density-functional theory
- Ramakrishnan-Youssouff
- Weighted density approximation
Interesting reading
- Robert Evans "Density Functionals in the Theory of Nonuniform Fluids", in "Fundamentals of Inhomogeneous Fluids" (ed. D. Henderson). Marcel Dekker.
- Robert G. Parr "Density Functional Theory", Annual Review of Physical Chemistry 34 pp. 631-656 (1983)
- C. Ebner, H. R. Krishnamurthy and Rahul Pandit "Density-functional theory for classical fluids and solids", Physical Review A 43 pp. 4355 - 4364 (1991)