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Apple Academic Press eBooks

Y-Density Functional Theory of Bose–Einstein Condensation

Mihai V. Putz

Published Jun 6, 2013• 0 citations
Publisher

Abstract

Potential ........................................................................................................... 143 6.7Exchange Density Functional of Homogeneous Systems-–Bosonic Case ..... 150 Keywords ................................................................................................................. 157 6.1 INTRODUCTION The basics of Density Functional Theory (DFT) and of Bose-Einstein Condensation (BEC) are merged such that the DFT enriches with the order parameter equation from the BEC modeling, while BEC acquires the new equation for the condensate density as provided by the DFT Hohenberg-KS analysis. Together, BEC-DFT may constitute as the next level of comprehension in modeling condensed matter in physics and chemical bond in chemistry, in particular, while providing the clue how the unified theory of physical-chemical phenomena should look like (Albus et al., 2003; Argaman and Band, 2011; Brand, 2004; Kim and Vetter, 1997; Nunes, 1999; Putz, 2011d; Zubarev, 2003).

DOI
10.1201/b14167-11

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Potential ........................................................................................................... 143 6.7Exchange Density Functional of Homogeneous Systems-–Bosonic Case ..... 150 Keywords ................................................................................................................. 157 6.1 INTRODUCTION The basics of Density Functional Theory (DFT) and of Bose-Einstein Condensation (BEC) are merged such that the DFT enriches with the order parameter equation from the BEC modeling, while BEC acquires the new equation for the condensate density as provided by the DFT Hohenberg-KS analysis. Together, BEC-DFT may constitute as the next level of comprehension in modeling condensed matter in physics and chemical bond in chemistry, in particular, while providing the clue how the unified theory of physical-chemical phenomena should look like (Albus et al., 2003; Argaman and Band, 2011; Brand, 2004; Kim and Vetter, 1997; Nunes, 1999; Putz, 2011d; Zubarev, 2003).
Since the nowadays growing interest in Bose-Einstein condensates (BEC) due to the expanded experimental evidence on various atomic systems within optical lattices in weak and strong coupling regimes, its many-body quantum bases and equations are elementarily presented emphasizing on the order parameter, pseudo-potential and mean field approaches, while emphasizing the common places with the Density Functional Theory, like the integral normalization of density or the chemical potential, as the main vehicles of both theories of matter (Putz, 2011d, 2011e).
Systems ............................................................................................................ 229 Keywords ................................................................................................................. 231 9.1 INTRODUCTION Within the Bose-Einstein condensates (BEC) – density functional Theory (DFT) context, the question of whether the quantum chemical bonding homopolar picture may allow for such special modeling extension is here responded in positive through employing the Gross-Pitaevsky equation for the condensed wave function of bosons as an extension to the consecrated Heitler-London quantum description when bonding and anti-bonding electrons are considered as pairing to form bosons with 0 and 1 magnetic moments (spins) respectively. The results show that the same form of the quantum chemical bonding and anti-bonding wave functions might characterize the bosonic condensed wave functions, respectively, however experiencing different energetic states (with the contribution of a BECChemBond term experiencing the gap of the so called bosonic-fermionic degeneracy of the chemical bonding) relying on the correcting the fermionic energetic spectrum by some fraction of it with the coupling related with the chemical hardness (from fermionic side) reduced by the bosonic strength (from the bosonic side). The present Heitler-London-Bose-Einstein (superfluid) picture may eventually lead with a reformulation and the control of the frontier reactivity as well as the more subtle quantum concepts as the delocalization, aromaticity or other collective manifestations in complex macromolecules and nanosystems assimilated with diluted systems of bosons of fermions (Putz, 2011d, 2011e, 2011f).
The thermodynamic approach to density-functional theory (DFT) is used to derive a versatile theoretical framework for the treatment of finite-temperature (and in the limit, zero-temperature) Bose-Einstein condensates (BECs). The simplest application of this framework, using the overall density of bosons alone, would yield the DFT of Nunes [J. Phys. B 32, 4293 (1999)]. It is argued that a significant improvement in accuracy may be obtained by using additional density fields: the condensate amplitude and the anomalous density. Thus, two advanced schemes are suggested, one corresponding to a generalized two-fluid model of condensate systems, and another scheme, which explicitly accounts for anomalous density contributions and anomalous effective potentials. The latter reduces to the Hartree-Fock-Bogoliubov approach in the limit of weak interactions. For stronger interactions, a local-density approximation is suggested, but its implementation requires accurate data for the thermodynamic properties of uniform interacting BEC systems, including fictitious perturbed states of such systems. Provided that such data become available (e.g., from quantum Monte Carlo computation), DFT can be used to obtain high-accuracy theoretical results for the equilibrium states of BECs of various geometries and external potentials.
Since the nowadays growing interest in Bose-Einstein condensates due to the expanded experimental evidence on various atomic systems within optical lattices in weak and strong coupling regimes, the connection with Density Functional Theory is firstly advanced within the mean field framework at three levels of comprehension: the many-body normalization condition, Thomas-Fermi limit, and the chemical hardness closure with the inter-bosonic strength and universal Hohenberg-Kohn functional. As an application the traditional Heitler-London quantum mechanical description of the chemical bonding for homopolar atomic systems is reloaded within the non-linear Schrödinger (Gross-Pitaevsky) Hamiltonian; the results show that a two-fold energetic solution is registered either for bonding and antibonding states, with the bosonic contribution being driven by the square of the order parameter for the Bose-Einstein condensate density in free (gas) motion, while the associate wave functions remain as in classical molecular orbital model.