Clusters in Separated Tubes of Tilted Dipoles

A few-body cluster is a building block of a many-body system in a gas phase provided the temperature at most is of the order of the binding energy of this cluster. Here we illustrate this statement by considering a system of tubes filled with dipolar distinguishable particles. We calculate the parti...

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Main Authors: Jeremy R. Armstrong, Aksel S. Jensen, Artem G. Volosniev, Nikolaj T. Zinner
Format: Article
Language:English
Published: MDPI AG 2020-04-01
Series:Mathematics
Subjects:
Online Access:https://www.mdpi.com/2227-7390/8/4/484
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spelling doaj-9734268b1fca44e7aba04943645059ca2020-11-25T03:08:39ZengMDPI AGMathematics2227-73902020-04-01848448410.3390/math8040484Clusters in Separated Tubes of Tilted DipolesJeremy R. Armstrong0Aksel S. Jensen1Artem G. Volosniev2Nikolaj T. Zinner3Department of Physics and Astronomy, University of Nebraska at Kearney, Kearney, NE 68849, USADepartment of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C, DenmarkInstitute of Science and Technology Austria, 3400 Klosterneuburg, AustriaDepartment of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C, DenmarkA few-body cluster is a building block of a many-body system in a gas phase provided the temperature at most is of the order of the binding energy of this cluster. Here we illustrate this statement by considering a system of tubes filled with dipolar distinguishable particles. We calculate the partition function, which determines the probability to find a few-body cluster at a given temperature. The input for our calculations—the energies of few-body clusters—is estimated using the harmonic approximation. We first describe and demonstrate the validity of our numerical procedure. Then we discuss the results featuring melting of the zero-temperature many-body state into a gas of free particles and few-body clusters. For temperature higher than its binding energy threshold, the dimers overwhelmingly dominate the ensemble, where the remaining probability is in free particles. At very high temperatures free (harmonic oscillator trap-bound) particle dominance is eventually reached. This structure evolution appears both for one and two particles in each layer providing crucial information about the behavior of ultracold dipolar gases. The investigation addresses the transition region between few- and many-body physics as a function of temperature using a system of ten dipoles in five tubes.https://www.mdpi.com/2227-7390/8/4/484cold dipolar moleculesFew-body to many-body crossoverharmonic approximation
collection DOAJ
language English
format Article
sources DOAJ
author Jeremy R. Armstrong
Aksel S. Jensen
Artem G. Volosniev
Nikolaj T. Zinner
spellingShingle Jeremy R. Armstrong
Aksel S. Jensen
Artem G. Volosniev
Nikolaj T. Zinner
Clusters in Separated Tubes of Tilted Dipoles
Mathematics
cold dipolar molecules
Few-body to many-body crossover
harmonic approximation
author_facet Jeremy R. Armstrong
Aksel S. Jensen
Artem G. Volosniev
Nikolaj T. Zinner
author_sort Jeremy R. Armstrong
title Clusters in Separated Tubes of Tilted Dipoles
title_short Clusters in Separated Tubes of Tilted Dipoles
title_full Clusters in Separated Tubes of Tilted Dipoles
title_fullStr Clusters in Separated Tubes of Tilted Dipoles
title_full_unstemmed Clusters in Separated Tubes of Tilted Dipoles
title_sort clusters in separated tubes of tilted dipoles
publisher MDPI AG
series Mathematics
issn 2227-7390
publishDate 2020-04-01
description A few-body cluster is a building block of a many-body system in a gas phase provided the temperature at most is of the order of the binding energy of this cluster. Here we illustrate this statement by considering a system of tubes filled with dipolar distinguishable particles. We calculate the partition function, which determines the probability to find a few-body cluster at a given temperature. The input for our calculations—the energies of few-body clusters—is estimated using the harmonic approximation. We first describe and demonstrate the validity of our numerical procedure. Then we discuss the results featuring melting of the zero-temperature many-body state into a gas of free particles and few-body clusters. For temperature higher than its binding energy threshold, the dimers overwhelmingly dominate the ensemble, where the remaining probability is in free particles. At very high temperatures free (harmonic oscillator trap-bound) particle dominance is eventually reached. This structure evolution appears both for one and two particles in each layer providing crucial information about the behavior of ultracold dipolar gases. The investigation addresses the transition region between few- and many-body physics as a function of temperature using a system of ten dipoles in five tubes.
topic cold dipolar molecules
Few-body to many-body crossover
harmonic approximation
url https://www.mdpi.com/2227-7390/8/4/484
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AT artemgvolosniev clustersinseparatedtubesoftilteddipoles
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