Loading…
Non-condensate fraction of a weakly interacting Bose gas confined between two parallel plates within improved Hartree-Fock approximation at zero temperature
By analytically solving the nonlinear gap and Schwinger-Dyson equations, the non-condensate fraction of a weakly interacting Bose-Einstein condensate (BEC) confined between two parallel plates at zero temperature is investigated within the improved Hartree-Fock approximation. It is proved that the f...
Saved in:
Published in: | Physics letters. A 2023-10, Vol.486, p.129099, Article 129099 |
---|---|
Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | |
---|---|
cites | cdi_FETCH-LOGICAL-c259t-3c0acb9222a4cb1ddd56f3fda024bda691ae7184f8f8cee7aa65f1051d59c1553 |
container_end_page | |
container_issue | |
container_start_page | 129099 |
container_title | Physics letters. A |
container_volume | 486 |
creator | Thu, Nguyen Van |
description | By analytically solving the nonlinear gap and Schwinger-Dyson equations, the non-condensate fraction of a weakly interacting Bose-Einstein condensate (BEC) confined between two parallel plates at zero temperature is investigated within the improved Hartree-Fock approximation. It is proved that the finite-size effect increases the non-condensate fraction compared with the one of the same homogeneous BEC. Our result also shows that the non-condensate fraction can be expressed as a sum of two terms: the first term corresponds to the non-condensate fraction of the homogeneous dilute BEC and the other appears because of the confinement. Both terms are universal. A comparison with the experimental data is made.
•Equation for condensate fraction of a dilute Bose gas is established in the improved Hartree-Fock approximation.•The effect caused by the confinement along z-direction on the condensate fraction is investigated at zero temperature.•The contribution of finite-size is proportional to ratio of scattering length to distance between two parallel plates.•Taking into account the influence of finite-size effect, the condensate fraction is still universal.•A comparison with experimental data is made. |
doi_str_mv | 10.1016/j.physleta.2023.129099 |
format | article |
fullrecord | <record><control><sourceid>elsevier_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1016_j_physleta_2023_129099</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0375960123004796</els_id><sourcerecordid>S0375960123004796</sourcerecordid><originalsourceid>FETCH-LOGICAL-c259t-3c0acb9222a4cb1ddd56f3fda024bda691ae7184f8f8cee7aa65f1051d59c1553</originalsourceid><addsrcrecordid>eNqFkEtOwzAQhrMAifK4ApoLpNhJk9Y7HqKAhGADa2tqj1u3qR3ZpqWchcNiKKxZjfRr_oe-ojjnbMgZby-Ww36xix0lHFasqoe8EkyIg2LA6nFTipbxo-I4xiVj-ZuJQfH55F2pvNPkIiYCE1Al6x14AwhbwlW3A-sS_ehuDtc-EswxQjYZ60jDjNKWyEHaeugxYNdRB32X0yJsbVpYB3bdB7_Jv_cYUiAqp16tAPusvts1_hRigg8KHhKt-9yW3gKdFocGu0hnv_ekeJ3evtzcl4_Pdw83V4-lqhqRyloxVDNRVRWO1IxrrZvW1EYjq0Yzja3gSGM-GZmJmSiiMWLbGM4arhuheNPUJ0W7z1XBxxjIyD7kWWEnOZPfXOVS_nGV31zlnms2Xu6NlNdtLAUZlSWnSNtAKknt7X8RX2EdjNw</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Non-condensate fraction of a weakly interacting Bose gas confined between two parallel plates within improved Hartree-Fock approximation at zero temperature</title><source>Elsevier:Jisc Collections:Elsevier Read and Publish Agreement 2022-2024:Freedom Collection (Reading list)</source><creator>Thu, Nguyen Van</creator><creatorcontrib>Thu, Nguyen Van</creatorcontrib><description>By analytically solving the nonlinear gap and Schwinger-Dyson equations, the non-condensate fraction of a weakly interacting Bose-Einstein condensate (BEC) confined between two parallel plates at zero temperature is investigated within the improved Hartree-Fock approximation. It is proved that the finite-size effect increases the non-condensate fraction compared with the one of the same homogeneous BEC. Our result also shows that the non-condensate fraction can be expressed as a sum of two terms: the first term corresponds to the non-condensate fraction of the homogeneous dilute BEC and the other appears because of the confinement. Both terms are universal. A comparison with the experimental data is made.
•Equation for condensate fraction of a dilute Bose gas is established in the improved Hartree-Fock approximation.•The effect caused by the confinement along z-direction on the condensate fraction is investigated at zero temperature.•The contribution of finite-size is proportional to ratio of scattering length to distance between two parallel plates.•Taking into account the influence of finite-size effect, the condensate fraction is still universal.•A comparison with experimental data is made.</description><identifier>ISSN: 0375-9601</identifier><identifier>DOI: 10.1016/j.physleta.2023.129099</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Bose-Einstein condensate ; Finite-size effect ; Non-condensate fraction ; Universal properties</subject><ispartof>Physics letters. A, 2023-10, Vol.486, p.129099, Article 129099</ispartof><rights>2023 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c259t-3c0acb9222a4cb1ddd56f3fda024bda691ae7184f8f8cee7aa65f1051d59c1553</cites><orcidid>0000-0002-9868-381X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Thu, Nguyen Van</creatorcontrib><title>Non-condensate fraction of a weakly interacting Bose gas confined between two parallel plates within improved Hartree-Fock approximation at zero temperature</title><title>Physics letters. A</title><description>By analytically solving the nonlinear gap and Schwinger-Dyson equations, the non-condensate fraction of a weakly interacting Bose-Einstein condensate (BEC) confined between two parallel plates at zero temperature is investigated within the improved Hartree-Fock approximation. It is proved that the finite-size effect increases the non-condensate fraction compared with the one of the same homogeneous BEC. Our result also shows that the non-condensate fraction can be expressed as a sum of two terms: the first term corresponds to the non-condensate fraction of the homogeneous dilute BEC and the other appears because of the confinement. Both terms are universal. A comparison with the experimental data is made.
•Equation for condensate fraction of a dilute Bose gas is established in the improved Hartree-Fock approximation.•The effect caused by the confinement along z-direction on the condensate fraction is investigated at zero temperature.•The contribution of finite-size is proportional to ratio of scattering length to distance between two parallel plates.•Taking into account the influence of finite-size effect, the condensate fraction is still universal.•A comparison with experimental data is made.</description><subject>Bose-Einstein condensate</subject><subject>Finite-size effect</subject><subject>Non-condensate fraction</subject><subject>Universal properties</subject><issn>0375-9601</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNqFkEtOwzAQhrMAifK4ApoLpNhJk9Y7HqKAhGADa2tqj1u3qR3ZpqWchcNiKKxZjfRr_oe-ojjnbMgZby-Ww36xix0lHFasqoe8EkyIg2LA6nFTipbxo-I4xiVj-ZuJQfH55F2pvNPkIiYCE1Al6x14AwhbwlW3A-sS_ehuDtc-EswxQjYZ60jDjNKWyEHaeugxYNdRB32X0yJsbVpYB3bdB7_Jv_cYUiAqp16tAPusvts1_hRigg8KHhKt-9yW3gKdFocGu0hnv_ekeJ3evtzcl4_Pdw83V4-lqhqRyloxVDNRVRWO1IxrrZvW1EYjq0Yzja3gSGM-GZmJmSiiMWLbGM4arhuheNPUJ0W7z1XBxxjIyD7kWWEnOZPfXOVS_nGV31zlnms2Xu6NlNdtLAUZlSWnSNtAKknt7X8RX2EdjNw</recordid><startdate>20231028</startdate><enddate>20231028</enddate><creator>Thu, Nguyen Van</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-9868-381X</orcidid></search><sort><creationdate>20231028</creationdate><title>Non-condensate fraction of a weakly interacting Bose gas confined between two parallel plates within improved Hartree-Fock approximation at zero temperature</title><author>Thu, Nguyen Van</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c259t-3c0acb9222a4cb1ddd56f3fda024bda691ae7184f8f8cee7aa65f1051d59c1553</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Bose-Einstein condensate</topic><topic>Finite-size effect</topic><topic>Non-condensate fraction</topic><topic>Universal properties</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Thu, Nguyen Van</creatorcontrib><collection>CrossRef</collection><jtitle>Physics letters. A</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Thu, Nguyen Van</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Non-condensate fraction of a weakly interacting Bose gas confined between two parallel plates within improved Hartree-Fock approximation at zero temperature</atitle><jtitle>Physics letters. A</jtitle><date>2023-10-28</date><risdate>2023</risdate><volume>486</volume><spage>129099</spage><pages>129099-</pages><artnum>129099</artnum><issn>0375-9601</issn><abstract>By analytically solving the nonlinear gap and Schwinger-Dyson equations, the non-condensate fraction of a weakly interacting Bose-Einstein condensate (BEC) confined between two parallel plates at zero temperature is investigated within the improved Hartree-Fock approximation. It is proved that the finite-size effect increases the non-condensate fraction compared with the one of the same homogeneous BEC. Our result also shows that the non-condensate fraction can be expressed as a sum of two terms: the first term corresponds to the non-condensate fraction of the homogeneous dilute BEC and the other appears because of the confinement. Both terms are universal. A comparison with the experimental data is made.
•Equation for condensate fraction of a dilute Bose gas is established in the improved Hartree-Fock approximation.•The effect caused by the confinement along z-direction on the condensate fraction is investigated at zero temperature.•The contribution of finite-size is proportional to ratio of scattering length to distance between two parallel plates.•Taking into account the influence of finite-size effect, the condensate fraction is still universal.•A comparison with experimental data is made.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.physleta.2023.129099</doi><orcidid>https://orcid.org/0000-0002-9868-381X</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0375-9601 |
ispartof | Physics letters. A, 2023-10, Vol.486, p.129099, Article 129099 |
issn | 0375-9601 |
language | eng |
recordid | cdi_crossref_primary_10_1016_j_physleta_2023_129099 |
source | Elsevier:Jisc Collections:Elsevier Read and Publish Agreement 2022-2024:Freedom Collection (Reading list) |
subjects | Bose-Einstein condensate Finite-size effect Non-condensate fraction Universal properties |
title | Non-condensate fraction of a weakly interacting Bose gas confined between two parallel plates within improved Hartree-Fock approximation at zero temperature |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-24T12%3A16%3A04IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-elsevier_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Non-condensate%20fraction%20of%20a%20weakly%20interacting%20Bose%20gas%20confined%20between%20two%20parallel%20plates%20within%20improved%20Hartree-Fock%20approximation%20at%20zero%20temperature&rft.jtitle=Physics%20letters.%20A&rft.au=Thu,%20Nguyen%20Van&rft.date=2023-10-28&rft.volume=486&rft.spage=129099&rft.pages=129099-&rft.artnum=129099&rft.issn=0375-9601&rft_id=info:doi/10.1016/j.physleta.2023.129099&rft_dat=%3Celsevier_cross%3ES0375960123004796%3C/elsevier_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c259t-3c0acb9222a4cb1ddd56f3fda024bda691ae7184f8f8cee7aa65f1051d59c1553%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |