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Fortran and C programs for the time-dependent dipolar Gross–Pitaevskii equation in an anisotropic trap
Many of the static and dynamic properties of an atomic Bose–Einstein condensate (BEC) are usually studied by solving the mean-field Gross–Pitaevskii (GP) equation, which is a nonlinear partial differential equation for short-range atomic interaction. More recently, BEC of atoms with long-range dipol...
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Published in: | Computer physics communications 2015-10, Vol.195, p.117-128 |
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container_title | Computer physics communications |
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creator | Kumar, R. Kishor Young-S., Luis E. Vudragović, Dušan Balaž, Antun Muruganandam, Paulsamy Adhikari, S.K. |
description | Many of the static and dynamic properties of an atomic Bose–Einstein condensate (BEC) are usually studied by solving the mean-field Gross–Pitaevskii (GP) equation, which is a nonlinear partial differential equation for short-range atomic interaction. More recently, BEC of atoms with long-range dipolar atomic interaction are used in theoretical and experimental studies. For dipolar atomic interaction, the GP equation is a partial integro-differential equation, requiring complex algorithm for its numerical solution. Here we present numerical algorithms for both stationary and non-stationary solutions of the full three-dimensional (3D) GP equation for a dipolar BEC, including the contact interaction. We also consider the simplified one- (1D) and two-dimensional (2D) GP equations satisfied by cigar- and disk-shaped dipolar BECs. We employ the split-step Crank–Nicolson method with real- and imaginary-time propagations, respectively, for the numerical solution of the GP equation for dynamic and static properties of a dipolar BEC. The atoms are considered to be polarized along the z axis and we consider ten different cases, e.g., stationary and non-stationary solutions of the GP equation for a dipolar BEC in 1D (along x and z axes), 2D (in x–y and x–z planes), and 3D, and we provide working codes in Fortran 90/95 and C for these ten cases (twenty programs in all). We present numerical results for energy, chemical potential, root-mean-square sizes and density of the dipolar BECs and, where available, compare them with results of other authors and of variational and Thomas–Fermi approximations.
Program title: (i) imag1dZ, (ii) imag1dX, (iii) imag2dXY, (iv) imag2dXZ, (v) imag3d, (vi) real1dZ, (vii) real1dX, (viii) real2dXY, (ix) real2dXZ, (x) real3d
Catalogue identifier: AEWL_v1_0
Program summary URL:http://cpc.cs.qub.ac.uk/summaries/AEWL_v1_0.html
Program obtainable from: CPC Program Library, Queens University, Belfast, N. Ireland
Licensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.html
No. of lines in distributed program, including test data, etc.: 111384
No. of bytes in distributed program, including test data, etc.: 604013
Distribution format: tar.gz |
doi_str_mv | 10.1016/j.cpc.2015.03.024 |
format | article |
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Program title: (i) imag1dZ, (ii) imag1dX, (iii) imag2dXY, (iv) imag2dXZ, (v) imag3d, (vi) real1dZ, (vii) real1dX, (viii) real2dXY, (ix) real2dXZ, (x) real3d
Catalogue identifier: AEWL_v1_0
Program summary URL:http://cpc.cs.qub.ac.uk/summaries/AEWL_v1_0.html
Program obtainable from: CPC Program Library, Queens University, Belfast, N. Ireland
Licensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.html
No. of lines in distributed program, including test data, etc.: 111384
No. of bytes in distributed program, including test data, etc.: 604013
Distribution format: tar.gz</description><identifier>ISSN: 0010-4655</identifier><identifier>EISSN: 1879-2944</identifier><identifier>DOI: 10.1016/j.cpc.2015.03.024</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Atomic interactions ; Bose–Einstein condensate ; C (programming language) ; Dipolar atoms ; FORTRAN ; Fortran and C programs ; Gross–Pitaevskii equation ; Mathematical analysis ; Mathematical models ; Real- and imaginary-time propagation ; Split-step Crank–Nicolson scheme ; Summaries ; Three dimensional ; Two dimensional</subject><ispartof>Computer physics communications, 2015-10, Vol.195, p.117-128</ispartof><rights>2015 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c472t-e2166562f087b78e71be2cf70165573f66cf8b12858a0b282f5380bfcb250b843</citedby><cites>FETCH-LOGICAL-c472t-e2166562f087b78e71be2cf70165573f66cf8b12858a0b282f5380bfcb250b843</cites><orcidid>0000-0002-5435-1688</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Kumar, R. Kishor</creatorcontrib><creatorcontrib>Young-S., Luis E.</creatorcontrib><creatorcontrib>Vudragović, Dušan</creatorcontrib><creatorcontrib>Balaž, Antun</creatorcontrib><creatorcontrib>Muruganandam, Paulsamy</creatorcontrib><creatorcontrib>Adhikari, S.K.</creatorcontrib><title>Fortran and C programs for the time-dependent dipolar Gross–Pitaevskii equation in an anisotropic trap</title><title>Computer physics communications</title><description>Many of the static and dynamic properties of an atomic Bose–Einstein condensate (BEC) are usually studied by solving the mean-field Gross–Pitaevskii (GP) equation, which is a nonlinear partial differential equation for short-range atomic interaction. More recently, BEC of atoms with long-range dipolar atomic interaction are used in theoretical and experimental studies. For dipolar atomic interaction, the GP equation is a partial integro-differential equation, requiring complex algorithm for its numerical solution. Here we present numerical algorithms for both stationary and non-stationary solutions of the full three-dimensional (3D) GP equation for a dipolar BEC, including the contact interaction. We also consider the simplified one- (1D) and two-dimensional (2D) GP equations satisfied by cigar- and disk-shaped dipolar BECs. We employ the split-step Crank–Nicolson method with real- and imaginary-time propagations, respectively, for the numerical solution of the GP equation for dynamic and static properties of a dipolar BEC. The atoms are considered to be polarized along the z axis and we consider ten different cases, e.g., stationary and non-stationary solutions of the GP equation for a dipolar BEC in 1D (along x and z axes), 2D (in x–y and x–z planes), and 3D, and we provide working codes in Fortran 90/95 and C for these ten cases (twenty programs in all). We present numerical results for energy, chemical potential, root-mean-square sizes and density of the dipolar BECs and, where available, compare them with results of other authors and of variational and Thomas–Fermi approximations.
Program title: (i) imag1dZ, (ii) imag1dX, (iii) imag2dXY, (iv) imag2dXZ, (v) imag3d, (vi) real1dZ, (vii) real1dX, (viii) real2dXY, (ix) real2dXZ, (x) real3d
Catalogue identifier: AEWL_v1_0
Program summary URL:http://cpc.cs.qub.ac.uk/summaries/AEWL_v1_0.html
Program obtainable from: CPC Program Library, Queens University, Belfast, N. Ireland
Licensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.html
No. of lines in distributed program, including test data, etc.: 111384
No. of bytes in distributed program, including test data, etc.: 604013
Distribution format: tar.gz</description><subject>Atomic interactions</subject><subject>Bose–Einstein condensate</subject><subject>C (programming language)</subject><subject>Dipolar atoms</subject><subject>FORTRAN</subject><subject>Fortran and C programs</subject><subject>Gross–Pitaevskii equation</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Real- and imaginary-time propagation</subject><subject>Split-step Crank–Nicolson scheme</subject><subject>Summaries</subject><subject>Three dimensional</subject><subject>Two dimensional</subject><issn>0010-4655</issn><issn>1879-2944</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kM9q3DAQh0VpoNtNHqA3HXOxM5KtPyansjRpINAckrOQ5VFW213LK2kDveUd-oZ9ktpsz4WBuczvN3wfIV8Y1AyYvNnVbnI1ByZqaGrg7QeyYlp1Fe_a9iNZATCoWinEJ_I55x0AKNU1K7K9i6kkO1I7DnRDpxRfkz1k6mOiZYu0hANWA044DjgWOoQp7m2i9ynm_Of991MoFt_yzxAoHk-2hDjSsJTNE3IsKU7B0fnBdEkuvN1nvPq31-Tl7tvz5nv1-OP-YfP1sXKt4qVCzqQUknvQqlcaFeuRO69mRiFU46V0XveMa6Et9FxzLxoNvXc9F9DrtlmT63PvjHI8YS7mELLD_d6OGE_ZMAWdaqTsllN2PnULTUJvphQONv0yDMxi1ezMbNUsVg00ZrY6Z27PGZwZ3gImk13A0eEQErpihhj-k_4L7eaBKA</recordid><startdate>20151001</startdate><enddate>20151001</enddate><creator>Kumar, R. Kishor</creator><creator>Young-S., Luis E.</creator><creator>Vudragović, Dušan</creator><creator>Balaž, Antun</creator><creator>Muruganandam, Paulsamy</creator><creator>Adhikari, S.K.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SC</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>JQ2</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope><orcidid>https://orcid.org/0000-0002-5435-1688</orcidid></search><sort><creationdate>20151001</creationdate><title>Fortran and C programs for the time-dependent dipolar Gross–Pitaevskii equation in an anisotropic trap</title><author>Kumar, R. Kishor ; Young-S., Luis E. ; Vudragović, Dušan ; Balaž, Antun ; Muruganandam, Paulsamy ; Adhikari, S.K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c472t-e2166562f087b78e71be2cf70165573f66cf8b12858a0b282f5380bfcb250b843</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Atomic interactions</topic><topic>Bose–Einstein condensate</topic><topic>C (programming language)</topic><topic>Dipolar atoms</topic><topic>FORTRAN</topic><topic>Fortran and C programs</topic><topic>Gross–Pitaevskii equation</topic><topic>Mathematical analysis</topic><topic>Mathematical models</topic><topic>Real- and imaginary-time propagation</topic><topic>Split-step Crank–Nicolson scheme</topic><topic>Summaries</topic><topic>Three dimensional</topic><topic>Two dimensional</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kumar, R. Kishor</creatorcontrib><creatorcontrib>Young-S., Luis E.</creatorcontrib><creatorcontrib>Vudragović, Dušan</creatorcontrib><creatorcontrib>Balaž, Antun</creatorcontrib><creatorcontrib>Muruganandam, Paulsamy</creatorcontrib><creatorcontrib>Adhikari, S.K.</creatorcontrib><collection>CrossRef</collection><collection>Computer and Information Systems Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>Computer physics communications</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kumar, R. Kishor</au><au>Young-S., Luis E.</au><au>Vudragović, Dušan</au><au>Balaž, Antun</au><au>Muruganandam, Paulsamy</au><au>Adhikari, S.K.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fortran and C programs for the time-dependent dipolar Gross–Pitaevskii equation in an anisotropic trap</atitle><jtitle>Computer physics communications</jtitle><date>2015-10-01</date><risdate>2015</risdate><volume>195</volume><spage>117</spage><epage>128</epage><pages>117-128</pages><issn>0010-4655</issn><eissn>1879-2944</eissn><abstract>Many of the static and dynamic properties of an atomic Bose–Einstein condensate (BEC) are usually studied by solving the mean-field Gross–Pitaevskii (GP) equation, which is a nonlinear partial differential equation for short-range atomic interaction. More recently, BEC of atoms with long-range dipolar atomic interaction are used in theoretical and experimental studies. For dipolar atomic interaction, the GP equation is a partial integro-differential equation, requiring complex algorithm for its numerical solution. Here we present numerical algorithms for both stationary and non-stationary solutions of the full three-dimensional (3D) GP equation for a dipolar BEC, including the contact interaction. We also consider the simplified one- (1D) and two-dimensional (2D) GP equations satisfied by cigar- and disk-shaped dipolar BECs. We employ the split-step Crank–Nicolson method with real- and imaginary-time propagations, respectively, for the numerical solution of the GP equation for dynamic and static properties of a dipolar BEC. The atoms are considered to be polarized along the z axis and we consider ten different cases, e.g., stationary and non-stationary solutions of the GP equation for a dipolar BEC in 1D (along x and z axes), 2D (in x–y and x–z planes), and 3D, and we provide working codes in Fortran 90/95 and C for these ten cases (twenty programs in all). We present numerical results for energy, chemical potential, root-mean-square sizes and density of the dipolar BECs and, where available, compare them with results of other authors and of variational and Thomas–Fermi approximations.
Program title: (i) imag1dZ, (ii) imag1dX, (iii) imag2dXY, (iv) imag2dXZ, (v) imag3d, (vi) real1dZ, (vii) real1dX, (viii) real2dXY, (ix) real2dXZ, (x) real3d
Catalogue identifier: AEWL_v1_0
Program summary URL:http://cpc.cs.qub.ac.uk/summaries/AEWL_v1_0.html
Program obtainable from: CPC Program Library, Queens University, Belfast, N. Ireland
Licensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.html
No. of lines in distributed program, including test data, etc.: 111384
No. of bytes in distributed program, including test data, etc.: 604013
Distribution format: tar.gz</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.cpc.2015.03.024</doi><tpages>12</tpages><orcidid>https://orcid.org/0000-0002-5435-1688</orcidid><oa>free_for_read</oa></addata></record> |
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language | eng |
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source | ScienceDirect Freedom Collection |
subjects | Atomic interactions Bose–Einstein condensate C (programming language) Dipolar atoms FORTRAN Fortran and C programs Gross–Pitaevskii equation Mathematical analysis Mathematical models Real- and imaginary-time propagation Split-step Crank–Nicolson scheme Summaries Three dimensional Two dimensional |
title | Fortran and C programs for the time-dependent dipolar Gross–Pitaevskii equation in an anisotropic trap |
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