Quantum second virial coefficient calculation for the 4He dimer on a recent potential

Detalhes bibliográficos
Autor(a) principal: Costa,Éderson D'Martin
Data de Publicação: 2013
Outros Autores: Lemes,Nelson H. T., Alves,Márcio O., Sebastião,Rita C. O., Braga,João P.
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Journal of the Brazilian Chemical Society (Online)
Texto Completo: http://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-50532013000300001
Resumo: This paper focuses on the calculation of the quantum second virial coefficient, under a recently developed potential. This coefficient was determined to within 4-5 significant figures in the temperature range from 3 to 100 K. Our results are within experimental error. The three contributions to the overall value of the coefficient are the quantum scattering (continuum state contribution), the bound state (discrete state contribution) and the quantum ideal gas; we discuss these contributions separately. The most significant contribution is from the scattering states, whereas the smaller contributions are from the discrete states. A sensitivity analysis was performed as a function of temperature for one parameter in the short-range region of the potential and for three parameters in the long-range regions of the potential. For both temperatures considered, 10 and 100 K, the C6 dispersion coefficient was the most significant, and the C10 dispersion term was the least significant to the overall result. In general, the precision required to describe the potential decays as the temperature increases. The overall accuracy and the relationship of the parameters to the experimental errors are discussed.
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spelling Quantum second virial coefficient calculation for the 4He dimer on a recent potentialquantum virialhelium-heliumscattering phase shiftThis paper focuses on the calculation of the quantum second virial coefficient, under a recently developed potential. This coefficient was determined to within 4-5 significant figures in the temperature range from 3 to 100 K. Our results are within experimental error. The three contributions to the overall value of the coefficient are the quantum scattering (continuum state contribution), the bound state (discrete state contribution) and the quantum ideal gas; we discuss these contributions separately. The most significant contribution is from the scattering states, whereas the smaller contributions are from the discrete states. A sensitivity analysis was performed as a function of temperature for one parameter in the short-range region of the potential and for three parameters in the long-range regions of the potential. For both temperatures considered, 10 and 100 K, the C6 dispersion coefficient was the most significant, and the C10 dispersion term was the least significant to the overall result. In general, the precision required to describe the potential decays as the temperature increases. The overall accuracy and the relationship of the parameters to the experimental errors are discussed.Sociedade Brasileira de Química2013-03-01info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersiontext/htmlhttp://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-50532013000300001Journal of the Brazilian Chemical Society v.24 n.3 2013reponame:Journal of the Brazilian Chemical Society (Online)instname:Sociedade Brasileira de Química (SBQ)instacron:SBQ10.5935/0103-5053.20130046info:eu-repo/semantics/openAccessCosta,Éderson D'MartinLemes,Nelson H. T.Alves,Márcio O.Sebastião,Rita C. O.Braga,João P.eng2013-05-24T00:00:00Zoai:scielo:S0103-50532013000300001Revistahttp://jbcs.sbq.org.brONGhttps://old.scielo.br/oai/scielo-oai.php||office@jbcs.sbq.org.br1678-47900103-5053opendoar:2013-05-24T00:00Journal of the Brazilian Chemical Society (Online) - Sociedade Brasileira de Química (SBQ)false
dc.title.none.fl_str_mv Quantum second virial coefficient calculation for the 4He dimer on a recent potential
title Quantum second virial coefficient calculation for the 4He dimer on a recent potential
spellingShingle Quantum second virial coefficient calculation for the 4He dimer on a recent potential
Costa,Éderson D'Martin
quantum virial
helium-helium
scattering phase shift
title_short Quantum second virial coefficient calculation for the 4He dimer on a recent potential
title_full Quantum second virial coefficient calculation for the 4He dimer on a recent potential
title_fullStr Quantum second virial coefficient calculation for the 4He dimer on a recent potential
title_full_unstemmed Quantum second virial coefficient calculation for the 4He dimer on a recent potential
title_sort Quantum second virial coefficient calculation for the 4He dimer on a recent potential
author Costa,Éderson D'Martin
author_facet Costa,Éderson D'Martin
Lemes,Nelson H. T.
Alves,Márcio O.
Sebastião,Rita C. O.
Braga,João P.
author_role author
author2 Lemes,Nelson H. T.
Alves,Márcio O.
Sebastião,Rita C. O.
Braga,João P.
author2_role author
author
author
author
dc.contributor.author.fl_str_mv Costa,Éderson D'Martin
Lemes,Nelson H. T.
Alves,Márcio O.
Sebastião,Rita C. O.
Braga,João P.
dc.subject.por.fl_str_mv quantum virial
helium-helium
scattering phase shift
topic quantum virial
helium-helium
scattering phase shift
description This paper focuses on the calculation of the quantum second virial coefficient, under a recently developed potential. This coefficient was determined to within 4-5 significant figures in the temperature range from 3 to 100 K. Our results are within experimental error. The three contributions to the overall value of the coefficient are the quantum scattering (continuum state contribution), the bound state (discrete state contribution) and the quantum ideal gas; we discuss these contributions separately. The most significant contribution is from the scattering states, whereas the smaller contributions are from the discrete states. A sensitivity analysis was performed as a function of temperature for one parameter in the short-range region of the potential and for three parameters in the long-range regions of the potential. For both temperatures considered, 10 and 100 K, the C6 dispersion coefficient was the most significant, and the C10 dispersion term was the least significant to the overall result. In general, the precision required to describe the potential decays as the temperature increases. The overall accuracy and the relationship of the parameters to the experimental errors are discussed.
publishDate 2013
dc.date.none.fl_str_mv 2013-03-01
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
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status_str publishedVersion
dc.identifier.uri.fl_str_mv http://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-50532013000300001
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dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv 10.5935/0103-5053.20130046
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
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dc.format.none.fl_str_mv text/html
dc.publisher.none.fl_str_mv Sociedade Brasileira de Química
publisher.none.fl_str_mv Sociedade Brasileira de Química
dc.source.none.fl_str_mv Journal of the Brazilian Chemical Society v.24 n.3 2013
reponame:Journal of the Brazilian Chemical Society (Online)
instname:Sociedade Brasileira de Química (SBQ)
instacron:SBQ
instname_str Sociedade Brasileira de Química (SBQ)
instacron_str SBQ
institution SBQ
reponame_str Journal of the Brazilian Chemical Society (Online)
collection Journal of the Brazilian Chemical Society (Online)
repository.name.fl_str_mv Journal of the Brazilian Chemical Society (Online) - Sociedade Brasileira de Química (SBQ)
repository.mail.fl_str_mv ||office@jbcs.sbq.org.br
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