Bose–Einstein condensation and heat capacity of spin-polarized atomic hydrogen

The condensation fraction, transition temperature, and heat capacity per particle have been calculated for the spin-polarized atomic hydrogen system using the static fluctuation approximation (SFA). The transition temperature has been found to be greater than that for the noninteracting gas, which i...

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Veröffentlicht in:Physica. B, Condensed matter Condensed matter, 2010-05, Vol.405 (9), p.2171-2174
Hauptverfasser: Al-Sugheir, M.K., Sandouqa, A.S., Joudeh, B.R., Al-Omari, S., Awawdeh, M., Rawwagah, F.
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container_end_page 2174
container_issue 9
container_start_page 2171
container_title Physica. B, Condensed matter
container_volume 405
creator Al-Sugheir, M.K.
Sandouqa, A.S.
Joudeh, B.R.
Al-Omari, S.
Awawdeh, M.
Rawwagah, F.
description The condensation fraction, transition temperature, and heat capacity per particle have been calculated for the spin-polarized atomic hydrogen system using the static fluctuation approximation (SFA). The transition temperature has been found to be greater than that for the noninteracting gas, which is consistent with dilute systems results. The heat capacity has a cusp at the transition temperature similar to liquid helium-4. The results obtained indicate that superfluidity behavior occurs in spin-polarized atomic hydrogen system.
doi_str_mv 10.1016/j.physb.2010.01.130
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1873-2135
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subjects Approximation
Bose–Einstein condensation (BEC)
Condensed matter
Condensed matter: structure, mechanical and thermal properties
Condensing
Exact sciences and technology
Heat capacity
Liquids
Mathematical analysis
Physics
Quantum fluids and solids
liquid and solid helium
Specific heat
Spin-polarized hydrogen
Spin-polarized hydrogen and helium
Static fluctuation approximation (SFA)
Transition temperature
title Bose–Einstein condensation and heat capacity of spin-polarized atomic hydrogen
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