Quantum Statistics and Slow Neutron Scattering by Gases
dc.contributor.author | Plummer, J. P. | en_US |
dc.contributor.author | Summerfield, G. C. | en_US |
dc.contributor.author | Zweifel, Paul Frederick | en_US |
dc.date.accessioned | 2010-05-06T22:51:44Z | |
dc.date.available | 2010-05-06T22:51:44Z | |
dc.date.issued | 1967-12-15 | en_US |
dc.identifier.citation | Plummer, J. P.; Summerfield, G. C.; Zweifel, P. F. (1967). "Quantum Statistics and Slow Neutron Scattering by Gases." The Journal of Chemical Physics 47(12): 4923-4929. <http://hdl.handle.net/2027.42/70882> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/70882 | |
dc.description.abstract | A surprisingly simple expression in ``closed form'' for the cross section d2σ/dΩdϵ for the scattering of thermal neutrons (including polarized neutrons) from an ideal quantum gas is derived. This result extends the work of Van Hove on the quantum gas. An expansion is obtained for dσ/dϵ. The case of elastic scattering is treated separately. From these expressions is obtained a criterion for ignoring the statistics of the scatterer in favor of classical (Boltzmann) statistics. This criterion should have some validity for weakly interacting systems. It is shown that the effects of statistics on the neutron cross section for a helium‐4 gas range from 5% or less for the noninteracting gas up to as much as 40% for the interacting system. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 495124 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Quantum Statistics and Slow Neutron Scattering by Gases | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Nuclear Engineering, The University of Michigan, Ann Arbor, Michigan | en_US |
dc.contributor.affiliationother | Department of Physics, Queens College, City University of New York, Flushing, New York | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/70882/2/JCPSA6-47-12-4923-1.pdf | |
dc.identifier.doi | 10.1063/1.1701741 | en_US |
dc.identifier.source | The Journal of Chemical Physics | en_US |
dc.identifier.citedreference | M. Nelkin, Phys. Rev. 127, 979 (1962); W. E. Parry and R. E. Turner, Ann. Phys. (N.Y.) 17, 301 (1962); J. A. Young and J. U. Koppel, Phys. Rev. 135, A603 (1964). | en_US |
dc.identifier.citedreference | S. K. Sinha and G. Venkataraman, Phys. Rev. 149, 1 (1966); P. Michael, 138, A692 (1965). | en_US |
dc.identifier.citedreference | P. M. Morse, Thermal Physics (W. A. Benjamin, Inc., New York, 1964). | en_US |
dc.identifier.citedreference | G. Placzek, Proc. Symp. Math. Statistics Probability 2nd Berkeley, Calif., 69 (1951). | en_US |
dc.identifier.citedreference | L. Van Hove, Phys. Rev. 95, 249 (1954). | en_US |
dc.identifier.citedreference | See, for example, R. J. Glauber, in Lectures in Theoretical Physics (Interscience Publishers, Inc., New York, 1962), Vol. 4. | en_US |
dc.identifier.citedreference | See D. Falkoff, “The N‐Body Problem,” in The Many Body Problem, Christian Fronsdal, Ed. (W. A. Benjamin, Inc., New York, 1962). | en_US |
dc.identifier.citedreference | (a) See J. P. Plummer, thesis, The University of Michigan, 1964; (b) J. P. Plummer, Idaho Nuclear Corp. Rept. (unpublished). | en_US |
dc.identifier.citedreference | This sign convention is observed throughout this paper. | en_US |
dc.identifier.citedreference | See, for example, S. Yip, R. K. Osborn, and C. Kikuchi, “Neutron Acoustodynamics,” University of Michigan Rept. No. IP‐524, Chap. 8 (1961). | en_US |
dc.identifier.citedreference | There is an apparent oversight in Ref. 5. In the definition of a quantity called n±(r,t),n±(r,t), and later n(r, t) for the condensed‐phase BE gas, a factor of (2S0+1)(2S0+1) is missing. Also Van Hove absorbs a factor of (2πℏ/m)(2πℏ∕m) into his definition of the scattering length a. | en_US |
dc.identifier.citedreference | Equations (8) and (9) must be divided by N, the number of scatterers, to give the cross section per atom. | en_US |
dc.identifier.citedreference | E. P. Wigner and J. E. Wilkins, Jr., U.S. Atomic Energy Commission Rept. No. AECD‐2275 (1944). | en_US |
dc.identifier.citedreference | Argon, Helium, and the Rare Gases G. A. Cook, Ed. (Interscience Publishers, Inc., New York, 1961), Vol. 1. | en_US |
dc.owningcollname | Physics, Department of |
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