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Momentum sharing in imbalanced Fermi systems | | O. Hen
; M. Sargsian
; L.B. Weinstein
; E. Piasetzky
; H. Hakobyan
; D. W. Higinbotham
; M. Braverman
; W.K. Brooks
; S. Gilad
; K. P. Adhikari
; J. Arrington
; G. Asryan
; H. Avakian
; J. Ball
; N. A. Baltzell
; M. Battaglieri
; A. Beck
; S. May-Tal Beck
; I. Bedlinskiy
; W. Bertozzi
; A. Biselli
; V. D. Burkert
; T. Cao
; D. S. Carman
; A. Celentano
; S. Chandavar
; L. Colaneri
; P. L. Cole
; V. Crede
; A. DAngelo
; R. De Vita
; A. Deur
; C. Djalali
; D. Doughty
; M. Dugger
; R. Dupre
; H. Egiyan
; A. El Alaoui
; L. El Fassi
; L. Elouadrhiri
; G. Fedotov
; S. Fegan
; T. Forest
; B. Garillon
; M. Garcon
; N. Gevorgyan
; Y. Ghandilyan
; G. P. Gilfoyle
; F. X. Girod
; J. T. Goetz
; R. W. Gothe
; K. A. Griffioen
; M. Guidal
; L. Guo
; K. Hafidi
; C. Hanretty
; M. Hattawy
; K. Hicks
; M. Holtrop
; C. E. Hyde
; Y. Ilieva
; D. G. Ireland
; B.I. Ishkanov
; E. L. Isupov
; H. Jiang
; H. S. Jo
; K. Joo
; D. Keller
; M. Khandaker
; A. Kim
; W. Kim
; F. J. Klein
; S. Koirala
; I. Korover
; S. E. Kuhn
; V. Kubarovsky
; P. Lenisa
; W. I. Levine
; K. Livingston
; M. Lowry
; H. Y. Lu
; I. J. D. MacGregor
; N. Markov
; M. Mayer
; B. McKinnon
; T. Mineeva
; V. Mokeev
; A. Movsisyan
; C. Munoz Camacho
; B. Mustapha
; P. Nadel-Turonski
; S. Niccolai
; G. Niculescu
; I. Niculescu
; M. Osipenko
; L. L. Pappalardo
; R. Paremuzyan
; K. Park
; E. Pasyuk
; W. Phelps
; S. Pisano
; O. Pogorelko
; J. W. Price
; S. Procureur
; Y. Prok
; D. Protopopescu
; A. J. R. Puckett
; D. Rimal
; M. Ripani
; B. G. Ritchie
; A. Rizzo
; G. Rosner
; P. Rossi
; P. Roy
; F. Sabatie
; D. Schott
; R. A. Schumacher
; Y. G. Sharabian
; G. D. Smith
; R. Shneor
; D. Sokhan
; S. S. Stepanyan
; S. Stepanyan
; P. Stoler
; S. Strauch
; V. Sytnik
; M. Taiuti
; S. Tkachenko
; M. Ungaro
; A. V. Vlassov
; E. Voutier
; D. Watts
; N. K. Walford
; X. Wei
; M. H. Wood
; S. A. Wood
; N. Zachariou
; L. Zana
; Z. W. Zhao
; X. Zheng
; I. Zonta
; | | Date: |
29 Nov 2014 | | Abstract: | The atomic nucleus is composed of two different kinds of fermions, protons
and neutrons. If the protons and neutrons did not interact, the Pauli exclusion
principle would force the majority fermions (usually neutrons) to have a higher
average momentum. Our high-energy electron scattering measurements using 12C,
27Al, 56Fe and 208Pb targets show that, even in heavy neutron-rich nuclei,
short-range interactions between the fermions form correlated high-momentum
neutron-proton pairs. Thus, in neutron-rich nuclei, protons have a greater
probability than neutrons to have momentum greater than the Fermi momentum.
This finding has implications ranging from nuclear few body systems to neutron
stars and may also be observable experimentally in two-spin state, ultra-cold
atomic gas systems. | | Source: | arXiv, 1412.0138 | | Services: | Forum | Review | PDF | Favorites | |
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