Measured total cross sections of slow neutrons scattered by gaseous and liquid H22
(21)
Atchison, F
a,b,c,d,e
Van Den Brandt, B
a,b,c,d,e
Brys T
a,b,c,d,e
Daum, M
a,b,c,d,e
Fierlinger, P
a,b,c,d,e
Hautle, P
a,b,c,d,e
Henneck, R
a,b,c,d,e
Kirch, K
a,b,c,d,e
Kohlbrecher, J
a,b,c,d,e
Kuhne G
a,b,c,d,e
Konter, J A
a,b,c,d,e
Pichlmaier, A
a,b,c,d,e
Wokaun, A
a,b,c,d,e
Bodek, K
b,c,d,e
Kasprzak, M
b,c,d,e
Kuniak M
b,c,d,e
Geltenbort, P
c,d,e
Giersch, M
d,e
Zmeskal, J
d,e
Hino, M
e
Utsuro, M
e
more..
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In fact, we are not aware of any cross section data for deuterium below a neutron energy of 0.9 meV, the lowest energy of.
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In fact, we are not aware of any cross section data for deuterium below a neutron energy of 0.9 meV, the lowest energy of.
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U=2π2mnN0bcoh was calculated using for the liquid H22: N0=0.042mol/cm3 and bcoh=2×6.67fm.
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U=2π2mnN0bcoh was calculated using for the liquid H22: N0=0.042mol/cm3 and bcoh=2×6.67fm.
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Details about the derivation of the limit of slow neutron velocities compared to the molecular velocities are found, e.g., in Ref., Eq.(5.4) and p. 127.
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Details about the derivation of the limit of slow neutron velocities compared to the molecular velocities are found, e.g., in Ref., Eq.(5.4) and p. 127.
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