Momentum Distributions of Isotopes Produced by Fragmentation of Relativistic<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>12</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>16</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>Projectiles
D. GreinerLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720P. J. LindstromLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720H. H. HeckmanLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720B. CorkLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720F. BieserLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720
1975lv
ABI
Annotatsiya
The fragment momentum distributions in the projectile rest frame are, typically, Gaussian shaped, narrow, consistent with isotropy, depend on fragment and projectile, and have no significant correlation with target mass or beam energy. The nuclear temperature is inferred from the momentum distributions of the fragments and is approximately equal to the projectile nuclear binding energy, indicative of small energy transfer between target and fragment.
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