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Fragmentation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">He</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>4</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>,<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>,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">N</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>14</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>nuclei in nuclear emulsion at 2.1 GeV/nucleon

H. H. HeckmanLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720D. 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 94720Hla ShweLawrence Berkeley Laboratory and Space Sciences Laboratory, University of California, Berkeley, California 94720
1978lv
ABI

Annotatsiya

A comparative study of the fragmentation of $^{4}\mathrm{He}$, $^{12}\mathrm{C}$, $^{14}\mathrm{N}$, and $^{16}\mathrm{O}$ nuclei, $E=2.1$ GeV/nucleon, has been made by using nuclear emulsion detectors. The interaction mean-free paths (cm) for these nuclei in emulsion are 21.8 \ifmmode\pm\else\textpm\fi{} 0.7, 13.8 \ifmmode\pm\else\textpm\fi{} 0.5, 13.1 \ifmmode\pm\else\textpm\fi{} 0.5, and 13.0 \ifmmode\pm\else\textpm\fi{} 0.5, respectively. These data are discussed in terms of optical models and geometrical theories. Fragmentation reactions initiated by $^{12}\mathrm{C}$, $^{14}\mathrm{N}$, and $^{16}\mathrm{O}$ projectiles that exhibit no target excitation, i.e., that possess no low energy particle emission. are selected for special study of projectile fragmentation. The projected angular distributions of $Z=1 \mathrm{and} 2$ secondaries from these interactions are reported, as are the prong-number and charge-multiplicity distributions. The angular distributions are independent of the projectile and exhibit features of limiting fragmentation.NUCLEAR REACTIONS Emulsion exp., $^{4}\mathrm{He}$, $^{12}\mathrm{C}$, $^{14}\mathrm{N}$, and $^{16}\mathrm{O}$ at 2.1 GeV/A; measured mean-free-path lengths; projectile fragmentation reactions; angular, number, and charge multiplicity distributions. Optical and geometrical models; limiting fragmentation.

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