Nuclear Collective Flow in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>197</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Au-Emulsion Interactions at 10.6<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="italic">A</mml:mi></mml:math>GeV
P. L. JainHigh Energy Experimental Laboratory, Department of Physics, State University of New York at Buffalo, Buffalo, New York 14260G. SinghHigh Energy Experimental Laboratory, Department of Physics, State University of New York at Buffalo, Buffalo, New York 14260A. MukhopadhyayHigh Energy Experimental Laboratory, Department of Physics, State University of New York at Buffalo, Buffalo, New York 14260
1995lv
ABI
Annotatsiya
In ${}^{197}$Au-emulsion interactions at $10.6A\mathrm{GeV}$ from the Alternating Gradient Synchrotron at Brookhaven National Laboratory, the projectile fragments (PFs) of charge $Z\ensuremath{\ge}2$ exhibit collective flow which is observed in all interactions with different impact parameters. Collective flow increases with the charge of the PFs. But in the case of ${}^{28}$Si-emulsion interactions at $14.5A\mathrm{GeV}$, the PFs of ${}^{28}$Si do not show collective flow.
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