Multiplicity Distribution and Spectra of Negatively Charged Hadrons in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>A</mml:mi><mml:mi>u</mml:mi><mml:mo>+</mml:mo><mml:mi>A</mml:mi><mml:mi>u</mml:mi></mml:math>Collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi>NN</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:msqrt><mml:mspace/><mml:mo>=</mml:mo><mml:mspace/><mml:mn>130</mml:mn><mml:mn/><mml:mi/><mml:mi>GeV</mml:mi></mml:math>
Аннотация
The minimum-bias multiplicity distribution and the transverse momentum and pseudorapidity distributions for central collisions have been measured for negative hadrons ( ${h}^{\ensuremath{-}}$) in $\mathrm{Au}+\mathrm{Au}$ interactions at $\sqrt{{s}_{\mathrm{NN}}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}130\mathrm{GeV}$. The multiplicity density at midrapidity for the $5%$ most central interactions is ${\mathrm{dN}}_{{h}^{\ensuremath{-}}}/d\ensuremath{\eta}{|}_{\ensuremath{\eta}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}280\ifmmode\pm\else\textpm\fi{}1(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}20(\mathrm{syst})$, an increase per participant of $38%$ relative to $p\overline{p}$ collisions at the same energy. The mean transverse momentum is $0.508\ifmmode\pm\else\textpm\fi{}0.012\mathrm{GeV}/c$ and is larger than in central $\mathrm{Pb}+\mathrm{Pb}$ collisions at lower energies. The scaling of the ${h}^{\ensuremath{-}}$ yield per participant is a strong function of ${p}_{\ensuremath{\perp}}$. The pseudorapidity distribution is almost constant within $|\ensuremath{\eta}|<1$.
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