<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mi>ρ</mml:mi><mml:mn>0</mml:mn></mml:msup></mml:math>Production and Possible Modification in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">A</mml:mi><mml:mi mathvariant="normal">u</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">A</mml:mi><mml:mi mathvariant="normal">u</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mi>p</mml:mi></mml:math>Collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>200</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi mathvariant="normal">G</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mi mathvariant="normal">V</mml:mi></mml:math>
Аннотация
We report results on $\ensuremath{\rho}(770{)}^{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ production at midrapidity in $p+p$ and peripheral $\mathrm{A}\mathrm{u}+\mathrm{A}\mathrm{u}$ collisions at $\sqrt{{s}_{NN}}=200\text{ }\text{ }\mathrm{G}\mathrm{e}\mathrm{V}$. This is the first direct measurement of $\ensuremath{\rho}(770{)}^{0}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ in heavy-ion collisions. The measured ${\ensuremath{\rho}}^{0}$ peak in the invariant mass distribution is shifted by $\ensuremath{\sim}40\text{ }\text{ }\mathrm{M}\mathrm{e}\mathrm{V}/{c}^{2}$ in minimum bias $p+p$ interactions and $\ensuremath{\sim}70\text{ }\text{ }\mathrm{M}\mathrm{e}\mathrm{V}/{c}^{2}$ in peripheral $\mathrm{A}\mathrm{u}+\mathrm{A}\mathrm{u}$ collisions. The ${\ensuremath{\rho}}^{0}$ mass shift is dependent on transverse momentum and multiplicity. The modification of the ${\ensuremath{\rho}}^{0}$ meson mass, width, and shape due to phase space and dynamical effects are discussed.
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