\begin{document}$ \Upsilon(1S) $\end{document} suppression that occurs due to the fast heating process at the early stage of the fireball, instead of its finite decay width in a finite temperature medium generated by heavy ion collisions. We calculate the transition probability after the fast heating dissociation as a function of the temperature of the medium and the nuclear modification factor in central collisions and find that the suppression is not negligible at RHIC, even if the width of \begin{document}$ \Upsilon(1S) $\end{document} becomes zero."> Fast heating dissociation of <inline-formula><tex-math id="M1">\begin{document}${ \Upsilon(1S) }$\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/3d7b52bd-d066-492f-8dce-403e37d9a19c/CPC-2020-0360_M1.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="//www.macurncorp.com/hepnp/article/app/id/3d7b52bd-d066-492f-8dce-403e37d9a19c/CPC-2020-0360_M1.png"/></alternatives></inline-formula> in heavy ion collisions at RHIC -
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