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The masses of open bottom mesons ($B$($B^+$,$B^0$),$\bar{B}$($B^-$,$\bar{B^0}$), $B_s$(${B_{s}}^0$, $\bar{{B_s}^0}$)) and upsilonstates ($\Upsilon(1S)$, $\Upsilon(2S)$, $\Upsilon(3S)$, $\Upsilon(4S)$, and$\Upsilon(1D)$) are investigated in the isospin asymmetric strange hadronicmedium at finite temperature in the presence of strong magnetic fields using achiral effective Lagrangian approach. For charged baryons, the magnetic fieldintroduces contribution from Landau energy levels. The masses of the openbottom mesons get modified through their interactions with the baryons and thescalar mesons, which undergo modifications in a magnetized medium. The chargedopen bottom mesons have additional positive mass shifts due to Landauquantization in the presence of the magnetic field. The medium mass shift ofthe upsilon states originates from the modification of the gluon condensatessimulated by the variation of dilaton field ($\chi$) and a quark mass term inthe magnetized medium. The open bottom mesons and upsilon states experience amass drop in the magnetized medium. The masses of these mesons initiallyincrease with a rise in temperature, and beyond a high value of temperature,their masses are observed to drop. When the temperature is below 90 MeV, thein-medium masses of the mesons increase with an increase in the magnetic field.However, at high temperatures (T $>$ 90 MeV), the masses are observed to dropwith an increase in the magnetic field. The dominant in-medium effects are thedensity effects, which can have observable effects in asymmetric heavy-ioncollisions planned at compressed baryonic matter experiments at FAIR at thefuture facility of GSI.

Open Bottom Mesons and Upsilon States in Hot Magnetized Strange Hadronic Matter