论文标题
在有强磁场的情况下,炭状态的质量和衰减宽度
Masses and Decay widths of Charmonium states in presence of strong magnetic fields
论文作者
论文摘要
在存在强磁场的情况下,研究了炭状态的质量和衰减宽度。观察到静止时分和矢量炭态之间的混合观察到在高磁场的情况下真空/辐射培养基中伪尺度(载体的纵向成分)慈善状态的质量(载体纵向成分)的质量上有明显的负(正(正)移位。在标量DILATON场的培养基变化中,在有效的手性模型中计算出的Hadronic培养基中的伪尺度和矢量炭质量,由于混合效应而具有额外的显着修改。在手性有效模型中计算了磁化强化物质中$ d $和$ \ bar d $介体的质量。使用Quark/Antiquark成分的复合Hadron的现场理论模型计算了矢量炭状态到$ d \ b d $的部分衰减宽度,并将其与使用有效的HADRONIC LAGRANGIAN计算的衰减宽度进行了比较。观察到混合的作用会导致对伪符号和矢量炭状态的质量的显着贡献,并且在巨大磁场值下,衰减宽度$ψ(3770)\ rightarrow d \ d \ d $可显着增加。这些对强磁场中炭状态的研究应对Dilepton光谱以及超相对论重离子碰撞实验中的开放式魅力膜和炭态产生可观察的后果。
The masses and decay widths of charmonium states are studied in the presence of strong magnetic fields. The mixing between the pseudoscalar and vector charmonium states at rest is observed to lead to appreciable negative (positive) shifts in the masses of the pseudoscalar (longitudinal component of the vector) charmonium states in vacuum/hadronic medium in the presence of high magnetic fields. The pseudoscalar and vector charmonium masses in the hadronic medium, calculated in an effective chiral model from the medium changes of a scalar dilaton field, have additional significant modifications due to the mixing effects. The masses of the $D$ and $\bar D$ mesons in the magnetized hadronic matter are calculated within the chiral effective model. The partial decay widths of the vector charmonium state to $D\bar D$ are computed using a field theoretical model for composite hadrons with quark/antiquark constituents, and are compared to the decay widths calculated using an effective hadronic Lagrangian. The effects of the mixing are observed to lead to significant contributions to the masses of the pseusoscalar and vector charmonium states, and an appreciable increase in the decay width $ψ(3770) \rightarrow D\bar D$ at large values of the magnetic fields. These studies of the charmonium states in strong magnetic fields should have observable consequences on the dilepton spectra, as well as on the production of the open charm mesons and the charmonium states in ultra relativistic heavy ion collision experiments.