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Superfluid-normal phase transition in finite systems and its effect on damping of hot giant resonances

机译:有限体系中的超流体 - 正常相变及其对有限元的影响   阻止热巨人共振

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摘要

Thermal fluctuations of quasiparticle number are included making use of thesecondary Bogolyubov's transformation, which turns quasiparticles operatorsinto modified-quasiparticle ones. This restores the unitarity relation for thegeneralized single-particle density operator, which is violated within theHartree-Fock-Bogolyubov (HFB) theory at finite temperature. The resultingtheory is called the modified HFB (MHFB) theory, whose limit of a constantpairing interaction yields the modified BCS (MBCS) theory. Within the MBCStheory, the pairing gap never collapses at finite temperature T as it doeswithin the BCS theory, but decreases monotonously with increasing T. It isdemonstrated that this non-vanishing thermal pairing is the reason why thewidth of the giant dipole resonance (GDR) does not increase with T up to Taround 1 MeV. At higher T, when the thermal pairing is small, the GDR widthstarts to increase with T. The calculations within the phonon-damping modelyield the results in good agreement with the most recent experimentalsystematic for the GDR width as a function of T. A similar effect, which causesa small GDR width at low T, is also seen after thermal pairing is included inthe thermal fluctuation model.
机译:利用二次Bogolyubov变换将准粒子数的热波动包括在内,该转换将准粒子算子转换为修饰准粒子算子。这恢复了广义单粒子密度算子的统一性关系,这在有限温度下违反了Hartree-Fock-Bogolyubov(HFB)理论。由此产生的理论称为改进的HFB(MHFB)理论,其恒定配对相互作用的极限产生了改进的BCS(MBCS)理论。在MBCS理论中,配对间隙从未像在BCS理论中那样在有限的温度T时崩溃,而是随着T的增加而单调减小。这证明了这种不消失的热配对是巨型偶极子共振(GDR)的宽度确实如此的原因。不会随着T的增加而增加到Taround 1 MeV。在较高的T下,当热配对较小时,GDR宽度开始随T增加。声子阻尼模型中的计算得出的结果与最新实验系统对GDR宽度作为T的函数非常吻合。在热波动模型中包含热配对后,还可以看到在低T时会导致GDR宽度变窄的。

著录项

  • 作者

    Dang, Nguyen Dinh;

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  • 年度 2006
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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