论文标题
凝结物中的极性子
Polarons in condensed matter
论文作者
论文摘要
极性物质是复合准颗粒,其中包括电子电荷载体,以及它们在周围的凝结物质中诱导的变化。当电子电荷载体自我捕获时,强耦合极性子形成:在潜在的井中结合了载体的稳定。独特的是,令人兴奋的这些结合载体会产生广泛的吸收带。强耦合极性子较慢且巨大,因为移动它们需要原子运动。它们的运输与常规电子电荷载体的定性不同。较大的(强耦合)极性子与温度升高的迁移率连贯地移动。这些巨大的准粒子非常弱的散射产生的室温迁移率要比传统的电子电荷载体允许的迁移率要低得多。此外,与大极弱散射相关的较长散射时间将其主交流(Drude)的转运降低到声子频率下方。小(强耦合)极性子与较低的热辅助迁移率不连贯地移动。令人惊讶的是,磁场通常以相反的意义使小极性子偏转,从而产生异常签名的大厅效应。在特殊情况下,携带者会成对自我陷阱,从而形成大小的双皮子。一些运输功能将它们与极地区分开。载体诱导的原子位移模式之间的干扰会产生类似带电的极性子与相对带电极性之间的短距离排斥相互作用之间的吸引人的相互作用。
Polarons are composite quasiparticles comprising electronic charge carriers taken together with the alterations they induce in surrounding condensed matter. Strong-coupling polarons form when electronic charge carriers become self-trapped: bound within potential wells stabilized by carriers presence. Distinctively, exciting these bound carriers generates broad absorption bands. Strong-coupling polarons are slow and massive since moving them requires atomic motion. Their transport differs qualitatively from that of conventional electronic charge carriers. Large (strong-coupling) polarons move coherently with mobilities that fall with rising temperature. These massive quasiparticles very weak scatterings by phonons produce much lower room-temperature mobilities than those permitted of conventional electronic charge carriers. Moreover, the long scattering times associated with large polarons weak scattering relegates their principal ac (Drude) transport to below phonon frequencies. Small (strong-coupling) polarons move incoherently with even lower thermally assisted mobilities. Strikingly, a magnetic field often deflects small polarons in the opposite sense than it does conventional charge carriers, thereby producing anomalously signed Hall Effects. In exceptional circumstances charge carriers self-trap in pairs thereby forming large and small bipolarons. Some transport features distinguish them from polarons. Interference between carrier-induced atomic displacement patterns produce attractive interactions between like-charged polarons and short-range repulsive interactions between oppositely charged polarons.