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相干晶格振动驱动 BaFe2As2 正常态中超快瞬态自旋密度波序的产生。

Ultrafast transient generation of spin-density-wave order in the normal state of BaFe2As2 driven by coherent lattice vibrations.

出版信息

Nat Mater. 2012 Apr 8;11(6):497-501. doi: 10.1038/nmat3294.

DOI:10.1038/nmat3294
PMID:22484832
Abstract

The interplay among charge, spin and lattice degrees of freedom in solids gives rise to intriguing macroscopic quantum phenomena such as colossal magnetoresistance, multiferroicity and high-temperature superconductivity. Strong coupling or competition between various orders in these systems presents the key to manipulate their functional properties by means of external perturbations such as electric and magnetic fields or pressure. Ultrashort and intense optical pulses have emerged as an interesting tool to investigate elementary dynamics and control material properties by melting an existing order. Here, we employ few-cycle multi-terahertz pulses to resonantly probe the evolution of the spin-density-wave (SDW) gap of the pnictide compound BaFe(2)As(2) following excitation with a femtosecond optical pulse. When starting in the low-temperature ground state, optical excitation results in a melting of the SDW order, followed by ultrafast recovery. In contrast, the SDW gap is induced when we excite the normal state above the transition temperature. Very surprisingly, the transient ordering quasi-adiabatically follows a coherent lattice oscillation at a frequency as high as 5.5 THz. Our results attest to a pronounced spin-phonon coupling in pnictides that supports rapid development of a macroscopic order on small vibrational displacement even without breaking the symmetry of the crystal.

摘要

固体中的电荷、自旋和晶格自由度的相互作用产生了有趣的宏观量子现象,如庞磁电阻、多铁性和高温超导性。在这些系统中,各种有序之间的强耦合或竞争为通过外部扰动(如电场、磁场或压力)来操纵其功能特性提供了关键。超短和强的光学脉冲已经成为一种有趣的工具,可以通过熔化现有有序来研究基本动力学和控制材料性质。在这里,我们采用多太赫兹的少周期脉冲来共振探测铁砷化合物 BaFe(2)As(2)的自旋密度波(SDW)能隙在飞秒光脉冲激发后的演化。当从低温基态开始时,光激发导致 SDW 有序的熔化,随后超快恢复。相比之下,当我们在相变温度以上激发正常态时,SDW 间隙被诱导出来。非常令人惊讶的是,瞬态有序几乎是绝热地跟随晶格振动的相干振荡,其频率高达 5.5 THz。我们的结果证明了在磷化物中存在明显的自旋-声子耦合,这种耦合支持在不破坏晶体对称性的情况下,即使在小的振动位移上也能快速发展宏观有序。

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