Underdamped longitudinal soft modes in ionic crystallites-lattice and charge motions observed by ultrafast x-ray diffraction.

IF 2.3 2区 物理与天体物理 Q3 CHEMISTRY, PHYSICAL Structural Dynamics-Us Pub Date : 2022-03-08 eCollection Date: 2022-03-01 DOI:10.1063/4.0000143
Isabel Gonzalez-Vallejo, Azize Koç, Klaus Reimann, Michael Woerner, Thomas Elsaesser
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Abstract

Soft modes in crystals are lattice vibrations with frequencies that decrease and eventually vanish as the temperature approaches a critical point, e.g., a structural change due to a phase transition. In ionic para- or ferroelectric materials, the frequency decrease is connected with a diverging electric susceptibility and, for infrared active modes, a strong increase in oscillator strength. The traditional picture describes soft modes as overdamped transverse optical phonons of a hybrid vibrational-electronic character. In this context, potassium dihydrogen phosphate (KH2PO4, KDP) has been studied for decades as a prototypical material with, however, inconclusive results regarding the soft modes in its para- and ferroelectric phase. There are conflicting assignments of soft-mode frequencies and damping parameters. We report the first observation of a longitudinal underdamped soft mode in paraelectric KDP. Upon impulsive femtosecond Raman excitation of coherent low-frequency phonons in the electronic ground state of KDP crystallites, transient powder diffraction patterns are recorded with femtosecond hard x-ray pulses. Electron density maps derived from the x-ray data reveal oscillatory charge relocations over interatomic distances, much larger than the sub-picometer nuclear displacements, a direct hallmark of soft-mode behavior. The strongly underdamped character of the soft mode manifests in charge oscillations persisting for more than 10 ps. The soft-mode frequency decreases from 0.55 THz at T =295 K to 0.39 THz at T =175 K. An analysis of the Raman excitation conditions in crystallites and the weak damping demonstrate a longitudinal character. Our results extend soft-mode physics well beyond the traditional picture and pave the way for an atomic-level characterization of soft modes.

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离子晶体的欠阻尼纵向软模式——超快x射线衍射观察到的晶格和电荷运动。
晶体中的软模式是晶格振动,其频率随着温度接近临界点而降低并最终消失,例如,由于相变引起的结构变化。在离子对电或铁电材料中,频率的降低与电磁化率的发散有关,而对于红外主动模式,则与振荡器强度的强烈增加有关。传统图像将软模描述为振动电子混合特性的过阻尼横向光学声子。在这种情况下,磷酸二氢钾(KH2PO4, KDP)作为一种原型材料已经被研究了几十年,然而,关于其对电相和铁电相的软模式,没有确定的结果。软模频率和阻尼参数的分配存在冲突。我们报告了在准电KDP中首次观察到的纵向欠阻尼软模式。在KDP晶体电子基态的相干低频声子的飞秒拉曼脉冲激发下,用飞秒硬x射线脉冲记录了瞬态粉末衍射图样。来自x射线数据的电子密度图揭示了振荡电荷在原子间距离上的重定位,远大于亚皮米核位移,这是软模式行为的直接标志。软模的弱阻尼特性表现为持续10 ps以上的电荷振荡,软模频率从T = 295 K时的0.55 THz下降到T = 175 K时的0.39 THz。对微晶中的拉曼激发条件和弱阻尼的分析表明其具有纵向特征。我们的研究结果将软模式物理扩展到传统图像之外,并为软模式的原子级表征铺平了道路。
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来源期刊
Structural Dynamics-Us
Structural Dynamics-Us CHEMISTRY, PHYSICALPHYSICS, ATOMIC, MOLECU-PHYSICS, ATOMIC, MOLECULAR & CHEMICAL
CiteScore
5.50
自引率
3.60%
发文量
24
审稿时长
16 weeks
期刊介绍: Structural Dynamics focuses on the recent developments in experimental and theoretical methods and techniques that allow a visualization of the electronic and geometric structural changes in real time of chemical, biological, and condensed-matter systems. The community of scientists and engineers working on structural dynamics in such diverse systems often use similar instrumentation and methods. The journal welcomes articles dealing with fundamental problems of electronic and structural dynamics that are tackled by new methods, such as: Time-resolved X-ray and electron diffraction and scattering, Coherent diffractive imaging, Time-resolved X-ray spectroscopies (absorption, emission, resonant inelastic scattering, etc.), Time-resolved electron energy loss spectroscopy (EELS) and electron microscopy, Time-resolved photoelectron spectroscopies (UPS, XPS, ARPES, etc.), Multidimensional spectroscopies in the infrared, the visible and the ultraviolet, Nonlinear spectroscopies in the VUV, the soft and the hard X-ray domains, Theory and computational methods and algorithms for the analysis and description of structuraldynamics and their associated experimental signals. These new methods are enabled by new instrumentation, such as: X-ray free electron lasers, which provide flux, coherence, and time resolution, New sources of ultrashort electron pulses, New sources of ultrashort vacuum ultraviolet (VUV) to hard X-ray pulses, such as high-harmonic generation (HHG) sources or plasma-based sources, New sources of ultrashort infrared and terahertz (THz) radiation, New detectors for X-rays and electrons, New sample handling and delivery schemes, New computational capabilities.
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