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玻璃形成体甘油中次级弛豫的特征长度尺度。

Characteristic length scales of the secondary relaxations in glass-forming glycerol.

作者信息

Gupta S, Mamontov E, Jalarvo N, Stingaciu L, Ohl M

机构信息

JCNS-SNS, Biology and Soft-matter Division, Neutron Sciences Directorate, Oak Ridge National Laboratory (ORNL), Bethel Valley Road, PO BOX 2008 MS6473, 37831, Oak Ridge, TN, USA.

Chemical and Engineering Materials Division, Neutron Sciences Directorate, Oak Ridge National Laboratory (ORNL), PO BOX 2008 MS6473, 37831-6473, Oak Ridge, TN, USA.

出版信息

Eur Phys J E Soft Matter. 2016 Mar;39(3):40. doi: 10.1140/epje/i2016-16040-7. Epub 2016 Mar 29.

Abstract

We investigate the secondary relaxations and their link to the main structural relaxation in glass-forming liquids using glycerol as a model system. We analyze the incoherent neutron scattering signal dependence on the scattering momentum transfer, Q , in order to obtain the characteristic length scale for different secondary relaxations. Such a capability of neutron scattering makes it somewhat unique and highly complementary to the traditional techniques of glass physics, such as light scattering and broadband dielectric spectroscopy, which provide information on the time scale, but not the length scales, of relaxation processes. The choice of suitable neutron scattering techniques depends on the time scale of the relaxation of interest. We use neutron backscattering to identify the characteristic length scale of 0.7 Å for the faster secondary relaxation described in the framework of the mode-coupling theory (MCT). Neutron spin-echo is employed to probe the slower secondary relaxation of the excess wing type at a low temperature ( ∼ 1.13T g . The characteristic length scale for this excess wing dynamics is approximately 4.7 Å. Besides the Q -dependence, the direct coupling of neutron scattering signal to density fluctuation makes this technique indispensable for measuring the length scale of the microscopic relaxation dynamics.

摘要

我们以甘油作为模型体系,研究玻璃形成液体中的次级弛豫及其与主要结构弛豫的联系。我们分析非相干中子散射信号对散射动量转移Q的依赖性,以获得不同次级弛豫的特征长度尺度。中子散射的这种能力使其具有一定的独特性,并且与玻璃物理学的传统技术(如光散射和宽带介电谱)高度互补,后者提供了弛豫过程的时间尺度信息,但未提供长度尺度信息。合适的中子散射技术的选择取决于感兴趣的弛豫的时间尺度。我们使用中子背散射来确定在模式耦合理论(MCT)框架中描述的较快次级弛豫的特征长度尺度为0.7 Å。在低温(约1.13Tg)下,采用中子自旋回波来探测过剩翼型的较慢次级弛豫。这种过剩翼动力学的特征长度尺度约为4.7 Å。除了对Q的依赖性外,中子散射信号与密度涨落的直接耦合使得该技术对于测量微观弛豫动力学的长度尺度不可或缺。

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