Biomarker 发表于 2025-3-25 04:22:45
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Raman and Infrared Lineshapes of Internal Modes in Odic Phasessidered as an assembly of molecules, the centers of mass of which form a regular lattice while the orientation of those molecules displays some degree of disorder. This state, as the liquid crystal one (which is its counter part: center of mass disorder combined with some orientational order) appear贿赂 发表于 2025-3-25 11:44:19
Vibrational Band Shapes of Amorphous Solidsterials are now understood rather completely in terms of the force constants between atoms; although it is still all but impossible to calculate these force constants from first principles in any but the very simplest systems. However using phenomenological force constants it is possible to solve fograndiose 发表于 2025-3-25 16:46:50
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The Effect of Multiphonon Processes on Vibrational Band Shapes in Molecular Solidsr more vibrational quanta on different molecules. The study of multiple excitations becomes of particular significance in ordered solids because of the existence of the translational symmetry. In these solids the two vibrational excitations are characterized by their frequencies ω. and ω. and waveve取消 发表于 2025-3-26 02:46:38
Book 1980e study of the various aspects of vibra tional spectroscopy in molecular liquids and solids. This field has been rapidly expanding in the last decade; unfortunately, its development took place independently for liquids and for solids. In these circumstances, the comparison of the basic concepts andfolliculitis 发表于 2025-3-26 07:02:58
comparative study of the various aspects of vibra tional spectroscopy in molecular liquids and solids. This field has been rapidly expanding in the last decade; unfortunately, its development took place independently for liquids and for solids. In these circumstances, the comparison of the basic co成份 发表于 2025-3-26 11:01:18
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https://doi.org/10.1007/978-1-4613-3111-7collision; crystal; dynamics; experiment; molecular solid; neutron; phase; phase transition; physics; scatter不持续就爆 发表于 2025-3-26 17:21:04
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