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Crystallization parameter evaluation

Developments in instrumentation have allowed measurements of the single-crystal CD spectra of [(+ )D-Cr(en)3]3+ doped in [Ir(en)3]Cl3 between 7 and 293 K. Transitions to the excited states 4T2, 47i, ZE, 27i and 2T2 were observed.418 The discussion refers to much earlier work. The polarized electronic spectra of single crystals of several trans-Cr [XY(en)2] complexes have been assigned and ligand field parameters evaluated.419 CD, absorption and circularly polarized emission spectra have been reported for [Cr(en)3]3+ in the region of the A2g 2EgTig transitions.420... [Pg.797]

The crystallinity of the small crystal was evaluated from its melting point and the order parameter of the visible absorption in the photostationary state. The melting point of crystal 8 before photo irradiation was 164 ° C, and decreased to 45-5 5 0 C upon irradiation with ultraviolet light. The decrease in the melting point upon ultraviolet irradiation is due to the coexistence of two isomers in the same crystal. The crystal became colorless again on irradiation with visible light. The recovery of the melting... [Pg.170]

The conference report from the Crystal City III Workshop outlines the documentation requirements in detail [10]. The degree of documentation should be sufficient to recreate the validation. Prior to initiating a prestudy validation, an appropriate standard operating procedure or a detailed validation plan should be written. This plan can be a stand-alone document or can be contained in a laboratory notebook or some comparable format. The documentation should clearly state the intended use of the method and a summary of the performance parameters to be validated. The plan should include a summary of the proposed experiments and the target acceptance criteria for each performance parameter evaluated. [Pg.108]

Expressions for the force constant, i.r. absorption frequency, Debye temperature, cohesive energy, and atomization energy of alkali-metal halide crystals have been obtained. Gaussian and modified Gaussian interatomic functions were used as a basis the potential parameters were evaluated, using molecular force constants and interatomic distances. A linear dependence between spectroscopically determined values of crystal ionicity and crystal parameters (e.g. interatomic distances, atomic vibrations) has been observed. Such a correlation permits quantitative prediction of coefficients of thermal expansion and amplitude of thermal vibrations of the atoms. The temperature dependence (295—773 K) of the atomic vibrations for NaF, NaCl, KCl, and KBr has been determined, and molecular dynamics calculations have been performed on Lil and NaCl. Empirical values for free ion polarizabilities of alkali-metal, alkaline-earth-metal, and halide ions have been obtained from static crystal polarizabilities the results for the cations are in agreement with recent experimental and theoretical work. [Pg.14]

In many computational codes, second derivatives are evaluated numerically (this is also the case of CRYSTAL). This evaluation requires high numerical accuracy in the determination of the total energy. In particular, the lattice deformations involved in calculating lattice constants, which generally reduce the local symmetry, make basis set flexibility (additional sp shells, polarization functions, and so on) necessary. Consequently, a good basis set for the determination of total energy and lattice parameters may be inadequate for the more demanding estimation of these second derivatives. [Pg.62]

A very comprehensive analysis of the packing energetics of a number of crystal forms of PVDF has been carried out [9]. As a preliminary, extensive force field parameter development was undertaken. Hie CSM model described above in Sect. 4 was utilized. Structures of four known crystal forms were investigated and five new stable forms were found. In addition, crystal property evaluation along the lines described above under Sect. 5 was effected. TaUes 1 and 2 summarize the results. [Pg.25]

Where, 9 is the angle between the director and the long axis of each molecule. In an isotropic liquid, the average of the cosine terms is zero, and therefore the order parameter is equal to zero. For a perfect crystal, the order parameter evaluates to one. Typical values for order parameter of a liquid crystal range between 0.3 and 0.9, with exact value a function of temperature, as a result of kinetic molecular motion [1-10]. [Pg.390]

Although magma density is a function of the kinetic parameters fP and G, it often can be measured iadependentiy. In such cases, it should be used as a constraint ia evaluating nucleation and growth rates from measured crystal size distributions (62), especially if the system of iaterest exhibits the characteristics of anomalous crystal growth. [Pg.350]

Fast methods for evaluating these integrals for the case of gaussian basis functions are known [12], Also, Hall has described how to get the symmetry operators (B) 1SjB, r, for any crystal space group [13]. The parameters account for thermal smearing of the charge density. In this work I use the form recommended by Stewart [14],... [Pg.268]


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See also in sourсe #XX -- [ Pg.601 ]

See also in sourсe #XX -- [ Pg.601 ]

See also in sourсe #XX -- [ Pg.601 ]




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