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Titlebook: Direct Methods of Solving Crystal Structures; Henk Schenk Book 1991 Springer Science+Business Media New York 1991 DSI_D012

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41#
發(fā)表于 2025-3-28 15:13:51 | 只看該作者
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發(fā)表于 2025-3-29 06:01:04 | 只看該作者
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發(fā)表于 2025-3-29 09:51:49 | 只看該作者
0258-1221 Overview: 978-1-4899-3694-3978-1-4899-3692-9Series ISSN 0258-1221
46#
發(fā)表于 2025-3-29 12:11:31 | 只看該作者
Neural Mechanisms of Muscle Crampequalities hold: .where the (complex) normalized structure factor E. is defined by . H is an arbitrary reciprocal lattice vector, Z. is the atomic number and r. the position vector of the atom labeled j, N is the number of atoms in the unit cell, and ..
47#
發(fā)表于 2025-3-29 19:15:21 | 只看該作者
48#
發(fā)表于 2025-3-29 19:48:36 | 只看該作者
Martin Beck-Burridge,Jeremy Waltonof three structure factors via its characteristic function. Assuming an a priori probabilistic model of uniformly and independently distributed atoms, the calculations result in the well-known Cochran distribution for the triplet phase sum.
49#
發(fā)表于 2025-3-30 03:27:48 | 只看該作者
Sports Volunteers Around the Globeds would still be an esoteric, little used branch of crystallography rather than the most important technique available for solving the structures of ‘small’ molecules. The packages which will be discussed here are (in alphabetical order):
50#
發(fā)表于 2025-3-30 04:08:29 | 只看該作者
An Elementary Introduction to Direct Methods,ed straightforward from I. but the relative phases . are lost in the experiment and cause the so called phase problem. Direct methods try to evaluate phases . “directly” from the measured diffraction intensities I. by using relationships among the phases, relationships, whose values are based on the
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