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1 hanges in the crystallographic observables ("structure factors").
2 n to the first sharp diffraction peak in the structure factor.
3  inter-micellar interactions via analysis of structure factor.
4  intensity is found to scale with the static structure factor.
5 ction phi, we obtain a phi-dependent average structure factor.
6 tified by the principal peak position of the structure factor.
7 which are identified from the scaling of the structure factor.
8 erto-unexplained aspects of its dynamic spin structure factor.
9 rier transform vectors in the aperture array structure factor.
10 tations below the gap with an incommensurate structure factor.
11 nt within the error margins of the Yamaguchi structure factors.
12 t directional-dependence (anisotropy) in the structure factors.
13 eudo-atoms for normalization of the observed structure factors.
14 tron diffraction techniques by fitting their structure factors(1-3), but only if the sample is perfec
15               The resulting reciprocal-space structure factors agree quantitatively with neutron diff
16 e remaining 7 mus of the trajectory, and the structure factors agree well with experiment.
17 aller factor and charge radius, the measured structure factors also improve constraints on the streng
18                                              Structure factor amplitudes and phases can be computed d
19 rdingly, we redetermined the structure using structure factor amplitudes deposited in the Protein Dat
20 ameters necessary to make corrections to the structure factor amplitudes derived from electron cryomi
21                                              Structure factor amplitudes of a three-dimensional map o
22 accurate measurement of spherically averaged structure factor amplitudes of particles in solution but
23 rees tilt and increasing the completeness of structure factor amplitudes to 84.7 %.
24 ystem, the development of a peak in the spin structure factor and a staggered magnetization that is c
25 haracterized by a rapid decay of the dynamic structure factor and by a square root power law for the
26 using an entanglement witness based upon the structure factor and demonstrate its validity versus the
27                             By analyzing the structure factor and the radial distribution function, t
28 ments of the (220) and (400) neutron-silicon structure factors and achieved a factor-of-four improvem
29                                          The structure factors and coordinates of IGF2R domain 11 hav
30 iments agrees with reported x-ray scattering structure factors and intensities for Q > 6.5 A(-1).
31        The R-factor between the experimental structure factors and those derived from this unrestrain
32 tonians are precisely inherited by dynamical structure factors and, hence, offer in the same way the
33 ptors such as the pair correlation function, structure factor, and Voronoi statistics show a strong c
34 f electron density differences, extrapolated structure factors, and occupancy refinements are shown t
35 onent distributions, continuous and discrete structure factors, and overall scattering-density profil
36                                    Six total structure factors are analyzed (5 neutron + 1 X-ray) to
37 tically accessible variants of the dynamical structure factors are bounded-error quantum polynomial t
38 states are universal in the sense that their structure factors are characterised by a complete indepe
39                         Our results indicate structuring factors are related to the distribution of t
40 scattering, considering both form factor and structure factor, as well as the use of correlation func
41 n time of the suspension does not follow the structure factor, but that instead, it remains unchanged
42 e satisfactory for determining the phases of structure factors, but not their absolute values.
43 an) to liquid-like (Lorentzian) self-dynamic structure factor by incoherent quasi-elastic neutron sca
44              Nano-beam electron diffraction, structure factor calculation and x-ray reciprocal space
45  electron diffraction patterns compared with structure factor calculation found that the BiFeO(3) mai
46                                  Directional structure factor calculations were made from these simul
47                                              Structure factor calculations, in conjunction with resul
48  algorithms that jointly estimate scales and structure factors can address this limitation.
49 ure model are discussed, with a key focus on structure factor coarse-graining and hydration contribut
50                       The respective partial structure factor contributions to F(x)(Q) are obtained b
51  experimental x-ray scattering intensity and structure factor data for Q < 6.5 A(-1).
52                                          The structure factor data show that the first sharp diffract
53 everal important elements, effective residue structure factors derived from the Protein Data Bank, ex
54                                              Structure factors describe how incident radiation is sca
55 and by a resolution-dependent damping of the structure factor differences between data and model.
56  X-ray crystallography will yield consistent structure factors, even at low resolution, when image re
57                               The incoherent structure factor extracted from the velocity autocorrela
58 ficients (A2) were determined from the X-ray structure factors extrapolated to the origin.
59                                        Total structure factors (F(x)(Q)) are collected on the laser-h
60                 We show from analysis of the structure factor for this lattice that the sampling patt
61 e parameters correlate with crystallographic structure factors for Calpha carbons, suggesting that th
62 ggesting the latter's expansion to be a main structuring factor for the parasite.
63 hyperuniform fluid features a scaling in the structure factor [Formula: see text] in 2D, which is the
64                     In addition, the dynamic structure factor [Formula: see text] is rigorously recon
65 mula: see text]) dependence of the dynamical structure factor [Formula: see text] using neutron scatt
66 ifferent physical properties like the static structure factor [Formula: see text], the momentum distr
67 ents yield the scattering intensity (dynamic structure factor) [Formula: see text] as a function of [
68 lculate both the stress and the single-chain structure factor from first principles.
69      The atomic coordinates and experimental structure factors have been deposited in the PDB with th
70   Changes to the metastable solid and liquid structure factors have been dynamically measured.
71 es and other instrumental factors affect the structure factors, however, resulting in decreased accur
72 tering (INS), we measured the full dynamical structure factor in Al-doped h-YMnO(3) and confirmed the
73 owing for the determination of the dynamical structure factor in different architectures, including a
74 eground, soil properties and other spatially structured factors in explaining the heterogeneity in so
75 lin (PSM) surfactant peptides as key biofilm structuring factors in the premier biofilm-forming patho
76 lous diffusion results from a combination of structuring factors including protein-protein interactio
77 th the transcription machinery and chromatin structure, factors integral to nuclear receptor-regulate
78 y: 0.1-1.0 mum(-1)), altering the electronic structure factored into available density of states near
79 ts, an analytical expression for the dynamic structure factor is formulated for the BP excitation.
80 sed to confirm silica encapsulation, since a structure factor is observed at q approximately 0.25 nm(
81                                The dynamical structure factor is one of the experimental quantities c
82 space mapping of the second-order non-linear structure factor is the source of this contrast and deve
83 Q < 2.4 angstrom(-1), i.e., at and below the structure factor main peak, for Q > 2.4 angstrom(-1), be
84 trom(-1), beyond the first minimum above the structure factor main peak, the stretching exponent exhi
85 ns in the powder patterns preclude separated structure factor measurements for these data.
86 , but model refinement will require accurate structure factor measurements.
87                           The absolute-scale structure factors obtained in the experiments provided a
88 cts that the density excitation spectrum and structure factor of a condensed Bosonic system in the ph
89 ic X-ray scattering (REXS), we show that the structure factor of charge order previously identified b
90 nergies, dispersion relations, and dynamical structure factor of neutron scattering as well as macros
91 s work we analyze GISAXS measurements of the structure factor of Si surfaces evolving during 1 keV Ar
92  scattering wave vector, correlates with the structure factor of the material.
93 are consistent with the calculated dynamical structure factor of the tetrahedral triple-Q state.
94                          We compute the spin-structure factor of XXZ spin chains in the Heisenberg an
95                                              Structure factors of components in both leaves display a
96 for the observation of features of dynamical structure factors of correlated quantum matter in the pr
97  way as experimental data by determining the structure factors of the system and, via Fourier reconst
98 on and composition were found to be a strong structuring factor of their intrafamily diversity and tr
99 ce (correlation function) and Fourier space (structure factor) of the cell centroids in the early sta
100 indeed provides access to the spin dynamical structure factor once one considers the full influence o
101 al consistency, but also a more distinct and structured factor organization compared to the human cou
102 f shifts in radial distribution function and structure factor peaks associated with volume changes in
103 rystallizing the protein and determining the structure factor phases by the method of multiple-energy
104         The ability of the algorithm to find structure-factor phases rapidly is found to assist with
105 of such order is the first peak in the total structure factor, referred to as the first sharp diffrac
106                                  Static spin structure factors reveal ferromagnetic and ferrimagnetic
107         In concentrated mucin solutions, the structure factor S(q, t) derived from DLS measurements c
108 This technique directly measures the dynamic structure factor S(q,omega) which is the space-time Four
109  density fluctuations, or, equivalently, the structure factor S(q-->0) = 0; the smaller the value of
110                               Scaling of the structure factor, S(q) proportional, variant q(-1/nu), w
111  usually obtained by measuring the dynamical structure factor, S(Q, omega), using inelastic neutron o
112  to test the so-called fluid-minus method of structure-factor scaling.
113 ndles confirmed the theoretically predicated structure-factor scattering peak line shape.
114 pproach to quantify correlations between the structure factor sets.
115 ransition temperatures, the phonon dynamical structure factor shows a giant phonon-energy hardening a
116                                          The structure factor shows a hierarchy of timescales in the
117              During the whole procedure, the Structure Factor Size and Attenuation Estimator cellular
118                                          The Structure Factor Size and Attenuation Estimator is propo
119 n that can be quantified with the ultrasound Structure Factor Size and Attenuation Estimator.
120  measurements provide absolute values of the structure factor that encodes the microscopic arrangemen
121 pounds that vary in volatility and molecular structure-factors that influence their contributions to
122 rse magnetization, the reduced growth of the structure factor, that is, spin-wave excitations (SWE),
123 h is rooted in the sensitivity of the static structure factor to temperature variations.
124  I developed a new method of using molecular structure factors to solve the crystal structure, which
125 ed a factor-of-four improvement in the (111) structure factor uncertainty.
126  laser pulse, following which we measure the structure factor using femtosecond x-ray laser pulses.
127                            A noise-dependent structure factor weight is derived and used in conjuncti
128                     Amplitudes and phases of structure factors were computed and combined to produce
129 d to obtain the zeta potential from the SAXS structure factor which is in good agreement with directl
130  leaves a distinct signature in the system's structure factor, which exhibits two different power-law
131  generate a model for the electronic dynamic structure factor, which offers an avenue for measuring h
132 ise to anomalous power-law decay of the spin-structure factor, with continuously varying exponents, a
133 y to investigate interactions between fibrin structure, factor XIII Val34Leu, fibrinogen Aalpha Thr31

 
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