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1 the structure of ModE using multi-wavelength anomalous dispersion.
2 d using the technique of multiple wavelength anomalous dispersion.
3  a resolution of 2.9 A using multiwavelength anomalous dispersion.
4  biological samples with multiple wavelength anomalous dispersion.
5 ly assigned by XRD (X-ray diffraction) using anomalous dispersion.
6 ystal structure of PhzM determined by single anomalous dispersion.
7 UL44 to 1.85 A resolution by multiwavelength anomalous dispersion.
8  X-ray crystallography using multiwavelength anomalous dispersion.
9 Alcaligenes sp. AL3007 using multiwavelength anomalous dispersion.
10 hilus to 2.3 A resolution by multiwavelength anomalous dispersion.
11 tion of selenium and yttrium multiwavelength anomalous dispersion.
12 described, determined using multi-wavelength anomalous dispersion.
13 e twinning complexity renders differences in anomalous dispersion, already small, unreliable.
14 d at 2.0-A resolution by multiple-wavelength anomalous dispersion and crystallographic refinement.
15 ult of a favourable interplay between strong anomalous dispersion and optical nonlinearity around the
16 oli Lon has been solved by single-wavelength anomalous dispersion and refined at 1.75-A resolution.
17  isomorphous replacement and multiwavelength anomalous dispersion and refined to an R factor of 24.1%
18  SFGH to 2.3 A resolution by multiwavelength anomalous dispersion and used the structure to guide sit
19 gle-mode operation, high quality factor, and anomalous dispersion are attained simultaneously.
20 solved by selenomethionine single-wavelength anomalous dispersion at 1.8 A resolution.
21 ensional structure of PhzS, solved by single anomalous dispersion, at a resolution of 2.4 A.
22  modified to take into account the effect of anomalous dispersion before accurate effective path leng
23  of ultrashort laser pulses in the regime of anomalous dispersion can be scaled within a broad range
24 port we show for the first time that neutron anomalous dispersion can be used in a practical manner t
25 n) has been determined using multiwavelength anomalous dispersion data and refined at 2.3 A resolutio
26  PanK (BaPanK), solved using multiwavelength anomalous dispersion data and refined at a resolution of
27  CoADR has been solved using multiwavelength anomalous dispersion data and refined at a resolution of
28 ion was calculated using the multiwavelength anomalous dispersion data collected at the X-ray wavelen
29 ing sites were identified as determined from anomalous dispersion data from aerobically grown ferrous
30 at 2.0 A resolution by using multiwavelength anomalous dispersion data from selenomethionine-enriched
31                                Surprisingly, anomalous dispersion data suggest that the mononuclear s
32 etermined at 1.63A resolution using multiple anomalous dispersion data.
33 order about the butyl groups, analysis using anomalous dispersion establishes the absolute configurat
34                       Our method can realize anomalous dispersion for resonators at almost any wavele
35 e waves generated by an additional transient anomalous dispersion from gas ionization in the mid-infr
36 ving high energy ultrafast laser pulses from anomalous dispersion gain media.
37 omb generation from microresonators requires anomalous dispersion, imposing restrictions on materials
38                               We demonstrate anomalous dispersion in a 300 nm thick silicon nitride f
39 trong-field regime, the additional transient anomalous dispersion introduced by gas ionization would
40               The method of multi-wavelength anomalous dispersion is routinely used in protein crysta
41 termined by a combination of Se-Met multiple anomalous dispersion (MAD) and multiple isomorphous repl
42 d at 1.7 A resolution by the multiwavelength anomalous dispersion (MAD) approach exploiting both the
43                         Iron K-edge multiple anomalous dispersion (MAD) experiments unequivocally ide
44 e pathway, was solved by the multiwavelength anomalous dispersion (MAD) method and refined with data
45  we successfully applied the multiwavelength anomalous dispersion (MAD) method to solve the phase pro
46 idase, was determined by multiple wavelength anomalous dispersion (MAD) methodology and refined to 2.
47 DERA) has been determined by Se-Met multiple anomalous dispersion (MAD) methods at 0.99A resolution.
48                          Multiple wavelength anomalous dispersion (MAD) phasing from quasi-racemate c
49  resolution, employing SeMet multiwavelength anomalous dispersion (MAD) phasing methods.
50  x-ray crystallography using multiwavelength anomalous dispersion (MAD) phasing.
51 ng protein A with the use of multiwavelength anomalous dispersion (MAD) phasing.
52 lved at 1.85A resolution by multi-wavelength anomalous dispersion (MAD) phasing.
53 ed at 2.5 A resolution using multiwavelength anomalous dispersion (MAD) scattering by Se-Met residues
54 unds, has been determined by multiwavelength anomalous dispersion (MAD) techniques and refined to 1.7
55 ion of 1.3 A at pH 8.5 using multiwavelength anomalous dispersion (MAD) techniques.
56 ion, solved in a two-element multiwavelength anomalous dispersion (MAD) X-ray diffraction experiment.
57 solved to 1.8 A using Fe multiple-wavelength anomalous dispersion (MAD), and the positions of Met95 h
58 o 2.0 A resolution using multiple-wavelength anomalous dispersion (MAD).
59 ctor phases by the method of multiple-energy anomalous dispersion (MAD).
60 as been determined using the multiwavelength anomalous dispersion method and refined to 2.3 A resolut
61 actical approach to use the multi-wavelength anomalous dispersion method for lipid structures.
62 ucture was solved by the multiple-wavelength anomalous dispersion method using a set of three-wavelen
63 of KPR was determined by the multiwavelength anomalous dispersion method using the SeMet protein, for
64 f Psu solved by the Hg(2+) single wavelength anomalous dispersion method, which reveals that Psu exis
65 crystal X-ray diffraction analysis using the anomalous dispersion method.
66 , has been determined using multi-wavelength anomalous dispersion methods applied to a selenomethiony
67 ved to 2.1-A resolution by single-wavelength anomalous dispersion methods on a L-selenomethionine-sub
68 aNAT2 was determined using single-wavelength anomalous dispersion methods, and that of native aaNAT2,
69 mensional structure (using single-wavelength anomalous dispersion methods, harnessing extensive non-c
70 gher quality factor and obtain the necessary anomalous dispersion, multi-mode waveguides were previou
71 er-than-c propagation of light pulses, using anomalous dispersion near an absorption line, nonlinear
72 RF metamaterial structure, which can exhibit anomalous dispersion, normal dispersion or a stop band,
73 ed wave analysis is developed, incorporating anomalous dispersion of filter materials in the mid-IR s
74  indirect hypersonic phononic bandgap and an anomalous dispersion of the acoustic-like branch from in
75 o scale the pulse energy at 2 mum due to the anomalous dispersion of the gain fiber.
76 tion of labeled proteins for multiwavelength anomalous dispersion or single-wavelength anomalous disp
77 rmined to 1.4-A resolution by using multiple anomalous dispersion phasing and an automated building p
78 osphatase, was determined by multiwavelength anomalous dispersion phasing and refined at 2.5 A resolu
79 ved to 2.1-A resolution with multiwavelength anomalous dispersion phasing from samarium.
80 cement of methionine by selenomethionine for anomalous dispersion phasing has proven intractable in y
81 th anomalous dispersion or single-wavelength anomalous dispersion phasing in X-ray crystallography.
82  to a resolution of 1.9 A by multiwavelength anomalous dispersion phasing methods.
83 d to 2.4 A resolution with single-wavelength anomalous dispersion phasing methods.
84 2.7-A resolution using a multiple wavelength anomalous dispersion phasing strategy, by substituting t
85 vo structure determined by single-wavelength anomalous dispersion phasing upon soaking with selenoure
86  mutants of Pdx, solved by single-wavelength anomalous dispersion phasing using the [2Fe-2S] iron ato
87 to that of alpha-11 giardin, multiwavelength anomalous dispersion phasing was required to solve the a
88 was solved to 1.8 A by using multiwavelength anomalous dispersion phasing with protein that was expre
89 omethionine-substituted protein and multiple anomalous dispersion phasing, we have solved the crystal
90  in complex with AdoMet by single-wavelength anomalous dispersion phasing.
91 ypsinolysis, surface mutagenesis, and single anomalous dispersion phasing.
92 to 2.35 A resolution using single-wavelength anomalous dispersion phasing.
93 y FKBP51, to 2.8 A, by using multiwavelength anomalous dispersion phasing.
94                             We use the large anomalous dispersion property of the refractive lens mat
95                        Due to pumping in the anomalous dispersion region with two Zero Dispersion Wav
96 een its different frequency components in an anomalous dispersion region.
97 A resolution using sulphur single-wavelength anomalous dispersion reveals that much of the loop struc
98 structure was solved using single-wavelength anomalous dispersion (SAD) phasing of a selenomethionyl
99  been determined, by using single-wavelength anomalous dispersion (SAD) phasing, to 1.6-angstroms res
100 lution by selenomethionine single-wavelength anomalous dispersion (SAD) techniques.
101 re of BTA121 was solved by single-wavelength anomalous dispersion (SAD) using selenomethionine-deriva
102 resolution, determined using multiwavelength anomalous dispersion, shows that the C-terminal portion
103 lved using selenomethionyl single-wavelength anomalous dispersion, structures of C79S/C184S KpHpxA in
104 G)](2) was determined by the multiwavelength anomalous dispersion technique and refined to 1.1 A reso
105 pyrum pernix has been solved by the multiple anomalous dispersion technique using the signal from the
106  at 2.05 A resolution using multi-wavelength anomalous dispersion techniques and reveals the nature o
107 ed by sulfur and manganese single wavelength anomalous dispersion to a resolution of 2.0 A.
108             Here we use gain-assisted linear anomalous dispersion to demonstrate superluminal light p
109  of 1.8 A as determined by single-wavelength anomalous dispersion using phases derived from hexatanta
110 he structure was solved by single-wavelength anomalous dispersion using sodium-iodide-soaked crystals
111 iation of the combs requires global or local anomalous dispersion which leads to many limitations, su
112 o 2.0 A resolution using multiple wavelength anomalous dispersion with Se.
113 elength range, revealing clear signatures of anomalous dispersion, with anomalous group delays as lon
114 of (+)-verticillol (4) was revised after the anomalous dispersion X-ray analysis of (+)-verticillol p

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