-
1
-
-
85030292168
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-
2 By implication, even though diffuse scattering does not suffer the same degree of model degeneracy that Bragg scattering does, it still cannot guarantee the uniqueness of a model
-
2 By implication, even though diffuse scattering does not suffer the same degree of model degeneracy that Bragg scattering does, it still cannot guarantee the uniqueness of a model.
-
-
-
-
6
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0003459618
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W. H. Freeman & Company, New York
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A. Guinier, "X-Ray Diffraction." W. H. Freeman & Company, New York, 1963.
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X-Ray Diffraction
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Guinier, A.1
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7
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0024967611
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Doucet, J.1
Benoit, J.P.2
Cruse, W.B.T.3
Prange, T.4
Kennard, O.5
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8
-
-
85030297660
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-
Along the direction of the scattering vector
-
Along the direction of the scattering vector.
-
-
-
-
9
-
-
85030291382
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-
hkl
-
hkl.
-
-
-
-
14
-
-
85030296133
-
-
BT is Boltzmann's constant, and v is the velocity at which the normal modes propagate, i.e., the speed of sound for the solid
-
BT is Boltzmann's constant, and v is the velocity at which the normal modes propagate, i.e., the speed of sound for the solid.
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-
-
-
16
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-
85030298236
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-
I. D. Glover, G. W. Harris, J. R. Helliwell, and D. S. Moss, Acta Crystallogr. B47, 960.
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Acta Crystallogr.
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Glover, I.D.1
Harris, G.W.2
Helliwell, J.R.3
Moss, D.S.4
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20
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0023924794
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D. L. D. Caspar, J. Clarage, D. M. Salunke, and M. Clarage, Nature (London) 332, 659 (1988).
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Caspar, D.L.D.1
Clarage, J.2
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Clarage, M.4
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22
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85030293366
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j) with the homogeneous correlation function F(r) instead of with the expectation value predicted by normal modes
-
j) with the homogeneous correlation function F(r) instead of with the expectation value predicted by normal modes.
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-
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23
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0027974425
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A. Kolatkar, J. B. Clarage, and G. N. Phillips, Jr., Acta Crystallogr. D50, 210 (1994).
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Kolatkar, A.1
Clarage, J.B.2
Phillips Jr., G.N.3
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25
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-
85030295494
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Δ(r) is the delta function, which is unity at the origin and zero elsewhere
-
Δ(r) is the delta function, which is unity at the origin and zero elsewhere.
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-
-
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26
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12644294295
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Ph.D. thesis, Brandeis University, Waltham, Massachusetts
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J. Clarage, "Disorder in Protein Crystals." Ph.D. thesis, Brandeis University, Waltham, Massachusetts, 1989.
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Disorder in Protein Crystals
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Clarage, J.1
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27
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85030293755
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-
Again, like the isotopic expression in Eq. (9), this is the lowest order in a power series
-
Again, like the isotopic expression in Eq. (9), this is the lowest order in a power series.
-
-
-
-
28
-
-
85030296428
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-
29,30 from classic harmonic analysis, as pointed out in Ref. 21
-
29,30 from classic harmonic analysis, as pointed out in Ref. 21.
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-
29
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0004149484
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-
Cambridge University Press, Cambridge
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J. M. Ziman, "Models of Disorder." Cambridge University Press, Cambridge, 1979.
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Models of Disorder
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Ziman, J.M.1
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32
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85030291822
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note
-
2 derived from bulk properties include the entire spectrum of thermal fluctuations in the crystal, including all of the longer wavelength modes whose effects do not manifest themselves in crystallographically measured B values.
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-
33
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0000893332
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-
C. Edwards, S. B. Palmer, P. Emsley, J. R. Helliwell, I. D. Glover, G. W. Harris, and D. S. Moss, Acta Crystallogr. A46, 315 (1990).
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Edwards, C.1
Palmer, S.B.2
Emsley, P.3
Helliwell, J.R.4
Glover, I.D.5
Harris, G.W.6
Moss, D.S.7
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37
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-
85030291686
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-
Note that in addition to instrumental background, this technique also removes the diffraction effects arising from bulk crystal solvent, Compton scattering, and the completely uncorrelated Einstein component in the atomic displacements. An Einstein component, although a manifestation of atomic displacements in the macromolecule, is often not missed because one is concerned with correlated displacements
-
Note that in addition to instrumental background, this technique also removes the diffraction effects arising from bulk crystal solvent, Compton scattering, and the completely uncorrelated Einstein component in the atomic displacements. An Einstein component, although a manifestation of atomic displacements in the macromolecule, is often not missed because one is concerned with correlated displacements.
-
-
-
-
40
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-
0542452417
-
Wavelet based SAR speckle reduction and image compression
-
April 17-21, Orlando, Florida
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J. E. Odegard, H. Guo, M. Lang, C. S. Burrus, R. O. Wells, Jr., L. M. Novak, and M. Hiett, Wavelet based SAR speckle reduction and image compression. In "SPIE Symposium on OE/Aerospace Sensing and Dual Use Photonics, Algorithm for Synthetic Aperture Radar Imagery II." April 17-21, 1995, Orlando, Florida (http://jazz.rice.edu/publications/).
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SPIE Symposium on OE/Aerospace Sensing and Dual Use Photonics, Algorithm for Synthetic Aperture Radar Imagery II
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Odegard, J.E.1
Guo, H.2
Lang, M.3
Burrus, C.S.4
Wells Jr., R.O.5
Novak, L.M.6
Hiett, M.7
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41
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0028912595
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J. B. Clarage, T. Romo, B. K. Andrews, B. M. Pettitt, and G. N. Phillips, Jr., Proc. Natl. Acad. Sci. U.S.A. 92, 3288-3292 (1995).
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Proc. Natl. Acad. Sci. U.S.A.
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Clarage, J.B.1
Romo, T.2
Andrews, B.K.3
Pettitt, B.M.4
Phillips Jr., G.N.5
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42
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-
85030293395
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-
Although we have developed a suite of programs, XCADS, used to process and analyze diffuse data
-
Although we have developed a suite of programs, XCADS, used to process and analyze diffuse data.
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-
-
-
43
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12644277367
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M. E. Wall, S. E. Ealick, and S. M. Gruner, Proc. Natl. Acad. Sci., U.S.A. 94, 6180-6184 (1997).
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Wall, M.E.1
Ealick, S.E.2
Gruner, S.M.3
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44
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85030291998
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21
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21
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-
-
-
46
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-
85030291950
-
-
A generalization of the reciprocal lattice, defined as the Fourier dual of any real-space lattice, including those not generated by the primitive unit cell
-
A generalization of the reciprocal lattice, defined as the Fourier dual of any real-space lattice, including those not generated by the primitive unit cell.
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-
-
-
49
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12644298226
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A. Kolatkar, J. Clarage, and G. N. Phillips Jr., Rigaku J. 9(2), 4 (1992).
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, vol.9
, Issue.2
, pp. 4
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Kolatkar, A.1
Clarage, J.2
Phillips Jr., G.N.3
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50
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-
85030293655
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-
51 using Mössbauer radiation instead of the X radiation that is the focus of this book
-
51 using Mössbauer radiation instead of the X radiation that is the focus of this book.
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-
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-
51
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34748868767
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Nienhaus, G.U.1
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53
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0028382361
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Smith, J.C.5
Benoit, J.P.6
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