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Newman, M.E.2
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14
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0001827752
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W. Brown, Oxford University Press, New York, ch. 16
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D. A. Weitz and D. J. Pine, in Dynamic Light Scattering, ed. W. Brown, Oxford University Press, New York, 1993, ch. 16, p. 652–720.
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S.-H. Chen, J. S. Huang and P. Tartaglia, Kluwer Academic Publishers, Dordrecht
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D. A. Weitz, J. X. Zhu, D. J. Durian and D. J. Pine, in Structure and dynamics of strongly interacting colloids and supramolecular aggregates in solution, ed. S.-H. Chen, J. S. Huang and P. Tartaglia, Kluwer Academic Publishers, Dordrecht, 1992, p. 731.
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Pine, D.J.4
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17
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85034329736
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Part of the water has in fact been replaced by heavy water to adjust the neutron scattering length for subsequent SANS measurements (data not shown in this paper)
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Part of the water has in fact been replaced by heavy water to adjust the neutron scattering length for subsequent SANS measurements (data not shown in this paper).
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22
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0003944941
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P. Lindner and T. Zemb, Amsterdam, North-Holland
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J. P. Cotton, in Initial data treatment, in Neutron, X-Ray and Light Scattering: Introduction to an Investigative Tool for Colloidal and Polymeric Systems, ed. P. Lindner and T. Zemb, Amsterdam, North-Holland, 1989, p. 19–31.
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Cotton, J.P.1
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25
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85034362407
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The smearing induced by the instrumental setup has been included in the data analysis for the hard-sphere like suspensions. The ideal model scattering curves were smeared by the appropriate resolution function when the model scattering intensity was compared to the measured one.26,27 The parameters in the models were optimized by conventional least-squares analysis, and the errors of the parameters were calculated by conventional methods.28 For the gel analysis (I(q) is a slowly and monotonic decaying functions) the smearing induced by the instrumental setup is negligible and has therefore not been taken into account
-
The smearing induced by the instrumental setup has been included in the data analysis for the hard-sphere like suspensions. The ideal model scattering curves were smeared by the appropriate resolution function when the model scattering intensity was compared to the measured one.26,27 The parameters in the models were optimized by conventional least-squares analysis, and the errors of the parameters were calculated by conventional methods.28 For the gel analysis (I(q) is a slowly and monotonic decaying functions) the smearing induced by the instrumental setup is negligible and has therefore not been taken into account.
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37
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85034366786
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Here P(q) denotes the Mie scattering function of a single particle while the (different) SANS particle form factor, introduced in section IV, is called F(q)
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Here P(q) denotes the Mie scattering function of a single particle while the (different) SANS particle form factor, introduced in section IV, is called F(q).
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63
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85056019002
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M. R. Eskildsen K. Harada P. L. Gammel A. B. Abrahamsen N. H. Andersen G. Ernst A. P. Ramirez D. J. Bishop K. Mortensen D. G. Naugle K. D. D. Rathnayaka P. C. Canfield Nature 1998 391 563.
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Ernst, G.6
Ramirez, A.P.7
Bishop, D.J.8
Mortensen, K.9
Naugle, D.G.10
Rathnayaka, K.D.D.11
Canfield, P.C.12
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73
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85034311117
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3 weighing in the averaging integral (see also eqn. (18))14,64
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3 weighing in the averaging integral (see also eqn. (18))14,64.
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74
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0004070288
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P. Sheng, World Scientific, Singapore
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D. J. Pine, D. A. Weitz, G. Maret, P. E. Wolf, E. Herbolzheimer and P. M. Chaikin, in Scattering and localization of classical waves in random media, ed. P. Sheng, World Scientific, Singapore, 1990.
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Chaikin, P.M.6
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