By Glenda Elizabeth Gilmore

ISBN-10: 0393348180

ISBN-13: 9780393348187

"Remarkable . . . an eye-opening booklet [on] the liberty fight that modified the South, the country, and the world." —Washington Post The civil rights move that looms over the Nineteen Fifties and Sixties was once the end of an iceberg, the felony and political remnant of a extensive, raucous, deeply American move for social justice that flourished from the Nineteen Twenties during the Forties. This wealthy heritage of that early circulate introduces us to a contentious mixture of home-grown radicals, exertions activists, newspaper editors, black staff, and intellectuals who hired each approach conceivable to take Dixie down. In a dramatic narrative Glenda Elizabeth Gilmore deftly indicates how the circulation opened up opposed to nationwide and worldwide advancements, gaining concentration and eventually arriving at a slim yet potent felony approach for securing desegregation and political rights.

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Extra resources for Defying Dixie: The Radical Roots of Civil Rights: 1919-1950

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015%). In case of 2H, Eq. 31) is reduced to DnQ ¼ (3=4)(e2 qQ=h)(3 cos2 u À 1): (2:32) This orientation-dependent splitting of peaks yields a clue on how a C2H vector of a molecule under consideration is oriented to the applied magnetic field when single crystalline, mechanically, or magnetically oriented samples are utilized. In many instances, however, most of samples are not always homogeneously oriented with respect to B0, but are randomly distributed as in microcrystalline or powder samples.

For nuclei with 2p electrons such as 13C, 15N, etc. the Brief Outline of NMR Parameters 33 relative chemical shift is predominantly governed by the paramagnetic term, and for the 1H nucleus by the first and third terms. The paramagnetic term is expressed by a function of excitation energy, bond order, and electron density according to the sum-over-state (SOS) method in the simple form as follows:    À h2 e2 4pm2e ÞS r À3 2p ðEm À En ÞÀ1 Q, (3:4) s p ¼ À m0  where Em À En is the singlet–singlet excitation energy of the nth occupied and the mth unoccupied orbitals, and  Qis a factor including the bond order and electron density.

Yamaguchi, M. Tanio, H. Konishi, S. Inoue, A. Naito, R. Needleman, J. K. Lanyi, and H. Saitoˆ, 1999, Biophys. , 76, 1523–1531. [18] S. Yamaguchi, S. Tuzi, M. Tanio, A. Naito, J. K. Lanyi, R. Needleman, and H. Saitoˆ, 2000, J. Biochem. (Tokyo), 127, 861–869. [18a] S. Tuzi, A. Naito, and H. Saitoˆ, 1993, Eur. J. , 218. 837–844. [19] K. Schmidt-Rohr and H. W. Spiess, 1994, Multidimensional Solid-state NMR and Polymers, Academic Press, London. [20] N. Bloembergen and J. A. , 1, 731–746. [21] A. Abragam, 1961, The Principles of Nuclear Magnetism, Claredon Press, Oxford.

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