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Band Theory and the Hall Effect in Organic Crystals
1.O. H. LeBlanc, Jr., J. Chem. Phys. 35, 1275 (1961).
2.G. D. Thaxton, R. C. Jarnagin, and M. Silver, J. Phys. Chem. 66, 2461 (1962).
3.J. L. Katz, S. A. Rice, S. Choi, and J. Jortner, J. Chem. Phys. (to be published).
4.R. G. Kepler, Phys. Rev. 119, 1226 (1960);
4.Organic Semiconductor Conference, edited by J. J. Brophy (The MacMillan Company, New York, 1962).
5.M. Silver, J. R. Rho, and R. C. Jarnagin, J. Chem. Phys. 38, 3030 (1963).
6.The magnitude anomaly is also derived by L. Friedman, Ph.D. Thesis, Pittsburg, 1961, and L. Friedman and T. Holstein, Ann. Phys. 21, 494 (1963).
7.From, e.g., Eq. 235 in A. H. Wilson, The Theory of Metals (Cambridge University Press, Cambridge, England, 1936), p. 163, by assuming Boltzmann statistics and eliminating all terms in by partial integration.
8.The signs of the hole terms given here are opposite to those of Thaxton because in using Boltzmann statistics one must measure the hole energy down from the top of the band, whereas Thaxton’s energies are measured upwards from the bottom of the band.
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