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1See, e.g., S. W. Hawking and G. F. R. Ellis, Large Scale Structure of Spacetime (Cambridge U.P., New York, 1973); J. D. Birrell and P. C. W. Davies, Quantum Fields in Curved Spacetime (Cambridge U.P., New York, 1982).
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1See, e.g., S. W. Hawking and G. F. R. Ellis, Large Scale Structure of Spacetime (Cambridge U.P., New York, 1973); J. D. Birrell and P. C. W. Davies, Quantum Fields in Curved Spacetime (Cambridge U.P., New York, 1982).
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6See, e.g., B. R. Holstein, Topics in Advanced Quantum Mechanics (Addison-Wesley, Reading, MA, 1992), Chap. 8.
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course, if there exist any zero or negative eigenvalues, things must be handled more carefully - cf. S. Coleman, "Secret Symmetry: An Introduction to Spontaneous Symmetry Breakdown and Gauge Fields," in Aspects of Symmetry (Cambridge U.P., New York, 1985).
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Note that we have denoted the transverse directions x,y collectively by the symbol ⊥.
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Addison-Wesley, Reading, MA, Chap. III.6
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A careful reader will note that the imaginary component of ζ, which corresponds to a shift in the energy per unit volume due to quantum effects, diverges. This is simply the well-known vacuum energy contribution, which is removed by renormalization of the energy zero point - cf. B. R. Holstein, Topics in Advanced Quantum Mechanics (Addison-Wesley, Reading, MA, 1992), Chap. III.6.
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Holstein, B.R.1
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Die reflexion von elektronen an eimem potentialsprung nach der relativistischen dynamik von dirac
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Here the translation is by V. Telegdi in unpublished lecture notes (1995)
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Klein, "Die Reflexion von Elektronen an eimem Potentialsprung nach der Relativistischen Dynamik von Dirac," Z. Phys. 53, 157-165 (1929). Here the translation is by V. Telegdi in unpublished lecture notes (1995).
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M. G. Fuda and E. Furlani, "Zitterbewegung and the Klein Paradox for Spin-Zero Particles," Am. J. Phys. 50, 545-549 (1982).
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Fuda, M.G.1
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Pair production by a constant electric field
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A. I. Nishikov, "Pair Production by a Constant Electric Field," Sov. Phys. JETP 30, 660-662 (1969); "Barrier Scattering in Field Theory Removal of Klein Paradox," Nucl. Phys. B 21, 346-358 (1970).
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A. I. Nishikov, "Pair Production by a Constant Electric Field," Sov. Phys. JETP 30, 660-662 (1969); "Barrier Scattering in Field Theory Removal of Klein Paradox," Nucl. Phys. B 21, 346-358 (1970).
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19
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85033956870
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note
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0 is varied.
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20
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85033969523
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note
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0. (114)
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21
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0003553982
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See, e.g., J. F. Donoghue, E. Golowich, and B. R. Holstein, Dynamics of the Standard Model (Cambridge U.P., New York, 1992).
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85033964688
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note
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Since spin does not enter into the transmission or reflection probability, this replacement is merely a trick which removes the spin degrees of freedom from the problem.
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23
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Positron production in multiphoton light by light scattering
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D. L. Burke et al., "Positron Production in Multiphoton Light by Light Scattering," Phys. Rev. Lett. 79, 1626-1629 (1997).
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P. C. W. Davies, "Scalar Particle Production in Schwartzchild and Rindler Metrics," J. Phys. A 8, 609-616 (1975); W. G. Unruh, "Notes on Black Hole Evaporation," Phys. Rev. D 14, 870-892 (1976).
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Davies, P.C.W.1
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Notes on black hole evaporation
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P. C. W. Davies, "Scalar Particle Production in Schwartzchild and Rindler Metrics," J. Phys. A 8, 609-616 (1975); W. G. Unruh, "Notes on Black Hole Evaporation," Phys. Rev. D 14, 870-892 (1976).
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Unruh, W.G.1
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S. W. Hawking, "Particle Creation by Black Holes." Commun. Math. Phys. 43, 199-220 (1975); P. C. W. Davies, "Quantum Field Theory in Curved Spacetime," Nature (London) 263, 377-380 (1976).
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Nature (London)
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S. W. Hawking, "Particle Creation by Black Holes." Commun. Math. Phys. 43, 199-220 (1975); P. C. W. Davies, "Quantum Field Theory in Curved Spacetime," Nature (London) 263, 377-380 (1976).
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