Dirac equation
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1: 33.22 Particle Scattering and Atomic and Molecular Spectra
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§33.22(iv) Klein–Gordon and Dirac Equations
… ►The motion of a relativistic electron in a Coulomb field, which arises in the theory of the electronic structure of heavy elements (Johnson (2007)), is described by a Dirac equation. …2: 18.39 Applications in the Physical Sciences
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►Bound state solutions to the relativistic Dirac Equation, for this same problem of a single electron attracted by a nucleus with protons, involve Laguerre polynomials of fractional index.
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3: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
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►of the Dirac delta distribution.
Equation (1.18.19) is often called the completeness relation.
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►Applying the representation (1.17.13), now symmetrized as in (1.17.14), as ,
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►These latter results also correspond to use of the as defined in (1.17.12_1) and (1.17.12_2).
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►Thus, and this is a case where is not continuous, if , , there will be an eigenfunction localized in the vicinity of , with a negative eigenvalue, thus disjoint from the continuous spectrum on .
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4: 1.17 Integral and Series Representations of the Dirac Delta
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►Equations (1.17.12_1) through (1.17.16) may re-interpreted as spectral representations of completeness relations, expressed in terms of Dirac delta distributions, as discussed in §1.18(v), and §1.18(vi) Further mathematical underpinnings are referenced in §1.17(iv).
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5: Mathematical Introduction
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►These include, for example, multivalued functions of complex variables, for which new definitions of branch points and principal values are supplied (§§1.10(vi), 4.2(i)); the Dirac delta (or delta function), which is introduced in a more readily comprehensible way for mathematicians (§1.17); numerically satisfactory solutions of differential and difference equations (§§2.7(iv), 2.9(i)); and numerical analysis for complex variables (Chapter 3).
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6: 1.16 Distributions
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§1.16(iii) Dirac Delta Distribution
… ►The Dirac delta distribution is singular. … ►As distributions, the last equation reads … ►
1.16.40
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►Since the quantity on the extreme right of (1.16.41) is equal to , as distributions, the result in this equation can be stated as
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7: Bibliography T
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Uniform asymptotic approximation of Fermi-Dirac integrals.
J. Comput. Appl. Math. 31 (3), pp. 383–387.
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Rotating black holes: Separable wave equations for gravitational and electromagnetic perturbations.
Phys. Rev. Lett. 29 (16), pp. 1114–1118.
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High Speed Numerical Integration of Fermi Dirac Integrals.
Master’s Thesis, Naval Postgraduate School, Monterey, CA.
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Eigenfunction Expansions Associated with Second Order Differential Equations, Part 2, Partial Differential Equations.
Clarendon Press, Oxford.
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Rational Chebyshev approximation for the Fermi-Dirac integral
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Solid–State Electronics 41 (5), pp. 771–773.
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8: 2.6 Distributional Methods
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►To each function in this equation, we shall assign a tempered
distribution (i.
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►The Dirac delta distribution in (2.6.17) is given by
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►To derive the asymptotic expansion of , we recall equations (2.6.17) and (2.6.20).
…These equations again hold only in the sense of distributions.
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►For rigorous derivations of these results and also order estimates for , see Wong (1979) and Wong (1989, Chapter 6).
9: Software Index
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25.21(vii) Fermi–Dirac, Bose–Einstein | ✓ | ✓ | ✓ | ✓ | |||||||||||||||||||||
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28 Mathieu Functions and Hill’s Equation | |||||||||||||||||||||||||
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10: Bibliography L
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Some differential equations and associated integral equations.
Quart. J. Math. (Oxford) 5, pp. 81–97.
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Solutions to a generalized spheroidal wave equation: Teukolsky’s equations in general relativity, and the two-center problem in molecular quantum mechanics.
J. Math. Phys. 27 (5), pp. 1238–1265.
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Integral and series representations of the Dirac delta function.
Commun. Pure Appl. Anal. 7 (2), pp. 229–247.
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Well-posedness and blow-up solutions for an integrable nonlinearly dispersive model wave equation.
J. Differential Equations 162 (1), pp. 27–63.
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The second Painlevé equation.
Differ. Uravn. 7 (6), pp. 1124–1125 (Russian).
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