Quantum Mechanics of One- and Two-Electron Atoms

This classic of modern physics includes a vast array of approximation methods, mathematical tricks, and physical pictures useful in applying quantum mechanics to other fields. Students and professionals will find it an essential reference for calculations pertaining to hydrogen- and helium-like atoms and their comparison with experimental results. 1977 edition.
1009048108
Quantum Mechanics of One- and Two-Electron Atoms

This classic of modern physics includes a vast array of approximation methods, mathematical tricks, and physical pictures useful in applying quantum mechanics to other fields. Students and professionals will find it an essential reference for calculations pertaining to hydrogen- and helium-like atoms and their comparison with experimental results. 1977 edition.
119.99 In Stock
Quantum Mechanics of One- and Two-Electron Atoms

Quantum Mechanics of One- and Two-Electron Atoms

Quantum Mechanics of One- and Two-Electron Atoms

Quantum Mechanics of One- and Two-Electron Atoms

Paperback(Softcover reprint of the original 1st ed. 1977)

$119.99 
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Overview


This classic of modern physics includes a vast array of approximation methods, mathematical tricks, and physical pictures useful in applying quantum mechanics to other fields. Students and professionals will find it an essential reference for calculations pertaining to hydrogen- and helium-like atoms and their comparison with experimental results. 1977 edition.

Product Details

ISBN-13: 9780306200229
Publisher: Springer US
Publication date: 04/30/1977
Edition description: Softcover reprint of the original 1st ed. 1977
Pages: 370
Product dimensions: 5.98(w) x 9.02(h) x 0.03(d)

About the Author




The late Hans A. Bethe, a Nobel Laureate, was Professor of Physics at Cornell University. Edwin E. Salpeter is James Gilbert White Distinguished Professor of the Physical Sciences at Cornell University.

Table of Contents

Units.- I. The Hydrogen Atom Without External Fields.- a) Nonrelativistic theory.- 1. Separation of Schrödinger’s equation in spherical polar coordinates. Angularly dependent eigenfunctions and the angular momentum matrix.- 2. Derivation of Balmer’s formula.- 3. The radial eigenfunctions of the discrete spectrum.- 4. The eigenfunctions of the continuous spectrum.- 5. Motion of the nucleus.- 6. Separation of Schrödinger’s equation in parabolic coordinates.- 7. Methods for the continuous spectrum for a general central potential.- 8. Wave functions in momentum space. Discrete spectrum.- 9. Wave functions in momentum space. Continuous spectrum.- b) Dirac theory.- 10. General properties of the Dirac theory.- 11. Angular momentum.- 12. Pauli theory of the spin-electron.- 13. Pauli theory for a central potential.- 14. The exact solution of the Dirac equation.- 15. Dirac equation. Continuous spectrum.- 16. The Dirac equation in momentum space.- 17. The fine structure formula.- c) Radiative and other corrections.- 18. Radiative corrections. S-matrix theory.- 19. Radiative corrections. Bound states.- 20. Corrections for nuclear motion and structure.- 21. Fine structure and the Lamb shift.- 22. Hyperfine structure splitting.- 23. The fine structure of positronium.- II. The Helium Atom without External Fields.- a) Nonrelativistic theory.- 24. The Schrödinger equation for helium (symmetry).- 25. Discussion of variation and perturbation methods.- 26. Level scheme of helium.- 27. Survey of approximations to be used.- 28. First order Heisenberg’s method (excited states).- 29. Polarization for excited states.- 30. Fock’s method (excited S-states).- 31. Hartree’s method.- 32. Ritz variation method (helium ground state).- 33. Ground state of helium-like ions with arbitrary Z.- 34. The negative hydrogen ion.- 35. Variation method for excited states.- 36. Miscellaneous calculations I.- 37. Motion of the nucleus.- b) Relativistic theory.- 38. Discussion of the Breit equation.- 39. The Pauli approximation (low Z).- 40. Fine structure splitting of helium.- 41. Relativistc corrections for the ground state.- 42. Breit equation without external field.- 43. Treatment for large Z.- 44. Hyperfine structure.- III. Atoms in External Fields.- a) Zeeman effect.- 45. Zeeman effect for a single-electron atom.- 46. Dependence on magnetic field strength.- 47. Some corrections to the Zeeman effect.- 48. Extension to many-electron atoms.- 49. Comparison with precision experiments.- 50. The diamagnetism of helium.- b) Stark effect in hydrogen.- 51. Linear Stark effect.- 52. The quadratic Stark effect.- 53. Stark effect for strong fields.- 54. Ionization by the electric field. Quenching of the lines in the Stark effect.- 55. Stark effect of the fine structure of hydrogen.- c) Stark effect in helium.- 56. The Stark effect for weak fields.- 57. Dependence on field strength.- 58. The dielectric constant of helium.- IV. Interaction with Radiation.- a) Discrete spectrum.- 59. General formulas.- 60. Selection rules for orbital and magnetic quantum numbers.- 61. Sum rules.- 62. Proof of the sum rules.- 63. The transition probabilities for hydrogen in polar coordinates.- 64. Intensity of fine structure lines.- 65. Intensities in parabolic coordinates (Stark effect).- 66. Higher multipole radiation.- 67. Lifetimes of excited states in hydrogen.- 68. Alkali and X-ray spectra.- b) The photoeffect.- 69. General survey.- 70. The Born approximation.- 71. The absorption coefficient without retardation.- 72. Angular distribution and retardation.- 73. Relativistic effects.- 74. The optical region.- 75. Recombination.- c) Bremsstrahlung.- 76. General survey.- 77. Nonrelativistic Born approximation.- 78. Calculations for low energies.- 79. Relativistic effects.- Appendix on spherical harmonics.- Addenda and errata.- Further addenda and errata.- Author index.- Index of Tables.

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