Unidirectional saturation spectroscopy, II

1. M.SargentIII, P.E.Toschek, H.-G.Danielmeyer: Appl. Phys11, 55 (1976)10.1007/BF00895016 ↗

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7. An equation reference like (I. 11) refers to Eq. (11) of Ref. 1

8. The population differenceD is traditionally taken to decay at the rate −D/T 1 to its equilibrium valueD eq in the absence of the applied field interaction contribution (represented by $$\dot D_v $$ ), that is, $$\dot D = - (D - D_eq )/T_1 + \dot D_v $$ . An upper level populationN a decaying with the rateγ a N a to a non-decaying ground lower levelb causes the populationN b to correspondingly increase at the same rate. Hence the population differenceD=N a −N b decays at double that rate, namely $$\dot D = - 2\gamma _a N_a + \dot D_v = - \gamma _a (D + N) + \dot D_v $$ , whereN=N a +N b . This givesT 1=1/γ a } andD eq=−N

9. M.Sargent III: “Relaxation of Hot Holes in p-Ge”, to be published

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11. T.Hänsch, P.E.Toschek: IEEE J. Quant. Electr. QE-4, 530 (1968).10.1109/JQE.1968.1075383 ↗

12. Gain has also been predicted with completely modulated light: see S.Feneuille, M.-G.Schweighofer, G.Oliver: J. Phys., to be published

13. M.SargentIII, M.O.Scully, W.E.Lamb,Jr.:Laser Physics (Addison-Wesley Publ. Co., Reading, Mass 1974) Chap. 9

14. M.SargentIII: InApplications of Lasers to Atomic and Molecular Physics, Proc. Les Houches Summer School, Ed. by R. Balian and S. Haroche (North-Holland Publ. Co., Amsterdam 1976)

15. P.E.Toschek: In——, Proc. Les Houches Summer School, Ed. by R. Balian and S. Haroche (North-Holland Publ. Co., Amsterdam 1976) Les Houches lectures, pp. cit., [14]

16. C.Cohen-Tannoudji: 1968Cargèse Lectures in Physics 2, Ed. M.Lévy (Gordon and Breach, New York)

17. S.Haroche: Ann. Phys. Paris6, 189 (1971). See also K.Kolwas, M.Kolwas: Opt. Comm.17, 149 (1976) for a treatment involving AM modulated light10.1051/anphys/197114060189 ↗

18. S.Feneuille: J. Phys. B7, 1981 (1974), esp. Fig. 110.1088/0022-3700/7/15/006 ↗

19. P.Pringsheim:Fluorescence and Phosphorescence, (Interscience Publishers, New York 1949)

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21. For Δn 2>2, two interactions of the saturator light must take place consecutively, thus contributing only to ordinary saturation

22. L.S.Vasilenko, V.P.Chebotayev, A.V.Shishayev: Sov. Phys. JETP Lett.12, 161 (1970)

23. B.Cagnac, G.Grynberg, F.Biraben: J. de Physique34, 845 (1973)10.1051/jphys:019730034010084500 ↗

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27. J.B.Feldman, M.S.Feld: Phys. Rev. A12, 1013 (1975)10.1103/PhysRevA.12.1013 ↗

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31. M.SargentIII, W.E.Lamb,Jr., R.L.Fork: Phys. Rev.164, 450 (1967)10.1103/PhysRev.164.450 ↗

32. B.Decomps, M.Dumont: Compt. Rend. B265, 249 (1967)

33. M.SargentIII: Phys. Rev. A14, 524 (1976)10.1103/PhysRevA.14.524 ↗

34. See, e.g., G.W.Series: InQuantum Optics, Proc. Scottish Universities Summer School in Physics, 1969, Ed. by S.M.Kay and A.Maitland (Academic Press, New York 1970) p. 395

35. W.Hanle: Z. Physik30, 93 (1924)10.1007/BF01331827 ↗

36. G.W.Series: Proc. Phys. Soc.89, 1017 (1966)10.1088/0370-1328/89/4/325 ↗

37. W.Heitler:The Quantum Theory of Radiation (Oxford University Press, London 1954)

38. A.Smekal: Z. Physik34, 81 (1925)10.1007/BF01328457 ↗

39. This point in the context of saturation spectroscopy was called to our attention by Paul Liao. An outline of the diagonalization procedure was given in C.Cohen-Tannoudji, B.Diu, F.Laloë:Méchanique quantique, ComplémentF IV, Sec. 2b (Hermann, Paris 1973)

40. B.R.Mollow: Phys. Rev.188, 1969 (1969)10.1103/PhysRev.188.1969 ↗

41. C.Cohen-Tannoudji: InLaser Spectroscopy, Proc. 2nd Intern. Laser Spectroscopy Conf., Megève, France, 1975 (Springer, Berlin, Heidelberg, New York 1975) p. 32410.1007/3-540-07411-2_284 ↗