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By Detlef A.W. Wendisch

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Phys. 30: 648 9. Ciardelli F. Salvadori P (eds) (1973) Fundamental aspects and recent developments in optical rotatory dispersion and circular dichroism, Heyden, London 10. Snatzke G (ed) (1965) Optical rotatory dispersion and circular dichroism in organic chemistry (Including applications from inorganic chemistry and biochemistry), Proceedings of NATO Summer School, Bonn/Germany 11. a) Minkin VI (1977) Dipole moments and stereochemistry of organic compounds-Selected applications. In: Kagan HB (ed) Stereochemistry: Fundamentals and methods, Georg Thieme, Stuttgart, vol 2 p 2 b) Legrand M, Rougier MJ (1977) Application of the optical activity to stereochemical determinations.

Rev. 80: 580 Yan H, Chen B, Gore JC (1987) J. Magn. Reson. 75: 83 Hasenfeld A (1987) J. Magn. Reson. 72: 509 Levitt MH, Beshah K (1987) J. Magn. Reson. 75: 222 Addendum to the equation of motion (1): As we know, analysis of some NMR experiments requires the solution of the equation of motion of the relevant density matrix. The spin operator representation of the density matrix helps to derive a concise equation for the time development of the complete density operator, given the initial state of the system.

51: 775 Tycko R, Cho HM, Schneider E, Pines A (1985) 1. Magn. Reson. 61: 90 Tycko R, Pines A, Guckenheimer 1 (1985) 1. Chern. Phys. 83: 2775 Lurie D1 (1985) Magn. Reson. Imaging 3: 235 13. Lurie D1 (1986) 1. Magn. Reson. 70: 11 14. Sanctuary BC, Cole HBR (1987) 1. Magn. Reson. 71: 106 15. Shaka A1, Pines A (1987) 1. Magn. Reson. W. Provencher [1,2]. This is a generalized program capable of solving equations such as Eq. (1). Trnax Yk= S Fk(t k, T)S(T)dT+J3+ek (1) Tmin where Yk is the input data measured at times t k, F k is a known function (the socalled kernel), J3 corresponds to a constant baseline term, and S itself is the solution to be calculated.

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