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Simplified quantum oscillator solution American Journal of Physics, 69( 10): 1082-1083, October 2001 338 H Kaiser, E A George, and S A Werner Neutron interferometric search for quaternions in quantum mechanics Physical Review A, 29(4):2276-2279, April 1984 339 F Kanai On the quantization of the dissipative systems Progress in Theoretical Physics, 3:440-442, 1948 340 I Karatzas and S E Shreve Brownian Motion and Stochastic Calculus, volume 113 of Graduate Texts in Mathematics Springer-Verlag, Berlin, 2nd edition, 1997 341 A P Kazantsev and G I Surdutovich The quantum theory ofthe laser Progress in Quantum Electronics, 3(3):231-288,1974 342 O Keller Propagator picture of the spatial confinement of quantized light emitted from an atom Physical Review A, 58(5):3407-3425, November 1998 343 O Keller Attached and radiated electromagnetic fields of an electric point dipole Journal of the Optical Society of America B, 16(5):835-847, May 1999 344 O Keller.



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Xw 1 1 f Xn 2-133

Relation between spatial confinement of light and optical tunneling Physical Review A, 60(2): 1652-1671, August 1999 345 O Keller Near-field optics: The nightmare of the photon Journal of Chemical Physics, 112(18):7856-7863, May 8, 2000..





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in the limit of p r 1. The weight distribution (Eq. 2-131) is shown in Fig. 2-14 for several values of f . The extents of reaction have been adjusted to maintain a constant number-average degree of polymerization of 80 in all four cases. The size distribution becomes progressively narrower with increasing functionality of Af. This is also evident from Eq. 2-133, where X w =X n decreases from 2 for f 1 to 1.25 for f 4 (at p 1). Linear polymers are formed for f values of 1 or 2, while branched polymers are formed when f is greater than 2. The case of f 1 corresponds to the type 3 polymerization discussed in Sec. 2-6. The distribution is the exact same as the most probable distribution for linear polymerization (Sec. 2-7). Linear polymerization with f 2 is of interest in that the distribution is narrower than that for the usual linear polymerization. The linking of two statistically independent A type polymer chains into one B polymer molecule via an A molecule leads to a signi cantly narrower distribution that in A the usual polymerizations of the A or A plus B types. B A B

2-10

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346. O. Keller. Space-time description of photon emission from an atom. Physical Review A, 62(2):022111, August 2000. Keller takes the view that to fully understand the problem of photon localization we must consider the interaction with matter. See also [342]. 347. O. Keller. Optical tunneling: A fingerprint of the lack of photon localizability. Journal of the Optical Society of America B, 18(2):206-217, February 2001. 348. O. Keller. Nonlinear optics in the near-field zone of atoms. Journal ofNonlinear Optical Physics and Materials, 11(3):275-301,2002. 349. O. Keller. Polychromatic photons: Wave mechanics and spatial localization. In S. G. Pandalai, editor, Recent Research Developments in Optics, volume 2, part II, pp. 375-409. Research Signposf, Kerala, India, 2002. 350. O. Keller. Near-field optics and quantum optics: An assignation arranged by four kinds of photons. Journal of Microscopy, 209(3):272-276, March 2003. 351. E. H. Kennard. Zur Quantenmechanik einfacher Bewegungstypen. Zeitschrift for Physik, 44:326-352,1927.

Polymerization of the A plus Af system (with f > 2) in the presence of B will lead not B B only to branching but also to a crosslinked polymer structure. Branches from one polymer molecule will be capable of reacting with those of another polymer molecule because of the presence of the B reactant. Crosslinking can be pictured as leading to structure XVII, in B

352. O. Kenneth, I. Klich, A. Mann, and M. Revzen. Repulsive Casimir forces. Physical Review Leuers, 89(3):33001, July 15,2002. 353. O. Kenneth, I. Klich, A. Mann, and M. Revzen. Reply to comment on "Repulsive Casimir forces." Physical Review Leuers, 91(2):029102, July 11,2003. 354. A. M. Khazanov, G. A. Koganov, and E. P. Gordov. Macroscopic squeezing in three-level laser. Physical Review A, 42(5):3065-3069, September 1, 1990. 355. S. Ya. Kilin and T. B. Karlovich. Single-atom laser: Coherent and nonclassical effects in the regime of a strong atom-field correlation. Journal of Experimental and Theoretical Physics, 95(5):805-819, November 2002. 356. H. J. Kimble. Comment on "Deterministic single-photon source fordistrlbuted quantum networking." Physical Review Leuers, 90(24):249801, June 20,2003. 357. R. P. Kirshner. Throwing light on dark energy. Science, 300: 1914-1918, June 20,2003. 358. P. E. Kloeden and E. Platen. Numerical Solution ofStochastic Differential Equations, volume 23 of Applications of Mathematics: Stochastic Modelling and Applied Probability. Springer-Verlag, Berlin, 3rd edition, 1999. 359. P. L. Knight and L. Allen. Concepts of Quantum Optics. Pergamon Press, Oxford, 1983. 360. P. L. Knight and P. W. Milonni. Long-time deviations from exponential decay in atomic spontaneous emission theory. Physics Letters A, 56(4):275-278, April 5,1976.

which two polymer chains have been joined together (crosslinked) by a branch. The branch joining the two chains is referred to as a crosslink. A crosslink can be formed whenever there

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