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Advances in Spectroscopy for Lasers and Sensing by Baldassare Di Bartolo, Ottavio Forte

By Baldassare Di Bartolo, Ottavio Forte

This quantity offers the court cases of "New improvement in Optics and similar Fields," held in Italy in June, 2005. This assembly used to be geared up by way of the overseas college of Atomic and Molecular Spectroscopy of the "Ettore Majorana" middle for medical tradition. the aim of this Institute was once to supply a entire and coherent remedy of the hot suggestions and modern advancements in optics and comparable fields.

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Hornberger, K. and Sipe, J. E. (2003), Phys. Rev. A 68, 012105. Spohn, H. (1980), Rev. Mod. Phys. 53, 569. Kimura, G et al. (2001), Phys. Rev. A 63, 022103. Gerthsen, D. private communication. (a) Kalt, H. [1](e); (b) Lyssenko, V. Coh. Spectr. of SC Nanostruct. [1](e). (a) Tsitsishvili, E. et al. (2002), Phys. Rev. B 66, 161405(R); (b) Tsitsishvili, E. et al. (2003), Phys. Rev. B 67, 205330. Paillard, M. et al. (2001), Phys. Rev. Lett. 86, 1634. Flissikowski, T. et al. (2001), Phys. Rev. Lett. 86, 3172.

Advances in Spectroscopy for Lasers and Sensing, 63–72. © 2006 Springer. Printed in the Netherlands. 64 Norman P. Barnes Several spectroscopic techniques are available for the detection of threats. Perhaps the most straight forward technique is a measurement of the transmission of a probe beam tuned to an absorption feature of the species to be detected. A diminution in transmission is interpreted as the presence of the threat. Effects associated with the absorption of the probe beam, such as an increase in the temperature, can also be used.

Solid lines: Caldeira–Leggett model with a Drude form, dashed lines: Drude–model, dashed dotted lines: Rubin model. (Dimensionless quantities, M0 /M = 1). Lower panel: Real and imaginary parts of the electrical conductivity σ ∝ χ. 0 1 2 3 4 For a finite number of reservoire oscillators the total system will always return to its initial state after a finite (Poincar´ ´e) recurrence time or may ´e time become arbitrarily close to it. For N → ∞, however, the Poincar´ comes infinite, simulating dissipative behavior.

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