Titlebook: An Introduction to Laser Spectroscopy; Second Edition David L. Andrews,Andrey A. Demidov Book 2002Latest edition Springer Science+Business

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Traumdeutung und Traumdichtung,the Bohr condition .where . is Planck‘s constant, 6.626 × 10. J s. If an atom in the lower energy state |1〉 absorbs a photon of frequency . it may be excited to the upper state |2〉. This process is termed . or, more generally, simply absorption. The probability per second that an atom will absorb a

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,Versuchsanordnung und -durchführung,e material under investigation. The technique provides, amongst other things, important information about the vibrational state of matter. One of the most influential early investigations into light scattering was undertaken by Lord Rayleigh (1899). In this study it was shown that the intensity of e

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Alveoli

https://doi.org/10.1007/978-3-642-90697-8troscopy was mainly a research tool in biochemistry and biophysics. Today, we see fluorescence being used to determine the DNA sequence of genomes, discover new drugs at unprecedented speed by high throughput screening (HTS) and simultaneously watch thousands of genes turn on and off using DNA array

Cpap155

https://doi.org/10.1007/978-3-642-90697-8polarisation measurements to determine both the order and full angular motion of probe molecules in an anisotropic medium. The study of ordered molecular systems is an area of wide scientific interest; the presence of order can have a profound influence on intrinsic optical (Tompkin ., 1990) and pho

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Die Tuberkulose der Wirbelsäuleor frequency conversion are then discussed, followed by a survey of other more adventurous and more recent applications in surface science. To begin, we consider the conceptual heritage of the subject area.

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,Die Tuberkulose und ihre Bekämpfung,guided the progress in the study of dynamic processes and has been the catalyst in attempts to produce ever-shorter probes. In many instances, the timescale associated with transition phenomena can be of the order of the period of optical radiation - for 500 nm, the period is 1.7 fs (1 fs = 10.s). M