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Although a cavity mode is equivalent to a harmonic oscillator as an LG circuit is, a cavity has many modes How can we make sure that the photons will go all (or at least mostly) to a single mode Conservation of energy will provide selectivity by allowing emission only in the mode that lies within the linewidth of the atomic or molecular transition But how can this radiation generated by many independent atomic/molecular emissions be as coherent as that of a radio transmitter, which is generated by a single-dipole antenna It was Einstein who in 1905 discovered that excited atoms or molecules can emit light in two qualitatively different ways: spontaneous and stimulated emission In spontaneous emission, the photon is emitted randomly without particular preference for any mode (see 6).

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Direct investment in biotech from private investors has been relatively low since the boom in 2000 However, indirect investment in biotech, in the form of insurance premiums and in retirement funds, is signi cant Venture capital is relatively scarce for startups in the industry, but the prospects of funding are good for established companies seeking later stage funding Given that biotech rms are increasingly challenged to secure nanc ing, strategic alliances between domestic and foreign companies, between academic institutions and industry, and among domestic companies is in creasingly signi cant The Institute for Quantitative Biomedical Research (QB3) in the San Francisco Bay area is an example of a government-funded alliance between academia and industry Biotech Industries Although the state of nancing in the US.

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In stimulated emission, however, the photon is preferentially emitted into a mode that is already occupied by other photon(s), preserving the coherence of the radiation field Stimulated emission is a consequence of photons being bosons, as we shall see briefly next Emission of photons into a given mode k is represented by the term proportional to al in the coupling part of the Hamiltonian, as discussed in 5 A simple Fermi golden rule argument then shows that the probability of emission into a given mode k is proportional to 10,11'1/1)1 2 We can rewrite lall'l/l)12 as Nlakall'l/l) Using the commutator between ak and al, [ak, all = 1, which is a consequence of the photon being a boson, we find that lall'l/lW = 1 + nb where nk = ('I/Ilnkl'l/l) is the average number of photons in mode k Thus, the probability of emission into a mode that is.

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28 Jul 2016 ... Add, Edit Metadata of PDF Document using iText in Java ... package com. memorynotfound. pdf . itext ; import com. itextpdf . text .Document; import ...

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When any list is displayed, you can click the list button to open its menu and add new entries. Simply follow these steps: 1. Display the list to which you want to add an entry by selecting it from the Lists menu or by accessing it from the appropriate Navigator screen. The list you have selected to open appears on your screen.

already filled with nk photons on average is 1 + nk greater than that of emitting into an unpopulated mode. 4 With these ideas, we are already in a position to write down a "back of the envelope" description of a laser. In this "hand-waving" description, we will regard the various quantum-mechanical observables as if they were classical. Laser cavities are usually open, so some of the photons emitted can actually go into free space. Let us call (3 the fraction of emission into the lasing mode. Then if we call n the number of photons in the lasing mode, N the population of the upper lasing level, and I'll the decay rate of the upper lasing level to the lower lasing level, the rate at which stimulated emission photons will increase the population of the lasing mode is5 f3'YIiNn. Cavity damping will tend to decrease this population at a rate of -Kn, where K- 1 is the photon lifetime in the lasing mode. Absorption of photons by the population in the lower lasing level (making then a transition to the upper level) will also tend to decrease n. But if the lower lasing level is rapidly emptied into lower-lying levels that do not tak~: part in the laser, there will be no absorption. For simplicity, let us assume that this is the case. Then it is only the population N of the upper lasing level that appears in the laser equations. Last but not least, there is the spontaneous emission contribution to the population of the lasing mode, R"p = f3'YIiN. Putting all this together, we have

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24 May 2014 ... This tutorial explains to create underlined or striked-through text in a PDF in Java using IText .

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