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Two-photon emission

Two-photon emission is a process in which electronic transition between quantum levels occurs through the simultaneous emission of two photons. [27] presents more details about two-photon emission. Since metal clusters emit in the near-infrared region, they can be made useful for two-photon imaging with infrared excitation. Two-photon emission of Au25 clusters is observed at 830 nm by exciting at... [Pg.347]

Fig. 8 Optical absorption of An., and two-photon emission spectrum after excitation at 1,290 nm for Au25 clusters [23]... Fig. 8 Optical absorption of An., and two-photon emission spectrum after excitation at 1,290 nm for Au25 clusters [23]...
Figure 6.19. Relaxation rate tor Raman transitions (R) and two-photon emission (T) in a two-level system as a function of temperature. The value of asymmetry is 0, 4, and 32 cm 1 as indicated. The tunneling matrix element is 0.25 cm 1 and the Debye frequency is 80 cm 1. (From Silbey and Trommsdorf [1990].)... Figure 6.19. Relaxation rate tor Raman transitions (R) and two-photon emission (T) in a two-level system as a function of temperature. The value of asymmetry is 0, 4, and 32 cm 1 as indicated. The tunneling matrix element is 0.25 cm 1 and the Debye frequency is 80 cm 1. (From Silbey and Trommsdorf [1990].)...
Two-photon emission has been reported for (4/ ) in YF s (32,33] with a quantum efficiency of about 145%. The energy level scheme is given in Pig. 6.23. The Pr ion decays in two steps as indicated. The So level is at 46500 cm, and the H4 So transition parity forbidden. Excitation in a lamp has to occur in the 4/ configuration of Pr " which is above the So level. Therefore the low-pre.ssure mercury dischaige cannot be applied and another solution has to be found. [Pg.130]

Although two-photon emission would greatly enhance the efficiency of luminescent lamps, this concept has, up till now, found no practical realisation for lack of suitable materials and ultraviolet sources. [Pg.130]

Until now, downconversion based on the four concepts mentioned previously has been demonstrated. The first example was demonstrated in single Pr -doped phosphor. In this case, it requires the So level of Pr to be located below its lowest AfSd state. When Pr is pumped to its Sq level, two-photon emission is completed by two subsequent emissions of 405 nm for the Sq transition followed by radiation of 480 nm for the Pq H4 transition or of 610 nm for the Pq transition as shown Fig. 16.8. Until now, cascade emission from Pr has been found in a number of fluoride hosts [11-20] such as SrAlFs [11, 12], LnF(Ln = Y, La, Lu) [13-16], BaMgp4 [15], AYp4(A = Na, K) [13, 17], AMgF3(A = Na, K) [18, 19], and LiSrAIFe [20]. Figure 16.9 shows the emission spectrum of single... [Pg.515]

Fig. 16.8 Schematic energy-level diagram of ion, showing the concept of the two photon emission process under excitaion of one VUV photon. Reprinted from Ref. [10], Copyright 2010, with permission from Elsevier... Fig. 16.8 Schematic energy-level diagram of ion, showing the concept of the two photon emission process under excitaion of one VUV photon. Reprinted from Ref. [10], Copyright 2010, with permission from Elsevier...
While two-photon absorption spectroscopy has been widely applied for precision measurements of atomic structure, the polarization correlation of the simultaneous two-photon emission from the metastable Is state of atomic hydrogen has only been measured very recently. The emission of the coincident two photons can be described by a single state vector which determines the circular and linear two-photon polarization. Compared to the two-photon cascade experiments the polarization correlation of the simultaneous two-photon decay of metastable hydrogen is conceptually closer to the original proposals by Bell and Bohm for tests of the foundation of quantum mechanics. More than SO years have elapsed since the famous Einstein-Bohr debate on microphysical reality and quantum formalism. The present and future outcome of the hydrogen two-photon correlation experiment is considered to be a most crucial test with regard to the rivalry between quantum mechanics and local realistic theories. [Pg.537]

The selection rules for two-photon transitions are different and many dyes that have a large coefficient for one-photon absorption exhibit two-photon cross sections in the order of at most a few GM [14]. Correspondingly, a two-photon emission (excited state two photons) is observed as a weak emission, since only the total energy is conserved, not the energy of each individual photon. Thus, emission is a weak continuum of interest more of astrophysicists than of chemistry practitioners, but advancement in the field has been remarkable [15]. [Pg.190]

Ota Y, Iwamoto S, Kumagai N, Arakawa Y (2011) Spontaneous two-photon emission from a single quantum dot Phys Rev Lett 107 233602... [Pg.202]

Fig. 8.40a-d. Two-photon processes, (a) Stepwise excitation with a real in-termediate level (b) two-photon absorption, described by a virtual intermediate level (c) two-photon emission (d) Raman scattering... [Pg.438]

Spectral distribution of two-photon emission. From equation (7.14) we see that the spectral distribution is continuous and is also symmetric in and 0)2, which is to be expected since both photons are emitted simultaneously. [Pg.193]

At should be reduced by 2 and 3 per cent respectively, is clearly desirable that the decay rates of these highly-ionized atoms should be measured to an accuracy of one per cent or better. This would determine whether or not the discrepancy noted above was significant. It would also provide a more accurate check of the two-photon emission rates which so far have only been calculated using non-relativistic wavefunctions. [Pg.203]

The successful detection of two-photon emission in hy-drogenic systems prompted a more careful examination of the decay modes possible for metastable levels in two-electron atoms and ions. This has revealed further interesting features and we discuss the progress which has been made recently in the following section. [Pg.203]


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