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Lifetime function

Figure 6. Lifetime function f( ), defined in Eq. (3), is shown on a logarithmic scale as a function of the available energy E- Eq above threshold. Atomic time units are used (1 a.u. = 2.42 10 17 s). The numbers on the vertical axis indicate powers of 10. (Reprinted, with permission of the Royal Society of Chemistry, from Ref. 34.)... Figure 6. Lifetime function f( ), defined in Eq. (3), is shown on a logarithmic scale as a function of the available energy E- Eq above threshold. Atomic time units are used (1 a.u. = 2.42 10 17 s). The numbers on the vertical axis indicate powers of 10. (Reprinted, with permission of the Royal Society of Chemistry, from Ref. 34.)...
Extracting decay rates k(i) from the spectra is simple if the resonances are isolated. In that case the lifetime function, for example, is to a good approximation given by... [Pg.759]

Fig. 1.6. Lifetime function l ip) for box C. The spikes in I indicate the presence of scattering singularities. Fig. 1.6. Lifetime function l ip) for box C. The spikes in I indicate the presence of scattering singularities.
Fig. 9.2. Lifetime function T e) for the scattering potential shown in Fig. 9.1. (From Bliimel (1993b).)... Fig. 9.2. Lifetime function T e) for the scattering potential shown in Fig. 9.1. (From Bliimel (1993b).)...
Fig. 9.5. Lifetime function T 6q) for the Csl scattering model. Frames (b) and (c) show successive magnifications of T( o) displayed in frame (a). (Prom Bliimel (1993b).)... Fig. 9.5. Lifetime function T 6q) for the Csl scattering model. Frames (b) and (c) show successive magnifications of T( o) displayed in frame (a). (Prom Bliimel (1993b).)...
The capital cost estimates are generated by the Engineering function, often based on 50/50 estimates (equal probability of cost overrun and underrun). It is recommended that the operating expenditure is estimated based on the specific activities estimated during the field lifetime (e.g. number of workovers, number of replacement items, cost of forecast manpower requirements). In the absence of this detail it is common, though often inaccurate, to assume that the opex will be composed of two elements fixed opex and variable opex. [Pg.308]

Figure C 1.5.10. Nonnalized fluorescence intensity correlation function for a single terrylene molecule in p-terjDhenyl at 2 K. The solid line is tire tlieoretical curve. Regions of deviation from tire long-time value of unity due to photon antibunching (the finite lifetime of tire excited singlet state), Rabi oscillations (absorjDtion-stimulated emission cycles driven by tire laser field) and photon bunching (dark periods caused by intersystem crossing to tire triplet state) are indicated. Reproduced witli pennission from Plakhotnik et al [66], adapted from [118]. Figure C 1.5.10. Nonnalized fluorescence intensity correlation function for a single terrylene molecule in p-terjDhenyl at 2 K. The solid line is tire tlieoretical curve. Regions of deviation from tire long-time value of unity due to photon antibunching (the finite lifetime of tire excited singlet state), Rabi oscillations (absorjDtion-stimulated emission cycles driven by tire laser field) and photon bunching (dark periods caused by intersystem crossing to tire triplet state) are indicated. Reproduced witli pennission from Plakhotnik et al [66], adapted from [118].
Figure C1.5.12.(A) Fluorescence decay of a single molecule of cresyl violet on an indium tin oxide (ITO) surface measured by time-correlated single photon counting. The solid line is tire fitted decay, a single exponential of 480 5 ps convolved witli tire instmment response function of 160 ps fwiim. The decay, which is considerably faster tlian tire natural fluorescence lifetime of cresyl violet, is due to electron transfer from tire excited cresyl violet (D ) to tire conduction band or energetically accessible surface electronic states of ITO. (B) Distribution of lifetimes for 40 different single molecules showing a broad distribution of electron transfer rates. Reprinted witli pennission from Lu andXie [1381. Copyright 1997 American Chemical Society. Figure C1.5.12.(A) Fluorescence decay of a single molecule of cresyl violet on an indium tin oxide (ITO) surface measured by time-correlated single photon counting. The solid line is tire fitted decay, a single exponential of 480 5 ps convolved witli tire instmment response function of 160 ps fwiim. The decay, which is considerably faster tlian tire natural fluorescence lifetime of cresyl violet, is due to electron transfer from tire excited cresyl violet (D ) to tire conduction band or energetically accessible surface electronic states of ITO. (B) Distribution of lifetimes for 40 different single molecules showing a broad distribution of electron transfer rates. Reprinted witli pennission from Lu andXie [1381. Copyright 1997 American Chemical Society.
Equation (C3.5.3) shows tire VER lifetime can be detennined if tire quantum mechanical force-correlation Emotion is computed. However, it is at present impossible to compute tliis Emotion accurately for complex systems. It is straightforward to compute tire classical force-correlation Emotion using classical molecular dynamics (MD) simulations. Witli tire classical force-correlation function, a quantum correction factor Q is needed 5,... [Pg.3036]

Projecting the nuclear solutions Xt( ) oti the Hilbert space of the electronic states (r, R) and working in the projected Hilbert space of the nuclear coordinates R. The equation of motion (the nuclear Schrddinger equation) is shown in Eq. (91) and the Lagrangean in Eq. (96). In either expression, the terms with represent couplings between the nuclear wave functions X (K) and X (R). that is, (virtual) transitions (or admixtures) between the nuclear states. (These may represent transitions also for the electronic states, which would get expressed in finite electionic lifetimes.) The expression for the transition matrix is not elementaiy, since the coupling terms are of a derivative type. [Pg.151]

The lifetime of polystyrene radicals at 50 C was measuredt by the rotating sector method as a function of the extent of conversion to polymer. The following results were obtained ... [Pg.418]

Fig. 7. Useful lifetime of Parylenes N, C, and D as a function of temperature in air. Failure = 50% loss in tensile strength. Fig. 7. Useful lifetime of Parylenes N, C, and D as a function of temperature in air. Failure = 50% loss in tensile strength.
Thushigh internal quantum efficiency requires short radiative and long nonradiative lifetimes. Nonradiative lifetimes are generally a function of the semiconductor material quaUty and are typically on the order of microseconds to tens of nanoseconds for high quahty material. The radiative recombination rate, n/r, is given by equation 4 ... [Pg.115]

Recreational surfaces must provide certain performance characteristics with acceptable costs, lifetimes, and appearance. Arbitrary but useful distinctions may be made for classification purposes, depending on the principal function a covering intended primarily to provide an attractive surface for private leisure activities, eg, patio surfaces a surface designed for service in a specific sport, eg, track surfaces or a grass-like surface designed for a broad range of heavy-duty recreational activities, including professional athletics, eg, artificial turf for outdoor sports. [Pg.531]

Transition Widths and Strengths. The widths and strengths of spectroscopic transitions determine the information that can be extracted from a spectmm, and are functions of the molecular parameters summarized in Table 2. Detectivity is deterrnined by spectral resolution and transition strength. Resolution, the abiUty to distinguish transitions of nearly equal wavelength, depends on both the widths of the spectral features and characteristics of the instmmentation. Unperturbed transitions have natural, Av widths owing to the intrinsic lifetimes of the states involved. The full width at... [Pg.311]

The main chemico-analytical properties of the designed ionoselective electrodes have been determined. The work pH range of the electrodes is 1 to 5. The steepness of the electrode function is close to the idealized one calculated for two-charged ions (26-29 mV/pC). The electrode function have been established in the concentration range from 0.1 to 0.00001 mole/1. The principal advantage of such electrodes is the fact that thiocyanate ions are simultaneously both complexing ligands and the ionic power. The sensitivity (the discovery limits), selectivity (coefficient of selectivity) and the influence of the main temporal factors (drift of a potential, time of the response, lifetime of the membranes) were determined for these electrodes. [Pg.35]

Details of the function and service conditions of the component part are ascertained, this including the expected lifetime and maximum service temperature. [Pg.200]


See other pages where Lifetime function is mentioned: [Pg.756]    [Pg.219]    [Pg.223]    [Pg.50]    [Pg.207]    [Pg.756]    [Pg.219]    [Pg.223]    [Pg.50]    [Pg.207]    [Pg.297]    [Pg.2496]    [Pg.2501]    [Pg.438]    [Pg.242]    [Pg.244]    [Pg.155]    [Pg.513]    [Pg.10]    [Pg.276]    [Pg.223]    [Pg.422]    [Pg.433]    [Pg.434]    [Pg.336]    [Pg.158]    [Pg.312]    [Pg.124]    [Pg.234]    [Pg.77]    [Pg.705]   
See also in sourсe #XX -- [ Pg.756 , Pg.758 ]




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