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Transient transmittance

Transient transmittance of single-walled carbon nanotubes (SWNTs) in suspension was modulated at two periods of T40 and 21 fs, corresponding to the RBM and G mode, respectively [54,55]. The amplitude and the frequency of the coherent RBMs exhibited a clear excitation-wavelength dependence (Fig. 2.15) [54]. The different frequencies were attributed to SWNTs with different diameters coming to the excitonic resonance. The FT spectra of the coherent RBMs in Fig. 2.15 had noticeable differences from the resonant Raman spectra, such as the different intensities and better frequency resolution. [Pg.37]

Fig. 2.15. Left oscillatory part of the transient transmittance of SWNTs in a suspension excited and measured with 50 fs pulses at different photon energies. Right a 3D plot of its FT spectrum obtained over a photon energy range of 1.746-1.459 eV (wavelength of 710-850 nm). From [54]... Fig. 2.15. Left oscillatory part of the transient transmittance of SWNTs in a suspension excited and measured with 50 fs pulses at different photon energies. Right a 3D plot of its FT spectrum obtained over a photon energy range of 1.746-1.459 eV (wavelength of 710-850 nm). From [54]...
Fig. 3.11. Left spectrum of the tailored pump beam for different spectral separations Aw CC2 — oji between two spectral packets (oJi and Lof). The bottom case is resonant to the E2 phonon frequency l o- Right transient transmittance of GaN excited with the tailored pump pulses, showing the enhancement of coherent oscillation of the E2 phonon for u) — u)2 — Oo- From [28]... Fig. 3.11. Left spectrum of the tailored pump beam for different spectral separations Aw CC2 — oji between two spectral packets (oJi and Lof). The bottom case is resonant to the E2 phonon frequency l o- Right transient transmittance of GaN excited with the tailored pump pulses, showing the enhancement of coherent oscillation of the E2 phonon for u) — u)2 — Oo- From [28]...
In this chapter, we will focus on the discussion of experiments that directly monitor the time-evolution of the electronic excited-state dynamics. In particular, we shall consider transient transmittance, time-resolved fluorescence, and time-resolved ionization spectroscopy. This is because these techniques have the potential to directly observe the ultrafast photochemical excited-state processes triggered by conical intersections. [Pg.744]

Note that the application of the convolution scheme in the simple form (44) requires that the nonlinear polarization contains only a single interaction with the probe laser field. Apart from the transient transmittance spectrum considered above, this condition is also fulfilled for related detection schemes such as time-resolved fluorescence, ionization, and excited-state absorption. Coherent spectroscopic signals such as the photon-echo, on the other hand, contain two interactions with the probe laser field, thus requiring the calculation of the full three-time response function, followed by a double convolution. [Pg.760]

Fig. 1. The integral transient transmittance spectrum of pyrazine, calculated for a... Fig. 1. The integral transient transmittance spectrum of pyrazine, calculated for a...
Fig. 2. Decomposition of the integral transient transmittance spectrum into the stimulated-Raman (a) and stimulated-emission (b) contributions. Fig. 2. Decomposition of the integral transient transmittance spectrum into the stimulated-Raman (a) and stimulated-emission (b) contributions.
Although the model described above has been found to qualitatively reproduce femtosecond transient transmittance experiments on rhodopsin,it cannot reproduce the experimental fluorescence and resonance Raman spectra of rhodopsin.This is because the Raman spectra exhibit a number of vibrational modes that are not included in the model. While these modes may not directly be involved in the photochemical reaction... [Pg.789]

The transient transmittance PP signal is defined through the difference polarization Ppp (0 = Ppp(t) —Ppf(f) [1]. Here Ppp ( ) is the pump-offpolarization induced solely by the probe pulse, which is obtained from Eqs. 9.29 and 9.30 with = 0. Within the RWA and the slowly varying envelope approximation, the integral (int) and dispersed... [Pg.455]

It should be emphasized at this point that the speed of response is cnti-cal. The pressure transient pressure should not fall to less than 50% of the difference in pressure between the standby pump start pressure and the low oil pressure trip pressure. This is normally achievable with good design practice and the use of a switch and direct wiring. There is some tendency to use a transmitter and control through a remote computer. The latter arrangement is difficult to check on a shop test and normally is too slow to meet the requirement. An accumulator can be added and must be used if the requirement cannot be met. This additional hardware contributes to higher initial cost and possible reliability problems in the future. The direct switch method is therefore highly recommended. [Pg.314]

FIGURE 5.6 Calcitonin receptor responses, (a) Real-time melanin dispersion (reduced light transmittance) caused by agonist activation (with human calcitonin) of transfected human calcitonin receptors type II in melanophores. Responses to 0.1 nM (filled circles) and lOnM (open circles) human calcitonin, (c) Dose-response curves to calcitonin in melanophores (open circles) and HEK 293 cells, indicating calcium transient responses (filled circles). [Pg.83]

Transient Time-domain signal (FID) acquired in an FT experiment. Transmitter Coil of wire and accompanying electronics from which Rf energy is applied to the NMR sample. [Pg.420]

Figure 2.4 Noradrenergic inhibition of Ca " currents and transmitter release in sympathetic neurons and their processes, (a) Inhibition of currents through N-type Ca " channels by external application of noradrenaline (NA) or by over-expression of G-protein P y2 subunits, recorded from the soma and dendrite of a dissociated rat superior cervical sympathetic neuron. Currents were evoked by two successive 10 ms steps from —70 mV to OmV, separated by a prepulse to -1-90 mV. Note that the transient inhibition produced by NA (mediated by the G-protein Go) and the tonic inhibition produced by the G-protein Piy2 subunits were temporarily reversed by the -1-90 mV depolarisation. (Adapted from Fig. 4 in Delmas, P et al. (2000) Nat. Neurosci. 3 670-678. Reproduced with permission), (b) Inhibition of noradrenaline release from neurites of rat superior cervical sympathetic neurons by the 2-adrenoceptor stimulant UK-14,304, recorded amperometrically. Note that pretreatment with Pertussis toxin (PTX), which prevents coupling of the adrenoceptor to Gq, abolished inhibition. (Adapted from Fig. 3 in Koh, D-S and Hille, B (1997) Proc. Natl. Acad. Sci. USA 1506-1511. Reproduced with permission)... Figure 2.4 Noradrenergic inhibition of Ca " currents and transmitter release in sympathetic neurons and their processes, (a) Inhibition of currents through N-type Ca " channels by external application of noradrenaline (NA) or by over-expression of G-protein P y2 subunits, recorded from the soma and dendrite of a dissociated rat superior cervical sympathetic neuron. Currents were evoked by two successive 10 ms steps from —70 mV to OmV, separated by a prepulse to -1-90 mV. Note that the transient inhibition produced by NA (mediated by the G-protein Go) and the tonic inhibition produced by the G-protein Piy2 subunits were temporarily reversed by the -1-90 mV depolarisation. (Adapted from Fig. 4 in Delmas, P et al. (2000) Nat. Neurosci. 3 670-678. Reproduced with permission), (b) Inhibition of noradrenaline release from neurites of rat superior cervical sympathetic neurons by the 2-adrenoceptor stimulant UK-14,304, recorded amperometrically. Note that pretreatment with Pertussis toxin (PTX), which prevents coupling of the adrenoceptor to Gq, abolished inhibition. (Adapted from Fig. 3 in Koh, D-S and Hille, B (1997) Proc. Natl. Acad. Sci. USA 1506-1511. Reproduced with permission)...
However, as early as the 1970s, it was obvious that end-product inhibition of TH could not be the main factor regulating the rate of noradrenaline synthesis. Clearly, the hydroxylation of tyrosine takes place in the cytoplasm and so it must be cytoplasmic noradrenaline that governs enzyme activity. Yet, it is vesicle-bound transmitter that undergoes impulse-evoked release from the neuron. Also, when neurons are releasing noradrenaline, its reuptake from the synapse is increased and, even though some of this transmitter ends up in the vesicles, or is metabolised by MAO, there should be a transient increase in the concentration of cytoplasmic noradrenaline which would increase end-product inhibition of TH. [Pg.169]

Figure 13. Surface transients over Pt-alumina, starting with an oxidizing feed-stream (A) or with a reducing feedstream (B) (transmittance mode) at 723 K, 257 cmfi/s, 2,070 cm. 1, and 1 Hz switching frequency. Figure 13. Surface transients over Pt-alumina, starting with an oxidizing feed-stream (A) or with a reducing feedstream (B) (transmittance mode) at 723 K, 257 cmfi/s, 2,070 cm. 1, and 1 Hz switching frequency.
The high sensitivity of lock-in amplification can be applied to detect the small periodic changes in transmittance caused by modulated e.xcitation with UV light. Measurements of the amplitude and phase shift of the response signal allow us to determine the spectra and lifetimes of the transient species. [Pg.25]

The function of glutamate as a stimulatory transmitter in the brain is the cause of what is known as the Chinese restaurant syndrome. In sensitive individuals, the monosodium glutamate used as a flavor enhancer in Chinese cooking can raise the glutamate level in the brain to such an extent that transient mild neurological disturbances can occur (dizziness, etc.). [Pg.356]


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