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Half-amplitude

Fig. 10. The ESR signal produced at various points on the resonant line in a magnetic field modulated spectrometer. The vertical magnetic field modulation interacts with the bell-shaped adsorption curve [F(H)1 to produce the horizontal ESR signal. Here AH is the half amplitude line width and Hu is the center of resonance (S3). Fig. 10. The ESR signal produced at various points on the resonant line in a magnetic field modulated spectrometer. The vertical magnetic field modulation interacts with the bell-shaped adsorption curve [F(H)1 to produce the horizontal ESR signal. Here AH is the half amplitude line width and Hu is the center of resonance (S3).
As indicated in Section 5.4.5, it is not appropriate to consider the observed spectral absorption characteristic of a single chromophore as a single function and speak of the half-amplitude points as describing the waveform. The peak wavelength and the two half-amplitude points can be used for less critical work. However, the correct description of the waveform requires that the waveform on each side of the pseudo-peak be plotted as an exponential function and the wavelength specified at which this function is equal to 1/e of its peak value. These two 1/e values properly describe the measured spectral response. [Pg.35]

Mees James, and others, have noted that the absolute energy level of the top of the n-electron band (half-amplitude of the electron density profile of the n-band) in most chromophores of photography is located at an absolute energy level near 3.39 electron-volts74. This ground level is very near the first excited level of the hydrogen atom shown in [Figure 5.4.1-1], However, this may only be coincidental. [Pg.43]

The probability profile on the right is indicative of the absorption characteristic of each individual chromophore. Note the use of the symbols c and a to indicate the half amplitude points of this profile. Note also that the difference in two exponential profiles remains an exponential profile, albeit with modified parameters. These parameters, and the nominal center energy, represent the conjugated-dipole-molecular absorption band of the Rhodonines. This spectrum is frequently reported in the literature for the chromophores of vision. It is usually attributed to the putative rhodopsin. However, the presence of opsin is not required. Only a conventional concentration of Rhodonine is required to record this isotropic spectrum since it is the only feature in the visual range of the spectrum for these materials. [Pg.72]

The best empirical values for this spectral parameter vary somewhat due to experimental technique, particularly due to the solvent used. Although rounded due to the width of the spectral filter used, the values of Wald Brown are still the most widely quoted118. They are a = 447 nm, b = 502 nm, c = 549 nm. It would be easily to interpret the median of this waveform at the mean of the two half-amplitude points, 498 nm. It is common to find the waveform shifted slightly to a center wavelength at 495nm. However, the 502 nm wavelength is frequently reported in an attempt to relate it to the peak of the scotopic spectrum when that spectrum is measured with a broadband spectral filter. [Pg.72]

The theoretical half amplitude parameters defining the width of the absorption band of each chromophore are not... [Pg.78]

The difference between the long wavelength half-amplitude point of one chromophore and the short wavelength half-amplitude point of the next longer wavelength chromophore varies between 15 and 30 nm in this table. A difference of 30 nm between the M- and L- channel is mentioned in Kraft, et. al. (1990) based on Loppnow et. al. (1989), but without further substantiation. [Pg.80]

The resonance factor, Q, can be used as a guide to compare the laboratory results of various experimenters. It is calculated as the quotient of the peak wavelength divided by the difference between the wavelengths of the two half-amplitude points for the spectrum of each chromophore. When computing the precise spectral characteristics of the chromophores of vision as found in laboratory experiments (that occurs in Chapter 16 17) the appropriate Qwas determined. [Pg.80]

The half amplitude full width of these absorptions are in good agreement with the estimates of Wolbarsht when the broader peaks of Fermi-Dirac statistics compared to Gaussian statistics are recognized128. [Pg.81]

It should be noted that the Lamb equation is appropriate for a low frequency filter rather than a resonant phenomenon such as spectral absorption by the chromophores. Its asymptotic character at short wavelengths leads to a half-amplitude value that is quite different from the similar half-amplitude value for a resonant phenomenon of arbitrary resonance factor, Q. [Pg.81]

The half amplitude wavelengths for the subject must be known to a precision of <1.0 nm. These vary with the length of the outer segments of the retina of the individual and these lengths vary with location. [Pg.103]

By more completely suppressing the M-channel, the true spectral peak of the L-channel receptors can be determined. The long-dash overlay is for such a condition. The relative amplitudes for this overlay are Figure 5.5.10-10 Wald s figure 2 with overlays. The ksi ik O O 1000 with the same half-amplitudes as upper overlay (dashed line) shows the overall spectral above. Under this more complete adaptation, the peak in sensitivity function of this work. The lower the long wavelength receptor channel is seen to occur at overlay(dashed line) shows the overall spectral sensitivity 625 nm function of this work for a chromatically adapted subject. [Pg.103]

The most conspicuous non-resonant system showing nearly aligned periapses is v Andromedae. This system has been the object of many numerical and analytical studies (for references, see Michtchenko and Malhotra, 2004). The orbit of the planets c and d in this system are such that the distance between their periapses oscillates about zero with half-amplitude 60 degrees and period 7260 years. [Pg.257]

Fig. 8. Methylammonium ion (Grunwald et al., 1957). Half-width of the CH3 reeonance as function of the exchange rate. The ordinate is the quantity u = A/ Sco where A is the width of the line at half-amplitude. The other symbols are defined in the caption of Fig. 3-6 which shows samples of the curves from which the figure was obtained. Fig. 8. Methylammonium ion (Grunwald et al., 1957). Half-width of the CH3 reeonance as function of the exchange rate. The ordinate is the quantity u = A/ Sco where A is the width of the line at half-amplitude. The other symbols are defined in the caption of Fig. 3-6 which shows samples of the curves from which the figure was obtained.
The half-amplitude width of the signals of polySi4 and Sn6 are quite narrow and comparable with those of rubbery polymers. This infers that the side-chains involving nearby main-cti n in... [Pg.594]


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See also in sourсe #XX -- [ Pg.43 , Pg.71 , Pg.76 , Pg.77 , Pg.80 , Pg.81 , Pg.84 , Pg.100 , Pg.141 ]




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