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Spectral integrals

FIG. 66. Effects of modulating the RF excitation frequency (a) deposition rate and average light intensity as a function of the modulation frequency, with the deposition rate at cw conditions indicated by the dotted line, (b) measured spectrally integrated emission and calculated production of SiH3 radicals as a function of time, at a modulation frequency of 50 kHz and a 509f duty cycle. [From A. C. W. Biebericher. J, Bezemer. W. F. van der Weg, and W. J. Goedheer, Appl. Phys. Lett. 76, 2002 (2000), 2000, American Institute of Physics, w ith permission.]... [Pg.154]

Procedure Set up an acoustic reactor in a light-proof cabinet with a photomultiplier (PM) tube positioned facing the cell as shown in Fig. 15.3a and b. Fill the cell with distilled water and close the cabinet. A potential should now be applied to the PM tube, the output (spectrally integrated) of which is produced on an oscilloscope (note that the ultrasound cell can easily be placed inside a commercial spectrometer in order to record the emission spectrum). Switch on the ultrasound and you should observe on the oscilloscope a change in voltage, directly proportional to the intensity of sonoluminescence emission. The following experiments can be performed to explore the different types of light emission and some of the factors that influence these emission processes. [Pg.392]

Techniques of Spectral Integration and Spin-Spin Decoupling... [Pg.103]

The next group of problems (278-283) present data in text form rather than graphically. The formal style that is found in the presentation of spectral data in these problems is typical of that found in the experimental of a publication or thesis. This is a completely different type of data presentation and one that students will encounter frequently. Problems 284 - 291 involve the quantitative analysis of mixtures using H and NMR. These problems demonstrate the power of NMR in analysing samples that are not pure compounds and also develop skills in using spectral integration. [Pg.85]

Fig. 2. (a,b) Transient absorption on the v0h=1— 2 transition of OH/OH dimers (symbols). The spectrally integrated, anisotropy free absorption change AA is plotted as a function of the delay time between the pump centered at Ep=2950 cm 1 and the probe centered at Epr. Solid lines exponential decay with a time constant of 200 fs. Inset of Fig. (b) Fourier transform of the oscillatory component of the transient in Fig. (b) displaying an oscillation frequency of 145 cm 1. [Pg.159]

Fig. 3. (a-c) Time resolved changes of the O-H stretching absorption of OH/OH dimers as measured with spectrally integrated probe pulses centered at Epr and corrected for rotational diffusion (symbols, pump pulses centered at Ep=2950 cm"1). The solid lines represent numerical fits based on exponential kinetic components with time constants of 200 fs, 1 ps and 15 ps. Inset of Fig. (c) Time evolution up to a 70 ps delay time, (d-f) Oscillatory component of the signals in Figs, (a-c) and Fourier transforms (insets). [Pg.160]

J a Spectrum of individual conformers (c) From spectral integrals at low temperature, to give N and Na directly... [Pg.170]

The emissivity, 8, is the ratio of the radiant emittance of a body to that of a blackbody at the same temperature. Kirchhoff s law requires that a = e for all bodies at thermal equilibrium. For a blackbody, a = e = 1. Near room temperature, most clean metals have emissivities below 0.1, and most nonmetals have emissivities above 0.9. This description is of the spectrally integrated (or total) absorptivity, reflectivity, transmissivity, and emissivity. These terms can also be defined as spectral properties, functions of wavelength or wavenumber, and the relations hold for the spectral properties as well (71,74—76). [Pg.202]

Recently, Qi et al. made measurements on approximately 70 serum samples using an epi-illuminated waveguiding sample chamber, 160 mW of 830 nm excitation, up to 150 s of spectral integration, and PLS leave-one-out... [Pg.399]

Figure 15.8 Examples of spectral integration and normalization. Spectra shown were obtained with nitroxide label 14 (Fig. 15.3C). Acquisition parameters are listed in Table 15.1, except that number of scans = 4 and number of points = 1024. (A) Spectrum of an aqueous sample of a 23-nt RNA, together with its 1st and 2nd integrals. (B) Spectral comparison between a 23-nt RNA (40 gM, dotted line) and a 49-nt RNA (30 jiM, sobd Une). Comparison of the normalized spectra is not skewed by the different amount of labeled RNAs used in the measurement, and reports different nitroxide behavior due primarily to the difference in RNA size. (C) An example of spin counting. The calibration curve was generated by linear fitting (solid Une) of data points (sobd square) obtained using tempol solutions of various concentrations. Using this calibration curve, the sample measured in (A) was found to contain 37.5 gM of spins ( sample = 2.5). Based on an RNA concentration of 40 jiM, the nitroxide labeling efficiency was determined to be 93.6%. Figure 15.8 Examples of spectral integration and normalization. Spectra shown were obtained with nitroxide label 14 (Fig. 15.3C). Acquisition parameters are listed in Table 15.1, except that number of scans = 4 and number of points = 1024. (A) Spectrum of an aqueous sample of a 23-nt RNA, together with its 1st and 2nd integrals. (B) Spectral comparison between a 23-nt RNA (40 gM, dotted line) and a 49-nt RNA (30 jiM, sobd Une). Comparison of the normalized spectra is not skewed by the different amount of labeled RNAs used in the measurement, and reports different nitroxide behavior due primarily to the difference in RNA size. (C) An example of spin counting. The calibration curve was generated by linear fitting (solid Une) of data points (sobd square) obtained using tempol solutions of various concentrations. Using this calibration curve, the sample measured in (A) was found to contain 37.5 gM of spins ( sample = 2.5). Based on an RNA concentration of 40 jiM, the nitroxide labeling efficiency was determined to be 93.6%.
The command decoder will then request "THRESHOLD ". The threshold is used by the data acquisition programs to determine whether or not data is to be saved. If the threshold is set to 15, the data acquisition program will compare 15 with the value of the spectral integrator (TAC). If the spectral integrator is less than 15 then that spectrum will be rejected as containing baseline data. Thus storage of zero information is avoided. [Pg.149]

T4 dependency of radiation source term For the spectrally integrated RTE, the emission source term is... [Pg.560]

Besides the aforementioned n.m.r. parameters [chemical shift (8), coupling constant (J), and line width], spectral integration can give valuable information. The relative intensities of the structural-re-porter-group signals in the n.m.r. spectrum can be used as markers for the purity of the compound. Often, from the spectrum, it can be deduced whether or not the sample consists of more than one carbohydrate structure, and in which molar ratios the components of the mixture, and the sugar residues in each of these, occur. [Pg.213]

Addition of chiral LSR such as (+)tris[3-heptafluoropropyl hydroxymethylene]-D-[cam-phorato]Eu(III), Eu[(+)fpc]3 to a racemic mixture of diamagnetic Ni complex with propylenediamine backbone results in a composite of two overlapping spectra [92], The changes in the methyl doublet are shown in Fig. 10.27. Combined with spectral integration, this technique may be used for the analysis of mixtures of optically active complexes. [Pg.813]

Smith 1995). The static NMR spectrum of the alloy Mgi7Ali2 shows 3 sites with distinct Knight shifts (Figure 8.15B) and with intensity ratios determined by spectral integration as 1.1 3.6 12, in very close agreement with the ratio of 1 4 12 expected from the structure (Bastow and Smith 1995). [Pg.488]


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See also in sourсe #XX -- [ Pg.43 , Pg.44 , Pg.45 , Pg.46 , Pg.47 , Pg.48 ]




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