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Figure 8. Top right, APCI mass spectrum of perfume vapors on blotting paper two hours after application and others, APCI mass spectra of various subjects cutaneous emissions two hours after application of perfume. The average of all subjects spectra has been subtracted from each to accentuate any differences. Figure 8. Top right, APCI mass spectrum of perfume vapors on blotting paper two hours after application and others, APCI mass spectra of various subjects cutaneous emissions two hours after application of perfume. The average of all subjects spectra has been subtracted from each to accentuate any differences.
NaCl) and an NIR-absorbing species (amorphous sorbitol), using the intercept and slope obtained by subjecting spectra to MSC treatment as input parameters for PLSR. [Pg.382]

Mourjopoulos et al., 1992] Mourjopoulos, J., Kokkinakis, G., and Paraskevas, M. (1992). Noisy audio signal enhancement using subjective spectra. In Preprints of the AES 92nd Convention, Vienna. [Pg.556]

The Role of Computers in Activation Analysis.— For many years spectral data accumulated by m.c.a. have been analysed by digital computers. Many complex schemes of spectrum analysis have been developed involving least-squares methods, iterative Gaussian fits to peaks, correlation of the subject spectrum with ideal or measured spectrum shapes, convolution methods, and many combinations and variations of these schemes. Quittner... [Pg.107]

Dennison coupling produces a pattern in the spectrum that is very distinctly different from the pattern of a pure nonnal modes Hamiltonian , without coupling, such as (Al.2,7 ). Then, when we look at the classical Hamiltonian corresponding to the Darling-Deimison quantum fitting Hamiltonian, we will subject it to the mathematical tool of bifiircation analysis [M]- From this, we will infer a dramatic birth in bifiircations of new natural motions of the molecule, i.e. local modes. This will be directly coimected with the distinctive quantum spectral pattern of the polyads. Some aspects of the pattern can be accounted for by the classical bifiircation analysis while others give evidence of intrinsically non-classical effects in the quantum dynamics. [Pg.67]

Once the basic work has been done, the observed spectrum can be calculated in several different ways. If the problem is solved in tlie time domain, then the solution provides a list of transitions. Each transition is defined by four quantities the mtegrated intensity, the frequency at which it appears, the linewidth (or decay rate in the time domain) and the phase. From this list of parameters, either a spectrum or a time-domain FID can be calculated easily. The spectrum has the advantage that it can be directly compared to the experimental result. An FID can be subjected to some sort of apodization before Fourier transfomiation to the spectrum this allows additional line broadening to be added to the spectrum independent of the sumilation. [Pg.2104]

An example of enhanced ion production. The chemical equilibrium exists in a solution of an amine (RNH2). With little or no acid present, the equilibrium lies well to the left, and there are few preformed protonated amine molecules (ions, RNH3+) the FAB mass spectrum (a) is typical. With more or stronger acid, the equilibrium shifts to the right, producing more protonated amine molecules. Thus, addition of acid to a solution of an amine subjected to FAB usually causes a large increase in the number of protonated amine species recorded (spectrum b). [Pg.19]

Other instrumental advantages include its high sensitivity and a linear mass scale to m/z 10,000 at full sensitivity. The linearity of the mass scale means that it is necessary to calibrate the spectrometer using a single or sometimes two known mass standards. Some calibration is necessary because the start of the mass scale is subject to some instrumental zero offset. The digitized accumulation of spectra provides a better signal-to-noise ratio than can be obtained from one spectrum alone. [Pg.167]

Indazoles have been subjected to certain theoretical calculations. Kamiya (70BCJ3344) has used the semiempirical Pariser-Parr-Pople method with configuration interaction for calculation of the electronic spectrum, ionization energy, tt-electron distribution and total 7T-energy of indazole (36) and isoindazole (37). The tt-densities and bond orders are collected in Figure 5 the molecular diagrams for the lowest (77,77 ) singlet and (77,77 ) triplet states have also been calculated they show that the isomerization (36) -> (37) is easier in the excited state. [Pg.175]

The antitumor activity displayed by the mitosanes and many synthetic aziridines stems from their ability to act as alkylating agents which chemically modify (crosslink) DNA. For this reason, a large number have been screened for antitumor activity, the mechanism of which has been the subject of considerable research effort <75CJC289l). An excellent account of the broad spectrum of biological properties of a multitude of compounds containing the aziridinyl moiety has been published [Pg.93]

Can be purified by zone melting or by distn under vacuum at 0 , subjecting the middle fraction to several freeze-pump-thaw cycles. An impure sample containing higher nitroalkanes and traces of cyanoalkanes was purified (on the basis of its NMR spectrum) by crystn from diethyl ether at -60° (cooling in Dry-ice)(Parrett and Sun J Chem Educ 54 448 7977]. [Pg.311]

The deflagration flame arrester must he subjected to a series of at least 10 explosion (deflagration) tests in a rig with a pipe at least 5 feet (1.5 meters) long with various mixtures of propane in air and different test conditions to test the entire spectrum of possible deflagrations. Also, a series of 3 flashback tests, using a mixture of 4.2 volume percent of propane in air, must be conducted. [Pg.157]

There has been much discussion of the relative contributions of the no-bond and dative structures to the strength of the CT complex. For most CT complexes, even those exhibiting intense CT absorption bands, the dative contribution to the complex stability appears to be minor, and the interaction forces are predominantly the noncovalent ones. However, the readily observed absorption effect is an indication of the CT phenomenon. It should be noted, however, that electronic absorption shifts are possible, even likely, consequences of intermolecular interaetions of any type, and their characterization as CT bands must be based on the nature of the spectrum and the structures of the interaetants. This subject is dealt with in books on CT complexes. ... [Pg.394]

N-Acetylation of Kasugamycinic Acid (9a). A solution of kasugamycinic acid (225 mg.) dissolved in 10 ml. of water was treated with acetic anhydride (0.3 ml.) under cooling sodium bicarbonate was used to keep the pH 7.2 and stirring continued for 30 minutes. The reaction product was passed through Dowex 50W-X2 (H form) and the column was washed with water. The combined filtrate was subjected to lyophilization to afford 234 mg. of a crude N-acetyl derivative. Its infrared spectrum showed strong absorptions at 1740 cm-1 characteristic of oxamic acid group. The N-acetyl derivative (178 mg.) was treated with 40 ml. [Pg.43]


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Cumulative Subject ESR spectra

Fine spectrum Subject

Subject Raman spectra

Subject electronic spectra

Subject infrared spectra

Subject reflectance spectra

Subject reflection spectra

Subject ultraviolet spectrum

Subject vibrational spectra

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