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Spectrum normalization

Fig. 3.6. Density transformation of nitrogen isotropic Raman spectrum normalized to a maximum [89] (gas density is given in amagat). Fig. 3.6. Density transformation of nitrogen isotropic Raman spectrum normalized to a maximum [89] (gas density is given in amagat).
Rubrerythrin (Rr) was first isolated in 1988 from cellular extracts of D. vulgaris Hildenborough (38), and later also found in D. desulfuri-cans (39). Rr is constituted by two identical subunits of 22 kDa and it was shown that each monomer contains one Rd-like center, Fe(RS)4, and a diiron-oxo center similar to the ones found in methane monooxygenase (MMO) (40, 41) or ribonucleotide reductase (RNR-R2) (42). After aerobic purification, the UV-visible spectrum shows maxima at 492, 365, and 280 nm, and shoulders at 570 and 350 nm. This spectrum is similar to the ones observed for Rd proteins. From a simple subtraction of a typical Rd UV-vis spectrum (normalized to 492 nm) it is possible to show that the remainder of the spectrum (maxima at 365 nm and a shoulder at 460 nm) strongly resembles the spectrum of met-hemerythrin, another diiron-oxo containing protein. [Pg.367]

In the case of other elements, for instance Uranium, the emission spectrum normally displays thousands of narrowly spaced lines. However, the emission source possesses a fixed amount of energy which shall be spread up eventually amongst the thousands of lines thereby minimizing the sensitivity of each line. Hence, it is rather difficult to examine the less sensitive complex spectra of elements such as uranium. [Pg.360]

Fig. 2. Parameters affecting the efficiency of energy transfer. (A) Overlay of FITC emission spectrum and PE absorbance spectrum normalized to maximum fluorescence intensity and maximum optical density, respectively. FITC fluorescence intensity was measured as a function of emissions wavelength using a fluorimeter with an excitation wavelength of 488 nm. PE optical density was measured as a function of wavelength using a spectrophotometer. (B) Schematic representation of energy absorption and the possible pathways for the subsequent energy release (abbreviations as in the text). Fig. 2. Parameters affecting the efficiency of energy transfer. (A) Overlay of FITC emission spectrum and PE absorbance spectrum normalized to maximum fluorescence intensity and maximum optical density, respectively. FITC fluorescence intensity was measured as a function of emissions wavelength using a fluorimeter with an excitation wavelength of 488 nm. PE optical density was measured as a function of wavelength using a spectrophotometer. (B) Schematic representation of energy absorption and the possible pathways for the subsequent energy release (abbreviations as in the text).
In ISS, like in SIMS, gas ions such as helium or neon are bombarded on the sample surface at a fixed angle of incident. The ISS spectrum normally consists of a single peak of backscattered inelastic ion intensity at an energy loss that is characteristic of the mass of surface atom. From the pattern of scattered ion yield versus the primary ion energy, information about elements present on the sample surface can be obtained at ppm level. [Pg.20]

Zoom Mode Two options are available for zooming your 2D spectrum. Normal allows zooming using the standard rubber box method while Units uses predefined increments. [Pg.132]

Fourier transformation (FT) Mathematical operation to convert a time domain spectrum (FID) to a frequency domain spectrum (normal NMR spectrum). [Pg.837]

In the hypothesis of an exponential potential, the situation is even worse because Jeans instability is always reduced by the presence of quintessence (i.e., o ia is never equal to 1). More detailed calculation give the following value of the matter power spectrum normalization as as a function of Wq in Fig. 8.2. [Pg.145]

Relative intensities in the low-voltage (7-5 volts, uncorrected) mass spectrum, normalized to unreacted dichlorobenzene = 100. [Pg.26]

While empirical rules would fail to yield a correct conformational interpretation of the amide I spectrum, normal mode calculations using the SQM method clearly eliminate several possibilities and put forward a preferred structure for this peptide in water [70S], This approach can be extended to much larger peptides having stable secondary structures. We have collected spectra of several isotopomers of the 23-residue peptide magainin F. We observe in the difference spectra that the amide I bands corresponding to specific amino acids are much narrower than they are in the short peptides and clearly identify the amide I frequencies of these groups. [Pg.252]

The relationships existing within molecules possessing some asymmetric characteristics have been treated in detail by several authors. Protons HA and HB in a molecule such as I-III (with P, Q, and R different) are said to be diastereotopic, whereas if P = Q, they would be enantiotopic. In the latter case, as in the case of two enantiomeric molecules, the NMR spectrum normally does not distinguish between the two, and the chemical shifts of HA and HB are the same. However, in a chiral solvent the interactions between the solvent and the two protons are not necessarily equivalent, and chemical shift differences (usually small) may be found. [Pg.112]

Chlorquinaldol [ban, inn] (Capitrol ) is a hydroxyquino-line ANTIBACTERIAL and ANTIFUNGAL topical agent, which can be used to treat dandruff and seborrhoeic dermatitis, chlortalidone chlorthalidone, chlortetracycline [ban, inn] (chiortetracycline hydrochloride [usan] aureomycin Aureomycin ) Isa (tetracycline) ANTIBIOTIC. It can be used clinically as a broad-spectrum, normally topical, ANTIBACTERIAL to treat a variety of infections. [Pg.74]

Absorption Total Shape Spectrum Normal Glandular Prostate Tissue... [Pg.314]

A discrete stick spectrum, normalized to a total strength of unity, is given by... [Pg.74]

Historically, Woodward and Fieser s early empirical correlation of various organic substructures with their associated UV spectra (23,24) could be considered one of the first attempts to partially identify organic compounds on the basis of nondestructive physical characterization. Woodward was able to predict the X, ax for number of conjugated systems, such as variously substituted enones and dienes, based on literature precedent. Contemporary structure determination of purified compoimds now relies most heavily on NMR and MS techniques, the UV spectrum normally contributing only a minor component to this process. However, the advent of HPLC and UV diode array detectors has enabled the acquisition of a UV spectrum for every component represented in an HPLC chromatogram. Consequently, the UV spectrum has become one of the most readily accessible pieces of information pertaining to structure, and interest has revived in exploiting its usefulness. [Pg.293]

Fig. 12.1 Mossbauer spectra of Co sources in matrices of C0CI2, C0SO4, and their hydrates. Note that the hyperfine spectrum (which originates in the source in these experiments) is the mirror image of the spectrum normally observed in an absorber experiment. TheFe content increases with increasing degreeof hydration. [Ref.4, Figs. 1 and 2]... Fig. 12.1 Mossbauer spectra of Co sources in matrices of C0CI2, C0SO4, and their hydrates. Note that the hyperfine spectrum (which originates in the source in these experiments) is the mirror image of the spectrum normally observed in an absorber experiment. TheFe content increases with increasing degreeof hydration. [Ref.4, Figs. 1 and 2]...
Equation (4.47) is paramount to the realization that measurable spectra contain information about energy flow in molecules. Note that assignments of the spectra are not necessary. We take a spectrum, normalize the line intensities p, so that... [Pg.99]


See other pages where Spectrum normalization is mentioned: [Pg.164]    [Pg.122]    [Pg.26]    [Pg.263]    [Pg.302]    [Pg.150]    [Pg.30]    [Pg.151]    [Pg.164]    [Pg.1761]    [Pg.873]    [Pg.329]    [Pg.363]    [Pg.22]    [Pg.159]    [Pg.6104]    [Pg.159]    [Pg.1124]    [Pg.311]    [Pg.31]    [Pg.43]    [Pg.98]    [Pg.423]    [Pg.435]    [Pg.6103]   
See also in sourсe #XX -- [ Pg.180 , Pg.191 ]

See also in sourсe #XX -- [ Pg.172 ]




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Extinction spectrum, normalized

Intensities normal hydrocarbon spectra

Normal hydrocarbon spectra

Normal hydrocarbon spectra vibrations

Normal mass spectrum

Normal mode spectra

Normalization of spectra

Normalized light extinction spectrum

Normalized spectra

Normalized spectra

Normalized steady-state emission spectra

Spectra normal

Spectra normal-type

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