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Band strength

To complete the set of formulae required in analysis of intensities of spectral lines in absorption, an experimental measure of a band strength Si, is a sum of... [Pg.298]

FIGURE 14-10 Intrinsic infrared absorption band strengths of some potential greenhouse gases in the atmospheric window (from Ramanathan, 1988a, 1988b). [Pg.774]

X -Phosphorins as well as X -phosphorins have five characteristic bands between 1400 and 1600 cm . 1.1-Dialkoxy- and 1. l-diaryloxy-X -phosphorins have additional intense bands in the region 1180—1220 cm and at 1008 cm and 1040 cm , as well as a weak band at 1160cm which can be attributed to the P—0 vibration. In P—N compounds the band at 718 cm is probably due to the P—N vibration. With increasing P—N band strength it shifts to 785 cm ... [Pg.107]

Since the absorption band strength decreases about one order of magnitude with each increase in the order of harmonics (i.e., the vibrational quantum... [Pg.281]

Fig. 12.5. Series of Raman spectra of normal cornea (left) and drug-treated cornea (right) in the CH and OH stretch frequency region, obtained as function of probing depth into the cornea. Relative CH and OH Raman band strengths reveal local changes in corneal hydration. Adapted from [15]... Fig. 12.5. Series of Raman spectra of normal cornea (left) and drug-treated cornea (right) in the CH and OH stretch frequency region, obtained as function of probing depth into the cornea. Relative CH and OH Raman band strengths reveal local changes in corneal hydration. Adapted from [15]...
Among other new methods, tunable laser absorption spectroscopy using infrared diode lasers offers prospects for improved accuracy and specificity in concentration measurements, when a line-of-sight technique is appropriate. The present paper discusses diode laser techniques as applied to a flat flame burner and to a room temperature absorption cell. The cell experiments are used to determine the absorption band strength which is needed to properly interpret high temperature experiments. Preliminary results are reported for CO concentration measurements in a flame, the fundamental band strength of CO at STP, collision halfwidths of CO under flame conditions, and the temperature dependence of CO and NO collision halfwidths in combustion gases. [Pg.413]

An extensive series of room temperature experiments recently has been completed in our laboratory to determine the fundamental band strengths of CO and NO and to measure CO and NO collision halfwidths for N2, Ar and combustion gas broadening as a function of rotational and vibrational quantum number. Some preliminary results for CO are reported here. [Pg.417]

Figure 3. CO fundamental band strength at 273.2 K determined in room ture cell experiments (A). M = J P-branch (O), J + R-branch. S°ave... Figure 3. CO fundamental band strength at 273.2 K determined in room ture cell experiments (A). M = J P-branch (O), J + R-branch. S°ave...
Varghese, P. L. and Hanson, R. K., "Diode Laser Measurements of CO Collision Halfwidths and Fundamental Band Strength at Room Temperature" to be published. [Pg.426]

Figure 7.2 The relation between the particle growth in the disk mid-plane traced by the millimeter opacity index and that of the inner disk surface traced by the 9.7 pm silicate emission feature. The star symbols represent individual disks. Data points are from van Boekel etal. (2003), Natta etal. (2004),Furlanc/ al. (2006), Rodmann et al. (2006), and Lommen el al. (2007). Typical errors are 10-30% in both /3 and silicate band strength. Note also that differences in how the silicate band strengths were derived may introduce slight systematic offsets for the different data sets. The circle symbols represent dust opacity models calculated for the interstellar medium at a range of densities. From top to bottom the circles are Ry = 3.1 and Ry = 5.5 from Weingartner Draine (2001), a Spitzer-constrained dust opacity for dense clouds from Pontoppidan et al. (in preparation) and the particle growth simulation for protostellar envelopes [thin ice mantles, Ossenkopf Henning (1994)]. Figure 7.2 The relation between the particle growth in the disk mid-plane traced by the millimeter opacity index and that of the inner disk surface traced by the 9.7 pm silicate emission feature. The star symbols represent individual disks. Data points are from van Boekel etal. (2003), Natta etal. (2004),Furlanc/ al. (2006), Rodmann et al. (2006), and Lommen el al. (2007). Typical errors are 10-30% in both /3 and silicate band strength. Note also that differences in how the silicate band strengths were derived may introduce slight systematic offsets for the different data sets. The circle symbols represent dust opacity models calculated for the interstellar medium at a range of densities. From top to bottom the circles are Ry = 3.1 and Ry = 5.5 from Weingartner Draine (2001), a Spitzer-constrained dust opacity for dense clouds from Pontoppidan et al. (in preparation) and the particle growth simulation for protostellar envelopes [thin ice mantles, Ossenkopf Henning (1994)].
The radiative relaxation time tt of a vibrational mode v is inversely proportional to the band strength S . (See, for example, R. M. Goody, Atmospheric Radiation I. Theoretical Basis, Oxford Univ. Press, Oxford, 1964.) Thus one finds, for example, that the radiative lifetime of the bending mode, v2, of H20 is about 0.07 sec. [Pg.257]

Shimazaki and coworkers663 analyzed the c.d. spectrum of both toxin and agglutinin in the presence and absence of lactose. The spectra of the two proteins were similar, but there were differences in band strength between them. The toxin contains 15% of a-helix and 52% of /3-pIeated sheet the agglutinin, 13% of a-helix and 51% of -pleated... [Pg.272]

An extensive and regularly updated database listing line frequencies, broadening parameters and intensities of a variety of molecules with a small number of atoms has been compiled. This database is particularly valuable for atmospheric studies and fundamental laboratory spectroscopy research. The most recent contribution by Rothman et al. (1987) also provides an extensive list of references, adding further details to the original studies. In this context, we would like to recommend a publication by Pugh and Rao (1976), which reviews intensity data, i.e., infrared band strengths of molecular vibrations, and provides an extensive list and description of the pertinent measurement techniques. [Pg.276]

The earlier attempt of deriving spectral types for metal-poor stars relied upon hydrogen line strengths or G-band strength due to their strong... [Pg.175]

The analysis of cometary data requires knowing the vibrational transition band strengths in the state of CN. Two very different values for the Einstein coefficient (A) of the fundamental 1-0 vibrational band have been reported one based on analysis of cometary data and the other from measurements in a King furnace.Using the CASSCF/MRCI dipole moment function, the computed /fjo value was in excellent agreement with the value measured in the King furnace. The small uncertainty in the computed value suggests that some of the assumptions in the model used to analyze the cometary data are in error. [Pg.135]

Formulation of the Exponential Wideband Models. In exponential wideband models, the band strength parameter, or an integrated absorption coefficient of a given wideband, is defined as ... [Pg.571]


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See also in sourсe #XX -- [ Pg.298 ]

See also in sourсe #XX -- [ Pg.2 , Pg.273 ]




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Absorption band strength

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