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Microdensitometer trace

Figure 2. Microdensitometer traces of RIKES spectra of two solutions of cyclohexane in CClt in the C-H stretching region. The peak ruby pump power was ISO MW cm 2 and the pump beam was crossed with probe beam at about 10°. Figure 2. Microdensitometer traces of RIKES spectra of two solutions of cyclohexane in CClt in the C-H stretching region. The peak ruby pump power was ISO MW cm 2 and the pump beam was crossed with probe beam at about 10°.
Figure 3. Microdensitometer traces of the OHD-RIKES single-pulse spectra of 10% (v/v) solutions of benzene, (a) C-H stretching region, analyzer rotated —4° (b) conditions identical to (a) except analyzer rotated +4° (c) 992 cm 1 line with analyzer rotated —12° (d) conditions identical to (c) except analyzer rotated - -12°. A positive rotation is clockwise-observed from the spectrograph. Keep in mind that the apparent line shape is affected by the slope of the dye laser intensity. Figure 3. Microdensitometer traces of the OHD-RIKES single-pulse spectra of 10% (v/v) solutions of benzene, (a) C-H stretching region, analyzer rotated —4° (b) conditions identical to (a) except analyzer rotated +4° (c) 992 cm 1 line with analyzer rotated —12° (d) conditions identical to (c) except analyzer rotated - -12°. A positive rotation is clockwise-observed from the spectrograph. Keep in mind that the apparent line shape is affected by the slope of the dye laser intensity.
Figure 4. Microdensitometer traces of spectra from 10% (v/v) solutions of cyclohexane in CClt taken before and at 20 ysec after the flash intensity peak... Figure 4. Microdensitometer traces of spectra from 10% (v/v) solutions of cyclohexane in CClt taken before and at 20 ysec after the flash intensity peak...
Figure 6. Microdensitometer traces of IRS and OHD-RIKES spectra of 10% (v/v) cyclohexane solutions in CCLr (a) IRS spectra before flash (b) 12 psec after flash peak, peak ruby pump power, 150 MW/cm2 (c) 19 fisec after flash peak, peak ruby pump power, 700 MW/cm2. In (c) the ruby pump is linearly polarized parallel to dye polarization but the analyzer is rotated +5° out of null (d) and (e), microdensitometer traces of OHD-RIKES spectra of 10% (v/v) cyclohexane in CCl, before and at the peak of the flash, peak ruby pump power, 150 MW/cm2. The ruby pump polarization was oriented 45° to the linear dye probe and the analyzer was rotated +5° from the null position. Figure 6. Microdensitometer traces of IRS and OHD-RIKES spectra of 10% (v/v) cyclohexane solutions in CCLr (a) IRS spectra before flash (b) 12 psec after flash peak, peak ruby pump power, 150 MW/cm2 (c) 19 fisec after flash peak, peak ruby pump power, 700 MW/cm2. In (c) the ruby pump is linearly polarized parallel to dye polarization but the analyzer is rotated +5° out of null (d) and (e), microdensitometer traces of OHD-RIKES spectra of 10% (v/v) cyclohexane in CCl, before and at the peak of the flash, peak ruby pump power, 150 MW/cm2. The ruby pump polarization was oriented 45° to the linear dye probe and the analyzer was rotated +5° from the null position.
Fig. 1.3. Ultraviolet micrograph of transverse section of black spruce tracheid with the microdensitometer trace taken across dotted line... Fig. 1.3. Ultraviolet micrograph of transverse section of black spruce tracheid with the microdensitometer trace taken across dotted line...
Fig. 1.5 Portions of XRD powder patterns (microdensitometer traces of Guinier photographs) of (A) a-C S at 1500 C, (B) a -CjS at 1000°C and (C) P-C,S. Indices are based on axes used in Tabic 1.4. After Regourd and Guinier (Rl). Fig. 1.5 Portions of XRD powder patterns (microdensitometer traces of Guinier photographs) of (A) a-C S at 1500 C, (B) a -CjS at 1000°C and (C) P-C,S. Indices are based on axes used in Tabic 1.4. After Regourd and Guinier (Rl).
Fig. 2.5. Interference fringe patterns (X. = 546 nm) and microdensitometer traces of an unloaded and loaded (K, = 0.66 MPa )/m) crack and craze in PMMA... Fig. 2.5. Interference fringe patterns (X. = 546 nm) and microdensitometer traces of an unloaded and loaded (K, = 0.66 MPa )/m) crack and craze in PMMA...
Figure 3. Simulation of a periodic image of spatial frequency from the microdensitometer trace of the image of a shape edge (a), translated by 1/v (b), and reversed about the true edge and translated v(c). Figure 3. Simulation of a periodic image of spatial frequency from the microdensitometer trace of the image of a shape edge (a), translated by 1/v (b), and reversed about the true edge and translated v(c).
Figure 2. Typical experimental data for consecutive TPFof azulene in solution excited at 530 nm. The upper microdensitometer trace corresponds to the azulene pattern the lower trace is the TPFpattern ofa BBOT dye solution obtained simultaneously with the azulene data. (Reproduced with permission from Ref 20. Copyright 1978, Weizmann... Figure 2. Typical experimental data for consecutive TPFof azulene in solution excited at 530 nm. The upper microdensitometer trace corresponds to the azulene pattern the lower trace is the TPFpattern ofa BBOT dye solution obtained simultaneously with the azulene data. (Reproduced with permission from Ref 20. Copyright 1978, Weizmann...
Figure 1.7. Microdensitometer tracings of A mouse and B guinea pig liver DNA, centrifuged to equilibrium in CsCl (upper tracings) and Cs2S04/Ag (lower tracings) density gradients. (From Corneo et al., 1968). Figure 1.7. Microdensitometer tracings of A mouse and B guinea pig liver DNA, centrifuged to equilibrium in CsCl (upper tracings) and Cs2S04/Ag (lower tracings) density gradients. (From Corneo et al., 1968).
Fig. 4.8. Effect on the intensity distribution of the CI2 afterglow spectra of variable [Cl] and [M]. Spectra were obtained using argon carrier gas at 298 K microdensitometer traces are shown in the Figure. The long wavelength cut-offs are due to the negligible sensitivities beyond these wavelengths of the photographic emulsions used. Fig. 4.8. Effect on the intensity distribution of the CI2 afterglow spectra of variable [Cl] and [M]. Spectra were obtained using argon carrier gas at 298 K microdensitometer traces are shown in the Figure. The long wavelength cut-offs are due to the negligible sensitivities beyond these wavelengths of the photographic emulsions used.
FIGURE 6-7. Microdensitometer tracings of the granularity of photographic emulsions. [From a copyrighted Kodak publication. Courtesy Eastman Kodak Co.]... [Pg.132]

Tritium diffusion in single crystals of rutile was measured between 155 and 300C. The diffusivities were calculated from concentration profiles obtained from microdensitometer traces of autoradiographs generated by the P-decay of the tritium. The diffusivity was anisotropic, and was described by ... [Pg.259]

Figure 4.4 Preliminary flash-spectrographic investigation. Typical microdensitometer trace of a transient absorption. Upper trace, spectroflash profile alone lower trace, spectrum of 4-aminophenyl in hexane recorded at 10 ps after photolysis flash, showing transient absorption at 410 nm. From G. Porter and M.A. West, Ref. [2,b]. Figure 4.4 Preliminary flash-spectrographic investigation. Typical microdensitometer trace of a transient absorption. Upper trace, spectroflash profile alone lower trace, spectrum of 4-aminophenyl in hexane recorded at 10 ps after photolysis flash, showing transient absorption at 410 nm. From G. Porter and M.A. West, Ref. [2,b].
FIGURE 4.5 Meselson and Stahl experiment, with microdensitometer tracings of ultracentrifuge density gradients. The DNA of the parent molecule (0 generation) was completely labeled with replication was performed in Note the shift to lower densities and the equivalence of medium and light DNA at 1.9 generations. [Pg.38]


See other pages where Microdensitometer trace is mentioned: [Pg.112]    [Pg.152]    [Pg.131]    [Pg.300]    [Pg.386]    [Pg.2741]    [Pg.564]   


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