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2, ULTRAFAST DYNAMICS IN THE EXCITED STATES OF AZO COMPOUNDS              57





















                         o                                            0.0
                               400       500        600        700
                                         Wavelength (nm)

               FIG. 2.3 Absorption spectra of DMAAB/DMSO at 0.2 (solid curve) and 0.01 (dashed curve) mol
                  3
                dm" . The spectrum of NOPA (noncollinear optical parametric amplifier) output (dotted curve) was
                used for both pump and probe pulses.



               pump-probe experiments. The pulse spectrum has a small but finite overlap
               with the sample's n-n* absorption band tail. The absorption coefficients at
                                                                  1   2
               420nm(n-jc*) and 600nm(n-7t*) are 30,000 and ZSOmol-  dm , respectively.
               By separating the absorption spectrum into n-n* and n-7t*, the fraction of the
               former excitation is estimated as 70%.

               2.3.2.1 Wave Packet in the Ground and Excited States
                   It is well known that a coherent wave packet can be generated both in
               the ground and excited states and that the ratio between the amounts of the
               wave packets excited on the two potential curves is sensitive to the chirp
                       28 30
               direction. "  Positively chirped (PC) and Fourier-transform limited (TL)
               pulses excite a wave packet in the excited state much more efficiently than in
               the ground state, whereas negatively (NC) chirped pulses with an appropriate
               rate induces a wave packet more efficiently in the ground state. This is
               because the damping of the wave packet photogene rated by the leading edge
               of the pulse takes place by the trailing edge of the NC pulse in cases where
               the chirp rate is close to the lowering rate of the molecular system's potential
               energy in the excited state. We prepared NC, PC, and TL pulses for sample
               excitation by changing the insertion amount of a prism pair used as a pulse
               compressor in NOPA. The second-harmonic generation frequency-resolved
                                                    31 32
               optical gating (SHG-FROG) measurement '  was used for the pulse charac-
               terization. The quadratic phase terms <l>"(v} of the NC and PC pulses were
                                                                  2
               determined from the FROG traces to be -930 and 990 fs , respectively. The
               TL pulse is slightly down-chirped, but the absolute value of the residual chirp
                                   2
               is smaller than 330 fs  in the main part of the pulse. The full width at half
               maximum of the NC, PC, and TL pulses are 9.6, 8.4, and 7.4fs, respectively.
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