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Pump-probe electronic absorption spectroscopy

One of the most commonly apphed types of spectroscopy in the picosecond realm is pump-probe electronic absorption spectroscopy. The absorption spectra of reactive intermediates are usually just as featureless as those of the other two time domains described in this volume. It is simply the inherent nature of these spectra in condensed phases, most typically in solution. Spectroscopic studies in solution most closely mimic reaction conditions that reactive intermediates may find themselves involved in when they are formed and consumed during the course of an organic chemical reaction. [Pg.875]

Ethylene glycol is a very viscous liquid and the molecule presents two close OH groups. It has to be noticed that, among all the different solvents studied by pulse radiolysis, the transition energy of the solvated electron absorption band is maximum in liquid ethylene glycol. For these reasons, the electron in EG seems to have a special behaviour and it is of great interest to study the dynamics of the formation of equilibrated solvated electron. Within this context, the present communication deals with the dynamics of solvation in EG of electrons produced by photoionisation of the solvent at 263 nm. The formation of solvated electrons is followed by pump-probe transient absorption spectroscopy in the visible spectral range from 425 to 725 nm and also in near IR. For the first time, the absorption spectrum of the precursor of the equilibrated electron is observed in EG. Our results are shortly compared by those obtained in water and methanol. [Pg.241]

Electron injection dynamics in the conduction band of metal oxide materials from dye molecules or metal nanoparticles, which is important when applied to sensitized solar cells, can be monitored in the infrared by 100 fs time resolution. In this chapter, technical details of femtosecond visible-pump/IR-probe transient absorption spectroscopy and some typical spectroscopic data revealing the mechanism of electron injection process were described. A great advantage of this technique is that one can observe transient absorption of injected electrons easily because of the intense intraband transition of an electron at the bottom of or at the trap level just below the conduction band of the metal oxide that forms an electrode. In the case of dye-sensitized solar cells, the effects of metal oxide, dye, solvent and additive ions on the rate and efficiency of electron injection were discussed in detail. One recent discovery, plasmon-induced electron injection from a gold nanoparticle to a Ti02 nanoparticle, was presented to show how femtosecond visible-pump/IR-probe transient absorption spectroscopy is useful in studying this kind of new charge transfer dynamics in a nano-structured system. [Pg.312]

Pump-probe absorption experiments on the femtosecond time scale generally fall into two effective types, depending on the duration and spectral width of the pump pulse. If tlie pump spectrum is significantly narrower in width than the electronic absorption line shape, transient hole-burning spectroscopy [101. 102. 103. 104. 105. 106. 107. 108. 109. 110. 111. 112 and 113] can be perfomied. The second type of experiment, dynamic absorption spectroscopy [57, 114. 115. 116. 117. 118. 119. 120. 121 and 122], can be perfomied if the pump and probe pulses are short compared to tlie period of the vibrational modes that are coupled to the electronic transition. [Pg.1979]

We investigated the ultrafast dynamics in a Na-NaBr melt at 1073 K by fs pump probe absorption spectroscopy. A simple model was used to simulate the dynamics of polaron-, bipolaron- and Drude-type electrons. The relaxation times for polarons and bipolarons are 210 fs and 3 ps, respectively. The existence of an isosbestic point at 1.35 eV indicates an inter-conversion between bipolarons and Drude-type electrons. [Pg.249]

Ellington et al.40) used femtosecond pump-probe spectroscopy to probe directly the arrival of electrons injected into the TiOz film with near- and mid-IR that probe the absorption at 1.52 jum and in the range of 4.1-7.0 jUm. Their measurements indicate an instrument limited 50 fsec upper limit on the electron injection time. These observations suggest that electron injection from Dye 2 to... [Pg.347]

Figure 8. Absorption spectra for two isomers I and II of Na3p2 obtained from one electron frozen ionic bonds approximation [46] (upper part). Scheme of the multistate fs dynamics for NeExPo pump-probe spectroscopy of NasF2 including conical intersection with structures and energy intervals for the pump and probe steps [46]. See color insert. Figure 8. Absorption spectra for two isomers I and II of Na3p2 obtained from one electron frozen ionic bonds approximation [46] (upper part). Scheme of the multistate fs dynamics for NeExPo pump-probe spectroscopy of NasF2 including conical intersection with structures and energy intervals for the pump and probe steps [46]. See color insert.
Transient intermediates are most commonly observed by their absorption (transient absorption spectroscopy see ref. 185 for a compilation of absorption spectra of transient species). Various other methods for creating detectable amounts of reactive intermediates such as stopped flow, pulse radiolysis, temperature or pressure jump have been invented and novel, more informative, techniques for the detection and identification of reactive intermediates have been added, in particular EPR, IR and Raman spectroscopy (Section 3.8), mass spectrometry, electron microscopy and X-ray diffraction. The technique used for detection need not be fast, provided that the time of signal creation can be determined accurately (see Section 3.7.3). For example, the separation of ions in a mass spectrometer (time of flight) or electrons in an electron microscope may require microseconds or longer. Nevertheless, femtosecond time resolution has been achieved,186 187 because the ions or electrons are formed by a pulse of femtosecond duration (1 fs = 10 15 s). Several reports with recommended procedures for nanosecond flash photolysis,137,188-191 ultrafast electron diffraction and microscopy,192 crystallography193 and pump probe absorption spectroscopy194,195 are available and a general treatise on ultrafast intense laser chemistry is in preparation by IUPAC. [Pg.94]

Pump-probe absorption experiments on the femtosecond time scale generally fall into two effective types, depending on the duration and spectral width of the pump pulse. If the pump spectrum is significantly narrower in width than the electronic absorption line shape, transient hole-burning spectroscopy [101. 102. [Pg.1979]


See other pages where Pump-probe electronic absorption spectroscopy is mentioned: [Pg.244]    [Pg.121]    [Pg.244]    [Pg.24]    [Pg.28]    [Pg.308]    [Pg.300]    [Pg.263]    [Pg.1968]    [Pg.123]    [Pg.244]    [Pg.31]    [Pg.145]    [Pg.221]    [Pg.433]    [Pg.363]    [Pg.372]    [Pg.80]    [Pg.111]    [Pg.343]    [Pg.638]    [Pg.639]    [Pg.341]    [Pg.106]    [Pg.227]    [Pg.182]    [Pg.35]    [Pg.158]    [Pg.16]    [Pg.158]    [Pg.332]    [Pg.338]    [Pg.263]    [Pg.1968]    [Pg.1979]    [Pg.540]    [Pg.221]   


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Absorption Probes

Absorption pumps

Electron absorption

Electron absorption spectroscopy

Electron probes

Electron pumping

Electronic absorption

Electronic absorption spectroscopy

Electronic absorption spectroscopy probes

Electronic pumps

Pump probe absorption spectroscopy

Pump-probe

Pump-probe absorption

Spectroscopy probes

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