Abstract:For the electron acceptor/donor molecule N-phenylpyrrole (PP), the fast intramolecular charge transfer (ICT) reaction accompanied by dual fluorescence from a locally excited (LE) and an ICT state is investigated in alkyl cyanide solvents as a function of temperature. After a comparison of the X-ray crystal structure of PP with calculations from the literature, absorption and fluorescence spectra of PP in a series of solvents over a wide polarity range are discussed. ICT with PP strongly depends on solvent pola… Show more
“…2, the twist angle, \C2-N1-C6-C11, is negligibly small from both methods. The small twist angle implies that the first excited state of PP has almost planar geometry, which is consistent to the reported results by other authors [46,48,49]. The calculated structural parameters show that PP has also a Q-like geometry (listed in Fig.…”
Section: Properties and Structures Of Ground State Le State And Ict supporting
“…2, the twist angle, \C2-N1-C6-C11, is negligibly small from both methods. The small twist angle implies that the first excited state of PP has almost planar geometry, which is consistent to the reported results by other authors [46,48,49]. The calculated structural parameters show that PP has also a Q-like geometry (listed in Fig.…”
Section: Properties and Structures Of Ground State Le State And Ict supporting
“…As a consequence, the reciprocal of the shortest decay time t 2 is approximately equal to the LE!ICT rate constant k a (Scheme 1), see Equation (10). Although the apparent times t 2 obtained from the global analysis of the LE and ICT decays in Figures 6 and 7 are definitely too short (0.5-1.0 ps, i.e., the LE decay is hardly different from the excitation pulse) to be by themselves meaningful in the SPC experiments, [6,24,31] the absence of an LE decay time longer than 1 ps is of importance in the analysis of the LE and ICT femtosecond transient absorption measurements of the XABN4Fs in the following section.…”
Section: Le Picosecond Decays In N-hexane and Mecnmentioning
confidence: 94%
“…The excitation wavelength was 308 nm (XeCl, Lambda Physik EMG 101 excimer laser) with perylene as quencher, [29,30] or 266 nm from a frequency-quadrupled Nd:YAG laser (Continuum Surelight) when the energy acceptor was anthracene. [31] In view of the relatively short triplet lifetime of the XABN4Fs (11-19 ms), a 3-9 % correction was necessary, to compensate for the loss of transient absorption intensity caused by the competition of the first-order triplet decay and the energy transfer process.…”
Section: Methodsmentioning
confidence: 99%
“…The picosecond laser system (excitation wavelength l exc : 276 nm) consists of a mode-locked titanium-sapphire laser (Coherent, MIRA 900F) pumped by an argon ion laser (Coherent, Innova 415). [31] The instrument response function of the laser SPC system has a full width at half maximum (FWHM) of 19 ps. The time range was 300 ps (0.5 ps per channel in 1200 effective channels).…”
The five 2,3,5,6-tetrafluoro-4-aminobenzonitriles XABN4F with a dimethyl-amino (DMABN4F), diethyl-amino (DEABN4F), azetidinyl (AZABN4F), methyl-amino (MABN4F) or amino (ABN4F) group undergo ultrafast intramolecular charge transfer (ICT) at room temperature, in the polar solvent acetonitrile (MeCN) as well as in the nonpolar n-hexane. ICT also takes place with the corresponding non-fluorinated aminobenzonitriles DMABN, DEABN and AZABN in MeCN, whereas for these molecules in n-hexane only minor (DMABN, DEABN) or no (AZABN) ICT fluorescence is detected. For the secondary (MABN) and primary (ABN) amines, an ICT reaction does not occur, which makes ABN4F the first electron donor/acceptor molecule with an NH(2) group for which ICT is observed. The ICT state of the XABN4Fs has a dipole moment of around 14 D, clearly smaller than that of DMABN (17 D). This difference is attributed to the electron withdrawing from the CN group to the phenyl ring, exerted by the four F-substituents. The reaction from the initially prepared locally excited (LE) to the ICT state in n-hexane proceeds in the sub-picosecond time range: 0.35 ps (DMABN4F), 0.29 ps (DEABN4F) and 0.13 ps (AZABN4F), as determined from femtosecond transient absorption measurements. In the highly polar solvent MeCN, an ICT reaction time of around 90 fs is observed for all five XABN4Fs, irrespective of the nature of their amino group. This shows that with these molecules in MeCN the ICT reaction rate is limited by the solvent dielectric relaxation time of MeCN, for which a value of around 90 fs has been reported. It is therefore concluded that, during this ultrashort ICT reaction, a large-amplitude motion such as a full 90 degrees twist of the amino group is unlikely to occur in the XABN4Fs. The ICT state of the XABN4Fs is strongly quenched via internal conversion (IC), with a lifetime tau'(0) (ICT) down to 3 ps, possibly by a reaction passing through a conical intersection made accessible due to a deformation of the phenyl group by out-of-plane motions induced by vibronic coupling between low-lying pisigma* and pipi* states in the XABN4Fs.
“…The triplet yields (F ISC ) of the DMAP and its complexed forms were measured by laser flash photolysis using the energy transfer method with anthracene as energy acceptor [5]. The excitation wavelength was 266 nm, from a frequency-quadrupled Nd:YAG laser (Continuum Surelight).…”
Section: Determination Of the Triplet Formation Yield Of Dmap And Itsmentioning
Hydrogen-bonded complex formation often modifies significantly the physicochemical, spectroscopic and kinetic properties of organics. This observation is even more straightforwardly valid if the properties of the electronic excited states are considered. When the solvents have protic character, the absorption and emission maxima of the fluorophores shift out from the usual range; in addition, the quantum yields and the lifetimes of the excited molecules are often very dissimilar to those expected in solvents of comparable polarity. The first step to account for these phenomena is to construct a proper thermodynamic description of the excited-state hydrogen bonding process; however, relatively little effort has been made to develop a concise handling. The difficulties probably originate from the complex nature of the interaction (weak, competing solute-solvent and solvent-solvent interactions, where the distribution of the interaction energies are comparable), and from the fact that the lifetimes of the excited states are in the same range than the characteristic time of the processes in question.In this chapter, an inchoative but consistent methodology for dealing with this phenomenon is shown. Model systems where the effects are great enough for clear conclusions to be drawn and where disturbing side processes are probably negligible were chosen for examination. The hydrogen bond forming reactants were aliphatic alcohols, mostly fluorinated ones. By using a homologue series of alcohols, the effect of reaction enthalpy can be kept under control. The solvents used in this study were exclusively aprotic, first and foremost n-hexane. In paraffin solvents, not only are the solvent-solute and solvent-reactant interactions negligible but also the examined effects and interactions are much more pronounced.
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