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Pavel Matousek

Publications and source records attributed to Pavel Matousek.

44 records · Page 3Linked to original sources

Direct observation of competitive ultrafast CO dissociation and relaxation of an MLCT excited state: picosecond time-resolved infrared spectroscopic study of [Cr(CO)(4)(2,2'-bipyridine)].

Early excited-state dynamics of [Cr(CO)(4)(bpy)] were studied in a CH(2)Cl(2) solution by picosecond time-resolved IR spectroscopy, which made it possible to characterize structurally the individual species involved and to follow separately the temporal evolution of the IR bands due to the bleached ground-state absorption, the fac-[Cr(CO)(3)(Sol)(bpy)] photoproduct, and two (3)MLCT states. It was found that the fac-[Cr(CO)(3)(Sol)(bpy)] photoproduct is formed alongside population of two (3)MLCT states during the first picosecond after excitation at 400 or 500 nm by a branched evolution of the optically populated excited state. Vibrationally relaxed (3)MLCT excited states are unreactive, decaying directly to the ground state on a picosecond time scale. The photoproduct is long-lived, persistent into the nanosecond time domain. Changing the excitation wavelength from 400 to 500 nm strongly increases the extent of the bleach recovery and decreases the yield of the photoproduct formation relative to the initial yield of the population of the unreactive (3)MLCT states. The photochemical quantum yield of CO dissociation also decreases with increasing excitation wavelength (Víchová, J.; Hartl, F.; Vlcek, A., Jr. J. Am. Chem. Soc. 1992, 114, 10903). These observations demonstrate the relationship between the early dynamics of optically populated excited states and the overall outcome of a photochemical reaction and identify the limiting role of the branching of the initial excited-state evolution between reactive and relaxation pathways as a more general principle of organometallic photochemistry.

Journal Article↗

Picosecond Kerr-gated time-resolved resonance Raman spectroscopy of the [Ru(phen)(2)dppz](2+) interaction with DNA.

To investigate the basis of the 'light-switch' effect, the solvent dependence of the Kerr-gated picosecond-time resolved resonance Raman (TR(3)) spectra of [Ru(bpy)(2)dppz](2+), [Ru(phen)(2)dppz](2+), and the modified complex [Ru(phen)(2)cpdppzOMe](2+) and a dimer [mu-C4(cpdppz)(2)-(phen)(4)Ru(2)](4+) were studied. The investigation focussed on comparing the behaviour of [Ru(phen)(2)dppz](2+) in acetonitrile, ethanol, H(2)O, D(2)O, and DNA. The data are consistent with a model wherein excitation induces metal-to-ligand charge transfer (MLCT) to any of the ligands (termed the 'precursor' state) which, by interligand electron transfer (ILET), produces an excited state localised on the dppz ligand, MLCT(1). In water this state relaxes with a characteristic time of approximately 6 ps to a non-emissive state (MLCT(2)). The TR(3) spectra in water, acetonitrile and DNA are all distinctly different. However, the early (4 ps) water spectrum resembles the spectrum in DNA. This interesting observation suggests that the DNA-bound excited state of the complex can be thought of as a model for the initial, poorly solvated state in water.

Acetonitriles↗

Structural features of two distinct molecular complexes of copper(II) cationic porphyrin and deoxyribonucleotides.

The associations of the water-soluble cationic copper(II)-5,10,15,20-meso-tetrakis(4-N-methylpyridyl) porphyrin (CuP) with d(pT)9 oligothymidylate and its building blocks deoxythymidine (dT) and deoxythymidine 5'-monophosphate (dTMP) were investigated by spectrophotometric titration [absorption, nanosecond transient resonance Raman (ns-RR) and picosecond time-resolved resonance Raman (ps-TR3) spectroscopies] to elucidate the structural requirements for the CuP exciplex formation in molecular complexes with unchained mononucleotides. In the d(pT)9 a factor analysis and global fit of the CuP absorption spectra revealed the formation of a single spectral species attributable to a 1 : 1 CuP. d(pT)9 complex throughout a wide range of d(pT)9/CuP ratios (0-10). Using ps-TR3 spectroscopy, the CuP. d(pT)9 complex was shown to be fully responsible for exciplex formation. In contrast, CuP mixed with dTMP ([dTMP]/[CuP] < 3000) yielded two spectroscopically distinct types of molecular complexes with 1 : 1 (CuP. dTMP) and 1 : 2 (CuP. (dTMP)2) (or even higher for [dTMP]/[CuP] > 3000) stoichiometry, the latter being spectroscopically identical to the CuP. d(pT)9 and providing a microenvironment favorable for exciplex formation to the same extent as the oligothymidylate. On the other hand, the 1 : 1 CuP. dTMP complex (prevailing for [dTMP]/[CuP] < 100) yielded no exciplex features. Similar behavior was observed for the CuP complexed with dT. To explain the difference in the ability of the CuP. dTMP and CuP. (dTMP)2 species to form the exciplex, two types of molecular complexes were suggested and discussed, differing in the orientation of the thymine planes with respect to the porphyrin macrocycle.

Cations↗

Kerr-gated time-resolved Raman spectroscopy of equine cortical bone tissue.

Picosecond time-resolved Raman spectroscopy in equine cortical bone tissue is demonstrated. Using 400-nm pulsed laser excitation (1 ps at 1 kHz) it is shown that Kerr cell gating with a 4-ps window provides simultaneously time-resolved rejection of fluorescence and time-resolved Raman scatter enabling depth profiling through tissue. The Raman shifts are the same as those observed by conventional cw Raman spectroscopy using deep-red or near-infrared lasers. The time decay of Raman photons is shown to fit an inverse square root of time function, suggesting propagation by a diffusive mechanism. Using polystyrene behind a bone specimen, it is shown that the 400-nm laser light penetrates at least 0.31 mm below the surface of a fully mineralized bone tissue specimen and generates observable bone Raman scatter (approximately 415 to 430 nm) through most of this depth. These novel results demonstrate great promise for in vivo applications for studying diseased bone tissue, and ways to optimize the setup are discussed.

Animals↗

Use of picosecond Kerr-gated Raman spectroscopy to suppress signals from both surface and deep layers in bladder and prostate tissue.

Raman spectroscopy is an optical technique able to interrogate biological tissues, giving us an understanding of the changes in molecular structure that are associated with disease development. The Kerr-gated Raman spectroscopy technique uses a picosecond pulsed laser as well as fast temporal gating of collected Raman scattered light. Prostate samples for this study were obtained by taking a chip at the transurethral resection of the prostate (TURP), and bladder samples from a biopsy taken at transurethral resection of bladder tumor (TURBT) and TURP. Spectra obtained through the bladder and prostate gland tissue, at different time delays after the laser pulse, clearly show change in the spectra as depth profiling occurs, eventually showing signals from the uric acid cell and urea cell, respectively. We show for the first time, using this novel technique, that we are able to obtain spectra from different depths through both the prostate gland and the bladder. This has major implications in the future of Raman spectroscopy as a tool for diagnosis. With the help of Raman spectroscopy and Kerr gating, it may be possible to pick up the spectral differences from a small focus of adenocarcinoma of the prostate gland in an otherwise benign gland, and also stage the bladder cancers by assessing the base of the tumor post resection.

Adenocarcinoma↗