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C P Lawrence

Publications and source records attributed to C P Lawrence.

7 recordsLinked to original sources

FADD deficiency sensitises Jurkat T cells to TNF-alpha-dependent necrosis during activation-induced cell death.

Activation-induced cell death (AICD) in activated T lymphocytes is largely mediated by Fas/Fas ligand (FasL) interaction. The cytoplasmic adaptor molecule Fas-associated death domain protein (FADD) plays an essential role in the apoptotic signalling of the Fas death pathway. In the present study, we observed that FADD deficient (FADD(-/-)) Jurkat T cells undergo AICD to a similar extent as wild-type cells. AICD in wild-type Jurkat T cells is via apoptosis, whereas it is non-apoptotic in FADD(-/-) cells. The latter took up propidium iodide, exhibit a loss in mitochondrial membrane potential and have no detectable cleavage products of caspase-8 or -3 activation, suggesting that these cells die by necrosis. Wild-type Jurkat T cells undergo apoptosis when incubated with recombinant FasL and Trail but not with TNF-alpha. In contrast, FADD(-/-) Jurkat T cells are resistant to FasL and Trail but die of necrosis when incubated with TNF-alpha. We showed that neutralising anti-TNF-alpha blocked AICD as well as TNF-alpha-induced necrosis in FADD(-/-) Jurkat T cells. Furthermore, down regulating the receptor interacting protein, RIP, with geldanamycin treatment, which is essential for TNF-alpha signalling, markedly inhibited AICD in FADD(-/-) Jurkat T cells. In addition, caspase-8-deficient Jurkat T cells are resistant to Fas- and TNF-alpha-induced cell death. Taken together, our results suggest that a deficiency in FADD and not caspase-8 or the inhibition of the Fas signalling pathway sensitises Jurkat T cells to TNF-alpha-dependent necrosis during AICD.

Adaptor Proteins, Signal Transducing↗

Quantum corrections in vibrational and electronic condensed phase spectroscopy: line shapes and echoes.

Various linear and nonlinear vibrational and electronic spectroscopy experiments in liquids are usually analyzed within the second-cumulant approximation, and therefore the fundamental quantity of interest is the equilibrium time-correlation function of the fluctuating transition frequency. In the usual approach the "bath" variables responsible for the fluctuating frequency are treated classically, leading to a classical time-correlation function. Alternatively, sometimes a quantum correction appropriate for relatively high temperatures is included, which adds an imaginary part to the classical time-correlation function. This approach, although appealing, does not satisfy detailed balance. One can consider a similar correction, but where detailed balance is satisfied, by using the harmonic quantum correction factor. In this article, we compare these approaches for a model system and two realistic examples. Our conclusion is that for linear spectroscopy the classical result is usually adequate, whereas for nonlinear spectroscopy it can be more important to include quantum corrections.

Chemistry↗

Dynamics of water probed with vibrational echo correlation spectroscopy.

Vibrational echo correlation spectroscopy experiments on the OD stretch of dilute HOD in H(2)O are used to probe the structural dynamics of water. A method is demonstrated for combining correlation spectra taken with different infrared pulse bandwidths (pulse durations), making it possible to use data collected from many experiments in which the laser pulse properties are not identical. Accurate measurements of the OD stretch anharmonicity (162 cm(-1)) are presented and used in the data analysis. In addition, the recent accurate determination of the OD vibrational lifetime (1.45 ps) and the time scale for the production of vibrational relaxation induced broken hydrogen bond "photoproducts" ( approximately 2 ps) aid in the data analysis. The data are analyzed using time dependent diagrammatic perturbation theory to obtain the frequency time correlation function (FTCF). The results are an improved FTCF compared to that obtained previously with vibrational echo correlation spectroscopy. The experimental data and the experimentally determined FTCF are compared to calculations that employ a polarizable water model (SPC-FQ) to calculate the FTCF. The SPC-FQ derived FTCF is much closer to the experimental results than previously tested nonpolarizable water models which are also presented for comparison.

Deuterium↗

Spectral diffusion in a fluctuating charge model of water.

We apply the combined electronic structure/molecular dynamics approach of Corcelli, Lawrence, and Skinner [J. Chem. Phys. 120, 8107 (2004)] to the fluctuating charge (SPC-FQ) model of liquid water developed by Rick, Stuart, and Berne [J. Chem. Phys. 101, 6141 (1994)]. For HOD in H(2)O the time scale for the long-time decay of the OD stretch frequency time-correlation function, which corresponds to the time scale for hydrogen-bond rearrangement in the liquid, is about 1.5 ps. This result is significantly longer than the 0.9 ps decay previously calculated for the nonpolarizable SPC/E water model. Our results for the SPC-FQ model are in better agreement with recent vibrational echo experiments.

Chemistry, Physical↗

On the mode-coupling theory of vibrational line broadening in near-critical fluids.

Molecular-dynamics simulations of a neat atomic fluid, coupled with a simple model for vibrational frequency perturbations, are used to investigate vibrational line broadening near the liquid-gas critical point. All features of our simulations are in qualitative agreement with recent Raman experiments on nitrogen. We also use our simulation results to assess the validity of the mode-coupling theories that have been used to analyze experiment. We find that the theoretical results are not in good agreement with simulation, both for the temperature dependence of the linewidth, and for the frequency time-correlation functions. However, the mode-coupling prediction that critical line broadening is due to the diverging correlation time of the frequency fluctuations is shown to be correct.

Journal Article↗

Combined electronic structure/molecular dynamics approach for ultrafast infrared spectroscopy of dilute HOD in liquid H2O and D2O.

We present a new approach that combines electronic structure methods and molecular dynamics simulations to investigate the infrared spectroscopy of condensed phase systems. This approach is applied to the OH stretch band of dilute HOD in liquid D2O and the OD stretch band of dilute HOD in liquid H2O for two commonly employed models of water, TIP4P and SPC/E. Ab initio OH and OD anharmonic transition frequencies are calculated for 100 HOD x (D2O)n and HOD x(H2O)n (n = 4-9) clusters randomly selected from liquid water simulations. A linear empirical relationship between the ab initio frequencies and the component of the electric field from the solvent along the bond of interest is developed. This relationship is used in a molecular dynamics simulation to compute frequency fluctuation time-correlation functions and infrared absorption line shapes. The normalized frequency fluctuation time-correlation functions are in good agreement with the results of previous theoretical approaches. Their long-time decay times are 0.5 ps for the TIP4P model and 0.9 ps for the SPC/E model, both of which appear to be somewhat too fast compared to recent experiments. The calculated line shapes are in good agreement with experiment, and improve upon the results of previous theoretical approaches. The methods presented are simple, and transferable to more complicated systems.

Journal Article↗

Quantum dynamics in simple fluids.

We use quantum-correction factors to calculate approximately the quantum velocity time-correlation function (TCF) of supercritical Lennard-Jones argon from the classical TCF. We find that for this quite classical system, several different quantum-correction schemes yield essentially identical results for the real and imaginary parts of the quantum TCF, and also agree well with the recent forward-backward semiclassical dynamics (FBSD) results of Wright and Makri [J. Chem. Phys. 119, 1634 (2003)]. We also consider a more quantum-mechanical fluid of lighter atoms (neon) at a lower temperature. In this case different quantum-correction schemes give different results. FBSD calculations show that the harmonic quantum correction factor works the best for this system

Journal Article↗