29,637 research outputs found

    Radial distribution functions of water: Models vs experiments

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    We study the temperature behavior of the first four peaks of the oxygen-oxygen radial distribution function of water, simulated by the TIP4P/2005, MB-pol, TIP5P, and SPC/E models and compare to experimental X-ray diffraction data, including a new measurement which extends down to 235 K [H. Pathak et al., J. Chem. Phys. 150, 224506 (2019)]. We find the overall best agreement using the MB-pol and TIP4P/2005 models. We observe, upon cooling, a minimum in the position of the second shell simulated with TIP4P/2005 and SPC/E potentials, located close to the temperature of maximum density. We also calculated the two-body entropy and the contributions coming from the first, second, and outer shells to this quantity. We show that, even if the main contribution comes from the first shell, the contribution of the second shell can become important at low temperature. While real water appears to be less ordered at short distance than obtained by any of the potentials, the different water potentials show more or less order compared to the experiments depending on the considered length-scale

    Translational and rotational dynamics of high and low density TIP4P/2005 water

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    We use molecular dynamics simulations using TIP4P/2005 to investigate the self- and distinct-van Hove functions for different local environments of water, classified using the local structure index as an order parameter. The orientational dynamics were studied through the calculation of the time-correlation functions of different-order Legendre polynomials in the OH-bond unit vector. We found that the translational and orientational dynamics are slower for molecules in a low-density local environment and correspondingly the mobility is enhanced upon increasing the local density, consistent with some previous works, but opposite to a recent study on the van Hove function. From the analysis of the distinct dynamics, we find that the second and fourth peaks of the radial distribution function, previously identified as low density-like arrangements, show long persistence in time. The analysis of the time-dependent interparticle distance between the central molecule and the first coordination shell shows that particle identity persists longer than distinct van Hove correlations. The motion of two first-nearest-neighbor molecules thus remains coupled even when this correlation function has been completely decayed. With respect to the orientational dynamics, we show that correlation functions of molecules in a low-density environment decay exponentially, while molecules in a local high-density environment exhibit bi-exponential decay, indicating that dynamic heterogeneity of water is associated with the heterogeneity among high-density and between high-density and low-density species. This bi-exponential behavior is associated with the existence of interstitial waters and the collapse of the second coordination sphere in high-density arrangements, but not with H-bond strength

    Letter from Franklin K. Lane, Secretary of the Interior, to Representative Hayden

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    Letter from Franklin K. Lane to Carl T. Hayden expressing his support for bill S.390 in establishing the Grand Canyon as a National Park

    Measurement of the ratio of branching fractions B(B0→K∗0γ )/B(B0s→φγ ) and the directCP asymmetry inB 0→K∗0γ

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    The ratio of branching fractions of the radiative B decays B0→K⁎0γ and B0s→ϕγ has been measured using an integrated luminosity of 1.0 fb−1 of pp collision data collected by the LHCb experiment at a centre-of-mass energy of s√=7TeV. The value obtained is B(B0→K⁎0γ)B(B0s→ϕγ)=1.23±0.06(stat.)±0.04(syst.)±0.10(fs/fd), where the first uncertainty is statistical, the second is the experimental systematic uncertainty and the third is associated with the ratio of fragmentation fractions fs/fd. Using the world average value for B(B0→K⁎0γ), the branching fraction B(B0s→ϕγ) is measured to be (3.5±0.4)×10−5. The direct CP asymmetry in B0→K⁎0γ decays has also been measured with the same data and found to be ACP(B0→K⁎0γ)=(0.8±1.7(stat.)±0.9(syst.))%. Both measurements are the most precise to date and are in agreement with the previous experimental results and theoretical expectations

    DNA fusion gene vaccination mobilizes effective anti-leukemic cytotoxic T lymphocytes from a tolerized repertoire

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    The majority of known human tumor-associated antigens derive from non-mutated self proteins. T cell tolerance, essential to prevent autoimmunity, must therefore be cautiously circumvented to generate cytotoxic T cell responses against these targets. Our strategy uses DNA fusion vaccines to activate high levels of peptide-specific CTL. Key foreign sequences from tetanus toxin activate tolerance-breaking CD4+ T cell help. Candidate MHC class Ibinding tumor peptide sequences are fused to the C terminus for optimal processing and presentation. To model performance against a leukemia-associated antigen in a tolerized setting, we constructed a fusion vaccine encoding an immunodominant CTL epitopederived from Friend murine leukemia virus gag protein (FMuLVgag) and vaccinated tolerant FMuLVgag-transgenic (gag-Tg) mice. Vaccination with the construct induced epitopespecificIFN-c-producing CD8+ T cells in normal and gag-Tg mice. The frequency and avidity of activated cells were reduced in gag-Tg mice, and no autoimmune injury resulted. However, these CD8+ T cells did exhibit gag-specific cytotoxicity in vitro and in vivo. Also, epitope-specific CTL killed FBL-3 leukemia cells expressing endogenous FMuLVgag antigen and protected against leukemia challenge in vivo. These results demonstrate a simple strategy to engage anti-microbial T cell help to activate epitope-specific polyclonal CD8+ T cell responses from a residual tolerized repertoire

    The K-T Extinction

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    This chapter from the book History of Life describes the results of the K-T extinction and looks at the Impact theory and a giant volcanic eruption as possible causes. The essay covers the catastrophic scenarios for extinction that could result from these events. After reviewing the paleontological record across the K-T boundary, the author concludes that it is not clear that the catastrophes themselves can explain the extinction patterns that we see in the fossil record. Educational levels: Graduate or professional, Undergraduate lower division, Undergraduate upper division

    Excitation and dissociation of 3-chloro-3-methyldiazirine and 1-pyrazoline by low-energy electron impact

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    PT: J; CR: BATES DR, 1950, PHILOS T R SOC LON A, V243, P93 BRIDGE MR, 1969, J CHEM SOC A, P91 BUBERT H, 1971, J PHYS CHEM-US, V75, P769 CRAWFORD RJ, 1965, J AM CHEM SOC, V87, P3023 CRAWFORD RJ, 1966, J AM CHEM SOC, V88, P3959 DOERING JP, 1965, J CHEM PHYS, V42, P395 FINN TG, 1972, J CHEM PHYS, V56, P5632 FUKUI I, 1977, J PHYS CHEM, V81, P1252 FUKUI K, 1972, B CHEM SOC JPN, V45, P2278 FUKUI K, 1975, SHITSURYO BUNSEKI, V23, P105 GRAHAM WH, 1965, J AM CHEM SOC, V87, P4396 HOLLAND RF, 1972, J CHEM PHYS, V56, P5229 KNOWLTON JW, 1949, J RES NBS, V43, P113 LAIDLER KJ, 1955, CHEM KINETICS EXCITE, P21 LAUFER A, 1972, J PHYS CHEM-US, V76, P3504 LIU MTH, 1974, CHEM ENG NEWS 0909, P3 MASSEY HSW, 1931, P R SOC LOND A-CONTA, V132, P605 OCHKUR VI, 1964, SOV PHYS JETP, V18, P503 OPPENHEIMER JR, 1928, PHYS REV, V32, P361 PENNEY WG, 1932, PHYS REV, V39, P467 ROSENSTOCK HM, 1977, J PHYS CHEM REF D S1, V6 VROOM DA, 1969, J CHEM PHYS, V50, P573; NR: 22; TC: 4; J9: J PHYS CHEM; PG: 4; GA: KS409Source type: Electronic(1

    Local curvature-dimension condition implies measure-contraction property

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    AbstractWe prove that for non-branching metric measure spaces the local curvature condition CDloc(K,N) implies the global version of MCP(K,N). The curvature condition CD(K,N) introduced by the second author and also studied by Lott and Villani is the generalization to metric measure space of lower bounds on Ricci curvature together with upper bounds on the dimension. This paper is the following step of Bacher and Sturm (2010) [1] where it is shown that CDloc(K,N) is equivalent to a global condition CD⁎(K,N), slightly weaker than the usual CD(K,N). It is worth pointing out that our result implies sharp Bishop–Gromov volume growth inequality and sharp Poincaré inequality

    Structural determination of metallofullerene SC3C82 revisited: A surprising finding

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    PT: J; CR: AKASAKA T, 2000, J AM CHEM SOC, V122, P9316 AKASAKA T, 2001, J PHYS CHEM B, V105, P2971 AKASAKA T, 2002, ENDOFULLERENES NEW F BECKE AD, 1988, PHYS REV A, V38, P3098 BECKE AD, 1993, J CHEM PHYS, V98, P5648 CHAI Y, 1991, J PHYS CHEM-US, V95, P7564 FOWLER PW, 1995, ATLAS FULLERENES, P255 FRANCL MM, 1982, J CHEM PHYS, V77, P3654 HAY PJ, 1985, J CHEM PHYS, V82, P299 HEATH JR, 1985, J AM CHEM SOC, V107, P7779 KATO T, 1995, J PHYS CHEM-US, V99, P856 KOBAYASHI K, 1999, CHEM PHYS LETT, V313, P45 KOBAYASHI K, 2002, CHEM PHYS LETT, V362, P373 LEE C, 1988, PHYS REV B, V37, P785 NAGASE S, 1997, J MOL STRUC-THEOCHEM, V398, P221 NISHIBORI E, 1998, CHEM PHYS LETT, V298, P79 NISHIBORI E, 2000, CHEM PHYS LETT, V330, P497 NISHIBORI E, 2001, ANGEW CHEM INT EDIT, V40, P2998 NISHIBORI E, 2004, PHYS REV B, V69 SHINOHARA H, 1992, NATURE, V357, P52 SHINOHARA H, 1994, J PHYS CHEM-US, V98, P8597 STEVENSON S, 1999, NATURE, V401, P55 SUN BY, 2005, ANGEW CHEM INT EDIT, V44, P4568 TAKATA M, 1995, NATURE, V377, P46 TAKATA M, 1997, PHYS REV LETT, V78, P3330 TAKATA M, 1999, PHYS REV LETT, V83, P2214 TAKATA M, 2003, STRUCT CHEM, V14, P23 TAKATA M, 2004, STRUCT BOND, V109, P59 VANLOOSDRECHT PHM, 1994, PHYS REV LETT, V73, P3415 WAKAHARA T, 2002, CHEM PHYS LETT, V360, P235 WAKAHARA T, 2004, J AM CHEM SOC, V126, P4883 WANG CR, 2000, NATURE, V408, P426 WANG CR, 2001, ANGEW CHEM INT EDIT, V40, P397 YANNONI CS, 1992, SCIENCE, V256, P1191; NR: 34; TC: 6; J9: J AM CHEM SOC; PG: 2; GA: 966RQSource type: Electronic(1

    Heterogeneous and tissue-specific regulation of effector T cell responses by IFN-gamma during Plasmodium berghei ANKA infection.

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    IFN-γ and T cells are both required for the development of experimental cerebral malaria during Plasmodium berghei ANKA infection. Surprisingly, however, the role of IFN-γ in shaping the effector CD4(+) and CD8(+) T cell response during this infection has not been examined in detail. To address this, we have compared the effector T cell responses in wild-type and IFN-γ(-/-) mice during P. berghei ANKA infection. The expansion of splenic CD4(+) and CD8(+) T cells during P. berghei ANKA infection was unaffected by the absence of IFN-γ, but the contraction phase of the T cell response was significantly attenuated. Splenic T cell activation and effector function were essentially normal in IFN-γ(-/-) mice; however, the migration to, and accumulation of, effector CD4(+) and CD8(+) T cells in the lung, liver, and brain was altered in IFN-γ(-/-) mice. Interestingly, activation and accumulation of T cells in various nonlymphoid organs was differently affected by lack of IFN-γ, suggesting that IFN-γ influences T cell effector function to varying levels in different anatomical locations. Importantly, control of splenic T cell numbers during P. berghei ANKA infection depended on active IFN-γ-dependent environmental signals--leading to T cell apoptosis--rather than upon intrinsic alterations in T cell programming. To our knowledge, this is the first study to fully investigate the role of IFN-γ in modulating T cell function during P. berghei ANKA infection and reveals that IFN-γ is required for efficient contraction of the pool of activated T cells
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