Tellurium enhanced non-resonant third-order optical nonlinearity in a germano-silicate optical fiber

碲掺杂的高非线性石英光纤

All-optical switching application of germano-silicate optical fiber incorporated with Ag nanocrystals

银纳米晶体掺杂的高非线性石英光纤的全光转换应用

Intense green upconversion emission in Tb3+/Yb3+ co-doped alumino-germano-silicate optical fibers

Tb/Yb共掺的石英光纤的上转换绿光发光研究，研究了最佳浓度配比和发光机理。

圆斑蝰蛇毒磷脂酶A_2蛋白活性表现和分子进化探讨及菜花烙铁头、烙铁头蛇毒中Jerdonase、TmF的研究

磷脂酶AZ（PLA2）是蛇毒中含量较为丰富的一类作用于梭酷键的酶。迄今为止，己有多种形式的PLA2从不同地域、不同种属的蛇毒中得以纯化并进行了较为系统的研究。其中，以VipoXin为代表的异二聚体形式PLA2较为引人注目，原因在于这种形式不同于此类蛋白家族中的诸多其它个体。目前，己经有许多关于此异二聚体PL凡生物学特性的报道，包括对此类形式存在原因、活性变化、结构表现、系统进化等方面的讨论。然而至今，这种以异二聚体形式存在的PLA2仅发现于几种蛙亚科（ViperinaeSubfamily）蛇种的蛇毒中，其中就包括我国台湾岛的圆斑蜂蛇台湾亚种（Doboiarusselliiformosensis），而蝮亚科（CrotaiinaeSubfamil）蛇种的蛇毒至今却没有此类报道。我国大陆西南端接壤东南亚，存在于云南、福建一带的圆斑蛙蛇隶属圆斑蛙蛇泰国亚种（Daboiarusselliisiamensis），那么这种蛇毒中是否也含有异二聚体形式的PLA2呢？本工作就此疑问对云南产圆斑蛙蛇泰国亚种（D.r.siamensis）蛇毒中的PLA2进行了研究，结果得到三个新的PLAZ，分别命名为DRS-PLA2-I、DRS-PLA2-II和DRS-PLA2-III。其中，DRS-PLA2-I的分子量为13864.06Da，理论pI为4.56，PLA2活性为12.35μmol/mg/min；DRS-PLA2-II的分子量为13635.99Da，理论pI为8.74，PLA2活性为8.76μmol／mg/min；DRS-PLA2-III的分子量为13619.80Da，理论厂为4.61，无PLA2活性。这三个蛋白酶N端的30个氨基酸残基恰好和三个阳性克隆的cDNA序列推导的蛋白序列吻合，结合已经报道的PLA2蛋白家族蛋白序列的保守性表现，我们可以断定它们之间存在对应关系。分子系统学分析表明DRS-PLA2-II和DRS-PLA2-III在进化关系上和蛙亚科的异二聚体PLA2关系较近，并且二者酶活性分别与异二聚体PLA2的Normalchain和Inhibitorchain相一致，只是没有发现类似Vipoxin形式的异二聚体结合蛋白。这些分析表明DRS-PLA2-nORS-PLA2-III类似圆斑蛙蛇台湾亚种（D.r.forlnos翻s沽）中的PV-4/RV-7，是PLA2异二聚体的一种特殊形式，在进化上滞后于VinOXin。另夕卜本工作还相继从云南产菜花烙铁头（Trimeresrusjerdonii）蛇毒和湖南产烙铁头（Trimeresurusmucrosquamatus）蛇毒中分离得到Jerdonase和TmF。前者为一个丝氨酸蛋白酶性质的、具有纤维蛋白原水解作用和激肤释放酶原水解作用双重活性表现的、高分子量的份五brinogenase，其活性表现可以被PMSF彻底抑制，而EDTA对此却没有影响。其它的几种抑制剂如大豆胰蛋白酶抑制剂、l-cysteine、DTT对Jerdonase的活性表现也有不同程度的影响。在Jerdonase的这些生化特性上中，分子量的大小和对纤维蛋白酶水解的特性这两方面有别于蛇毒中诸多其它来源的同类蛋白；后者T淤为一个舒缓激肚增强肤（BradykninPQtentiatingPePtide，BPP），电离质谱分析表明其分子量为1110.7Da。此小肚氨基酸序列为促进舒缓激肚（Bradki垃n，BK）诱导的豚鼠回肠纵行肌收缩的活力单位为（1.13±0.3）（m留L），T妊抑制血管紧张素转化酶（ACE）对BK水解的半数抑制剂量IC50为2μg。比较已报道的从Agkistrodon属和Bothrops属中纯化得到的BPP氨基酸序列发现：BPP的N端都是特征性的pGlu，C端为IIe-Pro-Pro，有高度的保守性。另外，TmF是Trimeresurus属中此类小肤的首次纯化。总之，本研究对国产的几种常见蛇毒中的几种常见蛋白多肤进行了一定程度的探讨和分析，和相同类别的其它蛋白、多肤比较可以看到，有许多相同的地方，也有许多不同的表现，研究结果为相应领域的深入研究提供资料和思路。

Possible way to synthesize superheavy element Z=117

Within the framework of the dinuclear system model, the production of superheavy element Z = 117 in possible projectile-target combinations is analysed systematically. The calculated results show that the production cross sections are strongly dependent on the reaction systems. Optimal combinations, corresponding excitation energies and evaporation channels are proposed, such as the isotopes Bk-248,Bk-249 in Ca-48 induced reactions in 3n evaporation channels and the reactions Sc-45+Cm-246,Cm-248 in 3n and 4n channels, and the system V-51+Pu-244 in 3n channel.

System size dependence of associated yields in hadron-triggered jets STAR Collaboration

We present results on the system size dependence of high transverse momentum di-hadron correlations at root s(NN) = 200 GeV as measured by STAR at RHIC. Measurements in d + Au, Cu + Cu and Au + Au collisions reveal similar jet-like near-side correlation yields (correlations at small angular separation Delta phi similar to 0, Delta eta similar to 0) for all systems and centralities. Previous measurements have shown Chat the away-side (Delta phi similar to pi) yield is suppressed in heavy-ion collisions. We present measurements of the away-side Suppression as a function of transverse momentum and centrality in Cu + Cu and Au + Au collisions. The suppression is found to be similar in Cu + Cu and An + An collisions at a similar number of participants. The results are compared to theoretical calculations based on the patron quenching model and the modified fragmentation model. The observed differences between data and theory indicate that the correlated yields presented here will further constrain dynamic energy loss models and provide information about the dynamic density profile in heavy-ion collisions. (C) 2009 Elsevier B.V. All rights reserved.

Measurement of the Bottom Quark Contribution to Nonphotonic Electron Production in p plus p Collisions at root s=200 GeV

The contribution of B meson decays to nonphotonic electrons, which are mainly produced by the semileptonic decays of heavy-flavor mesons, in p + p collisions at root s = 200 GeV has been measured using azimuthal correlations between nonphotonic electrons and hadrons. The extracted B decay contribution is approximately 50% at a transverse momentum of p(T) >= 5 GeV/c. These measurements constrain the nuclear modification factor for electrons from B and D meson decays. The result indicates that B meson production in heavy ion collisions is also suppressed at high p(T).

Higher Moments of Net Proton Multiplicity Distributions at RHIC

200 GeV corresponding to baryon chemical potentials (mu(B)) between 200 and 20 MeV. Our measurements of the products kappa sigma(2) and S sigma, which can be related to theoretical calculations sensitive to baryon number susceptibilities and long-range correlations, are constant as functions of collision centrality. We compare these products with results from lattice QCD and various models without a critical point and study the root s(NN) dependence of kappa sigma(2). From the measurements at the three beam energies, we find no evidence for a critical point in the QCD phase diagram for mu(B) below 200 MeV.

Three-Particle Coincidence of the Long Range Pseudorapidity Correlation in High Energy Nucleus-Nucleus Collisions

We report the first three-particle coincidence measurement in pseudorapidity (Delta eta) between a high transverse momentum (p(perpendicular to)) trigger particle and two lower p(perpendicular to) associated particles within azimuth |Delta phi| < 0.7 in root s(NN) = 200 GeV d + Au and Au + Au collisions. Charge ordering properties are exploited to separate the jetlike component and the ridge (long range Delta eta correlation). The results indicate that the correlation of ridge particles are uniform not only with respect to the trigger particle but also between themselves event by event in our measured Delta eta. In addition, the production of the ridge appears to be uncorrelated to the presence of the narrow jetlike component.

gamma cross section in p plus p collisions at root s=200 GeV

We report on a measurement of the gamma(1S + 2S + 3S) -> e(+)e(-) cross section at midrapidity in p + p collisions at root s = 200 GeV. We find the cross section to be 114 +/- 38(stat + fit)(-24)(+23)(syst) pb. Perturbative QCD calculations at next-to-leading order in the color evaporation model are in agreement with our measurement, while calculations in the color singlet model underestimate it by 2 sigma. Our result is consistent with the trend seen in world data as a function of the center-of-mass energy of the collision and extends the availability of gamma data to RHIC energies. The dielectron continuum in the invariant-mass range near the gamma is also studied to obtain a combined yield of e(+)e(-) pairs from the sum of the Drell-Yan process and b-(b) over bar production.

Parton energy loss in heavy-ion collisions via direct-photon and charged-particle azimuthal correlations

Charged-particle spectra associated with direct photon (gamma(dir)) and pi(0) are measured in p + p and Au + Au collisions at center-of-mass energy root(S)(NN) = 200 GeV with the STAR detector at the Relativistic Heavy Ion Collider. A shower-shape analysis is used to partially discriminate between gamma(dir) and pi(0). Assuming no associated charged particles in the gamma(dir) direction ( near side) and small contribution from fragmentation photons (gamma(frag)), the associated charged-particle yields opposite to gamma(dir) (away side) are extracted. In central Au + Au collisions, the charged-particle yields at midrapidity (vertical bar eta vertical bar < 1) and high transverse momentum (3 < (assoc)(PT) < 16 GeV/c) associated with gamma(dir) and pi(0) (vertical bar eta vertical bar < 0.9, 8 < (trig)(PT) < 16 GeV/c) are suppressed by a factor of 3-5 compared with p + p collisions. The observed suppression of the associated charged particles is similar for gamma(dir) and pi(0) and independent of the gamma(dir) energy within uncertainties. These measurements indicate that, in the kinematic range covered and within our current experimental uncertainties, the parton energy loss shows no sensitivity to the parton initial energy, path length, or color charge.

Azimuthal di-hadron correlations in d plus Au and Au plus Au collisions at root s(NN)=200 GeV measured at the STAR detector

Yields, correlation shapes, and mean transverse momenta p(T) of charged particles associated with intermediate-to high-p(T) trigger particles (2.5 < p(T) < 10 GeV/c) in d + Au and Au + Au collisions at root s(NN) = 200 GeV are presented. For associated particles at higher p(T) greater than or similar to 2.5 GeV/c, narrow correlation peaks are seen in d + Au and Au + Au, indicating that the main production mechanism is jet fragmentation. At lower associated particle pT < 2 GeV/c, a large enhancement of the near- (Delta phi similar to 0) and away-side (Delta phi similar to pi) associated yields is found, together with a strong broadening of the away-side azimuthal distributions in Au + Au collisions compared to d + Au measurements, suggesting that other particle production mechanisms play a role. This is further supported by the observed significant softening of the away-side associated particle yield distribution at Delta phi similar to pi in central Au + Au collisions.

Balance functions from Au+Au, d+Au, and p+p collisions at root s(NN)=200 GeV

Balance functions have been measured for charged-particle pairs, identified charged-pion pairs, and identified charged-kaon pairs in Au + Au, d + Au, and p + p collisions at root s(NN) = 200 GeV at the Relativistic Heavy Ion Collider using the STAR detector. These balance functions are presented in terms of relative pseudorapidity, Delta eta, relative rapidity, Delta y, relative azimuthal angle, Delta phi, and invariant relative momentum, q(inv). For charged-particle pairs, the width of the balance function in terms of Delta eta scales smoothly with the number of participating nucleons, while HIJING and UrQMD model calculations show no dependence on centrality or system size. For charged-particle and charged-pion pairs, the balance functions widths in terms of Delta eta and Delta y are narrower in central Au + Au collisions than in peripheral collisions. The width for central collisions is consistent with thermal blast-wave models where the balancing charges are highly correlated in coordinate space at breakup. This strong correlation might be explained by either delayed hadronization or limited diffusion during the reaction. Furthermore, the narrowing trend is consistent with the lower kinetic temperatures inherent to more central collisions. In contrast, the width of the balance function for charged-kaon pairs in terms of Delta y shows little centrality dependence, which may signal a different production mechanism for kaons. The widths of the balance functions for charged pions and kaons in terms of q(inv) narrow in central collisions compared to peripheral collisions, which may be driven by the change in the kinetic temperature.

Inclusive pi(0), eta, and direct photon production at high transverse momentum in p plus p and d plus Au collisions at root s(NN)=200 GeV

We report a measurement of high-p(T) inclusive pi(0), eta, and direct photon production in p + p and d + Au collisions at root s(NN) = 200 GeV at midrapidity (0 < eta < 1). Photons from the decay pi(0) -> gamma gamma were detected in the barrel electromagnetic calorimeter of the STAR experiment at the Relativistic Heavy Ion Collider. The eta -> gamma gamma decay was also observed and constituted the first eta measurement by STAR. The first direct photon cross-section measurement by STAR is also presented; the signal was extracted statistically by subtracting the pi(0), eta, and omega(782) decay background from the inclusive photon distribution observed in the calorimeter. The analysis is described in detail, and the results are found to be in good agreement with earlier measurements and with next-to-leading-order perturbative QCD calculations.