Gravitational corrections to energy-levels of a hydrogen atom

The first-order perturbations of the energy levels of a hydrogen atom in central internal gravitational field are investigated. The internal gravitational field is produced by the mass of the atomic nucleus. The energy shifts are calculated for the relativistic 1S, 2S, 2P, 3S, 3P, 3D, 4S, and 4P levels with Schwarzschild metric. The calculated results show that the gravitational corrections are sensitive to the total angular momentum quantum number.

B-(*())(B)over-bar(()*()) intermediate states contribution to Gamma(4S, 5S) -> eta(b) + gamma radiative decay

In this work, we investigate the rescattering effects in the radiative decay Gamma(5S) -> eta(b) + gamma , which were suggested to be crucially important for understanding the anomalous largeness of the branching ratios B(Gamma(5S) -> Gamma(1S) + pi pi) and B(Gamma(5S) -> Gamma(1S) + eta). Our calculations show that the rescattering effects may enhance Gamma(Gamma(10860) -> eta(b) +gamma) by four orders, but the tetraquark structure does not. Recently the BABAR and CLEO collaborations have measured the mass of eta(b) and the branching ratios B(Gamma(2S) -> eta(b) +gamma), B(Gamma(3S) -> eta(b) +gamma). We hope that very soon, Gamma(10860) -> eta(b) + gamma) will be measured and it would be an ideal opportunity for testing whether the rescattering or the tetraquark structure is responsible for the anomaly of B(Gamma(5S) -> Gamma(nS) pi(+) pi(-))(n = 1, 2, 3)), i. e., the future measurements on the radiative decays of Gamma(5S) might be a touchstone of the two mechanisms.

Restudy on the wave functions of Gamma(nS) states in the light-front quark model and the radiative decays of Gamma(nS) -> eta(b) + gamma

The light-front quark model has been applied to calculate the transition matrix elements of heavy hadron decays. However, it is noted that using the traditional wave functions of the light-front quark model given in the literature, the theoretically determined decay constants of the Gamma(nS) obviously contradict the data. This implies that the wave functions must be modified. Keeping the orthogonality among the nS states and fitting their decay constants, we obtain a series of the wave functions for Gamma(nS). Based on these wave functions and by analogy with the hydrogen atom, we suggest a modified analytical form for the Gamma(nS) wave functions. Using the modified wave functions, the obtained decay constants are close to the experimental data. Then we calculate the rates of radiative decays of Gamma(nS) -> eta(b) + gamma. Our predictions are consistent with the experimental data on decays Gamma(3S) -> eta(b) + gamma within the theoretical and experimental errors.

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.

Iron XII to XXII spectra measurements between 250 and 400 angstrom

This paper reports laboratory measurements of the spectrum of the most abundant transition Fe ions in the universe. Spectrum of iron of low-lying excited states has been observed in the wavelength range 250-400 angstrom at Chinese Institute of Atomic Energy on the HI-13 tandem accelerator with beams of 130 MeV. A number of spectral lines have been mainly classified as transitions of magnesium-, sodium-, neon-, fluorine-like ions. A total of 54 lines have been measured. Most of them have been mainly ascribed to 3s3p(k)-3p(k+1), 3s(2)3p(k)-3s3p(k+1), 2p(5)3s-2p(5)3p, 3s3d-3p3d and 2p(5)3p-2p(5)3d resonance transitions. These spectral lines have been identified, among which 21 are new and accurately measured. The analysis of the spectra was based on a comparison with other experimental results and calculated values. (c) 2010 Elsevier Ltd. All rights reserved.

Relativistic photoionization cross sections for atomic Mg

The photoionization cross sections of the ground level (3s(2) S-1(0)) of atomic Mg have been studied theoretically in the energy region between the Mg+(3s) and Mg+(3p) threshold using the fully relativistic R-matrix method. The positions and widths of resonances have also been obtained and compared with a recent experiment (Wehlitz et al 2007 J. Phys. B 40 2385). Excellent agreement is shown between our theoretical calculations and experimental measurements. In the present calculations, five Rydberg series of doubly excited states have been exhibited, i.e. 3pns P-1, 3pnd P-1, 3pns P-3, 3pnd D-3 and 3pnd P-3, where 3pnd P-3 are confirmed as the fifth series in contrast to the previous theoretical results.

The effect of hyperfine interaction on the lifetime of the 3s3p P-3(2) level of Mg-like ions

On the basis of previous work, the hyperfine-induced 3s3p P-3(2) -> 3s(2) S-1(0) E1 transition probabilities of Mg-like ions were further calculated using the GRASP2K package based on the multiconfiguration Dirac-Hartree-Fock method. The contribution to the lifetime of the P-3(2) level from the 3s3p P-3(2) -> 3s(2) S-1(0) hyperfine-induced E1, 3s3p P-3(2) -> 3s3p P-3(1) M1, 3s3p P-3(2) -> 3s(2) S-1(0) M2 and 3s3p P-3(2) -> 3s3p P-3(0,1) E2 transition was discussed in detail. It was found that hyperfine interaction has an obvious effect on the lifetime at the beginning of the Mg-like isoelectronic sequence.

130Nd和140Tb的EC/ß+引衰变研究及其衰变纲图的建立

利用能量为220MeV左右的~(36)Ar重离子束轰击~(96)Ru和~(106)Cd浓缩同位素靶，通过Al降能片，使能量分布在161-176MeV之间，经过融合蒸发2p反应产生了缺中子同位素~(130)Nd, 经过融合蒸发pn反应生成~(140)Tb。藉助氦喷嘴带传输系统，用X-γ和γ-γ符合方法，分离鉴别了这两种核素，并进一步测定了它们的衰变性质。测定了~(130)Nd的半衰期为13 ± 3s，首次建议了它的EC/β~+衰变纲图，推测了其子核~(130)Pr的基态和低位能级的自旋宇称。修订了(140)Tb的原有极简单的EC/β~+衰变纲图，指认了~(140)Tb的基态自旋宇称为7~+。

GIS支持下岷江上游土壤侵蚀动态研究

利用TM数据,采用3S技术和通用土壤侵蚀方程(RUSLE)研究岷江上游地区3个典型时期的土壤侵蚀动态,并对影响侵蚀的主要因子进行初步分析.结果表明,研究区3个时期侵蚀面积分别占研究区总面积的1.28%、1.84%和1.70%;年平均侵蚀模数分别为832.64、1048.74和1362.11t.km-2,以微度侵蚀、轻度侵蚀为主,伴有少量的中度侵蚀.侵蚀面积比较小,侵蚀程度比较轻.侵蚀与坡度呈显著正相关,侵蚀大多发生在>25°的区域,1986年占总侵蚀量的93.65%,1995年为93.81%,2000年为92.71%;在海拔上,中山、亚高山、高山以及干旱河谷是侵蚀发生的主要地带,1986年占总侵蚀量的98.21%,1995年为97.63%,2000年为99.27%;不同类型的植被直接影响到侵蚀的发生,灌木林地以及新退耕的疏林地是3个时期侵蚀的主要发生地,过度放牧导致草场退化,也产生了微度侵蚀;侵蚀的发生和土壤类型密切相关,燥褐土、石灰性褐土最易发生侵蚀,是控制侵蚀的重点区域;人口的增长、户数的增加是侵蚀发生的驱动因子,人口与户数增长导致资源需求压力的增大,侵蚀呈线性增加.

Photodissociation dynamics of the methyl radical at 212.5 nm: Effect of parent internal excitation

Photodissociation dynamics of the CH3 radical at 212.5 nm has been investigated using the H atom Rydberg tagging time-of-flight method with a pure CH3 radical source generated by the photolysis of CH3I at 266 nm. Time-of-flight spectra of the H atom products from the photolysis of both cold and hot methyl radicals have been measured at different photolysis polarizations. Experimental results indicate that the photodissociation of the methyl radical in its ground vibrational state at 212.5 nm excitation occurs on a very fast time scale in comparison with its rotational period, indicating the CH3 dissociation at 212.5 nm occurs on the excited 3s Rydberg state surface. Experimental evidence also shows that the photodissociation of the methyl radical in the nu(2)=1 state of the umbrella mode at 212.5 nm excitation is characteristically different from that in the ground vibrational state. (C) 2004 American Institute of Physics.

基于RS和GIS的区域水土流失快速定量评价方法

区域水土流失的快速调查和评价对于水土保持宏观决策、灾情快速反应以及水土流失定期公告制的建立具有十分重要的意义。立足于区域水土流失问题的探索和 3S技术应用的研究 ,提出了区域水土流失宏观快速定量评价的方法及其实现的技术路线 ,并以整个黄土高原为研究区进行了实例研究 ,确定了一套适于该区水土流失宏观定量评价的指标 ,建立了相应的评价模型 ,并利用该模型对研究区一定年限内的水土流失状况进行了评价 ,获得了令人满意的结果

岷江上游景观变化研究——以汶川县为例

运用3S技术分析了岷江上游地区的景观变化,发现该区的景观是在逐年的破碎化,有林地是唯一一种减少的景观类型,草地、灌木林地、经济林、耕地和居民用地的面积在逐年的增加,而河流、湖泊和冰雪/裸岩的面积没有变化。在此基础上分析了景观变化的原因,认为人文因素是其变化的主要原因,人口的增长,加上片面追求地方经济的发展,森林资源的不合理、过度的开采,草地资源过度放牧和超载,导致了该区的生态环境受到巨大的破坏,森林面积减少,覆盖率降低,草场退化,水土流失严重。

岷江上游景观格局变化研究(英文)

岷江上游地区位于青藏高原向四川盆地的过渡地段,其源头到都江堰市,包括汶川县、茂县、理县、黑水县和松潘县五个县。它是四川省乃至全国的一个重要的林区。在过去的几十年里,其景观结构发生了重要的变化。本文应用3S 技术研究了该区在1986 年到2000 年之间的景观变化情况。该区的景观被划分为10 个景观生态类型,即耕地、有林地、灌木林地、经济林、草地、居民用地、河流、湖泊、沼泽和未利用地。研究结果表明,在岷江上游地区林地和草地是该区主要的景观类型,约占全区面积的91%,景观类型之间的变化主要发生在有林地、灌木林地、草地、耕地、居民用地和经济林之间,并且有林地面积从51.17%下降到47.56%。分析结果表明,岷江上游地区在过去的几十年里其景观的破碎化在加剧。图1表2 参20。

人类活动影响下岷江上游景观变化分析

综合利用多种数据源,结合3S技术,分析了岷江上游1986、1995和2000年3个时期的景观格局,重点探讨了森林、草地等主要景观类型在持续人类活动强度作用下的变化,确定了不同景观类型对人类活动强度的敏感程度。结果表明:1)岷江上游景观以草地、森林为主要景观类型。1986、1995和2000年3个时期森林、草地景观类型面积之和均高达96.1%、96.38%和95.23%,其它景观类型作为斑块镶嵌其中,森林和草地共同控制了整个研究区景观格局变化与生态过程;2)不同景观对人类活动强度的敏感性有显著差异。低强度的人类活动有利于有林地景观的恢复;高盖度草地对人类活动很敏感,严格减少干扰活动强度才有利于维持其景观;中盖度草地对中低强度的人类活动(如放牧)很敏感,景观退化,面积减少。

生境适宜度指数模型研究进展

生境适宜度指数(habitat suitability index,HSI)模型作为一种生境评价方法,在土地管理规划和评估中得到大量应用。本文总结了HSI模型在野生动物生境评价中的开发及应用,重点介绍了利用3S技术进行HSI建模及与其他模型耦合进行生境评价的现状;阐述了利用多种统计方法对HSI模型的评估和验证;探讨了HSI模型在主观性和非通用性等方面存在的问题和局限性,最后,就HSI模型在野生动物生境评价中的发展前景进行了展望。