高能量

If it is a high energy place, increase your own energy level.

如果那时一个高能量的地方，请调高你的能量水平。

A high beam energy is also used to stimulate x-ray emission of higher-energy peaks.

高能量电子束也能用来激发高能量x射线峰的发射。

In medium and high energy groups, histological cholestasis presented characterized by bile plugs in bile ducts, proliferation of interlobular bile ducts, bile pigments in Kupffer cells and hepatocytes, and above performances were more severe in high energy group. In medium energy group, there was only mild liver steatosis, whereas there was significant steatosis in high energy TPN group, and fat accumulation was periportal in distribution.

中能量和高能量TPN组肝组织出现胆栓形成、小叶间胆管增生、肝细胞和枯否氏细胞内胆色素沉积等淤胆特征，而以高能量组较严重，在中能量组仅出现轻度肝脂肪变性，而高能量组出现明显肝脂肪变性，脂肪沉积主要分布于门静脉周围区。

Because the energy from unimolecular decomposition of TPPO_3 is notenough for emitting such light, we think it may be emitted by big excited molecularwhich was generated through bimolecular collision under the condition of highTPPO3 concentration.

因为TPPO_3单分子分解的能量不足以发出此种宽带辐射光，我们认为这是在TPPO_3浓度较高时，由两个TPPO_3分子碰撞生成较高能量激发态大分子所辐射的。

In RESEE, a fuzzy gradient classification based next hop strategy was designed to balance the energy consumption as a whole. Reject and recommend strategy of low residual energy node, and reactivate strategy of high residual energy node were applied to equilibrize the energy consumption locally.

协议对节点间的梯度进行模糊分级，并将模糊等级选择策略与质量评价函数相结合选择下一跳节点，以实现全局的能量均衡；协议采用低能量节点的拒绝与推荐策略、高能量节点的激活策略，以实现局部的能量均衡。

In chapter 4, by AREELS, the Generalized Oscillator Strength Density Spectra were measured in the energy region from 56 to 66eV, with the incident energy 2. 5 keV and energy resolution 80 meV, at scattering angles from 0°to 6°, corresponding to the momentum transfer K〓=0.03~2. 01 a. u. The Fano profile parameters f〓 and q for the optically allowed transition 〓(0, 1)〓P°and the optically forbidden transitions 〓(1, 0)〓S〓and 〓(1, 0)〓D〓 were obtained as a function of K〓. With the hyperspherical coordinate wavefunctions, the dynamical correlation are discussed qualitatively. So, a new experimental way to study dynamical electron correlation effect is opened.In chapter 5, the widely used R-matrix theory was introduced. Then, the GOSDS for the optically allowed excitation series (1s〓)〓S〓→〓(0, 1)〓P°(n=2-4) were calculated by this method, and the Fano profile parameters f〓 and q were obtained sequently. So the electron correlation effect can be described by these parameters quantitatively, and the theoretical results were compared with our AREELS experimental results.

在第四章中，实验上，同样使用角分辨的高能量分辨快电子能量损失谱仪，在2.5keV电子入射能量和80meV的能量分辨下，测量了0°到6°散射角下的He原子双电子激发态在56~66eV的广义振子强度密度谱，这种情况，0°~6°对应的动量转移范围K〓=0.03~2.01a.u。，得到了光学允许跃迁的双电子激发态〓（0，1）〓P〓和光学禁戒跃迁的双电子激发态〓（1，0）〓S〓、〓（1，0）〓D〓的Fano线形参数f〓，q等随动量转移变化的曲线；观测到了几个强度很弱、能级很窄的光学允许和禁戒跃迁双电子激发态，用前人准确的理论结果进行了标识；通过比较弱共振〓（1，0）〓S〓和〓（-1，0）〓S〓的强度随动量转移K〓的变化规律，结合超球坐标理论计算的波函数，定性地阐述了在电子碰撞散射过程中它们各自不同的动力学电子关联效应，发展了一套在实验上研究电子关联效应的新方法。

It used the help of a Swedish production of gold, Germany advanced forging process, selected high toughness and hardness of the high-alloy materials, the bionic magnetized, low-temperature gold-plated, antimicrobial technology, such as the United States to import equipment plastic micro-needle, the application of advanced beauty High technology and breakthroughs in genetic engineering of the characteristics of active ingredients, use of plastic micro-needle the United States, used "to the point of" infiltration of AMD technology, multi-point, uniform, comprehensive, in-depth the high-energy original fluid, directly transported to the Skin, containing a variety of nutrition and active components of high-energy original fluid, rapidly absorbed by the skin organizations, play a role, resulting in effect, promoting skin metabolism, and maintain skin elasticity and Jiaomei.

它借助一只采用瑞典生产纯金、德国先进的锻造工艺，精选高韧度、高硬度的合金材料，经过仿生磁化、低温镀金、抗菌等工艺的导入仪器美塑微针，应用先进美容高新科技，突破生物基因工程活性成份的特点，利用微针，采用&点到面&超微渗透技术，多点、均匀、全面、深入的把高能量原生液，直接输送到所需的皮肤组织，让含有多种营养及活性成分的高能量原生液，迅速被肌肤组织吸收，发挥作用，从而产生疗效，促进皮肤新陈代谢，保持皮肤弹性和姣美。

The accumulated self-exciting dose for Na-24 is only 1.12 mGy during its average life-time for irradiation of total thermal neutron fluence of 3.6E12 nth/cm^2. Conclusions: Because of the self-exciting dose reduced from neutron activation can be neglected for gamma dose measurement in neutron and gamma mixed field, and the threshold of linear response is 2 Gy, the FWT-70-40 dosimeter not only can be used for high dose rate Co-60 irradiation field and the high energy electron beam for medical purpose, but also can be used for gamma dose measurement in an epithermal neutron beam for boron neutron capture therapy.

型号FWT-70-4OM）剂量计於BNCT高中子通量与剂量的中子、加马混合辐射场所产生的自激剂量，对加马剂量度量干扰可忽略，且对加马的最低剂量限值为2Gy，因此除可应用於钴60加马高剂量辐射场与放射治疗用高能量、高剂量电子射束的剂量度量外，亦可应用於BNCT照射治疗用高能量、高剂量的中子、加马混合辐射场的加马剂量度量。

It appearsthat condensed-phase 〓 would be a high energy fuel with high calorific value andan ideal high energy density material. It has the advantages as follows:(1)releasesenergy through self-dissociation mode;(2)does not need carrying another substancesupplying oxygen;(3)produces the final product 〓 molecule, which has very highstability and no environmental pollution.

通过对〓的密度、爆速、爆压和比冲的理论计算，可以得出〓是一种具有很高热值的高能燃料，是一种理想的高能量密度材料，它通过自身的分解释放能量，不需要另外携带供氧物质，并产生具有高稳定性的、对环境无污染的〓分子作功。

In chapter 2 and 3, experimentally, using the Angular-Resolved high-resolution fast Electron Energy Loss Spectrometer , at the condition of 2. 5 keV incident energy and 50-60 meV energy resolution, we measured the Optical Oscillator Strength Density Spectra for the excitations of 4p, 4s or 3d electron. The oscillator strengths for excitations of the valent shell 4p electron were obtained, and comparisons were done between presently experimental and previously experimental and theoretical results. The experimental results of different groups agree with each other approximately, but the semi-experientially theoretical results do not match with the experimental results. The delayed maximum in the photoabsorption spectra was discussed. It should arise from the transition of 4p→∈d. For the excitation of the inner-valent 4s electron, the discrepancies for the resonant structures in previous electron-impact results and photoionization results were clarified in present work, which confirms again that the fast electron impact method is suitable to measure the optical oscillator strengths. The autoionization Rydberg series 4s〓ns (n=5, 6, 7) and 4s〓nd (n=4, 5, 6, 7) were identified without ambiguity by the measurement at 0°, 2° and 4°scattering angles. The energy levels and natural widths of the excitations of Kr3d and Ar2p inner shell, including optically allowed and forbidden transitions, were determined. The widths of these inner shell excitations are nearly the same, which was interpreted by the Resonant Auger effect .

在第二章和第三章，实验上，使用角分辨的高能量分辨快电子能量损失谱仪，在2.5keV电子入射能量和50-60meV能量分辨下，测量了Kr原子由价壳层4p到内价壳层4s，再到内壳层3d电子激发的光学振子强度密度谱；得到了价壳层4p电子激发束缚态的光学振子强度，与前人实验和半经验理论结果作了细致的比较，说明几家实验是比较符合的，但半经验的理论计算存在问题；分析了光吸收谱中的延迟极大现象，说明在第一电离阈值以上几个eV范围内的极大值源于4p→εd跃迁产生的延迟极大；对于内价壳层4s激发的自电离区，澄清了前人实验中电子碰撞方法和光学方法在共振结构上存在差异的问题，再一次肯定了快电子碰撞方法是获得绝对光学振子强度的一种好方法；通过在非0°散射角的测量（如2°和4°），清楚地标识了4s电子激发的光学禁戒跃迁自电离里德堡系列4s〓ns（n=5，6，7）和4s〓nd（n=4，5，6，7）；通过在0°和4°散射角的测量，观测并标识了几个新的内壳层光学禁戒跃迁能级，得到了Kr原子3d和Ar原子2p内壳层激发态（包括光学允许和禁戒跃迁形成的）的能级位置和自然宽度，用共振俄歇效应解释了这些内壳层激发态（不管是光学允许还是禁戒跃迁产生的）的自然宽度彼此比较接近的原因。

In the negative and interrogative forms, of course, this is identical to the non-emphatic forms.

。但是，在否定句或疑问句里，这种带有"do"的方法表达的效果却没有什么强调的意思。

Go down on one's knees;kneel down

屈膝跪下。。。下跪祈祷