非弹性散射

π~－－~（12）C非弹性散射与π介子放射疗法

π￣ & ￣( 12 ) c inelastic scattering and negative π - meson therapy

α粒子结构下的π-~（12）C非弹性散射

Pion - ~ ( 12 ) c inelastic scattering in the α - particle model

22MeV质子在~（13）C上弹性及非弹性散射微分截面的全微观分析

Full Microscopic Analysis of 22 MeV Proton Scattering from ~ ( 13 ) C Nucleus

硫化锰电子结构的软X射线共振非弹性散射研究

Electronic structure of MnS studied by resonant inelastic soft X-ray scattering

深度非弹性散射中小x区物理新进展

New Progresses in Deep Inelastic Scattering in Small x Region

电子非弹性散射辐射修正的R函数方法

The r - function method for radiative corrections to the electron inelastic scattering

π~±和K~±介子在Ca原子核上的非弹性散射

Inelastic scattering of pion and Kaon mesons on Ca nucleus

N湮没势对反质子-核非弹性散射和弹性散射进行研究是少有的研究方法。

It is rare that we study antiproton-nuclear inelastic scattering and elastic scattering by using phenomenological annihilation potentials .

~（208）Pb平均振幅或形变参数系统研究及中子直接非弹性散射截面计算

Systematic Research on Amplitudes or Form Factors and Calculations of Neutron Direct Inelastic Scattering Cross Sections for 208 Pb

中子与~（116118120122124）Sn反应非弹性散射的理论计算和分析

Theoretical Calculations and Analysis of Inelastic Scattering for n + ~ ( 116,118,120,122,124 ) Sn Reactions

Xe-H2非弹性散射密耦合波包法研究

Study of close coupling wave packet for x_0-h_2 system of inelastic scattering

在电子非弹性散射的辐射修正中常用解开（unfolding）或折叠（folding）的方法。

The unfolding and folding methods are generally used in the radiative corrections to the electron inelastic seatterings .

金属氢化物（AlH3）n的热中子非弹性散射谱

Inelastic scattering spectra of thermal neutrons by aluminium hydride ( alh_3 ) _n

本文主要讨论了eA深度非弹性散射中喷注的能量损失问题。

In this thesis , I would like to explore the parton energy loss in eA deeply inelastic scattering ( DIS ) .

本文研究了在装有CS2的波导管中后向非弹性散射的相位共轭特性和在全息红宝石激光器中应用的可能性。

The phase conjugate property of backward inelastic Scattering of laser beam in a waveguide and the possibility of its application in holographic ruby lasers have been investigated .

e-p深度非弹性散射中粲夸克态的效应

The effects of the charm state in e-p deep inelastic scattering

本文用Glauber理论计算和分析了能量为260和280MeV的π~-~（12）C弹性和非弹性散射微分截面。

Using Glauber theory , the π - ~ ( 12 ) C elastic and inelastic scattering differential cross-sections at the energies 260 and 280 MeV are calculated and analyzed .

实验研究表明，在高里德伯态氢原子与D2的散射中，非弹性散射和化学反应散射都是重要的.在非弹性散射过程中，氘分子的核自旋是守恒的。

Experimental results show that both inelastic and reactive scattering are significant , and that nuclear spin is conserved in the former process .

在Glauber多重散射理论的框架下，使用跃迁密度方法分析了入射动量为800MeV/c的π~±介子在~（12）C上的非弹性散射的最新实验材料。

In the framework of Glauber theory the recent pion inelastic scattering data on ~ ( 12 ) C at 800MeV / c are analysed by using the transition density method .

给出多元介质中修正的Bethe方程计算低能电子非弹性散射能量损失。

The modified Bethe formula in polybasic medium is used for calculating energy loss of LEE inelastic scattering .

除F心信号外，首次观察到一个喇曼频移为147cm~（-1）的信号.这一信号被指认为Vk心的非弹性散射。

Besides the F center signals , a Raman signal with the peak position at 147cm ~ ( - 1 ) is observed first time , it is assigned to be inelastic scattering of V_ K center .

在Glauber理论基础上，在刚性炮弹近似下，给出了核-核非弹性散射振幅。

On the base of Glauber 's theory , nuclei-nuclei inelastic scattering amplitudes are given by using the rigid projectile approximation .

以Glauber理论分析、计算了高能α粒子在40,42,44,48Ca上的弹性和非弹性散射数据。

Elastic and inelastic scattering data of high-energy α particles on ~ ( 40,42,44,48 ) Ca are analyzed with the Glauber theory .

e-A深度非弹性散射中高纽度过程对喷注淬火效应的影响

Effects of High Twist Processes on Jet Quenching in e-A Deeply Inelastic Scattering

e-A深度非弹性散射中胶子辐射振幅的新计算方法

A New Calculational Approach to the Amplitude of Gluon Radiation in e-A DIS

通过轻子与原子核的深度非弹性散射、核Drell-Yan过程，可以了解原子核中的夸克&部分子分布的信息。

By deep inelastic scattering of leptons on nucleus and nuclear Drell-Yan processes one can learn the parton densities in nucleus .

用PND-S测井的非弹性散射信息求取储层的含水饱和度

Reservoir Water Saturation Derived with Inelastic Scattering Information of Pulsed Neutron Decay-spectrum ( PND-S ) Logging

粲夸克态对e-p深度非弹性散射中纵横虚光子吸收截面比的影响

The Influence of the Charm State on the Ratio of the Longitudinal and Transverse Section of virtual photon in e-p Deep Inelastic Scattering

密封，D-T脉冲式中子发生器是利用中子非弹性散射于体内碳与氧的活体量测上。

A sealed , D-T , pulsed neutron generator is used for the in vivo measurement of body carbon and oxygen by neutron inelastic scattering .

依据因子化定理，高能碰撞Drell-Yan过程的微分截面可以用类似深度非弹性散射中的色偶极截面来表示。

According to factorization theorem , the Drell-Yan cross section can be expressed in terms of the same dipole cross section that appears in deep inelastic scattering .