1) back-shock nucleus kinetic energy
反冲核动能
2) energetic recoil nucleus
高能反冲核
3) ~3He recoil
反冲~3He核
4) recoil nuclei
反冲核
1.
The methods to calculate the energy spectra of all kinds of emitting light particles and recoil nuclei for multilevel particle emission in medium energy region(≤250?MeV), comparison of the efficiency between this method and the traditional one and two calculated examples are given.
给出了在中能区(≤250MeV)多次粒子发射过程中计算各种出射轻粒子及各种反冲核之能谱的方法,指出它的计算效率远高于(两个数量级以上)传统方法,并给出了两个算例。
2.
The methods to calculate the energy spectra of six kinds of emitting light particles(n,p,a,d,t, ~3He)and all kinds of recoil nuclei as well as the double differential cross sections of these six kinds of particles for medium-heavy nuclei with the same six kinds of particles as projectiles in the energy region up to 250 MeV are given in this work.
给出了在中能区(≤250 MeV)多次粒子发射过程中计算6种出射轻粒子(n,p,α,d,t,~3He)及各种反冲核之能谱和双微分截面的方法。
5) recoil nuclide
反冲核
1.
The energy spectra of radioactive recoil nuclides sputtered from metallic target induced by 14.
９ Ｍｅ Ｖ 中子入射金属产生的反冲核的能谱。
6) recoil nucleon
反冲核子
1.
It is pointed out that contribution of the πNN processes to the structure functions of the nucleon should be calculated by taking the recoil nucleon as a physical nucleon.
指出在计算πNN过程对核子结构函数的贡献时 ,将反冲核子视为物理核子更为合理 。
补充资料：反冲核
分子式：
CAS号：
性质：当中能中子(0.1～20kev)或快中子(>20kev)与物质作用时，通过中子与原子核之间的弹性碰撞使该原子核获得足够能量并以很高的速度飞离母体而成为荷电粒子即为反冲核。这种反冲核在次级过程中能使介质原子或分子电离或激发并导致辐射化学效应。
CAS号：
性质：当中能中子(0.1～20kev)或快中子(>20kev)与物质作用时，通过中子与原子核之间的弹性碰撞使该原子核获得足够能量并以很高的速度飞离母体而成为荷电粒子即为反冲核。这种反冲核在次级过程中能使介质原子或分子电离或激发并导致辐射化学效应。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条