| 1. | In superconductors, the bosons are the pairs of bound electrons that form at the fermi surface .
在超导体中，玻色子是在费密表面形成的束缚态电子对。 |
| 2. | We solve the secular equation for the system ' s binding energy
我们采用解久期方程的方法来研究d ~ -中心的束缚态。 |
| 3. | Bound states of relativistic particles moving in the potentials with pseudo - spin symmetry
相对论情况下赝自旋对称性势场中运动粒子的束缚态 |
| 4. | Algebraic approach to eigenvalue of energy of bound states system under supersymmetric potential
超对称势作用下束缚态体系能量本征值的代数解法 |
| 5. | Through green ’ s function method , we find that a virtual bound state is induced by a point defect
格林函数方法计算态密度的结果表明,单个点缺陷在碳纳米管中引起准束缚态。 |
| 6. | So in theory , the numbers of bound states should be more and more versus the width of well becomes wider
所以从理论上分析， d ~ -中心的束缚态应该是随着阱宽的变宽而越来越多。 |
| 7. | This suggested that rapid increase of endogenous iaa induced by wounding could result from a release of the combined form into free iaa
这似表明，剥皮刺激诱导的内源iaa浓度的快速升高可能是束缚态iaa的快速释放，而不是芽和幼叶新合成的结果。 |
| 8. | We found that the number of bound states becomes more and more versus the quantum well wider , at the same time the critical magnet value becomes lower and lower
我们得到， d中心的束缚态随着阶宽的增加出现的越来越多，并且出现的临界磁场越来越低。 |
| 9. | If the magnetic field is strong enough , the number of bound states of d ~ centers is countless in three dimensional material , however in two dimensions only four bound states are found
如果磁场足够大，三维体材料中d ~ -中心有无穷多个束缚态，而二维d ~ -中心则只有四个束缚态存在。 |
| 10. | From an analytic treatment , the state is determined by the nanotube diameter rather than chirality . the corresponding image of local density of states in real space shows a highly localized state around the defect
然后逐点计算局域态密度发现,在实空间准束缚态是一个非常局域化的效应,离开缺陷即迅速衰减。 |
