| 1. | Spin - sin coupling constant
核磁共振自旋 |
| 2. | These effective coupling constants of mesons embody the feature of the dbhf results , such as short - range correlations and the structure of isospin
和。介子密度依赖的耦合常数，然后，在不对称系数p 0 |
| 3. | The effects of the thickness , the interfacial coupling constant and the temperature on the hysteresis of the bilayer are investigated
我们考察了薄膜厚度、界面耦合强度和温度对铁电双层薄膜电滞回线的影响。 |
| 4. | In the second chapter , we divide the polaron into two kinds by the coupling constant . one is big polaron and the other is small polaron
在第二章中，我们通过对耦合常数大小，把极化子划分为大极化子和小极化子。 |
| 5. | By introducing the nonlinear coupling constant . zm model has improved the effective nucleon mass indeed . but the physics mechanism is not deeply disclosed
通过引人非线性的耦合淑的确龈子的有效谴雕u了改善，但改善的机理没有被深入的揭示 |
| 6. | Here , through expanding the nonlinear coupling constant , we have discussed this mechanism . in addition , we find that the phase transition at high temperature in qhd - i model has been suppressed in zm model
本文通过展开非线性耦合常数，并逐阶求解进行分析，讨论了这一改善的机制，并发现qhd i模型在高温下的相变机制在zm模型中遭到了抑制 |
| 7. | Using above method with theories , we have computed the magnetic exchange coupling constants j values about ( vivo ) cr [ 1 ( cn ) 6 ] 2 / 3 . 10 / 3h2o compound and [ mo2 ( cn ) 11 ] 5 compound , respectively . the j values are equal to - 42 . 36cm - 1 and - 111 . 46cm - 1 , respectively
然后，分别对这两种配合物自旋密度分布加以分析，两种配合物中金属离子上的成单电子几乎是定域的，其自旋极化占主导作用。 |
| 8. | The effective coupling constants including isoscalar and mesons and isovector and mesons in the rmf are extracted from the dbhf results in symmetric and asymmetric nuclear matter . two sets of effective interactions in the rmf approach are deduced by imposing a condition , where the dbhf scalar and . vector self - energy or scalar self - energy and binding energy per nucleon at each density and asymmetry parameter are reproduced , respectively
为了使我们提取的有效相互作用能够准确地再现出dbhf计算的核状态方程以及密度依赖的不对称能，我们采用第二种万法提取有效介子核子耦合常数，即要求在对称核物质中，每个密度处ilif计算出的标量自能及总结合能与dbhf给出的标量自能及总结合能一致，提取出。 |
| 9. | It has been shown that : with the increase of the kerr medium intensity parameter u , the rabi oscillation extent of the mean photon number decrease and the rabi oscillation frequency becomes rapid , the antibunching effect becomes strengthened ; with the increase of n , the interaction between the field and atoms gradually becomes weak , however , the interaction between the field and the kerr medium gradually becomes strengthened and happen in advance ; with the increase of the coupling constants of two atoms , the rabi oscillation extent of the mean photon number decrease and the rabi oscillation frequency becomes rapid too , the antibunching effect becomes weak
结果表明：随着值的增加，光子统计演化曲线的rabi振荡的幅度减小，振荡频率变快，系统的反聚束效应增强；随着初始场强( ? )的增大，场与原子的相互作用逐渐减弱，而与介质的相互作用逐渐加强并提前发生。随着原子间耦合系数g的增大，光子统计演化曲线的rabi振荡的幅度减小且振荡周期缩短，同时，系统的反聚束效应减弱。 |
| 10. | The advantage is that it can be used to directly calculate the real physics quantities in an economic way . in this way , we need n ' t perform the analytical continuation from the result in the itf . this new rule has the following property ; the vertex is only related with the coupling constant and independent of the orientation of the momenta , one half of the vertex components vanish
它的优点在于能直接计算与实际物理相关的观测量，不用象虚时温度场论中做计算后再作解析延拓，使得计算得到一定的简化，并具有如下特点：顶角函数只与耦合常数相关，独立于外线动量方向，而且一半的分量为零。 |
