| 1. | Particles, such as electrons, requiring antisymmetric wave functions are called fermions .
要求反对称波函数的粒子，如电子，叫做费米子。 |
| 2. | The weak charge of fundament fermions
费米子的弱荷 |
| 3. | In a system , no two fermions can occupy the same quantum state ( position and velocity )
在一系统中,不能有两粒费米子?据相同的量子态(位置与速度) |
| 4. | Lu and huang extended their discussion to fermionic strings and green - schwarz superstrings
Lu和huang把brevik的讨论推广到玻色子开弦，费米子弦和超弦等情况。 |
| 5. | Then , we introduce the double - fermion representation of one - dimensional isotropic xy spin - 3 / 2 chain model
最后，我们介绍了一维各向同性xy自旋- 3 2链模型的双费米子表象。 |
| 6. | By using the double - fennion representation , we discuss the statistical relations of the s = 3 / 2 spin operator
基于双费米子表象，我们讨论了自旋值为3 2的自旋算符所遵循的统计关系。 |
| 7. | Unlike bosons , fermions are misanthropes ; the pauli exclusion principle prohibits them from existing in the same quantum state
费米子与玻色子不同，它们喜欢离群索居，包立不相容原理禁止它们处于同一个量子状态。 |
| 8. | Fermions are the basic building blocks of ordinary matter and include electrons , protons and neutrons individually , as well as atoms with an odd number of those constituents
费米子是一般物质的基本构成单位，个别的电子、质子、中子以及由奇数个这些粒子组成的原子都属于费米子。 |
| 9. | For example , the mass of an electron is really a coupling between a left handed electron and a right handed electron , which is the antiparticle of a left handed positron
它们与其他费米子不同处在于它们没有一种叫“色”的性质，所以它们的作用力（弱力、电磁力）会随距离增加变得越来越弱。 |
| 10. | We also discuss the statistical relations of the majorana lattice fermions and the majorana fermi fields respectively . chapter3 : new jordan - wigner - rype transformation between spin - 3 / 2 and fermions of two types is shown
第三章：介绍了在自旋- 3 2的自旋算符和双费米子之间构建出的一种新的“ jordan - wigner ”类型的变换。 |
