| 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. | Mass is really a coupling between a left handed fermion and a right handed fermion
电子与电子中微子，以及在第二、三代中相对应的粒子，被统称为轻子。 |
| 5. | She showed that her fermions did not exist as molecules ? that is , they had not become chemically bound together
不过费米凝聚的困难之处在于如何去观察它。 |
| 6. | 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。 |
| 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. | 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。 |
| 10. | In chapter we give out an explicit expression of classical capacity of general fermi quantum channel for single mode fermion system under the restriction of input average occupation numbers of fermions ( that is the input power restriction )
第二章给出了输入费米子平均占据数限定(平均输入功率限定)的条件下的单模费米系统量子信道的经典容量。 |
