米子

基本解释 (translations)

Yonago

与米子相关的网络例句 [注：此内容来源于网络，仅供参考]

Evaluate the determinant, taking into account that fermionic fields obey an antiperiodic boundary condition,.

估算行列式并考虑费米子场满足反周期边界条件。

We then consider the effect of a finite gauge boson mass on the behavior of dynamical CSB.

空穴子和无质量的规范场耦合，但和无质量的费米子之间没有直接的耦合。

By using the lattice index theorem, we identify the index of the massless overlap fermion operator to the topological charge of the background gauge configuration.

我们使用overlap费米子方案得到了一些有意义的成果，并提出了包括夸克一胶子等离子体理论在内的进一步研究方向。

In chapter 2, leading-out the difficulties of lattice fermion action based on the Lattice QCD theory.

第二章：通过格点QCD理论的基础引出格点上费米子作用量的困难，即手征对称性破缺与费米子加倍。

In the lepton sector, neutrino oscillations observed by Super-Kamiokande may provide the experimental evidence that the SM should be extended to include the massive neutrinos.

在轻子部分，Super-Kamiokande的中微子振荡实验是一个明显的实验证据能够说明标准模型需要扩充以包含有质量的费米子。

It is also pointed out that an n-mode boson coupled quadratic Hamiltonian can be diagonalized by a "negative unitary" matrix which is an element of complex symplectic group SP(2n,c),and an n-mode fermion coupled quadratic Hamiltonian can be diagonalized by a unitary matrix which is an element of complex fermion group F(2n,c).

并且指出，对于n模玻色子耦合二次型哈密顿量，通过一个负幺正矩阵它是复辛群SP(2n，c的元素可以把它对角化；对n模费米子耦合二次型哈密顿量，通过一个幺正矩阵它是复费米群F(2n，c的元素可以把它对角化。

In chapter 3, we represent the properties of Overlap fermion's small eigenvalues, and make it clear that the action how to resolve difficulties.

第三章：阐述Overlap费米子小本征值的特性，了解它对于解决格点费米子作用量中存在的两大困难的理论依据。

They found that the entanglement between the first and the second fermions can be enhanced or suppressed by altering the position of the third fermion.

第三个费米子的位置影响第一和第二个费米子之间的纠缠。当改变第三个费米子的位置时，系统的纠缠能被增强或者抑制。

Then show the importance of Overlap fermion after comparing variant lattice fermions.

然后通过比较各种费米子，得出Overlap费米子的重要性。

As to the higher Landau levels, we conducted systematically calculations for the various possible ground states, such as the Laughlin liquid, the composite fermion liquid, the Wigner crystal, and the charge density wave . We find that when the Landau level index N≥2, the fractional quantum Hall states are ruled out and the CDW and Wigner crystal dominate. An exception occurs at around v=4+1/6, where the composite fermion liquid may be more energetically preferable than the CDW and the Wigner crystal states. This result provides a new explanation to the so-called re-entrant integral quantum Hall effect. In fact, the feature of isotropically metallic property at this filling is discerned from the experiment.

对于高朗道能级，我们对各种可能的基态，比如量子霍耳态，复合费米子流体，Wigner晶体，电荷密度波等，做了系统的计算，我们发现，当朗道能级N≥2时，分数量子霍耳态不再出现，Wigner晶体和电荷密度波将占主导地位，一个例外就是在ν=4+1/6附近，复合费米子流体可能出现在从Wigner晶体到电荷密度波晶体之间，该结果为上述的重进入整数量子霍耳效应现象提出了一种新的解释。

与米子相关的网络解释 [注：此内容来源于网络，仅供参考]

Aglaia odorata：米兰,楝科,米子兰属

⒁月季,蔷薇科,蔷薇属,Rosa chinensis | ⒂米兰,楝科,米子兰属,Aglaia odorata | ⒃白果,连香树科,连香树属,Cercidi phyllum japonicum

fermi level：费米能级

费米能级(Fermi level)是绝对零度下电子的最高能级. 根据泡利不相容原理,一个量子态不能容纳两个或两个以上的费米子(电子),所以在绝对零度下,电子将从低到高依次填充各能级,除最高能级外均被填满,形成电子能态的"费米海".

baryon：重子

按其组成夸克的不同,强子还可以分为:重子(Baryon)---由三个夸克或三个反夸克组成,它们的自旋总是半数的;也就是说,重子是费米子,它们包括人们比较熟悉的组成原子核的质子和中子和一般鲜为人知的超子(Hyperon,

fermion：费米子

根据原子本身的自旋角动量(spin)是整数或半整数,我们可以将所有的原子区分成玻色子(boson)或费米子(fermion). 当4He之类的玻色原子被冷却到趋近绝对零度时,它们会全落到同一个量子基态而形成BEC;

Fermion field：费米子场

费米-狄拉克统计 Fermi-Dirac statistics | 费米子场 fermion field | 费米子场量化 fermion field quantization

heavy fermion：重费米子

Gravity Probe B重力探测器B | heavy fermion重费米子 | homology group 同调群

composite Fermion：复合费米子

复合电路 composite circuit | 复合费米子 composite fermion | 复合场算符 composite field operator

slave fermion：受制费米子

斯雷特行列式 Slater determinant | 受制费米子 slave fermion | 套管偶极 sleeve dipole

fermion field quantization：费米子场量化

费米子场 fermion field | 费米子场量化 fermion field quantization | 费米[子]弦 Fermionic string

Fermi-Dirac statistics：費米-狄拉克統計= 費米[-狄拉克]統計法

Fermi temperature 費米溫度 | Fermi-Dirac statistics 費米-狄拉克統計= 費米[-狄拉克]統計法 | fermionic string 費米[子]弦