代写毕业论文：哈密顿量理论。这些哈密顿量理论的本征态被认为是基于具有单个 4 动量的粒子的数量来定义的。在这种情况下，没有在完整的洛伦兹或庞加莱变换中确定的有限酉表示。这些源于洛伦兹助推器的非紧凑性。接下来代写毕业论文专家将对哈密顿理论进行分析与讨论。
Lorentz boosts 可以定义为发生在 Minkowski 中的旋转，沿空间和时间轴的线使用。在这个系统中，可以使用自旋 1/2 粒子的情况。认为不可能找到包括有限维表示以及标量积的构造，该标量积与在每篇文章中观察到的 4 分量狄拉克旋量之间存在的关系的表示保持一致。这些旋量变换由伽马矩阵生成的洛伦兹变换。这些被认为是保留的标量产品的一部分。这不是肯定的。该表述不能也不被视为单一表述。发现标准模型的粒子属于不可约表示。这些被表示为 Poincare 群、guage groip 及其酉群函数的乘积。这些被发现定义了标准模型的对称组。完整的对称群具有对称群的剩余部分。它们通常在自然界中被破坏。
庞加莱对称性流经物质在较小尺度上的不对称分布。这些是基于质子和中子的质量。这些世代通过不同质量的电子世代移动。两个不可约的费米子表示是夸克形式和轻子形式。这三个被表示为不可约的玻色子表示。胶子形成，Z-玻色子和W-玻色子是第二个因素，希格斯玻色子是第三个因素。这些表示中的每一个都被拆分为 Poincare 组使用的多个不可约表示。每个粒子都有固定的质量。质量被称为庞加莱李代数的卡西默算子。这些意义上的不同粒子由标准模型拉格朗日模型中出现的不同分量来观察。在这些概念中，自旋指数被抑制。在这些情况下，发现使用一个分裂代替 Poincare x Isospin SU (2) 的不可约表示。这些进入 3 夸克世代。这是基于中微子质量混合矩阵的存在。
后者不符合标准夸克和中微子的约定。换句话说，它也被称为属于 Poincare 群的不可约表示。对于中微子，有基于中微子振荡的解释。在这些情况下，没有用于三代电子的相应混合矩阵。这些都受制于超级选择规则的收费。这禁止了不同种类的电荷本征态的超位。由于质量混合，庞加莱群中使用的不可约表示不属于超级选择扇区。根据这个结果，没有用于质量的超级选择规则。在这种情况下，质量被认为是非平凡的操作。这是基于夸克的单个粒子。这些与非相对论力学形成对比。在这种情况下，伽利略群的结构导致了超选择规则。因此，观察到每个单个粒子扇区都以数值质量为特征。
总而言之，需要对基于可嵌入表示的不同常数的每个方程进行更多研究。本分析中讨论了不同理论的一些条件。这些可以用作开发各种条件的框架。
The Lorentz boosts can be defined as the rotations that takes place in the Minkowski that are used along the lines of the space and time axis. In this system, the case of spin 1/2 particles can be used. It is deemed not possible to find a construction that include the finite-dimensional representation along with the scalar product that is preserved with the representation of relationship that is present between the 4 component Dirac spinor that is observed in each article. These spinors transform the Lorentz transformation that is generated by the gamma matrices. These are considered to be a part of the scalar product that is preserved. This is not positive definite. The representation cannot and is not considered to be a unitary presentation. The particles of the standard model are found to fall into the irreducible representation. These are represented as the product of the Poincare group, guage groip and its unitary group functions. These are found to define the symmetry group of the standard model. The unbroken symmetry groups has the remaining part of the symmetry group. They are usually broken in nature.
The Poincare symmetry flows through the asymterical distribution of matter in a smaller scale. These are based on the masses of the proton and neutron. These generations move through the various masses of the electron generations. The two irreducible fermionic representations are the quarks form on and the leptons form in the other. These three are represented as irreducible bosonic represntations. The gluons form on, Z-boson and W-boson are the second factor and the higgs boson is the third. Each of these representations are split into the multiple irreducible representations that are used by the Poincare group. Each of the particles have a fixed mass. The mass is known as the Casimer operator of the Poincare Lie algebra. The different particles in these senses are viewed by the different components that are appearing in the standard model Lagrangian. In these notions, the spin index is suppressed. In these cases one splits are found to be used instead of the irreducible representations of the Poincare x Isospin SU (2). These get into the 3 quark generations. This is based on the existence of the neutrino mass mixing matrix.
The latter is defied by the convention of the standard quarks and neutrinos. In other words, it is also known as the irreducible representations that belong to the Poincare group. For the neutrinos, there is the explanation that is based on the neutrino oscillations. In these cases, there is no corresponding mixing matrix that are used for the three generations of the electrons. These are subjected to the changed to the charge of the super selection rule. This forbids the super positions of the different kinds of eigenstates of charges. Owing to the mass mixing, the irreducible representations that are used in the Poincare group do not be a part of the super selection sectors. According to this consequence, there is no super selection rule that is used for the mass. The mass in this case is considered to be the non-trivial operations. This is based on the single particle of quarks. These contrasts with the nonrelativistic mechanics. In this case, the structure of the Galilean group causes the super selection rule. Owing to this, every single particle sector is observed to be characterized by the numerical mass.
To conclude, more research is needed for each one of the equation based on the different constants that can be embedded in the representation. Some conditions have been discussed on the different theories in this analysis. These can use as a framework to develop the various conditions.
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