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夸克(u, d, t)和磁单极子自己对产量的施温格影响年底通货膨胀在招商银行的起源B-curl模式,创建和希格斯场的问题

作者(年代):Stefan Mehedinteanu

在目前的工作中,建立一个相关性与通货膨胀动态,特别是在再热的时代,当场足够强大,和真空的能量可以降低,为了创建由施温格效应对夸克(u, d, t),胶子,玻色子(WiA‚±),胶子(单极子),磁单极子本身(自旋1)。同样,在工作计算通货膨胀动态投入所有的证据时代(夸克,强子,轻子)。,我们允许观察潜在的临近年底再热(夸克时代)是减少,因此,在H m s iA€1 iA€½106 []iA‚®0.003,可能会出售= 100 gev;在监禁期满H m s iA€1 iA€½109 []iA‚®3.3 V = 100伏,和夸克对由施温格效果,得到2.6兆电子伏。因此,很显然,不是外部残留的希格斯场的领域。他人的话说,通货膨胀不能解释希格斯场,,如果我们考虑到顶部(t)和antitop (t)夸克对也,由施温格效应,它们形成一个束缚态,是一个复合的希格斯玻色子场Topcolor模型的框架。这是一个模型的动力电弱对称性破顶夸克和anti-top夸克组成一个顶夸克冷凝,并采取有效行动像希格斯玻色子。这是类似于超导现象。这些理论最终将被测试在LHC的——二世在2015年开始运行。在我们目前的模型中,也同样的东西,一个等价的模型与标准模型,给出了在以前authorAA’作品。因此,在我膨胀势模型,通过施温格效应在加热期间,产生各种各样的粒子:胶子,磁单极子,费米子(夸克,夸克)。 In the model, theses gluon-gluon interactions constrain color fields to string-like objects called “flux tubes”, which exert constant force when stretched. The difference with Standard Model, is that it results a probability  1 (or a continuously production rates) for gluons, and a number of 1090 quarks. Finally, at all the gluons are being captured by all 3 ï‚´ flux_tubes generated by ee quarks ( 1090) pairs, together forming nucleons of an incredibly exactly number  1090, which is the known number of particles in Universe. Since, the reheating potential continues to diminish, at approximately V  0.1[GeV]-that corresponding to confinement, the production of gluons (monopoles) quarks stops. But, a near .e. field it was created inside nucleons, as was found in previously authorÂ’s works. This field makes possible the beta decay of free neutrons, and later of isotopes. Also, this field creates a Lorenz force between quarks flux tube and gluons (in structures of gauge monopoles type current), that is found to explain the gravity of nucleons (mass). There are found the number and mass of top quarks pairs locked in Higgs field and its decay. Also, is discovered the exact origin of primordial magnetic field (PMF) which can B-imprints CMB, namely, the magnetic flux of magnetic (anti)monopole coupled in strings, and generated by a the same Schwinger effect. Thus, at the end of CMB time, all (1090) of magnetic monopoles pairs produced are already bounded in strings, and the light of B – curl type imprinted is due of theirs magnetic field resulted to be BPMF = BCMB  1.5 ï‚´ 10–12[T], either as itself, or by Faraday rotation of 0.051rad ï‚® 2.95ï‚° that gives l = 68, for a frequency of 41GHz. Therefore, the monopoles pairs suppression by bounding its in strings, that explains the magnetic monopoles absence mentioned in Iflation works. Also, in order to “pass” the plasma period as to be formed by particles, it needs to preserve the magnetic field in some way, like in theses strings, till CMB. That, it is not the case with gravitational field, which it is not affected by this plasma.