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Titlebook: An introduction to relativistic processes and the standard model of electroweak interactions; Carlo M. Becchi,Giovanni Ridolfi Textbook 20

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樓主: patch-test
31#
發(fā)表于 2025-3-26 21:23:51 | 只看該作者
Abhandlungen zur Mittelstandsforschungon . ? ., where . is any fermion in the standard model spectrum, is extremely good for most applications. In view of experimental results, however, it is interesting to study the possible ways neutrino mass terms can be consistently introduced.
32#
發(fā)表于 2025-3-27 01:25:09 | 只看該作者
Relativistic field theory,covariance, that guarantees the invariance of the equations of motion under changes of reference frame, and of the principle of causality, which is connected to the principle of locality, namely, the independence of variables associated to different points in space at the same time.
33#
發(fā)表于 2025-3-27 05:36:29 | 只看該作者
Spinor fields,th in Chapters 7 and 8) is provided by vector fields: . In the general case, we have a system of complex fields ., . = 1, ..., ., with the transformation law . where the matrix . obeys the condition . for any two Lorentz transformations .. The vector field is an obvious example; in that case, we have simply . ≡ .).
34#
發(fā)表于 2025-3-27 13:14:16 | 只看該作者
Neutrino masses and mixing,on . ? ., where . is any fermion in the standard model spectrum, is extremely good for most applications. In view of experimental results, however, it is interesting to study the possible ways neutrino mass terms can be consistently introduced.
35#
發(fā)表于 2025-3-27 16:23:05 | 只看該作者
36#
發(fā)表于 2025-3-27 17:54:53 | 只看該作者
37#
發(fā)表于 2025-3-28 00:54:27 | 只看該作者
38#
發(fā)表于 2025-3-28 02:27:43 | 只看該作者
Gauge symmetries, where ., . are real constants. Notice that we have inserted a Dirac mass term, which is allowed by the assumed invariance properties, while Majorana mass terms are not, as mentioned in Section 5.2. The conserved current is given by . and the constant e plays the role of elementary charge.
39#
發(fā)表于 2025-3-28 06:16:39 | 只看該作者
40#
發(fā)表于 2025-3-28 11:23:03 | 只看該作者
https://doi.org/10.1007/978-3-322-83371-6the interaction in eq. (7.1) is non-renormalizable, since it contains operators with mass dimension 6; it is an effective theory, in the sense that it can only be used to compute amplitudes in the semi-classical approximation.
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