• Keine Ergebnisse gefunden

Exercises to Lecture 2: Electroweak Sector of the SM

N/A
N/A
Protected

Academic year: 2022

Aktie "Exercises to Lecture 2: Electroweak Sector of the SM"

Copied!
2
0
0

Wird geladen.... (Jetzt Volltext ansehen)

Volltext

(1)

Exercises to Lecture 2: Electroweak Sector of the SM

Exercise 5 ( Projection properties of ):

In the lecture the projection properties of

have been discussed. It is obvious that . a)

Proof the following relation:

i.e. the corresponding operators are projection operators.

b)

Proof the following relation:

i.e. the two operators are orthogonal to each other.

c)

Proof the relation

i.e. the projector acts on the spinors in both directions. For this proof make use of the projector property that you have shown in a).

d)

Proof that

even though . For this proof make use of the orthogonality that you have shown in b).

(2)

Exercise 6 ( Chiral transformation ):

The transformation is called chiral transformation. It turns for instance axial vectors into vectors and vice versa.

a)

Check how the chiral transformation acts on the adjoint spinor . b)

Proof that are eigenstates to the chiral transformation with eigenvalues . c)

Proof that terms of type are covariant under chiral transformations, but terms of type are not.

Referenzen

ÄHNLICHE DOKUMENTE

A directed graph (gerichteter Graph) is as well a pair G=(V,E). However, the elements of E are ordered pairs of elements from V.. 2475 3) Multiply the entries of an

Infolgedessen versuchten einige Zum jetzigen Zeitpunkt Studenten die AET/EET -Prüfung im haben sich erst 4 Studenten umgekehrt, denn.... Unglückli- angemeldet - Eine

In both GraphML and GXL, nodes are represented as an unordered list of <node> elements, each having an obligatory unique identifier, and edges between nodes as

However, we have a lot of (gauge) redundancy, and not every asymptotic Killing vector generates an interesting sym- metry near the boundary; instead, some of the asymptotic

The transformation is called chiral transformation. It turns for instance axial vectors into vectors and vice

Covariant derivative corresponding to acts on isospin doublet only.... Covariant

Wolf: The Higgs Boson Discovery at the Large Hadron Collider, Springer 2015.

◦ Idea of the Higgs mechanism: examples of spontaneous symmetry breaking 2.5 The electroweak sector of the Standard Model – II. ◦ The Standard Model