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Weak isospin
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The weak isospin in particle physics is a quantum number relating to the weak interaction, and parallels the idea of isospin under the strong interaction. Weak isospin is usually given the symbol T or I with the third component written as Tz, T3, Iz or I3. Weak isospin is a component of the weak hypercharge, which unifies weak interactions with electromagnetic interactions.
Fermions with negative chirality (also called left-handed fermions) have T = and can be grouped into doublets with Tz = ± that behave the same under the weak interaction.

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Encyclopedia
The weak isospin in particle physics is a quantum number relating to the weak interaction, and parallels the idea of isospin under the strong interaction. Weak isospin is usually given the symbol T or I with the third component written as Tz, T3, Iz or I3. Weak isospin is a component of the weak hypercharge, which unifies weak interactions with electromagnetic interactions.
Fermions with negative chirality (also called left-handed fermions) have T = and can be grouped into doublets with Tz = ± that behave the same under the weak interaction. For example, "u" type quarks (u, c, t) have Tz = + and always transform in "d" type quarks (d, s, b) that have Tz = − and vice versa. On the other hand, a quark never decays into a quark of the same type. Something similar happens with left-handed leptons, which exist as doublets containing a charged lepton with Tz = − and a neutrino with Tz = .
Fermions with positive chirality (also called right-handed fermions) have T = 0 and form singlets that do not undergo weak interactions.
There is also a weak isospin conservation law: all weak interactions must preserve the weak isospin.
Weak isospin and the W bosons
The symmetry associated with spin is SU(2). This requires gauge bosons to transform between weak isospin charges: bosons , and . This implies that bosons have a T = 1, with three different values of Tz.
(Tz = +1) is emitted in transitions ,
boson (Tz = −1) is emitted in transitions .
boson (Tz = 0) would be emitted in reactions where Tz does not change. However, under electroweak unification, the boson mixes with the weak hypercharge gauge boson , resulting in the observed boson and the photon of Quantum Electrodynamics.
Sources and footnotes
See also
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