T3 is more important than T; typically "weak isospin" is used as short form of the proper term "3rd component of weak isospin".
The weak isospin conservation law relates to the conservation of weak interactions conserveT3. It is also conserved by the electromagnetic and strong interactions. However, interaction with the Higgs field does not conserve T3, as directly seen by propagation of fermions, mixing chiralities by dint of their mass terms resulting from their Higgs couplings. Since the Higgs field vacuum expectation value is nonzero, particles interact with this field all the time even in vacuum. Interaction with the Higgs field changes particles' weak isospin (and weak hypercharge). Only a specific combination of them, (electric charge), is conserved.
Relation with chiralityedit
Fermions with negative chirality (also called "left-handed" fermions) have and can be grouped into doublets with that behave the same way under the weak interaction. By convention, electrically charged fermions are assigned with the same sign as their electric charge.[c]
For example, up-type quarks (u, c, t) have and always transform into down-type quarks (d, s, b), which have and vice versa. On the other hand, a quark never decays weakly into a quark of the same Something similar happens with left-handed leptons, which exist as doublets containing a charged lepton ( e− , μ− , τ− ) with and a neutrino ( ν e, ν μ, ν τ) with In all cases, the corresponding anti-fermion has reversed chirality ("right-handed" antifermion) and reversed sign
Fermions with positive chirality ("right-handed" fermions) and anti-fermions with negative chirality ("left-handed" anti-fermions) have and form singlets that do not undergo charged weak interactions.[d]
All of the above left-handed (regular) particles have corresponding right-handed anti-particles with equal and opposite weak isospin.
All right-handed (regular) particles and left-handed anti-particles have weak isospin of 0.
Weak isospin and the W bosonsedit
The symmetry associated with weak isospin is SU(2) and requires gauge bosons with ( W+ , W− , and W0 ) to mediate transformations between fermions with half-integer weak isospin charges.  implies that W bosons have three different values of
The sum of negative isospin and positive charge is zero for each of the bosons, consequently, all the electroweak bosons have weak hypercharge so unlike gluons of the color force, the electroweak bosons are unaffected by the force they mediate.
Interaction with the Z0 is only related indirectly; its interaction is determined by weak charge, q.v.
This article uses T and T3 for weak isospin and its projection.
Regarding ambiguous notation, I is also used to represent the 'normal' (strong force) isospin, same for its third component I3 a.k.a. T3 or Tz . Aggravating the confusion, T is also used as the symbol for the Topness quantum number.
Lacking any distinguishing electric charge, neutrinos and antineutrinos are assigned the opposite their corresponding charged lepton; hence, all left-handed neutrinos are paired with negatively charged left-handed leptons with so those neutrinos have Since right-handed antineutrinos are paired with positively charged right-handed anti-leptons with those antineutrinos are assigned The same result follows from particle-antiparticle charge & parity reversal, between left-handed neutrinos () and right-handed antineutrinos ().
Particles with do not interact with W± bosons; however, they do all interact with the Z0 boson, with the possible exception of hypothetical sterile neutrinos not yet included in the Standard Model.
If they actually exist, sterile neutrinos would become the only elementary fermions in the Standard Model that do not interact with the Z0 boson.
"§2.3.1 isospin and SU(2), redux". Huerta's academic site. U.C. Riverside. Retrieved 15 October 2013.
^An introduction to quantum field theory, by M.E. Peskin and D.V. Schroeder (HarperCollins, 1995) ISBN 0-201-50397-2;
Gauge theory of elementary particle physics, by T.P. Cheng and L.F. Li (Oxford University Press, 1982) ISBN 0-19-851961-3;
The quantum theory of fields (vol 2), by S. Weinberg (Cambridge University Press, 1996) ISBN 0-521-55002-5.