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X and Y bosons

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X and Y bosons
CompositionElementary particle
StatisticsBosonic
FamilyGauge boson
StatusHypothetical
Types12
Mass≈ 1015GeV/c2
Decays intoX: two quarks, or one antiquark and one charged antilepton
Y: two quarks, or one antiquark and one charged antilepton, or one antiquark and one antineutrino
Electric chargeX: −43 e
Y: −13 e
Color chargenonzero
Spin1
Spin states2
Weak isospin projectionX: +12
Y: −12
Weak hypercharge53
BL23

In particle physics, the X and Y bosons (or sometimes collectively called just X bosons[1]) are hypothetical elementary particles analogous to the W and Z bosons, but corresponding to a new type of force predicted by the Georgi–Glashow model, a grand unified theory.

Details

The X and Y bosons couple quarks to leptons, allowing violation of the conservation of baryon number and thus permitting proton decay.

An X boson would have the following decay modes:[2]


X

u
+
u

X

e+
+
d

where the two decay products in each process have opposite chirality,
u
is an up quark,
d
is a down quark and
e+
is a positron.

A Y boson would have the following decay modes:[2]


Y

e+
+
u

Y

d
+
u

Y

d
+
ν
e

where the first decay product in each process has left-handed chirality and the second has right-handed chirality and
ν
e
is an electron antineutrino.

Similar decay products exist for the other quark-lepton generations

In these reactions, neither the lepton number (L) nor the baryon number (B) is conserved, but BL is. Different branching ratios between the X boson and its antiparticle (as is the case with the K-meson) would explain baryogenesis.

See also

References

  1. ^ Ta-Pei Cheng; Ling-Fong Li (1983). Gauge Theory of Elementary Particle Physics. Oxford University Press. p. 437. ISBN 0198519613.{{cite book}}: CS1 maint: multiple names: authors list (link)
  2. ^ a b Ta-Pei Cheng; Ling-Fong Li (1983). Gauge Theory of Elementary Particle Physics. Oxford University Press. p. 442. ISBN 0198519613.{{cite book}}: CS1 maint: multiple names: authors list (link)