1. Boson X Demo
2. Boson Physics
3. Boson X Mod
4. Boson X Online

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Discover Acceleron: Discover the Acceleron particle.
Discover Anti Acceleron: Discover the Anti Acceleron particle.
Discover Anti Geon: Discover the Anti Geon particle.
Discover Anti Graviton: Discover the Anti Graviton particle.
Discover Anti Radion: Discover the Anti Radion particle.
Discover Anti X Boson: Discover the Anti X Boson particle.
Discover Anti Y Boson: Discover the Anti Y Boson particle.
Discover Dark Acceleron: Discover the Dark Acceleron particle.
Discover Dark Geon: Discover the Dark Geon particle.
Discover Dark Graviton: Discover the Dark Graviton particle.
Discover Dark Radion: Discover the Dark Radion particle.
Discover Dark X Boson: Discover the Dark X Boson particle.
Discover Dark Y Boson: Discover the Dark Y Boson particle.
Discover Geon: Discover the Geon particle.
Discover Graviton: Discover the Graviton particle.
Discover Radion: Discover the Radio particle.
Discover X Boson: Discover the X Boson particle.
Discover Y Boson: Discover the Y Boson particle.

Boson X Demo

In particle physics, the X and Y bosons (sometimes collectively called 'X bosons'^[1]:437) 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[edit]

The X and Y bosons couple quarks to leptons (such as a positron), allowing violation of the conservation of baryon number, and thus permitting proton decay.

An X boson would have the following decay modes:^[1]:442 Outlook stuck synchronizing inbox.

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 antiquark and
e⁺
is a positron.

A Y boson would have the following decay modes:^[1]:442

Boson Physics

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 B − L is. Different branching ratios between the X boson and its antiparticle (as is the case with the K-meson) would explain baryogenesis. For instance, if an
X
⁺/
X
⁻ pair is created out of energy, and they follow the two branches described above:
X
⁺ →
u
+
u
,
X
⁻ →
d
+
e⁻
; re-grouping the result (
u
+
u
+
d
) +
e⁻
=
p
+
e⁻
shows it to be a hydrogen atom.

Origin[edit]

The X^± and Y^± bosons are defined respectively as the six Q = ± ​⁴⁄₃ and the six Q = ± ​¹⁄₃ components of the final two terms of the adjoint 24 representation of SU(5) as it transforms under the standard model's group:

${\displaystyle \mathbf{24}\to (8,1{)}_0\oplus (1,3{)}_0\oplus (1,1{)}_0\oplus (3,2{)}_{-\frac{5}{6}}\oplus (\overline{3},2{)}_{\frac{5}{6}}}$.

Thus, the positively-charged X and Y carry anti-color charges (equivalent to having two different color charges), while the negatively-charged X and Y carry normal color charges, and the signs of the Y bosons' weak isospins are always opposite the signs of their electric charges. In terms of their action on ${\displaystyle {\mathbb{C}}^5}$, X bosons rotate between a color index and the weak isospin-up index, while Y bosons rotate between a color index and the weak isospin-down index.

See also[edit]

References[edit]

1. ^ ^abcTa-Pei Cheng; Ling-Fong Li (1983). Gauge Theory of Elementary Particle Physics. Oxford University Press. ISBN0-19-851961-3.

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Boson X Mod

Boson X Online