The light U boson as the mediator of a new force, coupled to a combination of Q,B,L and dark matter
A new light gauge boson U may have both vector and axial couplings. In a large class of theories, however, the new U (1) current J F μ naturally combines with the weak neutral current J Z sm μ , both parity-violating, into a vectorial current J U μ , combination of the B , L and electromagnetic curr...
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Veröffentlicht in: | The European physical journal. C, Particles and fields Particles and fields, 2017, Vol.77 (1), Article 53 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | A new light gauge boson
U
may have both vector and axial couplings. In a large class of theories, however, the new
U
(1) current
J
F
μ
naturally combines with the weak neutral current
J
Z
sm
μ
, both parity-violating, into a vectorial current
J
U
μ
, combination of the
B
,
L
and electromagnetic currents with a possible dark-matter current.
U
μ
may be expressed equivalently as
cos
ξ
C
μ
+
sin
ξ
Z
sm
μ
(“mixing with the
Z
”) or
(
1
/
cos
χ
)
C
^
μ
+
tan
χ
A
μ
(“mixing with the photon”), with
C
^
coupled to
B
,
L
and dark matter. The
U
boson may be viewed as a generalized dark photon, coupled to SM particles through
Q
U
=
Q
+
λ
B
B
+
λ
i
L
i
, with strength
g
′
′
cos
ξ
cos
2
θ
=
e
tan
χ
. “Kinetic-mixing” terms, gauge invariant or not, simply correspond to a description in a non-orthogonal field basis (rather than to a new physical effect), with the dark photon in general also coupled to
B
and
L
.
In a grand-unified theory
Q
U
gut
=
Q
-
2
(
B
-
L
)
at the GUT scale for SM particles, invariant under the
SU
(4) electrostrong symmetry group, with a non-vanishing
ϵ
=
tan
χ
already present at the GUT scale, leading to
Q
U
≃
Q
-
1.64
(
B
-
L
)
at low energy. This also applies, for a very light or massless
U
boson, to a new long-range force, which could show up through apparent violations of the equivalence principle. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-016-4568-9 |