Abstract
AbstractWe study the full angular distribution of semileptonic rare charm baryon decays in which the secondary baryon undergoes weak decay with sizable polarization parameter, $$\Xi _c^+\rightarrow \Sigma ^+\,(\rightarrow p\pi ^0)\ell ^+\ell ^-$$
Ξ
c
+
→
Σ
+
(
→
p
π
0
)
ℓ
+
ℓ
-
, $$\Xi _c^0\rightarrow \Lambda ^0\,(\rightarrow p \pi ^-)\ell ^+\ell ^-$$
Ξ
c
0
→
Λ
0
(
→
p
π
-
)
ℓ
+
ℓ
-
and $$\Omega _c^0\rightarrow \Xi ^0\,(\rightarrow \Lambda ^{0} \pi ^0)\ell ^+\ell ^-$$
Ω
c
0
→
Ξ
0
(
→
Λ
0
π
0
)
ℓ
+
ℓ
-
. Such self-analyzing decay chains allow for seven additional observables compared to three-body decays such as $$\Lambda _c \rightarrow p \ell ^+ \ell ^-$$
Λ
c
→
p
ℓ
+
ℓ
-
, with different sensitivities to the $$|\Delta c|=|\Delta u|=1$$
|
Δ
c
|
=
|
Δ
u
|
=
1
weak couplings. Opportunities to test the standard model in $$c \rightarrow u$$
c
→
u
transitions with standard model null tests and other angular observables are worked out. We show that a joint model-independent analysis of the leptonic $$A_{\text {FB}}^\ell $$
A
FB
ℓ
, hadronic $$A_{\text {FB}}^{\text {H}}$$
A
FB
H
, and combined forward–backward asymmetry $$A_{\text {FB}}^{\ell \text {H}}$$
A
FB
ℓ
H
together with the fraction of longitudinally produced leptons, $$F_L$$
F
L
, is able to pin down the dipole couplings $$C_{7},C^\prime _{7}$$
C
7
,
C
7
′
and the semileptonic (axial-) vector ones $$C_{10},C^\prime _{9},C^\prime _{10}$$
C
10
,
C
9
′
,
C
10
′
. $$A_{\text {FB}}^{\text {H}}$$
A
FB
H
is also accessible with dineutrino $$c \rightarrow u \nu {\bar{\nu }}$$
c
→
u
ν
ν
¯
modes and probes right-handed currents.
Funder
Studienstiftung des Deutschen Volkes
Bundesministerium für Bildung und Forschung
Publisher
Springer Science and Business Media LLC
Subject
Physics and Astronomy (miscellaneous),Engineering (miscellaneous)
Cited by
4 articles.
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