Author:
Datta Alakabha,Marfatia Danny,Mukherjee Lopamudra
Abstract
AbstractWe explain recent LHCb measurements of the lepton universality ratios, $$R_{D^{(*)}}^{\tau /\ell }\equiv \frac{\mathcal {B}(\bar{B} \rightarrow D^{(*)+} \tau ^- \bar{\nu }_\tau )}{\mathcal {B}(\bar{B} \rightarrow D^{(*)+}\ell ^- \bar{\nu }_\ell )}$$
R
D
(
∗
)
τ
/
ℓ
≡
B
(
B
¯
→
D
(
∗
)
+
τ
-
ν
¯
τ
)
B
(
B
¯
→
D
(
∗
)
+
ℓ
-
ν
¯
ℓ
)
and $${R(\Lambda _c^+)}^{\tau /\ell } \equiv \frac{\mathcal {B}(\Lambda _b \rightarrow \Lambda _c^+ \tau ^- \bar{\nu }_{\tau })}{\mathcal {B}(\Lambda _b \rightarrow \Lambda _c^+ \ell ^- \bar{\nu }_{\ell })}$$
R
(
Λ
c
+
)
τ
/
ℓ
≡
B
(
Λ
b
→
Λ
c
+
τ
-
ν
¯
τ
)
B
(
Λ
b
→
Λ
c
+
ℓ
-
ν
¯
ℓ
)
with $$\ell =\mu $$
ℓ
=
μ
, via new physics that affects $$R_D^{\tau /\ell }$$
R
D
τ
/
ℓ
and $$R(\Lambda _c^+)^{\tau /\ell }$$
R
(
Λ
c
+
)
τ
/
ℓ
but not $$R_{D^*}^{\tau /\ell }$$
R
D
∗
τ
/
ℓ
. The scalar operator in the effective theory for new physics is indicated. We find that the forward-backward asymmetry and $$\tau $$
τ
polarization in $$\bar{B} \rightarrow D^+ \tau ^{-} \bar{\nu }_{\tau }$$
B
¯
→
D
+
τ
-
ν
¯
τ
and $$\Lambda _b \rightarrow \Lambda _c^+ \tau ^- \bar{\nu }_{\tau }$$
Λ
b
→
Λ
c
+
τ
-
ν
¯
τ
decays are significantly affected by the scalar interaction. We construct a simple two Higgs doublet model as a realization of our scenario and consider lepton universality in semileptonic charm and top decays, radiative B decay, B-mixing, and $$Z \rightarrow b \bar{b}$$
Z
→
b
b
¯
.
Funder
Division of Physics
U.S. Department of Energy
Publisher
Springer Science and Business Media LLC