Javascript must be enabled to continue!
The anatomy of $$K^+\rightarrow \pi ^+\nu {\bar{\nu }}$$ distributions
View through CrossRef
AbstractThe excellent experimental prospects to measure the invisible mass spectrum of the $$K^+\rightarrow \pi ^+\nu {\bar{\nu }}$$
K
+
→
π
+
ν
ν
¯
decay opens a new path to test generalised quark–neutrino interactions with flavour changing $$s\rightarrow d$$
s
→
d
transitions and as such to novel probes of Physics beyond the Standard Model. Such signals can be a consequence of new lepton-number violating or lepton-number conserving interactions, with their interpretations depending on the Majorana versus Dirac nature of the neutrinos. Furthermore, the possible existence of new massive sterile neutrinos can be tested via their distinctive imprints in the invariant mass spectrum. Within the model-independent framework of the weak effective theory at dimension-six, we study the New Physics effects of Majorana and Dirac neutrinos on the differential distribution of $$K^+\rightarrow \pi ^+\nu {\bar{\nu }}$$
K
+
→
π
+
ν
ν
¯
allowing for lepton-number violating interactions and potential new sterile neutrinos. We determine the current and expected future sensitivity on the corresponding $$\Delta S=1$$
Δ
S
=
1
neutral-current Wilson coefficients using the distribution measured by the NA62 collaboration and accounting for expected improvements based on the HIKE experiment. We present single-operator fits and also determine correlations among different type of operators. Even though we focus on $$s\rightarrow d\nu \nu $$
s
→
d
ν
ν
transitions, the operator bases for Majorana and Dirac and the classification of lepton-number-violating/conserving interactions is applicable also for the study of $$b\rightarrow s/d\nu \nu $$
b
→
s
/
d
ν
ν
and $$c\rightarrow u\nu \nu $$
c
→
u
ν
ν
transitions relevant in current phenomenology.
Springer Science and Business Media LLC
Title: The anatomy of $$K^+\rightarrow \pi ^+\nu {\bar{\nu }}$$ distributions
Description:
AbstractThe excellent experimental prospects to measure the invisible mass spectrum of the $$K^+\rightarrow \pi ^+\nu {\bar{\nu }}$$
K
+
→
π
+
ν
ν
¯
decay opens a new path to test generalised quark–neutrino interactions with flavour changing $$s\rightarrow d$$
s
→
d
transitions and as such to novel probes of Physics beyond the Standard Model.
Such signals can be a consequence of new lepton-number violating or lepton-number conserving interactions, with their interpretations depending on the Majorana versus Dirac nature of the neutrinos.
Furthermore, the possible existence of new massive sterile neutrinos can be tested via their distinctive imprints in the invariant mass spectrum.
Within the model-independent framework of the weak effective theory at dimension-six, we study the New Physics effects of Majorana and Dirac neutrinos on the differential distribution of $$K^+\rightarrow \pi ^+\nu {\bar{\nu }}$$
K
+
→
π
+
ν
ν
¯
allowing for lepton-number violating interactions and potential new sterile neutrinos.
We determine the current and expected future sensitivity on the corresponding $$\Delta S=1$$
Δ
S
=
1
neutral-current Wilson coefficients using the distribution measured by the NA62 collaboration and accounting for expected improvements based on the HIKE experiment.
We present single-operator fits and also determine correlations among different type of operators.
Even though we focus on $$s\rightarrow d\nu \nu $$
s
→
d
ν
ν
transitions, the operator bases for Majorana and Dirac and the classification of lepton-number-violating/conserving interactions is applicable also for the study of $$b\rightarrow s/d\nu \nu $$
b
→
s
/
d
ν
ν
and $$c\rightarrow u\nu \nu $$
c
→
u
ν
ν
transitions relevant in current phenomenology.
Related Results
CP-violating observables of four-body $$B_{(s)} \rightarrow (\pi \pi )(K\bar{K})$$ decays in perturbative QCD
CP-violating observables of four-body $$B_{(s)} \rightarrow (\pi \pi )(K\bar{K})$$ decays in perturbative QCD
AbstractIn this work, we investigate six helicity amplitudes of the four-body $$B_{(s)} \rightarrow (\pi \pi )(K\bar{K})$$
...
Testing the molecular nature of the $$\Omega (2012)$$ with the $$\psi (3770) \rightarrow \bar{\Omega } \bar{K} \Xi $$ and $$\psi (3770) \rightarrow \bar{\Omega } \bar{K} \Xi ^*(1530) (\bar{\Omega } \bar{K} \pi \Xi )$$ reactions
Testing the molecular nature of the $$\Omega (2012)$$ with the $$\psi (3770) \rightarrow \bar{\Omega } \bar{K} \Xi $$ and $$\psi (3770) \rightarrow \bar{\Omega } \bar{K} \Xi ^*(1530) (\bar{\Omega } \bar{K} \pi \Xi )$$ reactions
Abstract
We report on the reactions
$$\psi (3770)\rightarrow \bar{\Omega }^+ \bar{K} \Xi $$
...
Study of four-body decays $$B_{(s)} \rightarrow (\pi \pi )(\pi \pi )$$ in the perturbative QCD approach
Study of four-body decays $$B_{(s)} \rightarrow (\pi \pi )(\pi \pi )$$ in the perturbative QCD approach
AbstractIn this work, we make a systematical study on the four-body $$B_{(s)} \rightarrow (\pi \pi )(\pi \pi )$$
B
...
Study of the $$B^{+}\rightarrow \pi ^{+}\left( \pi ^{+}\pi ^{-}\right) $$ decay in PQCD approach
Study of the $$B^{+}\rightarrow \pi ^{+}\left( \pi ^{+}\pi ^{-}\right) $$ decay in PQCD approach
AbstractBased on the fitting results of the LHCb collaboration on the contributions of various intermediate resonances to the$$B^{+}\rightarrow \pi ^{+}\pi ^{+}\pi ^{-}$$B+→π+π+π-d...
D-wave effects in diffractive electroproduction of heavy quarkonia from the photon-like $$V\rightarrow Q{\bar{Q}}$$ transition
D-wave effects in diffractive electroproduction of heavy quarkonia from the photon-like $$V\rightarrow Q{\bar{Q}}$$ transition
AbstractWe analyse the validity of a commonly used identification between structures of the virtual photon$$\gamma ^*\rightarrow Q\bar{Q}$$γ∗→QQ¯and vector meson$$V\rightarrow Q{\b...
Dark-sector physics in the search for the rare decays $$K^+\rightarrow \pi ^+ \nu {\bar{\nu }}$$ and $$K_L\rightarrow \pi ^0 \nu {\bar{\nu }}$$
Dark-sector physics in the search for the rare decays $$K^+\rightarrow \pi ^+ \nu {\bar{\nu }}$$ and $$K_L\rightarrow \pi ^0 \nu {\bar{\nu }}$$
AbstractWe compute the contribution of the decays $$K_L \rightarrow \pi ^0 Q {\bar{Q}}$$
K
L
...
EESTIMATES OF BEST APPROXIMATIONS OF FUNCTIONS WITH LOGARITHMIC SMOOTHNESS IN THE LORENTZ SPACE WITH ANISOTROPIC NORM
EESTIMATES OF BEST APPROXIMATIONS OF FUNCTIONS WITH LOGARITHMIC SMOOTHNESS IN THE LORENTZ SPACE WITH ANISOTROPIC NORM
In this paper, we consider the anisotropic Lorentz space \(L_{\bar{p}, \bar\theta}^{*}(\mathbb{I}^{m})\) of periodic functions of \(m\) variables. The Besov space \(B_{\bar{p}, \ba...
Investigating full-heavy tetraquarks composed of $$cc{\bar{c}}{\bar{b}}$$ and $$bb{\bar{b}}{\bar{c}}$$
Investigating full-heavy tetraquarks composed of $$cc{\bar{c}}{\bar{b}}$$ and $$bb{\bar{b}}{\bar{c}}$$
AbstractThe full-heavy tetraquarks $$cc{\bar{c}}{\bar{b}}$$
c
c
...

