Erratum to: Visible energy and angular distributions of the charged particle from the τ-decay in b → cτ μ ν ¯ μ ν τ π ν τ ρ ν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },\pi {\nu}_{\tau },\rho {\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: Online-Ressource, 1 online resource.

Language: Englisch

Bibliographic citation: Erratum to: Visible energy and angular distributions of the charged particle from the τ-decay in b → cτ μ ν ¯ μ ν τ π ν τ ρ ν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },\pi {\nu}_{\tau },\rho {\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions ; volume:2023 ; number:3 ; day:2 ; month:3 ; year:2023 ; pages:1-2 ; date:3.2023
Journal of high energy physics ; 2023, Heft 3 (2.3.2023), 1-2, 3.2023

Classification: Physik

Creator: Penalva, Neus
Hernández, Eliecer
Nieves, Juan

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2023)011

URN: urn:nbn:de:101:1-2023092610144829643888

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:57 AM CEST

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Penalva, Neus
Hernández, Eliecer
Nieves, Juan
SpringerLink (Online service)

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$Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions$

Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

$B c − → J / ψ → μ + μ − τ − → π − ν τ ρ − ν τ ℓ − ν ¯ ℓ ν τ ν ¯ τ $$ B}_c^{-}\to J/\psi \left(\to \mu}^{+}{\mu}^{-}\right){\tau}^{-}\left(\to \pi}^{-}{\nu}_{\tau },\rho}^{-}{\nu}_{\tau },\ell}^{-}{\overline{\nu}}_{\ell }{\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ decays with visible final-state kinematics$

B c − → J / ψ → μ + μ − τ − → π − ν τ ρ − ν τ ℓ − ν ¯ ℓ ν τ ν ¯ τ $$ B}_c^{-}\to J/\psi \left(\to \mu}^{+}{\mu}^{-}\right){\tau}^{-}\left(\to \pi}^{-}{\nu}_{\tau },\rho}^{-}{\nu}_{\tau },\ell}^{-}{\overline{\nu}}_{\ell }{\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ decays with visible final-state kinematics

$New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays$

New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays

$Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

$Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

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$Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG$

Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG

$Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations$

Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations

$K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory$

K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory

Messung der tau-Polarisation aus dem Zerfall tau->a_1 nu_tau mit dem L3-Detektor am LEP

$Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2$

Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2

$The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle$

The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle

Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

B c − → J / ψ → μ + μ − τ − → π − ν τ ρ − ν τ ℓ − ν ¯ ℓ ν τ ν ¯ τ $$ B}_c^{-}\to J/\psi \left(\to \mu}^{+}{\mu}^{-}\right){\tau}^{-}\left(\to \pi}^{-}{\nu}_{\tau },\rho}^{-}{\nu}_{\tau },\ell}^{-}{\overline{\nu}}_{\ell }{\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ decays with visible final-state kinematics

$New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays$

New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays

$Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

$Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

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$Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG$

Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG

$Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations$

Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations

K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory

Messung der tau-Polarisation aus dem Zerfall tau->a_1 nu_tau mit dem L3-Detektor am LEP

$Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2$

Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2

The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle

Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

B c − → J / ψ → μ + μ − τ − → π − ν τ ρ − ν τ ℓ − ν ¯ ℓ ν τ ν ¯ τ $$ B}_c^{-}\to J/\psi \left(\to \mu}^{+}{\mu}^{-}\right){\tau}^{-}\left(\to \pi}^{-}{\nu}_{\tau },\rho}^{-}{\nu}_{\tau },\ell}^{-}{\overline{\nu}}_{\ell }{\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ decays with visible final-state kinematics

$New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays$

New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays

$Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

$Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Hochschulschrift

Observation of W tau-nu tau decays with the ATLAS experiment

$Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG$

Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG

$Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations$

Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations

K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory

Messung der tau-Polarisation aus dem Zerfall tau->a_1 nu_tau mit dem L3-Detektor am LEP

$Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2$

Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2

The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle

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Erratum to: Visible energy and angular distributions of the charged particle from the τ-decay in b → cτ μ ν ¯ μ ν τ π ν τ ρ ν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },\pi {\nu}_{\tau },\rho {\nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

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Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Observation of W tau-nu tau decays with the ATLAS experiment

Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG

Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations

K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory

Messung der tau-Polarisation aus dem Zerfall tau->a_1 nu_tau mit dem L3-Detektor am LEP

Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2

The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle

Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Observation of W tau-nu tau decays with the ATLAS experiment

Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG

Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations

K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory

Messung der tau-Polarisation aus dem Zerfall tau->a_1 nu_tau mit dem L3-Detektor am LEP

Excess of tau events at SNDLHC, FASER $$\nu $$ ν and FASER $$\nu $$ ν 2

The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle

Visible energy and angular distributions of the charged particle from the τ −decay in b → cτ μ ν ¯ μ ν τ πν τ ρν τ ν ¯ τ $$ b\to c\tau \left(\mu \overline{\nu}}_{\mu }{\nu}_{\tau },{\pi \nu}_{\tau },{\rho \nu}_{\tau}\right){\overline{\nu}}_{\tau } $$ reactions

New physics and the tau polarization vector in b → c τ ν ¯ τ $$ \mathrmc}\tau \overline{\nu}}_{\tau } $$ decays

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Measurement of the ratio of branching fractions $\mathcalB}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$

Observation of W tau-nu tau decays with the ATLAS experiment

Clustering of B ¯ → D ∗ τ − ν ¯ τ $$ \overlineB}\to D}^{\left(\ast \right)}\tau}^{-}{\overline{\nu}}_{\tau } $$ kinematic distributions with ClusterKinG

Phenomenology of Λ b → Λ c τ ν ¯ τ $$ \Lambda}_b\to \Lambda}_c\tau \overline{\nu}}_{\tau } $$ using lattice QCD calculations

K + → μ + ν μ ν ν ¯ $$ \mathrm{K}}^{+}\to \mu}^{+}{\nu}_{\mu}\nu \overline\nu} $$ and K + → e + ν e ν ν ¯ $$ \mathrm{K}}^{+}\to \mathrm{e}}^{+}{\nu}_{\mathrm{e}}\nu \overline\nu} $$ decays within the Chiral Perturbation Theory

Messung der tau-Polarisation aus dem Zerfall tau->a_1 nu_tau mit dem L3-Detektor am LEP

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The hadronic $$\tau $$ τ decay $$\tau ^-\rightarrow K_1^-\nu _\tau \rightarrow (K^-\omega ) \nu _\tau \rightarrow (K^- \pi ^+\pi ^-\pi ^0)\nu _\tau $$ τ - → K 1 - ν τ → ( K - ω ) ν τ → ( K - π + π - π 0 ) ν τ and the axial vector mixing angle

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