Related Experiment Video
Updated: Sep 13, 2025

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
6.9K
Evidence for B^{-}→D^{**0}τ^{-}ν_{τ}[over ¯] Decays
R Aaij1, A S W Abdelmotteleb2, C Abellan Beteta3
1Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands.
Physical Review Letters
|July 31, 2025
Summary
The LHCb experiment observed the first evidence of the B-meson decay into a D**0 meson and tau lepton. This finding provides new insights into B-meson decays and particle physics at high energies.
Area of Science:
- High Energy Physics
- Particle Physics
- Experimental Physics
Background:
- B-meson decays are crucial for testing the Standard Model of particle physics.
- Understanding rare B-meson decays can reveal new physics phenomena.
- Previous studies have focused on decays involving lighter leptons, leaving tauonic decays less explored.
Purpose of the Study:
- To search for and provide the first evidence of the B-meson decay B^{-}→D^{**0}τ^{-}ν[over ¯]_{τ}.
- To measure the branching fraction of this decay mode.
- To investigate the ratio of tauonic to muonic B-meson decays.
Main Methods:
- Analysis of proton-proton collision data collected by the LHCb experiment at 7, 8, and 13 TeV.
- Identification of D^{**0} mesons, which include D_{1}(2420)^{0}, D_{2}^{*}(2460)^{0}, and D_{1}^{'}(2400)^{0} states.
- Statistical analysis to establish the significance of the observed signal and measure branching fractions.
Main Results:
- First evidence for the decay B^{-}→D^{**0}τ^{-}ν[over ¯]_{τ} observed with a 3.5σ significance.
- Combined branching fraction B(B^{-}→D_{1,2}^{**0}τ^{-}ν[over ¯]_{τ})×B(D_{1,2}^{**0}→D^{*+}π^{-}) measured as [0.051±0.013(stat)±0.006(syst)±0.009(ext)]%.
- Ratio of tauonic to muonic decays R(D_{1,2}^{**0}) determined to be 0.13±0.03(stat)±0.01(syst)±0.02(ext).
Conclusions:
- The observation of B^{-}→D^{**0}τ^{-}ν[over ¯]_{τ} provides crucial experimental data for B-physics.
- The measured branching fraction and ratio R(D_{1,2}^{**0}) can be used to test theoretical models of New Physics.
- This result contributes to a more comprehensive understanding of semileptonic B-decays involving tau leptons.
Related Concept Videos
Atomic Nuclei: Nuclear Spin State Population Distribution
1.2K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
1.2K
Thomson's e/m Experiment
4.5K
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
4.5K
Nuclear Stability
20.0K
Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together...
To hold positively charged protons together...
20.0K
¹³C NMR: ¹H–¹³C Decoupling
1.2K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.2K
Types of Radioactivity
17.4K
The most common types of radioactivity are α decay, β decay, γ decay, neutron emission, and electron capture.
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
17.4K
Atomic Nuclei: Types of Nuclear Relaxation
389
Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
389

