Related Experiment Video
Updated: Mar 9, 2026

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
7.4K
Measurement of CP Violation in B^{0}→D^{+}D^{-} Decays
R Aaij1, B Adeva2, M Adinolfi3
1European Organization for Nuclear Research (CERN), Geneva, Switzerland.
Physical Review Letters
|January 7, 2017
Summary
Researchers observed CP violation in B0 decays to D+D- using LHCb data. This evidence for CP violation, a key phenomenon in particle physics, was found with a significance of 4.0 standard deviations.
Area of Science:
- Particle Physics
- High-Energy Physics
- Quantum Mechanics
Background:
- CP violation is a fundamental asymmetry in particle physics.
- Understanding CP violation is crucial for explaining the matter-antimatter asymmetry in the universe.
- The B0→D+D- decay channel provides a sensitive probe for CP violation studies.
Purpose of the Study:
- To measure CP violation observables S and C in the B0→D+D- decay.
- To search for direct CP violation and CP violation in the interference between mixing and decay.
- To constrain higher-order Standard Model corrections.
Main Methods:
- Analysis of proton-proton collision data collected by the LHCb experiment at 7 and 8 TeV.
- Utilizing a flavor-tagged, decay-time-dependent analysis.
- Statistical analysis of a large dataset corresponding to an integrated luminosity of 3 fb⁻¹.
Main Results:
- Measured CP violation observable S = -0.54 ± 0.17.
- Measured direct CP violation observable C = 0.26 ± 0.18.
- Evidence for CP violation established at 4.0 standard deviations.
- Constrained the phase shift from higher-order Standard Model corrections to Δϕ = -0.16 ± 0.19 rad.
Conclusions:
- The study provides significant evidence for CP violation in the B0→D+D- decay.
- The results contribute to a more precise understanding of CP violation within the Standard Model.
- The findings offer insights into the subtle differences between matter and antimatter.
Related Concept Videos
¹³C NMR: ¹H–¹³C Decoupling
2.0K
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...
2.0K
Thomson's e/m Experiment
7.3K
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 magnetic...
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 magnetic...
7.3K
Atomic Nuclei: Nuclear Magnetic Moment
3.5K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
3.5K
Calculation of First Law Quantities I
12
Thermodynamic systems undergoing phase transitions or temperature changes experience energy transfer in the form of heat (q) and work (w). For a reversible phase change at constant temperature (T) and pressure (p), the process involves no chemical reaction but results in energy exchange between distinct phases.The heat transferred during this process corresponds to the latent heat of transition, which is the amount of heat energy absorbed or released by a substance when it changes from one...
12
Nuclear Binding Energy
15.0K
The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons are bound...
15.0K
Moment-of-Momentum Equation
494
The moment-of-momentum equation is a critical tool for analyzing the torque produced by the rotating blades of a wind turbine. This equation is derived by applying Newton's second law to a fluid particle, which states that the rate of change of linear momentum is equal to the external force acting on the particle.
494

