Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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.
Atomic Nuclei: Nuclear Magnetic Moment00:59

Atomic Nuclei: Nuclear Magnetic Moment

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...
¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

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...
Nuclear Transmutation03:20

Nuclear Transmutation

Nuclear transmutation is the conversion of one nuclide into another. It can occur by the radioactive decay of a nucleus, or the reaction of a nucleus with another particle. The first manmade nucleus was produced in Ernest Rutherford’s laboratory in 1919 by a transmutation reaction, the bombardment of one type of nuclei with other nuclei or with neutrons. Rutherford bombarded nitrogen-14 atoms with high-speed α particles from a natural radioactive isotope of radium and observed protons being...
Consecutive Reactions01:22

Consecutive Reactions

Consecutive reactions involve a sequence where the product of a preceding reaction becomes the reactant for the subsequent one. In a simple scheme, A transforms into B, which further reacts to form C, with rate constants k1 and k2, respectively. This concept is evident in the radioactive decay series. Assuming an initial state with only A present, the conservation of matter leads to three coupled differential equations, determining the concentrations of A, B, and C over time.The rate of change...
Types of Radioactivity03:23

Types of Radioactivity

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:

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

High-precision measurement of the <i>W</i> boson mass with the CDF II detector.

Science (New York, N.Y.)·2022
Same author

Search for the Exotic Meson X(5568) with the Collider Detector at Fermilab.

Physical review letters·2018
Same author

Combined Forward-Backward Asymmetry Measurements in Top-Antitop Quark Production at the Tevatron.

Physical review letters·2018
Same author

Tevatron Combination of Single-Top-Quark Cross Sections and Determination of the Magnitude of the Cabibbo-Kobayashi-Maskawa Matrix Element V_{tb}.

Physical review letters·2015
Same author

Search for Resonances Decaying to Top and Bottom Quarks with the CDF Experiment.

Physical review letters·2015
Same author

Search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks using a matrix element method.

The European physical journal. C, Particles and fields·2015

Related Experiment Video

Updated: May 26, 2026

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

Search for B(s)(0) → μ+ μ- and B(0) → μ+ μ- decays with CDF II.

T Aaltonen1, B Álvarez González, S Amerio

  • 1Division of High Energy Physics, Department of Physics, University of Helsinki and Helsinki Institute of Physics, FIN-00014, Helsinki, Finland.

Physical Review Letters
|December 21, 2011
PubMed
Summary
This summary is machine-generated.

Researchers searched for rare B meson decays into muon pairs. The study found no evidence for B0 to muon pairs but observed an intriguing excess in B(s)0 to muon pairs, suggesting new physics possibilities.

More Related Videos

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
10:42

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh

Published on: May 3, 2019

Carrier Lifetime Measurements in Semiconductors through the Microwave Photoconductivity Decay Method
07:38

Carrier Lifetime Measurements in Semiconductors through the Microwave Photoconductivity Decay Method

Published on: April 18, 2019

Related Experiment Videos

Last Updated: May 26, 2026

Setting Limits on Supersymmetry Using Simplified Models
07:46

Setting Limits on Supersymmetry Using Simplified Models

Published on: November 15, 2013

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
10:42

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh

Published on: May 3, 2019

Carrier Lifetime Measurements in Semiconductors through the Microwave Photoconductivity Decay Method
07:38

Carrier Lifetime Measurements in Semiconductors through the Microwave Photoconductivity Decay Method

Published on: April 18, 2019

Area of Science:

  • Particle Physics
  • High-Energy Physics
  • Collider Physics

Background:

  • Rare B meson decays are sensitive probes of fundamental physics.
  • The decay B(s)0 → μ+ μ- is highly suppressed in the Standard Model, making it a key channel for searching for new physics beyond the Standard Model.

Purpose of the Study:

  • To search for the rare decays B(s)0 → μ+ μ- and B0 → μ+ μ-.
  • To set limits on or measure the branching fractions of these decays.

Main Methods:

  • Analysis of 7 fb(-1) of integrated luminosity data collected by the CDF II detector at the Fermilab Tevatron collider.
  • Candidate selection for B(s)0 and B0 mesons decaying into muon pairs.
  • Statistical analysis to determine significance and set limits.

Main Results:

  • An upper limit on the branching fraction of B(B0 → μ+ μ-) < 6.0 × 10(-9) at 95% confidence level was established.
  • An excess of B(s)0 candidates was observed, with a probability of 0.27% for background alone to produce such an excess.
  • The branching fraction for B(s)(0) → μ+ μ- was measured as (1.8(-0.9) (+1.1)) × 10(-8), with an upper limit of < 4.0 × 10(-8) at 95% confidence level.

Conclusions:

  • The results for B0 → μ+ μ- are consistent with Standard Model background expectations.
  • The observed excess in B(s)0 → μ+ μ- warrants further investigation and may hint at contributions from new physics phenomena.
  • The measurements provide stringent constraints on new physics scenarios.