Related Experiment Video
Updated: Jun 7, 2025

07:46
Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
8.5K
Antiproton annihilation at rest in thin solid targets and comparison with Monte Carlo simulations
Summary
Antiproton-nucleus annihilation at rest remains poorly understood. New measurements using antiprotons at CERN on carbon, molybdenum, and gold nuclei show current models do not fully explain the observed charged particle data.
Area of Science:
- Nuclear Physics
- Particle Physics
- Hadron Physics
Background:
- The mechanism of antiproton-nucleus annihilation at rest is a complex phenomenon with ongoing theoretical and experimental investigations.
- Despite extensive research, a complete understanding of the annihilation process and its resulting particle production is still lacking.
Purpose of the Study:
- To experimentally investigate antiproton-nucleus annihilation at rest by measuring charged particle multiplicities and energy deposits.
- To compare experimental results with predictions from established simulation tools (Geant4, FLUKA) and various theoretical models.
Main Methods:
- Utilized slow extracted antiprotons from the ASACUSA apparatus at CERN.
- Conducted experiments involving antiproton annihilation at rest on carbon, molybdenum, and gold targets.
- Measured charged particle multiplicities and their energy deposits.
Main Results:
- Collected detailed data on charged particle production and energy deposition for antiproton annihilations on different nuclei.
- Observed discrepancies between experimental data and predictions from current simulation models.
- Identified specific features of the annihilation process not adequately reproduced by existing models.
Conclusions:
- Current theoretical models and simulation tools do not fully account for the observed features of antiproton-nucleus annihilation at rest.
- Further experimental measurements, particularly at low energies, are crucial for validating and refining theoretical models.
- The study highlights the need for improved models to accurately describe antiproton-nucleus interactions.
Related Concept Videos
Mass Analyzers: Common Types
570
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
570
Atomic Absorption Spectroscopy: Lab
311
For AAS measurements, samples must be introduced as clear solutions, often requiring extensive preliminary treatment to dissolve materials like soils, animal tissues, and minerals. Common methods for sample preparation include treatment with hot mineral acids, wet ashing, combustion in closed containers, high-temperature ashing, or fusion with reagents.
Solutions containing organic solvents, such as low-molecular-mass alcohols, esters, or ketones, enhance absorbances by increasing...
Solutions containing organic solvents, such as low-molecular-mass alcohols, esters, or ketones, enhance absorbances by increasing...
311
Mass Analyzers: Overview
596
The mass analyzer is a crucial component of the mass spectrometer. In the ionization chamber, the vaporized sample is bombarded with a high-energy electron beam to generate a radical cation and further fragment into neutral molecules, radicals, and cations. A series of negatively charged accelerator plates accelerate the cations into the mass analyzer. The mass analyzer separates ions according to their mass-to-charge (m/z) ratios and then directs them to the detector. The common types of mass...
596
Proton (¹H) NMR: Chemical Shift
1.5K
Organic molecules primarily contain carbon and hydrogen atoms. While all the hydrogen isotopes are NMR-active, protium or hydrogen-1 is the most abundant. It has a significant energy separation between its nuclear spin states due to its large gyromagnetic ratio. As per Boltzmann's distribution, an increase in the energy separation implies a greater excess population of nuclei available for excitation, resulting in a strong NMR absorption signal.
Absorption signals of all the protium nuclei...
Absorption signals of all the protium nuclei...
1.5K
Atomic Nuclei: Nuclear Spin State Population Distribution
948
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.
948
Nuclear Transmutation
17.4K
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...
17.4K

