Related Experiment Video
Updated: May 27, 2026

08:14
Atom Probe Tomography Analysis of Exsolved Mineral Phases
Published on: October 25, 2019
Spallation model for the titanium-rich supernova remnant cassiopeia A
Rachid Ouyed1, Denis Leahy, Amir Ouyed
1Department of Physics and Astronomy, University of Calgary, 2500 University Drive NW, Calgary, Alberta T2N 1N4 Canada.
Physical Review Letters
|November 24, 2011
Summary
A novel model explains rare titanium-rich supernovae. A neutron star
Area of Science:
- * Astrophysics
- * Nuclear Astrophysics
- * Supernova Physics
Background:
- * Titanium-rich subluminous supernovae are rare and pose challenges to existing nucleosynthesis models.
- * Understanding the formation of these supernovae is crucial for refining astrophysical models.
Purpose of the Study:
- * To propose a new model explaining the formation of titanium-rich subluminous supernovae.
- * To investigate the role of neutron star explosions (quark novas) in supernova nucleosynthesis.
- * To reconcile the observed abundances and low luminosity of certain supernovae.
Main Methods:
- * Modeling the interaction between ejecta from a standard supernova and a subsequent neutron star explosion (quark nova).
- * Analyzing spallation reactions occurring due to the impact of the second explosion.
- * Performing basic calculations of spallation products and their abundances.
Main Results:
- * The proposed model, involving a quark nova impacting supernova ejecta, can explain titanium-rich supernovae.
- * A delay of approximately 5 days between the two explosions is calculated to reproduce the observed abundance of Titanium-44 (44Ti) in Cassiopeia A (Cas A).
- * This model accounts for the destruction of Nickel-56 (56Ni), explaining the low luminosity of these supernovae.
Conclusions:
- * The model provides a viable explanation for titanium-rich subluminous supernovae.
- * The findings have significant implications for understanding the light curves of both subluminous and superluminous supernovae.
- * This research advances the understanding of nucleosynthesis processes in extreme astrophysical events.
Related Concept Videos
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...
Atomic Emission Spectroscopy: Overview
Atomic emission spectroscopy (AES) is an analytical technique used to determine the elemental composition of a sample by analyzing the light emitted from excited atoms. In AES, atoms in a sample are excited to higher energy levels by thermal energy from high-temperature sources, such as plasma, arcs, or sparks. When these excited atoms return to lower energy states, they emit light at specific wavelengths characteristic of each element. The resulting atomic emission spectrum, which consists of...
Nuclear Fusion
The process of converting very light nuclei into heavier nuclei is also accompanied by the conversion of mass into large amounts of energy, a process called fusion. The principal source of energy in the sun is a net fusion reaction in which four hydrogen nuclei fuse and ultimately produce one helium nucleus and two positrons.
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...
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.
Thomson's e/m Experiment
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...
Atomic Emission Spectroscopy: Instrumentation
The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers. Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.

