Nucleon-nucleon, axion bremsstrahlung is the primary mechanism for axion emission from the nascent neutron star associated with SN 1987A, and the rate for this process has been calculated in the one pion exchange approximation (OPE). The axion mass limit which follows from SN 1987A, m sub a less than or approx equal to 10 to the -3 eV, is the most stringent astrophysical bound, and has received much scrutiny. It has been suggested that by using OPE to calculate the cross section for the analog process, pp yields pp + pi sup o, and comparing the result of the experimental data one can test the validity of this approximation, and further, that such a comparison indicates that OPE leads to a value for this cross section which is a factor of 30...
Direct Chandra observations of a surface temperature of isolated neutron star in Cassiopeia A (Cas A...
In order to solve the strong CP problem, a new neutral particle with spin-parity 0^{-}, the axion, w...
An axion with a mass greater than 1 eV should be detectable through its decay into two photons. The ...
We re-examine the very stringent limits on the axion mass based on the strength and duration of the ...
The most efficient axion production mechanism in a supernova (SN) core is the nucleon-nucleon bremss...
The rates of axion emission by nucleon-nucleon bremsstrahlung are calculated with the inclusion of t...
We re-examine the very stringent limits on the axion mass based on the strength and duration of the ...
If an axion of mass between about 10(exp -3) and 10 eV exists, axion emission would have significant...
Supernovae provide fascinating opportunities to study various particles and their interactions. Amon...
The effect of free-streaming axion emission on numerical models for the cooling of the newly born ne...
We calculate the axion emission rate from reactions involving thermal pions in matter encountered in...
Peccei-Quinn symmetry with attendant axion is a most compelling, and perhaps the most minimal, exten...
Open Access ©The Authors. Article funded by SCOAP3 We examine the axion emission from supernovae wit...
Axion emission by hot and dense plasmas is a new energy-loss channel for stars. Observational conseq...
We perform general relativistic one-dimensional supernova (SN) simulations to identify observable si...
Direct Chandra observations of a surface temperature of isolated neutron star in Cassiopeia A (Cas A...
In order to solve the strong CP problem, a new neutral particle with spin-parity 0^{-}, the axion, w...
An axion with a mass greater than 1 eV should be detectable through its decay into two photons. The ...
We re-examine the very stringent limits on the axion mass based on the strength and duration of the ...
The most efficient axion production mechanism in a supernova (SN) core is the nucleon-nucleon bremss...
The rates of axion emission by nucleon-nucleon bremsstrahlung are calculated with the inclusion of t...
We re-examine the very stringent limits on the axion mass based on the strength and duration of the ...
If an axion of mass between about 10(exp -3) and 10 eV exists, axion emission would have significant...
Supernovae provide fascinating opportunities to study various particles and their interactions. Amon...
The effect of free-streaming axion emission on numerical models for the cooling of the newly born ne...
We calculate the axion emission rate from reactions involving thermal pions in matter encountered in...
Peccei-Quinn symmetry with attendant axion is a most compelling, and perhaps the most minimal, exten...
Open Access ©The Authors. Article funded by SCOAP3 We examine the axion emission from supernovae wit...
Axion emission by hot and dense plasmas is a new energy-loss channel for stars. Observational conseq...
We perform general relativistic one-dimensional supernova (SN) simulations to identify observable si...
Direct Chandra observations of a surface temperature of isolated neutron star in Cassiopeia A (Cas A...
In order to solve the strong CP problem, a new neutral particle with spin-parity 0^{-}, the axion, w...
An axion with a mass greater than 1 eV should be detectable through its decay into two photons. The ...