The radiation background produced by the 21 cm spin-flip transition of neutral hydrogen at high redshifts can be a pristine probe of fundamental physics and cosmology. At z~30–300, the intergalactic medium (IGM) is visible in 21 cm absorption against the cosmic microwave background (CMB), with a strength that depends on the thermal (and ionization) history of the IGM. Here we examine the constraints this background can place on dark matter decay and annihilation, which could heat and ionize the IGM through the production of high-energy particles. Using a simple model for dark matter decay, we show that, if the decay energy is immediately injected into the IGM, the 21 cm background can detect energy injection rates>~10^-24 eV cm^-3 sec^-1. I...
The H atoms inside minihalos (i.e., halos with virial temperatures T-vir <= 10(4) K, in the mass ran...
It is extremely important to understand the processes through which the thermal state of the inter-g...
Dark Matter annihilations after recombination and during the epoch of structure formation deposit en...
The radiation background produced by the 21 cm spin-flip transition of neutral hydrogen at high reds...
The radiation background produced by the 21 cm spin-flip transition of neutral hydrogen at high reds...
Measurements of the temperature of the baryons at the end of the cosmic dark ages can potentially se...
We use the latest cosmic microwave background (CMB) observations to provide updated constraints on t...
Beyond reionization epoch cosmic hydrogen is neutral and can be directly observed through its 21-cm ...
The observation of an absorption feature in the 21-cm spectrum at redshift z≈17 implies bounds on da...
If dark matter decays to electromagnetically interacting particles, it can inject energy into the ba...
International audienceThe annihilation or decay of Dark Matter (DM) particles could affect the therm...
We examine the maximum possible strength of the global 21-cm absorption dip on the cosmic background...
We derived the evolution of the energy deposition in the intergalactic medium (IGM) by different dec...
We consider particle decays during the cosmic dark ages with two aims: (1) to explain the high optic...
We derive the evolution of the energy deposition in the intergalactic medium (IGM) by dark matter (D...
The H atoms inside minihalos (i.e., halos with virial temperatures T-vir <= 10(4) K, in the mass ran...
It is extremely important to understand the processes through which the thermal state of the inter-g...
Dark Matter annihilations after recombination and during the epoch of structure formation deposit en...
The radiation background produced by the 21 cm spin-flip transition of neutral hydrogen at high reds...
The radiation background produced by the 21 cm spin-flip transition of neutral hydrogen at high reds...
Measurements of the temperature of the baryons at the end of the cosmic dark ages can potentially se...
We use the latest cosmic microwave background (CMB) observations to provide updated constraints on t...
Beyond reionization epoch cosmic hydrogen is neutral and can be directly observed through its 21-cm ...
The observation of an absorption feature in the 21-cm spectrum at redshift z≈17 implies bounds on da...
If dark matter decays to electromagnetically interacting particles, it can inject energy into the ba...
International audienceThe annihilation or decay of Dark Matter (DM) particles could affect the therm...
We examine the maximum possible strength of the global 21-cm absorption dip on the cosmic background...
We derived the evolution of the energy deposition in the intergalactic medium (IGM) by different dec...
We consider particle decays during the cosmic dark ages with two aims: (1) to explain the high optic...
We derive the evolution of the energy deposition in the intergalactic medium (IGM) by dark matter (D...
The H atoms inside minihalos (i.e., halos with virial temperatures T-vir <= 10(4) K, in the mass ran...
It is extremely important to understand the processes through which the thermal state of the inter-g...
Dark Matter annihilations after recombination and during the epoch of structure formation deposit en...