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Colliding clusters and dark matter self-interactions
When a dark matter halo moves through a background of dark matter particles, self-interactions can lead to both deceleration and evaporation of the halo and thus shift its centroid relative to the collisionless stars and galaxies. We study the magnitude and time evolution of this shift for two class...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1093/mnras/stt2097 http://cds.cern.ch/record/1581350 |
_version_ | 1780931074849767424 |
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author | Kahlhoefer, Felix Schmidt-Hoberg, Kai Frandsen, Mads T. Sarkar, Subir |
author_facet | Kahlhoefer, Felix Schmidt-Hoberg, Kai Frandsen, Mads T. Sarkar, Subir |
author_sort | Kahlhoefer, Felix |
collection | CERN |
description | When a dark matter halo moves through a background of dark matter particles, self-interactions can lead to both deceleration and evaporation of the halo and thus shift its centroid relative to the collisionless stars and galaxies. We study the magnitude and time evolution of this shift for two classes of dark matter self-interactions, viz. frequent self-interactions with small momentum transfer (e.g. due to long-range interactions) and rare self-interactions with large momentum transfer (e.g. contact interactions), and find important differences between the two cases. We find that neither effect can be strong enough to completely separate the dark matter halo from the galaxies, if we impose conservative bounds on the self-interaction cross-section. The majority of both populations remain bound to the same gravitational potential and the peaks of their distributions are therefore always coincident. Consequently any apparent separation is mainly due to particles which are leaving the gravitational potential, so will be largest shortly after the collision but not observable in evolved systems. Nevertheless the fraction of collisions with large momentum transfer is an important characteristic of self-interactions, which can potentially be extracted from observational data and provide an important clue as to the nature of dark matter. |
id | cern-1581350 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-15813502021-10-27T02:15:48Zdoi:10.1093/mnras/stt2097http://cds.cern.ch/record/1581350engKahlhoefer, FelixSchmidt-Hoberg, KaiFrandsen, Mads T.Sarkar, SubirColliding clusters and dark matter self-interactionsAstrophysics and AstronomyWhen a dark matter halo moves through a background of dark matter particles, self-interactions can lead to both deceleration and evaporation of the halo and thus shift its centroid relative to the collisionless stars and galaxies. We study the magnitude and time evolution of this shift for two classes of dark matter self-interactions, viz. frequent self-interactions with small momentum transfer (e.g. due to long-range interactions) and rare self-interactions with large momentum transfer (e.g. contact interactions), and find important differences between the two cases. We find that neither effect can be strong enough to completely separate the dark matter halo from the galaxies, if we impose conservative bounds on the self-interaction cross-section. The majority of both populations remain bound to the same gravitational potential and the peaks of their distributions are therefore always coincident. Consequently any apparent separation is mainly due to particles which are leaving the gravitational potential, so will be largest shortly after the collision but not observable in evolved systems. Nevertheless the fraction of collisions with large momentum transfer is an important characteristic of self-interactions, which can potentially be extracted from observational data and provide an important clue as to the nature of dark matter.When a dark matter halo moves through a background of dark matter particles, self-interactions can lead to both deceleration and evaporation of the halo and thus shift its centroid relative to the collisionless stars and galaxies. We study the magnitude and time evolution of this shift for two classes of dark matter self-interactions, namely frequent self-interactions with small momentum transfer (e.g. due to long-range interactions) and rare self-interactions with large momentum transfer (e.g. contact interactions), and find important differences between the two cases. We find that neither effect can be strong enough to completely separate the dark matter halo from the galaxies, if we impose conservative bounds on the self-interaction cross-section. The majority of both populations remain bound to the same gravitational potential, and the peaks of their distributions are therefore always coincident. Consequently, any apparent separation is mainly due to particles which are leaving the gravitational potential, so will be largest shortly after the collision but not observable in evolved systems. Nevertheless, the fraction of collisions with large momentum transfer is an important characteristic of self-interactions, which can potentially be extracted from observational data and provide an important clue as to the nature of dark matter.When a dark matter halo moves through a background of dark matter particles, self-interactions can lead to both deceleration and evaporation of the halo and thus shift its centroid relative to the collisionless stars and galaxies. We study the magnitude and time evolution of this shift for two classes of dark matter self-interactions, viz. frequent self-interactions with small momentum transfer (e.g. due to long-range interactions) and rare self-interactions with large momentum transfer (e.g. contact interactions), and find important differences between the two cases. We find that neither effect can be strong enough to completely separate the dark matter halo from the galaxies, if we impose conservative bounds on the self-interaction cross-section. The majority of both populations remain bound to the same gravitational potential and the peaks of their distributions are therefore always coincident. Consequently any apparent separation is mainly due to particles which are leaving the gravitational potential, so will be largest shortly after the collision but not observable in evolved systems. Nevertheless the fraction of collisions with large momentum transfer is an important characteristic of self-interactions, which can potentially be extracted from observational data and provide an important clue as to the nature of dark matter.arXiv:1308.3419CERN-PH-TH-2013-194NSF-KITP-13-140CP3-ORIGINS-2013-029DIAS-2013-29OUTP-13-14PCERN-PH-TH-2013-194NSF-KITP-13-140CP3-ORIGINS-2013-029 DNRF90DIAS-2013-29OUTP-13-14Poai:cds.cern.ch:15813502013-08-15 |
spellingShingle | Astrophysics and Astronomy Kahlhoefer, Felix Schmidt-Hoberg, Kai Frandsen, Mads T. Sarkar, Subir Colliding clusters and dark matter self-interactions |
title | Colliding clusters and dark matter self-interactions |
title_full | Colliding clusters and dark matter self-interactions |
title_fullStr | Colliding clusters and dark matter self-interactions |
title_full_unstemmed | Colliding clusters and dark matter self-interactions |
title_short | Colliding clusters and dark matter self-interactions |
title_sort | colliding clusters and dark matter self-interactions |
topic | Astrophysics and Astronomy |
url | https://dx.doi.org/10.1093/mnras/stt2097 http://cds.cern.ch/record/1581350 |
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