Cargando…
Halo-Independent Direct Detection Analyses Without Mass Assumptions
Results from direct detection experiments are typically interpreted by employing an assumption about the dark matter velocity distribution, with results presented in the $m_\chi-\sigma_n$ plane. Recently methods which are independent of the DM halo velocity distribution have been developed which pre...
Autores principales: | , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2015
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1475-7516/2015/10/012 http://cds.cern.ch/record/2008997 |
_version_ | 1780946446714929152 |
---|---|
author | Anderson, Adam J. Fox, Patrick J. Kahn, Yonatan McCullough, Matthew |
author_facet | Anderson, Adam J. Fox, Patrick J. Kahn, Yonatan McCullough, Matthew |
author_sort | Anderson, Adam J. |
collection | CERN |
description | Results from direct detection experiments are typically interpreted by employing an assumption about the dark matter velocity distribution, with results presented in the $m_\chi-\sigma_n$ plane. Recently methods which are independent of the DM halo velocity distribution have been developed which present results in the $v_{min}-\tilde{g}$ plane, but these in turn require an assumption on the dark matter mass. Here we present an extension of these halo-independent methods for dark matter direct detection which does not require a fiducial choice of the dark matter mass. With a change of variables from $v_{min}$ to nuclear recoil momentum ($p_R$), the full halo-independent content of an experimental result for any dark matter mass can be condensed into a single plot as a function of a new halo integral variable, which we call $\tilde{h}(p_R)$. The entire family of conventional halo-independent $\tilde{g}(v_{min})$ plots for all DM masses are directly found from the single $\tilde{h}(p_R)$ plot through a simple rescaling of axes. By considering results in $\tilde{h}(p_R)$ space, one can determine if two experiments are inconsistent for all masses and all physically possible halos, or for what range of dark matter masses the results are inconsistent for all halos, without the necessity of multiple $\tilde{g}(v_{min})$ plots for different DM masses. We conduct a sample analysis comparing the CDMS II Si events to the null results from LUX, XENON10, and SuperCDMS using our method and discuss how the mass-independent limits can be strengthened by imposing the physically reasonable requirement of a finite halo escape velocity. |
id | cern-2008997 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2015 |
record_format | invenio |
spelling | cern-20089972023-03-14T19:34:34Zdoi:10.1088/1475-7516/2015/10/012http://cds.cern.ch/record/2008997engAnderson, Adam J.Fox, Patrick J.Kahn, YonatanMcCullough, MatthewHalo-Independent Direct Detection Analyses Without Mass AssumptionsParticle Physics - PhenomenologyResults from direct detection experiments are typically interpreted by employing an assumption about the dark matter velocity distribution, with results presented in the $m_\chi-\sigma_n$ plane. Recently methods which are independent of the DM halo velocity distribution have been developed which present results in the $v_{min}-\tilde{g}$ plane, but these in turn require an assumption on the dark matter mass. Here we present an extension of these halo-independent methods for dark matter direct detection which does not require a fiducial choice of the dark matter mass. With a change of variables from $v_{min}$ to nuclear recoil momentum ($p_R$), the full halo-independent content of an experimental result for any dark matter mass can be condensed into a single plot as a function of a new halo integral variable, which we call $\tilde{h}(p_R)$. The entire family of conventional halo-independent $\tilde{g}(v_{min})$ plots for all DM masses are directly found from the single $\tilde{h}(p_R)$ plot through a simple rescaling of axes. By considering results in $\tilde{h}(p_R)$ space, one can determine if two experiments are inconsistent for all masses and all physically possible halos, or for what range of dark matter masses the results are inconsistent for all halos, without the necessity of multiple $\tilde{g}(v_{min})$ plots for different DM masses. We conduct a sample analysis comparing the CDMS II Si events to the null results from LUX, XENON10, and SuperCDMS using our method and discuss how the mass-independent limits can be strengthened by imposing the physically reasonable requirement of a finite halo escape velocity.Results from direct detection experiments are typically interpreted by employing an assumption about the dark matter velocity distribution, with results presented in the m(χ)−σn plane. Recently methods which are independent of the DM halo velocity distribution have been developed which present results in the v(min)−tilde g plane, but these in turn require an assumption on the dark matter mass. Here we present an extension of these halo-independent methods for dark matter direct detection which does not require a fiducial choice of the dark matter mass. With a change of variables from v(min) to nuclear recoil momentum (pR), the full halo-independent content of an experimental result for any dark matter mass can be condensed into a single plot as a function of a new halo integral variable, which we call tilde h(pR). The entire family of conventional halo-independent tilde g(v(min)) plots for all DM masses are directly found from the single tilde h(pR) plot through a simple rescaling of axes. By considering results in tilde h(pR) space, one can determine if two experiments are inconsistent for all masses and all physically possible halos, or for what range of dark matter masses the results are inconsistent for all halos, without the necessity of multiple tilde g(v(min)) plots for different DM masses. We conduct a sample analysis comparing the CDMS II Si events to the null results from LUX, XENON10, and SuperCDMS using our method and discuss how the results can be strengthened by imposing the physically reasonable requirement of a finite halo escape velocity.Results from direct detection experiments are typically interpreted by employing an assumption about the dark matter velocity distribution, with results presented in the $m_\chi-\sigma_n$ plane. Recently methods which are independent of the DM halo velocity distribution have been developed which present results in the $v_{min}-\tilde{g}$ plane, but these in turn require an assumption on the dark matter mass. Here we present an extension of these halo-independent methods for dark matter direct detection which does not require a fiducial choice of the dark matter mass. With a change of variables from $v_{min}$ to nuclear recoil momentum ($p_R$), the full halo-independent content of an experimental result for any dark matter mass can be condensed into a single plot as a function of a new halo integral variable, which we call $\tilde{h}(p_R)$. The entire family of conventional halo-independent $\tilde{g}(v_{min})$ plots for all DM masses are directly found from the single $\tilde{h}(p_R)$ plot through a simple rescaling of axes. By considering results in $\tilde{h}(p_R)$ space, one can determine if two experiments are inconsistent for all masses and all physically possible halos, or for what range of dark matter masses the results are inconsistent for all halos, without the necessity of multiple $\tilde{g}(v_{min})$ plots for different DM masses. We conduct a sample analysis comparing the CDMS II Si events to the null results from LUX, XENON10, and SuperCDMS using our method and discuss how the mass-independent limits can be strengthened by imposing the physically reasonable requirement of a finite halo escape velocity.arXiv:1504.03333CERN-PH-TH-2015-073FERMILAB-PUB-15-096-TMIT-CTP-4661CERN-PH-TH-2015-073FERMILAB-PUB-15-096-TMIT-CTP-4661oai:cds.cern.ch:20089972015-04-13 |
spellingShingle | Particle Physics - Phenomenology Anderson, Adam J. Fox, Patrick J. Kahn, Yonatan McCullough, Matthew Halo-Independent Direct Detection Analyses Without Mass Assumptions |
title | Halo-Independent Direct Detection Analyses Without Mass Assumptions |
title_full | Halo-Independent Direct Detection Analyses Without Mass Assumptions |
title_fullStr | Halo-Independent Direct Detection Analyses Without Mass Assumptions |
title_full_unstemmed | Halo-Independent Direct Detection Analyses Without Mass Assumptions |
title_short | Halo-Independent Direct Detection Analyses Without Mass Assumptions |
title_sort | halo-independent direct detection analyses without mass assumptions |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1088/1475-7516/2015/10/012 http://cds.cern.ch/record/2008997 |
work_keys_str_mv | AT andersonadamj haloindependentdirectdetectionanalyseswithoutmassassumptions AT foxpatrickj haloindependentdirectdetectionanalyseswithoutmassassumptions AT kahnyonatan haloindependentdirectdetectionanalyseswithoutmassassumptions AT mcculloughmatthew haloindependentdirectdetectionanalyseswithoutmassassumptions |