Searching for Dark Photon Dark Matter with Cosmic Ray Antideuterons

 
Searching for Dark Photon Dark
Matter with Cosmic Ray
Antideuterons
 
Lisa Randall
(w/Linda Xu)
 
Mary K Fest Sept, 2019
 
Why Antideuteron Searches
 
“Indirect detection” one of three pillars of WIMP searches
Antiparticle and distinctive photon signatures have potential to find
unusual cosmological processes
What to look for?
Positrons, photons, antiprotons
However, few DM models favor first two
More importantly, background difficult to calculate
“Discoveries” have taught us some interesting unanticpated astronphysics
Antiproton searches promising, but  background big there too
Antideuteron searches for same type of dark matter as antiprotons
But background low at small kinetic energy (astro background
higher KE)
Makes it a potentially essentially background free measurement
Only a few detections suffice for discovery
 
Why So Little Background?
 
Assuming proton collides with X in ISM,
To make an antiproton,  at least four nucleons in final state
To make an antideuteron, you need at least six
Threshold energy
First case 7 mp
Antideuteron 17 mp
Binding energy is 2.2 MeV
Hard to slow down without dissociating
 
Low background targets are good places to search
DM annihilations usually close to at rest
Possibility antiproton and antineutron produced with relatively
small momentum difference
In which case can coalesce
Rare process
But background calculable and essentially nonexistent (for low T)
 
Is anyone looking? Yes!!
 
In principle AMS II
General AntiParticle Spectrometer (GAPS)
Antarctic balloon mission
Looks for antideuteron <0.25 GeV/n
Uses an exotic atom technique
Slow low energy antiparticles so they get captured by
a nucleus
Exotic atom decays emitting X-ray
Correlated pion, proton from subsequent nuclear
annihilation
GAPS
 
Long duration balloon experiment
Antideuterons captured and result in exotic atom in final state
Decays into X-rays at well-defined energies
Plus a correlated pion signature
Time of flight detection to tag events and particle velocities
Distinguish from eg antiprotons
Si/Li detctors for X-ray resolution and particle tracking
Schedule
2011 prototype
2014 full experiment from
Antarctica
 
That was then. This is now.
 
Last slide from talk in 2010
Even then struggling to see which direct dark
matter models permitted in light of direct
detection
But…
GAPs now planned for 2020/21
What can it do?
 
WIMP status?
 
Dark Matter searches important but so far
negative results
WIMPs based on thermal relic density
compelling
But constrained if directly interacting with SM
Viable option: Hidden Sector Dark Matter
DM annihilates to other dark particles
They in turn annihilate to SM
Dark gauge fields most promising
 
Dark Matter/Dark Photon
 
Dark photons mix with SM photon
Permits Cascade annihilation if kinematically
allowed
Energy injected into radiation, leptons, baryons
Provide constraints and detection prospectsas we will
see
We will argue antideuterons probe an as-yet
unexplored mass range
Tens of GeV
 
Dark Photon Dark Matter
 
 
Relevant Feynman Diagrams
 
Constraints from Previous
Measurements
 
Indirect detection provides bulk of constraints
Mass vs cross section
Limits on CMB energy injection
Limits from photon searches
Limits from antipositrons
Limits from antiprotons
 
Current Bounds
 
 Constraints on Mixing 
ϵ
 
Indirect detection essentially  independent of
mixing
Upper bounds mostly from Direct Detection
Production essentially insensitive to 
ϵ
Lower bounds to avoid BBN interference
 
 
Also bound for observability
Don’t escape halo before froming antideuterons
 
Indirect Detection Constraints
 
Other light dark photon dark matter
searches
 
Antideuteron
 
We will show can probe tens of GeV range
through antideuteron searches
Challenge to theorist is correctly predicting
Lots of uncertainties as we will discuss
Still very promising
 
Theory Challenges
 
 
Theory Steps
 
 
Need to compute injection
Compute antideuteron formation
Coalescence model
Background: pp->pppbar, ppnbar
Monte Carlo
Annihilation to quarks, gauge bosons
Subseqeuent hadronization and fragmentation
K
n
- k
p
<(2m
p
B)
1/2
~70MeV,~p
coal
 most likely form antideuteron
  
Use data from Z decay
  
p
coal
~150MeV
Diffusion and convection of cosmic ray density
Transport in solar environment: modulation and structure of magnetic field
 
 
 
 
Also Need Halo Profile
 
 
 
These results we use Einasto
 
 
 
 
Less important than sensitivity to transport parameters
 
 Propagation Through Galaxy and
Heliosphere
 
Need transport through
ISM and
Heliosphere (ToA; top of atmosphere)
 
 
 
Again phenomenological parameter choices
Use diffusion model
 
 
Results
 
 
Variation with Parameters
 
 
More Results
 
 
Antihelium? Who knows…
 
 
Conclusion
 
Dark matter (by definition) elusive
We should look in all ways possible
Models play a big role—suggest new searches
Dark photon dark matter receives a lot of attention
WIMP still possible
But hard to find
Antideuteron promising for interesting tens of GeV
range
Not necessarily all parameters but sizable reach
Discovery possible!
Hopefully launch successfully soon!
 
Extra Slides
 
 
Results
 
Injection Spectra
 
How Many Events?
 
Slide Note
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Exploring the use of cosmic ray antideuterons for dark matter detection is a promising avenue in astrophysics. Antideuteron searches offer a low-background environment, making them ideal for detecting certain types of dark matter particles. Unlike antiproton searches, which face significant background challenges, antideuteron searches benefit from the production process that keeps background levels low. Instruments like the General AntiParticle Spectrometer (GAPS) are actively involved in this research field, utilizing exotic atom techniques to capture low-energy antiparticles and studying their interactions to uncover potential dark matter signatures.

  • Dark Matter
  • Antideuterons
  • Cosmic Rays
  • Dark Photon
  • Astrophysics

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  1. Searching for Dark Photon Dark Matter with Cosmic Ray Antideuterons Lisa Randall (w/Linda Xu) Mary K Fest Sept, 2019

  2. Why Antideuteron Searches Indirect detection one of three pillars of WIMP searches Antiparticle and distinctive photon signatures have potential to find unusual cosmological processes What to look for? Positrons, photons, antiprotons However, few DM models favor first two More importantly, background difficult to calculate Discoveries have taught us some interesting unanticpated astronphysics Antiproton searches promising, but background big there too Antideuteron searches for same type of dark matter as antiprotons But background low at small kinetic energy (astro background higher KE) Makes it a potentially essentially background free measurement Only a few detections suffice for discovery

  3. Why So Little Background? Assuming proton collides with X in ISM, To make an antiproton, at least four nucleons in final state To make an antideuteron, you need at least six Threshold energy First case 7 mp Antideuteron 17 mp Binding energy is 2.2 MeV Hard to slow down without dissociating Low background targets are good places to search DM annihilations usually close to at rest Possibility antiproton and antineutron produced with relatively small momentum difference In which case can coalesce Rare process But background calculable and essentially nonexistent (for low T)

  4. Is anyone looking? Yes!! In principle AMS II General AntiParticle Spectrometer (GAPS) Antarctic balloon mission Looks for antideuteron <0.25 GeV/n Uses an exotic atom technique Slow low energy antiparticles so they get captured by a nucleus Exotic atom decays emitting X-ray Correlated pion, proton from subsequent nuclear annihilation

  5. GAPS Long duration balloon experiment Antideuterons captured and result in exotic atom in final state Decays into X-rays at well-defined energies Plus a correlated pion signature Time of flight detection to tag events and particle velocities Distinguish from eg antiprotons Si/Li detctors for X-ray resolution and particle tracking Schedule 2011 prototype 2014 full experiment from Antarctica

  6. That was then. This is now. Last slide from talk in 2010 Even then struggling to see which direct dark matter models permitted in light of direct detection But GAPs now planned for 2020/21 What can it do?

  7. WIMP status? Dark Matter searches important but so far negative results WIMPs based on thermal relic density compelling But constrained if directly interacting with SM Viable option: Hidden Sector Dark Matter DM annihilates to other dark particles They in turn annihilate to SM Dark gauge fields most promising

  8. Dark Matter/Dark Photon Dark photons mix with SM photon Permits Cascade annihilation if kinematically allowed Energy injected into radiation, leptons, baryons Provide constraints and detection prospectsas we will see We will argue antideuterons probe an as-yet unexplored mass range Tens of GeV

  9. Dark Photon Dark Matter

  10. Relevant Feynman Diagrams

  11. Constraints from Previous Measurements Indirect detection provides bulk of constraints Mass vs cross section Limits on CMB energy injection Limits from photon searches Limits from antipositrons Limits from antiprotons

  12. Current Bounds

  13. Constraints on Mixing Indirect detection essentially independent of mixing Upper bounds mostly from Direct Detection Production essentially insensitive to Lower bounds to avoid BBN interference Also bound for observability Don t escape halo before froming antideuterons

  14. Indirect Detection Constraints

  15. Other light dark photon dark matter searches

  16. Antideuteron We will show can probe tens of GeV range through antideuteron searches Challenge to theorist is correctly predicting Lots of uncertainties as we will discuss Still very promising

  17. Theory Challenges

  18. Theory Steps Need to compute injection Compute antideuteron formation Coalescence model Background: pp->pppbar, ppnbar Monte Carlo Annihilation to quarks, gauge bosons Subseqeuent hadronization and fragmentation Kn- kp<(2mpB)1/2~70MeV,~pcoal most likely form antideuteron Use data from Z decay pcoal~150MeV Diffusion and convection of cosmic ray density Transport in solar environment: modulation and structure of magnetic field

  19. Also Need Halo Profile These results we use Einasto Less important than sensitivity to transport parameters

  20. Propagation Through Galaxy and Heliosphere Need transport through ISM and Heliosphere (ToA; top of atmosphere) Again phenomenological parameter choices Use diffusion model

  21. Results

  22. Variation with Parameters

  23. More Results

  24. Antihelium? Who knows

  25. Conclusion Dark matter (by definition) elusive We should look in all ways possible Models play a big role suggest new searches Dark photon dark matter receives a lot of attention WIMP still possible But hard to find Antideuteron promising for interesting tens of GeV range Not necessarily all parameters but sizable reach Discovery possible! Hopefully launch successfully soon!

  26. Extra Slides

  27. Results

  28. Injection Spectra

  29. How Many Events?

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