Brownsberger, Kramer, Rowan, Xu Whats post-modern? As with particle - - PowerPoint PPT Presentation

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Brownsberger, Kramer, Rowan, Xu Whats post-modern? As with particle - - PowerPoint PPT Presentation

LR w/ Fan, Katz, Reece Agrawal, Cyr-Racine, Scholtz, Brownsberger, Kramer, Rowan, Xu Whats post-modern? As with particle physics, easy times are probably at an end Need to look at subtle effects Basically (as with SM) CDM SM


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LR w/ Fan, Katz, Reece Agrawal, Cyr-Racine, Scholtz, Brownsberger, Kramer, Rowan, Xu

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What’s post-modern?

 As with particle physics, easy times are probably at an

end

 Need to look at subtle effects  Basically (as with SM) ΛCDM SM essentially works  But we don’t know if it’s whole story  Several things I’m working on (which to present?)

 Black hole mergers and what they can tell you  Hubble expansion: most interesting discrepancy! **  Dark matter: how to find what it is from astronomical

measurements

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Nature of Dark Matter??

 Compact objects or particle  If a particle, what is it

 Mass, interactions?

 If not a WIMP, can we observe its consequences?

Astronomical MEASUREMENTS AND STRUCTURE

 Our program:

 Propose models

 Systematic exploration of simple possibilities

 Analytic and numerical predictions  Make measurements

 Emphasize could be ONLY way we learn about dark matter’s

identity

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Self-Interacting Dark Matter

 Dark matter that interacts with itself

 Not necessarily with ordinary matter

 Has testable consequences  Might even address issues with CDM  How to pursue this theoretically?  And determine consequences?

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Particular Focus: Darkly-Charged Dark Matter

 Simple idea: Assume dark matter charged under its own

“electromagnetism”: “dark light”

 Dark matter charge, U(1)

 Could be light and heavy (like proton and electron)  Could be just heavy dark matter candidate (and antiparticle)

 Thought to be very constrained

 Even though NOT a WIMP

 Turns out can be weak scale mass with EM-type coupling  Or if a fraction of dark matter can be even less constrained

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Second Focus: PIDM/DDDM Partially Interacting/Double Disk

 Dark matter with its own force

 Rather than assume all dark matter  Assume it’s only a fraction

 Maybe like baryons?  Nonminimal assumption  But one with significant consequences

 Will be tested  Leads to rethinking of implications of almost all dark matter,

astronomical, cosmological measurements

 Since we don’t know what dark matter is

 Should keep an open mind  Especially in light of abundance of astronomical data

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Simple(st?) Model: DCDM

 Dark “proton” aka Charged WIMP  gD Aµ

D X γµ X

 +Dark electron  gD Aµ

D C γµ C

 +Kinetic Mixing  -ε/2 FD

µνFµν

  • WIMP miracle
  • Asymmetirc

freezeout

  • Neff
  • Matter power

spectrum

  • Asymmetric

recombination

  • CMB
  • Cores
  • Halo shapes
  • SIDM
  • Dark Disk
  • Point Sources
  • Direct Detction
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I: Darkly-Charged Dark Matter Model

Dark matter charged under its own “electromagnetism”

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Why Dark Charges Disfavored ”Constraints”

 Ellipticity of halos  Bullet Cluster type constraints  Survival of dwarf galaxies in halos (lack of

evaporation)

 Seemed to significantly impinge on parameter space

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Why Dark Charges Disfavored ”Constraints”

 Ellipticity of halos  Bullet Cluster type constraints  Survival of dwarf galaxies in halos (lack of

evaporation)

 Seemed to significantly impinge on parameter space

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Previous Constraints too Stonrg

 Galaxy ellipticity was strongest constraint  Ellipticity tricky to calculate  It’s a function of radius  And only one galaxy measured anyway  Dwarf galaxy survival calculation different when

massless mediator: strong internal interactions in dwarf

 Bullet cluster relies on initial distributions

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Ellipticity as function of radius

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Darkly-Charged Dark Matter

Clearly viable!!

 Constraints on mass considerably weaker than stated  Not yet reliable

 Simulations can help

 Exciting possibility that dark matter has its own world

  • f interactions

 And that conceivably we can detect them  Weak mass particles with even EM-type strength

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New Regime of Interactions

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Partially Interacting Dark Matter

 Nonminimal assumption: why would we care?  Implications of a subdominant component

 Can be relevant for signals if it is denser

  • Can be relevant for structure –like baryons

 Baryons matter because formed in a dense disk

 Perhaps same for component of dark matter

 Dark disk inside galactic plane  Or Point sources after fragmentation  Potentially significant consequences

 Leads to rethinking of implications of almost all dark matter,

astronomical, cosmological measurements

 Detectable!

Velocity distributions in or near galactic plane constrain fraction to be comparable or less to that of baryons

Further constraints from CMB

But because it is in disk and dense signals can be rich

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Simple DDDM Model New Ingredient: Light C

 Could be U(1) or a nonabelian group  U(1)D, αD  Two matter fields: a heavy fermion X and a light

fermion C

 For “coolant” as we will see

 qX=1, qC=-1  (In principle, X and C could also be scalars)  (in principle nonconfining nonabelian group)  This in addition to dark matter particle that makes up

the halo

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Summary of model

 A heavy component  Brehm and inverse Compton

 For disk to form, require light component

 With these conditions, expect a dark disk

 Even narrower than the gaseous disk

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Traditional Methods

 Smaller direct detection, small velocity

 Possibly other noncanonical possibilities

 Indirect detection

 Possible if mediation between visible, invisible sectors

 Good thing there is distinctive shape to signal if present  Best search: directly with GAIA data  Use density, velocity measurements to deduce gravitational

potential

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Also: Satellites of Andromeda Galaxy

 About half the satellites are approximately in a (big plane)

 14kpc thick, 400 kpc wide

 Hard to explain  Proposed explanation: tidal force of two merging galaxies  Fine except of excessive dark matter content  Tidal force would usually pull out only baryonic matter

from disk

 Not true if dark disk  Pulls out dark matter

 Slower velocity—more likely to be bound  So even subdominant component in disk can be dominant in

dwarfs

w/Scholtz

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Also potentially Point sources

 Evidence for GeV excess  Seems to come from point sources  Argued that pulsars are the source  Could also be point sources from COMPACT dark matter

  • bjects

 Possible when dissipative!  Dark photon leads to cooling  Instabilities leads to compact objects  Annihilations through Z’ lead to visible signals

 Due to mixing with photon

 Would appear as point sources

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New Work: Dwarfs: predicted prolate “observed” oblate

Linda Xu

 We consider the morphologies of dwarf spheroidals

(dsphs) in and around

 the Local Group (LG).  Ellipticities and associated 3-D shapes, and whether

they might be prolate or oblate.

 Compare CDM- sourced simulations to observations

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How to measure?

 Dsphs: common, little gas, eqm stars determined from grav

potential

 Simulations: prolate halos so we expect the stellar

distributions of dsphs sourced from CDM haloes should be likewise prolate. But how to deduce 3D structure when we make 2d

  • bservations?

 Expect the surface brightness of a prolate galaxy is anti-

correlated with its projected ellipticity, while the opposite is true of oblate galaxies.

 Use this to deduce 3d structure

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Results

Discrepancy between the morphologies of LG dwarf galaxies with mass-to-light ratio > 100M/L and those

  • f the FIRE dwarf galaxies
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Statistically significant deviation from expectations

Linda Xu

  • New feature to look for when checking ΛCDM predictions
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General Lesson

 Role for particle physics approach in astronomy  “constraint” on dark disk came from fitting standard

components

 Turns out errors on standard components not properly

accounted for

 Reddening important near midplane  Has to be done self-consistently

 Here different components influence each other through

gravity

 Big messy data sets  Targeting a model helps

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Conclusions

 Very interesting new possibility for dark matter

 That one might expect to see in observations

 ard to know whether or not it’s likely

 How much should dark matter resemble SM  But not be part of it

 But presumably would affect structure

 Just like baryons do  Research area

 Rich arena: lots of questions to answer