Cosmological Energy Budget of Cosmological First Order Phase - - PowerPoint PPT Presentation

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Cosmological Energy Budget of Cosmological First Order Phase - - PowerPoint PPT Presentation

Energy Budget of Cosmological Energy Budget of Cosmological First Order Phase Transitions First Order Phase Transitions Jose Miguel No Jose Miguel No King's College London King's College London Making the EW Phase Transition


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SLIDE 1

Jose Miguel No Jose Miguel No King's College London King's College London

Energy Energy

Budget

Budget of

  • f Cosmological

Cosmological First First

Order

Order

Phase

Phase

Transitions

Transitions

Making the EW Phase Transition (Theoretically) Strong Making the EW Phase Transition (Theoretically) Strong

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SLIDE 2

1

Motivation: Why Bubbles

Why Bubbles

?

Cosmological First Order Phase Transitions

Nucleation & Growth of Bubbles

Baryogenesis Baryogenesis

Could be Detected by LISA

Electroweak Electroweak Phase Transition Phase Transition

Gravitational waves Gravitational waves

Bubble Expansion & Interaction

  • w. Plasma Can Yield Baryogenesis

Bubble Collisions & (anisotropic) Plasma Motions Produce Stochastic Gravitational Wave Signature

Large Interferometer Space Antenna Courtesy of David Weir

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SLIDE 3

2

Dynamics of Thermal Plasma

Expanding Bubbles Perturb Thermal Plasma

 = 0  = v

Bubble Wall

V+ T+ V- T-  = 0  = v

Close to Phase Boundary Far from Phase Boundary

Energy-Momentum Conservation

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SLIDE 4

3

Looking Closely at the Phase Boundary:

matching Across Bubble wall matching Across Bubble wall

+ +

Bubble Wall

V+ T+ V- T-  = 0  = v

Wall Reference Frame

Perfect Fluid

Energy-Momentum Conservation Across Bubble Wall Steady State Bubble Expansion

Simple Ansatz for Fluid E.O.S.

(Bag E.O.S.)

Dynamics of Thermal Plasma

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SLIDE 5

4

Looking Closely at the Phase Boundary:

matching Across Bubble wall matching Across Bubble wall

V+ T+ V- T-  = 0

Wall Reference Frame

Bubble Wall

➊ ➋

Only if

( )

Two Branches of Solutions

 = v

Dynamics of Thermal Plasma

➋ ➊

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SLIDE 6

5

Looking Far from the Phase Boundary:

Fluid Motion Fluid Motion

Self-Similar Ansatz

 

Fluid MOTION Fluid TEMPERATURE = 0.577... Plasma Speed of Sound

Dynamics of Thermal Plasma

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SLIDE 7

5

Looking Far from the Phase Boundary:

Fluid Motion Fluid Motion

Self-Similar Ansatz

 

Fluid MOTION Fluid TEMPERATURE

Fluid Velocity Eq. Matching Conditions on Bubble Wall

+

Solutions Solutions for

for Fluid Motion

Fluid Motion

”Bubble Expansion Modes”

Boundary conditions

= 0.577... Plasma Speed of Sound

Dynamics of Thermal Plasma

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SLIDE 8

6

Looking Far from the Phase Boundary:

Fluid Motion Fluid Motion

Inspecting Inspecting

Is Single – Valued Function

Dynamics of Thermal Plasma

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SLIDE 9

7

Solutions for Fluid Motion

DEtonations DEtonations DEflagrations DEflagrations hybrids hybrids

Dynamics of Thermal Plasma

Supersonic Fluid at Rest in Front of Wall Rarefaction Wave Behind Wall Subsonic Fluid at Rest Behind Wall Compression Wave in Front of Wall Supersonic Both Compression & Rarefaction Waves Ends in a Shock Front

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SLIDE 10

8

Solutions for Fluid Motion

Deflagrations Deflagrations   hybrids hybrids   detonations detonations

For

= cte

Continuous Evolution as vw Increases

Dynamics of Thermal Plasma

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SLIDE 11

9

Collection of Relevant Effects...

Dynamics of Thermal Plasma

DEflagrations DEflagrations

Slow Moving Bubbles

Good for Baryogenesis

Fast Moving Bubbles

DEtonations DEtonations

Bad(?) for Baryogenesis

Local Symmetry Restoration

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SLIDE 12

10

Energy Budget of the Phase Transition

Bubbles Expanding in Vacuum Bubbles Expanding in Thermal Plasma

Energy Liberated During the Phase Transition Acts as Source of Gravitational Waves Perfect Conversion of Liberated Energy into Kinetic Energy NOT Perfect Conversion of Liberated Energy into Kinetic Energy Efficiency Factor

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SLIDE 13

10

Energy Budget of the Phase Transition

Bubbles Expanding in Vacuum Bubbles Expanding in Thermal Plasma

Energy Liberated During the Phase Transition Acts as Source of Gravitational Waves Perfect Conversion of Liberated Energy into Kinetic Energy NOT Perfect Conversion of Liberated Energy into Kinetic Energy Efficiency Factor

Depends on TN , vW , α

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11

Energy Budget of the Phase Transition

Controls Energy Budget

Energy not transformed into plasma bulk motion ( 1- ) used to increase plasma thermal energy

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SLIDE 15

11

Energy Budget of the Phase Transition

Controls Energy Budget

Energy not transformed into plasma bulk motion ( 1- ) used to increase plasma thermal energy

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SLIDE 16

12

Energy Budget of the Phase Transition

e.g. Sound Waves as GW Source e.g. Sound Waves as GW Source

Gravitational Wave Amplitude Depends Quadratically on 

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SLIDE 17

12

Energy Budget of the Phase Transition

e.g. Sound Waves as GW Source e.g. Sound Waves as GW Source

Gravitational Wave Amplitude Depends Quadratically on 

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SLIDE 18

12

Energy Budget of the Phase Transition

e.g. Sound Waves as GW Source e.g. Sound Waves as GW Source

Gravitational Wave Amplitude Depends Quadratically on 

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SLIDE 19
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SLIDE 20

References

Bubble Expansion Solutions

P . J. Steinhardt, Phys. Rev. D 25 (1982) 2074

  • M. Laine, Phys. Rev. D 49 (1994) 3847
  • H. Kurki-Suonio and M. Laine, Phys. Rev. D 51 (1995) 5431
  • M. Kamionkowski, A. Kosowsky and M. S. Turner

, Phys. Rev. D 49 (1994) 2837

  • J. Ignatius, K. Kajantie, H. Kurki-Suonio and M. Laine, Phys. Rev. D 49 (1994) 3854-3868

Efficiency Coefficients Energy Budget –

  • J. R. Espinosa, T. Konstandin, J. M. No. and G. Servant, JCAP 1006:028 (2010)

Implications for Baryogenesis

  • J. M. No, Phys. Rev. D 84 (2011) 124025
  • C. Caprini and J. M. No, JCAP 1201:031 (2012)
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SLIDE 21

Probing the EW Epoch with GW

Courtesy of D. Weir (Stavanger) Courtesy of D. Weir (Stavanger)

GW Bubble soUrces GW Bubble soUrces Sound Waves Sound Waves

Hindmarsh, Huber, Rummukainen, Weir, Phys. Rev. Lett 112 (2014) 041301

Turbulence Turbulence

Caprini, Durrer, Servant, JCAP 0912 (2009) 024

ϵ

(Stochastic) GW Signal Detectable by LISA! !

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SLIDE 22

(e)LISA

The Next/Future step The Next/Future step Gravitational Wave Astronomy in Space

LISA

  • n its way!
  • n its way!

Large Interferometer Space Antenna

(success of eLISA Pathfinder) (success of eLISA Pathfinder)

2-5 2-5 3 3rd

rd Arm

Arm As of Sept. 2016

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SLIDE 23

LISA LISA Sensitivity to BSM Sensitivity to BSM

for the (e) for the (e)

LISA Cosmology Working Group

LISA Cosmology Working Group

Caprini et al, JCAP 1604 (2016) 001

Probing the EW Epoch with GW