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Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

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Dynamics of Qballs http://leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000. L. Perivolaropoulos http://leandros.chem.democritos.gr Institute for Nuclear Physics Research Demokritos Research Center Work in collaboration with M. Axenides, E. Floratos Demokritos Research Center and - PowerPoint PPT Presentation
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Dynamics of Qballs http://leandros.chem.demokritos.gr/qb alls Phys.Rev.D62:047301,2000 L. Perivolaropoulos http:// leandros.chem.democritos.gr Institute for Nuclear Physics Research Demokritos Research Center Work in collaboration with M. Axenides, E. Floratos Demokritos Research Center and S. Komineas Univ. of Bayreuth (Germany)
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Page 1: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Dynamics of Qballshttp://leandros.chem.demokritos.gr/qballs

Phys.Rev.D62:047301,2000

L. Perivolaropouloshttp://leandros.chem.democritos.gr

Institute for Nuclear Physics Research

Demokritos Research Center

Work in collaboration with

M. Axenides, E. FloratosDemokritos Research Center

and

S. KomineasUniv. of Bayreuth (Germany)

Page 2: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Structure of Talk

1. Introduction What is a Q Ball

Q Ball FormationThe Role of Dynamics

2. Q Balls on the lineExistence - Stability - Virial TheoremInteractions - Scattering

3. Q Balls on the PlaneFusion or Fision?

4. Scattering in 3D5. Conclusion

Motivation: Understand the evolution ofQ Balls in a cosmological setup

Page 3: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

What is a Qball?Dynamically Stable Time Dependent Solutionwith a rotating internal phase. Its stability is due to the conservation of Noether charge.

Simplest Example:

Field Equation (1+1 dim):

Qball ansatz:

Conserved Noether Charge

Solution Exists for:

Page 4: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Q Ball FormationInstabilities of Coherent Affleck-Dine Scalar

due to flat directions of SUSY breaking induced potentials

Example of Affleck-Dine Potential

( K < 0 )

Affleck-Dine Field:

Fluctuations:2

22

0 3 Q Ball Formationk

m K Instabilitiesa

Kasuya - Kawasakihep-ph/0002285

Page 5: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

The Role of Dynamics

MSSM: Qballs form as condensates of squarks and sleptons with conserved charge the Baryon and Lepton number.

Thus:

•Qballs can form by the Aflecck-Dine mechanism(Instabilities of Homogeneously Rotating AD Scalar)

•Large Stable Qballs can form Cold Dark Matter

•Unstable Qballs can lead to Baryon AsymmetryIsocurvature baryon fluctuations

Q: How do interactions and scattering affect thecosmological evolution of Qballs?

Page 6: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Q Balls on the Line I:Existence - Stability

Energy:

For Stability:20 (qball solution), 0Q QE E

Find B, ω for 0 eigevalue Ground State

x

x

Page 7: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Virial Theorem

The Qball energy may be written as:

Rescale Spatial Coordinate x:

Minimize with respect to rescaling parameter α:

Virial Theorem

Condition for stabilityalways satisfied.

Page 8: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Q Balls on the Line II:Interactions - Scattering

Ansatz for two interacting Qballs at distance 2 x0

1 0 2 0where ( ), ( )x x x x

DominantTerm

2 24, 0.9,

9B

Analytic

Numerical

Spatial Oscilation Frequency is Double the Internal Rotation Symmetry

BreatherOscillations

Page 9: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Scattering

Define:

Boosted Configuration:

Initial Conditions:

Evolved System 0 1 2

40.2, 0.51, B=

9v

Long-lived central Q Ball

Page 10: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Q Balls on the PlaneFusion or Fision I

1 2 00.75, v 0.2 Fusion (merging)

1 2 00.75, v 0.4 Fision (right angle)

Page 11: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Q Balls on the PlaneFusion or Fision I

1 2 00.75, v 0.8 Pass Through

Qualitative Preliminary Result (not published)

cv

Q

Particle Behavior (pass through)

Particle Behavior (merge)

Soliton Behavior (fision)

Page 12: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Q Balls on the PlaneFusion or Fision

1 2 1 2i f0.75, v 0.4 0.6, v 0.25i i f f

Q/Q0: Fractional Charge in Forward Scattering

Page 13: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Scattering in 3D I

Head on Collision (unpublished preliminary results)

Page 14: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Scattering in 3D II

Non-zero impact parameter

Page 15: Dynamics of Qballs leandros.chem.demokritos.gr/qballs Phys.Rev.D62:047301,2000

Conclusion

Studied Dynamics of Q Balls in 1D, 2D, 3D.

1D: Stability Sector, Virial Theorem,Breather Oscillations of Q Ball pairs

int( ) 2 space

2D Scattering:

1

1 2

2

( )

c

c c

c

v v fusion

v v v fision right angle

v v Pass Through

3D Scattering (Preliminary):Q Ring Formation

Implications:Q Ball Cosmological EvolutionFision implies tha Q Ball number may increasewhile size decreases leading to instabilities.


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