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Exploring Oscillon Interactions
Anamitra Paul
Advisor: Mustafa Amin
Rice University
Roadmap
Introduce oscillons and
their physical significance
Present theoretical
calculations of oscillon
interaction dynamics
Compare theory to
numerical simulations
Axionic Dark Matter
 Introduced to resolve the strong CP problem1
 Weak interaction strength makes them good dark matter
candidates2
 Described as a real-valued scalar field
(Amin et al., 2011)
1 Peccei and Quinn (1977)
2 Dine & Fischler (1983)
Oscillons
 Long-lived, spatially localized, oscillatory field
excitations3 4
 Provide insight into structure formation of axionic
dark matter
 Oscillon interactions produce gravitational waves
and electromagnetic radiation5
3 Gleiser (1993)
4 Zhang et al. (2020)
5 Amin & Mou (2020)
How do Oscillons Interact?
 Oscillons may attract or repel each other
 Quantify the “force” between two oscillons in 1+1 D
spacetime (1 spatial dimension plus time)
 We will ignore gravity (for simplicity)
Equation of Motion in 1+1 D Spacetime
Approximate Superposition Solution
Approximate sum solution at 𝑡 = 0 with 𝜃 = 0
Force between Oscillons
Equal Amplitude Oscillons
Unequal Amplitude Oscillons
Numerical Simulations
 Leapfrog finite difference scheme
 Absorbing boundary conditions
 Tracked the center of the left oscillon
 Computed acceleration from “fitted” trajectories
Tracked oscillon with
amplitude 𝜖1
𝜖 = 0.2, θ = 0
Oscillon Center
Trajectory
Oscillon Acceleration
𝜖 = 0.2, θ = 𝜋
Oscillon Center
Trajectory
Oscillon Acceleration
𝜖 = 0.2, θ =
𝜋
2
Oscillon Center
Trajectory
Oscillon Acceleration
𝜖1 = 0.2, 𝜖2 = 0.1, θ = 0
Oscillon Center
Trajectory
Oscillon Acceleration
𝜖1 = 0.2, 𝜖2 = 0.1, θ = 𝜋
Oscillon Center
Trajectory
Oscillon Acceleration
𝜖1 = 0.2, 𝜖2 = 0.1, θ =
𝜋
2
Oscillon Center
Trajectory
Oscillon Acceleration
Conclusions and Future Steps
 In and out of phase calculations agree well in the equal amplitude case
 Qualitative agreement in the unequal amplitude case
 Discrepancies may be explained by energy transfer between the oscillons
 Extend theory 1+1 D to oscillons with relative velocities
 Simulate in 3+1 D spacetime
Acknowledgements
 Work supported by the Rorschach scholarship from the Rice P&A department
 Dr. Mustafa Amin (Advisor)
 Hongyi Zhang (Graduate Student, Rice)
 Rohith Karur (Undergraduate Student, UC Berkeley)
Questions?

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Exploring Oscillon interactions

  • 1. Exploring Oscillon Interactions Anamitra Paul Advisor: Mustafa Amin Rice University
  • 2. Roadmap Introduce oscillons and their physical significance Present theoretical calculations of oscillon interaction dynamics Compare theory to numerical simulations
  • 3. Axionic Dark Matter  Introduced to resolve the strong CP problem1  Weak interaction strength makes them good dark matter candidates2  Described as a real-valued scalar field (Amin et al., 2011) 1 Peccei and Quinn (1977) 2 Dine & Fischler (1983)
  • 4. Oscillons  Long-lived, spatially localized, oscillatory field excitations3 4  Provide insight into structure formation of axionic dark matter  Oscillon interactions produce gravitational waves and electromagnetic radiation5 3 Gleiser (1993) 4 Zhang et al. (2020) 5 Amin & Mou (2020)
  • 5. How do Oscillons Interact?  Oscillons may attract or repel each other  Quantify the “force” between two oscillons in 1+1 D spacetime (1 spatial dimension plus time)  We will ignore gravity (for simplicity)
  • 6. Equation of Motion in 1+1 D Spacetime
  • 7. Approximate Superposition Solution Approximate sum solution at 𝑡 = 0 with 𝜃 = 0
  • 11. Numerical Simulations  Leapfrog finite difference scheme  Absorbing boundary conditions  Tracked the center of the left oscillon  Computed acceleration from “fitted” trajectories Tracked oscillon with amplitude 𝜖1
  • 12. 𝜖 = 0.2, θ = 0 Oscillon Center Trajectory Oscillon Acceleration
  • 13. 𝜖 = 0.2, θ = 𝜋 Oscillon Center Trajectory Oscillon Acceleration
  • 14. 𝜖 = 0.2, θ = 𝜋 2 Oscillon Center Trajectory Oscillon Acceleration
  • 15. 𝜖1 = 0.2, 𝜖2 = 0.1, θ = 0 Oscillon Center Trajectory Oscillon Acceleration
  • 16. 𝜖1 = 0.2, 𝜖2 = 0.1, θ = 𝜋 Oscillon Center Trajectory Oscillon Acceleration
  • 17. 𝜖1 = 0.2, 𝜖2 = 0.1, θ = 𝜋 2 Oscillon Center Trajectory Oscillon Acceleration
  • 18. Conclusions and Future Steps  In and out of phase calculations agree well in the equal amplitude case  Qualitative agreement in the unequal amplitude case  Discrepancies may be explained by energy transfer between the oscillons  Extend theory 1+1 D to oscillons with relative velocities  Simulate in 3+1 D spacetime
  • 19. Acknowledgements  Work supported by the Rorschach scholarship from the Rice P&A department  Dr. Mustafa Amin (Advisor)  Hongyi Zhang (Graduate Student, Rice)  Rohith Karur (Undergraduate Student, UC Berkeley)