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Evolving Metric Perturbations and Self-Force Calculations in the Lorenz Gauge: progress report

Evolving Metric Perturbations and Self-Force Calculations in the Lorenz Gauge: progress report. Lior Burko Kristen Lackeos, Gaurav Khanna, Leor Barack. Approaches for SF numerical calculations. Frequency domain Easy in Schwarzschild Hard to generalize to generic Kerr orbits

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Evolving Metric Perturbations and Self-Force Calculations in the Lorenz Gauge: progress report

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  1. Evolving Metric Perturbations and Self-Force Calculations in the Lorenz Gauge: progress report Lior Burko Kristen Lackeos, Gaurav Khanna, Leor Barack Capra 12, Bloomington, IN

  2. Approaches for SF numerical calculations • Frequency domain • Easy in Schwarzschild • Hard to generalize to generic Kerr orbits • Time domain • Natural extension to generic worldlines ? Regularization method Capra 12, Bloomington, IN

  3. Lorenz gauge RW gauge Radiation gauge Our approach • Metric perturbations • no need to do metric reconstruction from Weyl scalars • Lorenz Gauge • avoid need for gauge transformations • particle singularity is isotropic and isolated • manifest hyperbolicity • Time domain in 2+1D • generic orbits are natural • much experience gained from the Teukolsky • Equation • Regularization • m mode regularization / puncture method Credits: L. Barack Capra 12, Bloomington, IN

  4. Field equations Capra 12, Bloomington, IN

  5. Field equations Capra 12, Bloomington, IN

  6. Numerical setup Krivan, Laguna, Papadopoulos and Andersson (1997): Solution is then obtained by the Lax-Wendroff 2-step scheme Capra 12, Bloomington, IN

  7. Numerical setup II E.g., in Schwarzschild: Capra 12, Bloomington, IN

  8. Field equations 20 equations like: Capra 12, Bloomington, IN

  9. 4 gauge conditions like: Capra 12, Bloomington, IN

  10. First runs Vacuum, Minkowski Static ID that satisfy the Lorenz gauge Capra 12, Bloomington, IN

  11. A time dependent solution (exact solution known and oscillatory) Capra 12, Bloomington, IN

  12. Lorenz violating initial data Capra 12, Bloomington, IN

  13. Coupled modes Capra 12, Bloomington, IN

  14. Gauge violating modes Numerical errors violate the Lorenz gauge. Gauge violating damping terms Evolve the fields with the full Einstein equations The full field (physical fields AND numerical error) does not satisfy It satisfies Capra 12, Bloomington, IN

  15. satisfies the Einstein equations in the Lorenz gauge violates the Einstein equations in the Lorenz gauge; When evolved with the Lorenz-gauge equations, it’s not the Einstein equations we’re solving! Capra 12, Bloomington, IN

  16. Does this equation remove the problem with gauge violating modes? Capra 12, Bloomington, IN

  17. Problem: The new field equations mix terms Solution: Define new fields which restore the equations to a single term But ID need to be satisfied in the Lorenz gauge Notice: 4 equations become elliptic: 8 constraints 6 are hyperbolic Capra 12, Bloomington, IN

  18. ID for a static field, Excites also Capra 12, Bloomington, IN

  19. ID for oscillating Excites other fields: Capra 12, Bloomington, IN

  20. Excited (initially zero) fields: Capra 12, Bloomington, IN

  21. Lorenz gauge Elliptic Einstein equations Capra 12, Bloomington, IN

  22. Gauge violating damping terms Allows to pose Lorenz-violating ID Capra 12, Bloomington, IN

  23. Numerical instability in Schwarzschild and Kerr Capra 12, Bloomington, IN

  24. Quasi-circular Schwarzschild orbits should be doable now! Results by next Capra meeting (not the Florida one!) Quasi-self-consistency Comparison with the “radiation reaction without radiation reaction” approach. Conservative effects? Self force integrated waveforms: Capra 12, Bloomington, IN

  25. Focus on gauge-independent quantities: the waveform • Barack and Ori (2001): “The meaningful description of the gravitational self force must include both and the metric perturbations .” • Detweiler (2008): “The value in calculating the self force, in any particular gauge, is to apply it to a question whose answer is related to some physical observable. And a physical observable ought to be independent of the gauge choice.” Capra 12, Bloomington, IN

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