Fast flavor conversion of neutrinos Tobias Stirner Introduction - - PowerPoint PPT Presentation

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Fast flavor conversion of neutrinos Tobias Stirner Introduction - - PowerPoint PPT Presentation

Introduction Neutrino Collider Conclusions Fast flavor conversion of neutrinos Tobias Stirner Introduction Neutrino Collider Conclusions Why do neutrinos oscillate? Introduction Neutrino Collider Conclusions Why do neutrinos oscillate?


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Introduction Neutrino Collider Conclusions

Fast flavor conversion of neutrinos

Tobias Stirner

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Introduction Neutrino Collider Conclusions

Why do neutrinos oscillate?

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Introduction Neutrino Collider Conclusions

Why do neutrinos oscillate?

Two bases for fields:

  • massive µ(x) =

µ1 µ2

  • and flavor φ(x) =

φe φτ

  • related via SO(2) mixing matrix φ(x) = ˆ

Uµ(x) → propagating dof = interacting dof mixing is environment dependent

  • scillation length in vacuum: L ∼ 10km

in high neutrino density: L ∼ 1m

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Introduction Neutrino Collider Conclusions

Equation of Motion

description with Wigner transform ˆ ρ(x, k, t) =

  • d3ye−ik·yφ
  • x − y

2

  • φ†

x + y

2

D S S∗ 1 − D

  • Hamiltonian ˆ

H =

  • k2 + ˆ

M2 + √ 2GF

  • d3q

(2π)3

  • ˆ

ρ − ˆ ¯ ρ

  • (1 − cos θqk)

Liouville equation i (∂t + v · ∂x) ˆ ρ =

  • ˆ

H, ˆ ρ

  • interpretations: particle transport & wave equation
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Introduction Neutrino Collider Conclusions

Two beams

assume: flavor correlation small S ≪ 1 → i (∂t + v · ∂x) Sv = − dv′

4π (1 − cos θ) Gv′Sv′

Gv: particle content simplification: 2 beams in 1 + 1d parameters: velocities (↿ ↾, ↿ ⇂) & particle content (ν, ¯ ν) look for unstable regions in dispersion relation ω(k) → ω or k complex in S ∼ e−i(ωt−k·x)

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Introduction Neutrino Collider Conclusions

Stable cases

parallel v, only ν no excluded regions → completely stable antiparallel v, only ν gap in ω modes with small energy damped

k ω k ω

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Introduction Neutrino Collider Conclusions

Instable case

parallel v, ν and ¯ ν gaps in ω and k convective instability antiparallel v, ν and ¯ ν gap in k absolute instability

k ω k ω

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Introduction Neutrino Collider Conclusions

Conclusions

  • oscillation is a misleading term
  • self-interactions can cause complex regions in dispersion

relation

  • depending on the gaps different instabilities arise
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Introduction Neutrino Collider Conclusions

Bibliography

  • Izaguirre et al.: ”Fast Pairwise Conversion of Supernova

Neutrinos: A Dispersion-Relation Approach”, arXiv:1610.01612

  • Capozzi et al: ”Fast flavor conversion of supernova neutrinos:

Classifying instabilities via dispersion relations”, arXiv:1706.03360

  • TS et al.: ”Liouville term for neutrinos: Flavor structure and

wave interpretation”, arXiv:1803.04693