IRREVERSIBLE DYNAMICS OF SUPERFLUID VORTEX RECONNECTIONS DAVIDE - - PowerPoint PPT Presentation
IRREVERSIBLE DYNAMICS OF SUPERFLUID VORTEX RECONNECTIONS DAVIDE - - PowerPoint PPT Presentation
manuscript in preparation IRREVERSIBLE DYNAMICS OF SUPERFLUID VORTEX RECONNECTIONS DAVIDE PROMENT, UNIVERSITY OF EAST ANGLIA (UK) Joint work with: Alberto Villois and Giorgio Krstulovic RECONNECTIONS IN SUPERFLUIDS ( t ) [Paoletti et
RECONNECTIONS IN SUPERFLUIDS
[Serafini et al., PRL 2015] [Paoletti et al., PNAS 2008]
δ−(t) δ+(t)
φ t
Vortex reconnections in superfluid liquid helium (top) and BEC of cold atoms (bottom)
THE GROSS-PITAEVSKII MODEL Madelung transformation
∂ρ ∂t + ∇ ⋅ (ρu) = 0 ∂u ∂t + (u ⋅ ∇)u = ∇ − g m ρ + 1 mV + ℏ2 2m2 ∇2 ρ ρ
ψ = ρ exp(ıϕ)
u = ℏ/m∇ϕ , ρ = m|ψ|2
- inviscid, compressible, and irrotational fluid
- vortices are topological defects
- circulation quantised
ıℏ∂ψ ∂t + ℏ2 2m ∇2ψ − g|ψ|2ψ = 0
given bulk density ρ0 ξ = ℏ2/(2mgρ0) c = gρ0/m
κ = h/m
[Pitaevskii & Stringari, 2003]
TWO ENERGY FAMILIES IN THE GP MODEL
Ekin = 1 4 ∫ ( ρ v)
2
dV , Eq = 1 4 ∫ (2∇ ρ)
2
dV , Eint = 1 2 ∫ (ρ − ρ0)
2 dV
E = ∫ |∇ψ|2dV + 1 2 ∫ (|ψ|2 − ρ0)
2
dV
[Nore et al., PoF 1997]
ρ v = ( ρ v)
i
+ ( ρ v)
c
density perturbations: Ec
kin = 1
4 ∫ [( ρ v)
c
]
2
dV quantised vortices: Ei
kin = 1
4 ∫ [( ρ v)
i
]
2
dV
Using Helmoltz’s decomposition
- total energy is a constant of motion
- energy transfers between vortices and sound families
OUR NUMERICAL EXPERIMENTS ON RECONNECTIONS
- decay of two linked rings
- vary the offset , spanning over 49 different
configurations
- track vortex filaments and measure sound
d
ABOUT RECONNECTION: LINEAR THEORY APPROXIMATION δ±(t) = A± κ|t − tr| ϕ− = 2 arctan(A+/A−)
[Nazarenko & West, JLTP 2003]
φ−
<latexit sha1_base64="NAuFnSTeLNicUZ4QmEFrCuwL6QY=">ACBHicdVDLSgMxFM3UV62vqks3wSK4cjUPndFNy4r2Ae0Y8mkaRubmQxJRihDt67d6je4E7f+h5/gX5hpK2jRAxcO59zLvfd4IWdKI/RhpVZW19Y30puZre2d3b3s/kFTiUgS2iC9n2sKcBbShmea0HUqKfY/Tlje+TPzWPZWKieBGT0Lq+ngYsAEjWBup2Q1H7Pasl80hG5WcaqUEkV0o56uFoiFOvlhCDo2miEHFqj3sp/dviCRTwNOFaq46BQuzGWmhFOp5lupGiIyRgPacfQAPtUufHs2ik8MUofDoQ0FWg4U39OxNhXauJ7ptPHeqSWvUT80sULQRXSwfoQcWNWRBGmgZkvn8QcagFTBKBfSYp0XxiCaSmRcgGWGJiTa5ZUw23wHA/0kzbzvndv6kKtdLFJKgyNwDE6BA8qgBq5AHTQAXfgETyBZ+vBerFerbd5a8pazByCX7DevwBQJpkJ</latexit>δ±(t) ≤ ξ ⟹ ıℏ∂ψ ∂t + ℏ2 2m ∇2ψ − g|ψ|2ψ = 0
- same scaling before
and after, only the pre- factors change
- filaments follow locally the
branches of an hyperbola δ ∝ t1/2 A±
ASYMMETRY IN RATES OF APPROACH AND SEPARATION
Red circles correspond to data of the present work, all other symbols are from [Villois et al., PRFluids 2018]
0.5 1 1.5 2 2.5 0.5 1 1.5 2 2.5
HOW TO EXPLAIN THIS ASYMMETRY?
δ±(t) = A± κ|t − tr|
A TYPICAL EVOLUTION Evolution of various measurable quantities during the reconnection, including energy components
COMPRESSIBLE KINETIC ENERGY GROWTH
∆EC
kin
10 A+/A−
100 101
∆EC
kin
10-6 10-5 10-4
Growth of the compressible kinetic energy during the reconnection vs. the ratio for the 49 different realisations A+/A−
Example of energy growth during a reconnection
HOW TO PREDICT THIS BEHAVIOUR?
A PHENOMENOLOGICAL MATCHING THEORY
- when nonlinear theory using vortex filament model
- r local induction approximation (LIA)
- when linear theory as described before
- matching of the two theories at
δ(t) ≥ δlin δ(t) ≤ δlin δ(t) = δlin
A PHENOMENOLOGICAL MATCHING THEORY momentum: P±
fil = κ
2 ∮ R± × dR± energy: E±
fil ∝ |κ|2
∮ |dR±| ⟹ ΔPfil = P+
fil − P− fil
ΔEfil = E+
fil − E− fil
[Pismen, 1999]
from nonlinear theory
CONVERSION OF FILAMENT’S MOMENTUM INTO SOUND ΔPwav = − ΔPfil ∝ (0, 0, 1 + A+/A− A+/A− ) ⟹ ΔPwav,z > 0
- 30
- 20
- 10
10 20 30 0.97 0.98 0.99 1 1.01
Example of sound pulse emission propagating orthogonally to the reconnection plane
- propagation at almost
speed of sound (dashed green lines)
- some dispersion
- reduction in the
sound minimum
∝ 1 (t − tr − z/c)2
CONVERSION OF FILAMENT’S ENERGY INTO SOUND
- a range of values are allowed, when considering that reconnecting
filaments do not lie exactly on a plane
- is a measure of the concavity in the z direction
γ ΔEwav = − ΔEfil ∝ Δℒ/ℒ (using LIA)
CONCLUSIONS
- linear momentum always lost
in the negative direction (orthogonal to the reconnection plane), sound pulse has positive momentum
- because it is
energetically favourable
- energy radiated depends on
the reconnecting angle
- phenomenological matching
between linear and nonlinear theory A+ ≥ A− ϕ− = 2 arctan(A+/A−)
THANKS FOR YOUR ATTENTION!
Acknowledgments G.K., D.P . and A.V. were supported by the cost-share Royal Society International Exchanges Scheme (IE150527) in conjunction with CNRS. A.V. and D.P . were supported by the EPSRC First Grant scheme (EP/P023770/1). D.P . acknowledges the Fédération Doeblin for the support while visiting Nice in November 2017.