Hawking radiation in 1D quantum fluids

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Hawking radiation in 1D quantum fluids Stefano Giovanazzi bosons fermions vs Valencia 2009

description

vs. fermions. bosons. Valencia 2009. Hawking radiation in 1D quantum fluids. Stefano Giovanazzi. … before starting with 1D stuff …. How to make subsonic to supersonic transitions ? The Atom laser is a beautiful example of a sonic black hole. From Cennini et al. Tuebingen. Why 1D? - PowerPoint PPT Presentation

Transcript of Hawking radiation in 1D quantum fluids

Hawking radiation in 1D quantum fluids

Stefano Giovanazzi

bosons fermionsvs

Valencia 2009

From Cennini et al.Tuebingen

How to make subsonic to supersonic transitions ?

The Atom laser is a beautiful example of a sonic black hole.

… before starting with 1D stuff …

•Why 1D?

•Why fermions?

•Introducing the non-ideal flow of non-interacting fermions

•Superfluidity in 1D? Bosons vs fermions

•Presenting an exact microscopic model for Hawking radiation

•Hawking temperature: Bosons vs fermions

Description of the flow of non-interacting fermions

The many-particles wave-function can be easily written as a Slater determinant (scattering description)

reservoirreservoir1D channel

µL µR

T=0 T=0

Hydrodynamic description …. ->

From the semiclassical to the hydrodynamic description

Thermal distribution of right-coming fermions

reservoirreservoir1D channel

µL µR

T=0 T≠0

What happens if the reservoir on the right is replaced by a sonic event horizon with a non-negligible Hawking temperature?

Reflection coefficient from the very smooth barrier

What are the quantum effects?

where is related to the curvature of the potential barrier

V (x) ≈V(0) +12mω x

2x2

ω x

Reflection coefficient from the very smooth barrier

What are the quantum effects?

Expressing Hawking temperature in terms of the external potential parameters

Using hydrodynamics of a general 1D quantum fluid is possible to prove that

where for a 1D Bose gas in the mean field regime

and for a 1D Bose gas in the Tonks-Girardeau regime or for 1D non-interacting Fermi gas

η =3

4

η =1

Aspects of Hawking radiations:

• Statistic of fluid’s particles plays no role in Hawking temperature formula

• Correlations on opposite side of the event horizon

• Incoherence of the radiation when probed only on one side of the horizon

• Thermal distribution

Which are the aspects that survives kTH ≈ mc2 ?

Thank you for listening !Thank you for listening !

bosonsfermions

vs

SG, C. Farrell, T. Kiss, and U. Leonhardt, PRA 70, 063602 (2004);SG, PRL 94, 061302 (2005); SG, JPB 39, S109 (2006).

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