Hawking radiation in 1D quantum fluids Stefano Giovanazzi bosons fermionsvs Valencia 2009.

Slides:



Advertisements
Similar presentations
Classical and Quantum Gases
Advertisements

Trapped ultracold atoms: Bosons Bose-Einstein condensation of a dilute bosonic gas Probe of superfluidity: vortices.
Statistical Physics 2.
Markus Büttiker University of Geneva The Capri Spring School on Transport in Nanostructures April 3-7, 2006 Scattering Theory of Conductance and Shot Noise.
Singularities in hydrodynamics of degenerate 1D quantum systems P. Wiegmann Together with Abanov.
World of ultracold atoms with strong interaction National Tsing-Hua University Daw-Wei Wang.
World of zero temperature --- introduction to systems of ultracold atoms National Tsing-Hua University Daw-Wei Wang.
Universality in ultra-cold fermionic atom gases. with S. Diehl, H.Gies, J.Pawlowski S. Diehl, H.Gies, J.Pawlowski.
Eugene Demler Harvard University Robert Cherng, Adilet Imambekov,
Probing interacting systems of cold atoms using interference experiments Harvard-MIT CUA Vladimir Gritsev Harvard Adilet Imambekov Harvard Anton Burkov.
Universality in ultra-cold fermionic atom gases. with S. Diehl, H.Gies, J.Pawlowski S. Diehl, H.Gies, J.Pawlowski.
STATISTICAL MECHANICS PD Dr. Christian Holm PART 0 Introduction to statistical mechanics.
Temperature scale Titan Superfluid He Ultracold atomic gases.
Probing phases and phase transitions in cold atoms using interference experiments. Anatoli Polkovnikov, Boston University Collaboration: Ehud Altman- The.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Interference of fluctuating condensates Anatoli Polkovnikov Harvard/Boston University Ehud Altman Harvard/Weizmann Vladimir Gritsev Harvard Mikhail Lukin.
by Silke Weinfurtner Victoria University of Wellington, New Zealand Stefano Liberati SISSA/INFN Trieste, Italy Constraining quantum gravity phenomenology.
The 2d gravity coupled to a dilaton field with the action This action ( CGHS ) arises in a low-energy asymptotic of string theory models and in certain.
University of Trento INFM. BOSE-EINSTEIN CONDENSATION IN TRENTO SUPERFLUIDITY IN TRAPPED GASES University of Trento Inauguration meeting, Trento
Chapter 18 Bose-Einstein Gases Blackbody Radiation 1.The energy loss of a hot body is attributable to the emission of electromagnetic waves from.
Ultracold Fermi gases University of Trento BEC Meeting, Trento, 2-3 May 2006 INFM-CNR Sandro Stringari.
The Helmholtz free energyplays an important role for systems where T, U and V are fixed - F is minimum in equilibrium, when U,V and T are fixed! by using:
Experiments with Trapped Potassium Atoms Robert Brecha University of Dayton.
Fermionic quantum criticality and the fractal nodal surface Jan Zaanen & Frank Krüger.
School of something FACULTY OF OTHER School of Physics and Astronomy FACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES “Classical entanglement” and cat states.
Lecture 21. Grand canonical ensemble (Ch. 7)
Examples: Reif Show that C P and C V may be related to each other through quantities that may be determined from the equation of state (i.e. by knowing.
Few-body physics with ultracold fermions Selim Jochim Physikalisches Institut Universität Heidelberg.
Quantum Shock Waves Hydrodynamic Singularities in Degenerate 1D quantum systems P. Wiegmann Together with Alexander Abanov.
Quantum Monte Carlo methods applied to ultracold gases Stefano Giorgini Istituto Nazionale per la Fisica della Materia Research and Development Center.
Blackbody Radiation Wien’s displacement law : Stefan-Boltzmann law :
by Silke Weinfurtner, Matt Visser and Stefano Liberati Massive minimal coupled scalar field from a 2-component Bose-Einstein condensate ESF COSLAB Network.
Horizon in Hawking radiation and in Random Matrix Theory Vladimir Kravtsov Abdus Salam ICTP,Trieste, Italy Collaboration: Fabio Franchini, ICTP July 6,
Fermi-Luttinger Liquid Michael Pustilnik, Georgia Tech
Physics and Astronomy Dept. Kevin Strecker, Andrew Truscott, Guthrie Partridge, and Randy Hulet Observation of Fermi Pressure in Trapped Atoms: The Atomic.
Holographic Models for High-Tc superconductors Jiunn-Wei Chen (NTU) w/ Ying-Jer Kao, Debaprasad Maity, Wen-Yu Wen and Chen-Pin Yeh (talk largely based.
Lecture III Trapped gases in the classical regime Bilbao 2004.
Lecture IV Bose-Einstein condensate Superfluidity New trends.
B.E.C.(Bose-Einstein Condensation) 발표자 : 이수룡 (98).
Statistical mechanics How the overall behavior of a system of many particles is related to the Properties of the particles themselves. It deals with the.
Experimental determination of Universal Thermodynamic Functions for a Unitary Fermi Gas Takashi Mukaiyama Japan Science Technology Agency, ERATO University.
Eiji Nakano, Dept. of Physics, National Taiwan University Outline: 1)Experimental and theoretical background 2)Epsilon expansion method at finite scattering.
Atoms in optical lattices and the Quantum Hall effect Anders S. Sørensen Niels Bohr Institute, Copenhagen.
Optical lattices for ultracold atomic gases Sestri Levante, 9 June 2009 Andrea Trombettoni (SISSA, Trieste)
Pairing Gaps in the BEC-BCS crossover regime 15/06/2005, Strong correlations in Fermi systems Cheng Chin JFI and Physics, University of Chicago Exp.: Rudolf.
Optically Trapped Low-Dimensional Bose Gases in Random Environment
18.3 Bose–Einstein Condensation
Application of AdS/CFT Correspondence to Studies on Non-equilibrium Steady States Shin Nakamura (Chuo University and ISSP, U. Tokyo) Refs. S. N. and H.
Electron-hole duality and vortex formation in quantum dots Matti Manninen Jyväskylä Matti Koskinen Jyväskylä Stephanie Reimann Lund Yongle Yu Lund Maria.
Bose-Einstein Condensates The Coldest Stuff in the Universe Hiro Miyake Splash! November 17, 2012.
D. Jin JILA, NIST and the University of Colorado $ NIST, NSF Using a Fermi gas to create Bose-Einstein condensates.
Basics of edge channels in IQHE doing physics with integer edge channels studies of transport in FQHE regime deviations from the ‘accepted’ picture Moty.
Exploring many-body physics with synthetic matter
Precision collective excitation measurements in the BEC-BCS crossover regime 15/06/2005, Strong correlations in Fermi systems A. Altmeyer 1, S. Riedl 12,
Spectral function in Holographic superconductor Wen-Yu Wen (NTU) Taiwan String Theory Workshop 2010.
Is a system of fermions in the crossover BCS-BEC regime a new type of superfluid? Finite temperature properties of a Fermi gas in the unitary regime.
Application of AdS/CFT Correspondence to Non-equilibrium Physics Shin Nakamura (Chuo University) 中央大学理工学部.
Measuring Entropy and Quantum Viscosity in a Strongly Interacting Atomic Fermi Gas Support: ARO NSF DOE NASA* John E. Thomas Ken O’Hara* Mike Gehm* Stephen.
Functional Integration in many-body systems: application to ultracold gases Klaus Ziegler, Institut für Physik, Universität Augsburg in collaboration with.
Superfluidity and Quantum Vortices. Outline of the presentation Bose-Einstein Condensation Superfluidity Quantum Vortix.
Induced density correlations in a sonic black hole condensate
Small fermionic systems : the common methods and challenges
ultracold atomic gases
Cyrille Marquet Columbia University
Fermi and Bose particles
Ehud Altman Anatoli Polkovnikov Bertrand Halperin Mikhail Lukin
Spectroscopy of ultracold bosons by periodic lattice modulations
周黎红 中国科学院物理研究所 凝聚态理论与材料计算实验室 指导老师: 崔晓玲 arXiv:1507,01341(2015)
Introduction Is there entanglement of black body radiation such as cosmic background radiation or black hole radiation? Entanglement of non-interacting.
Pairing in Imbalanced Fermi Mixtures: Cold Atom Clouds and Neutron Stars printen Utrecht University.
Presentation transcript:

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) reservoir 1D channel µLµL µRµR T=0 Hydrodynamic description …. ->

From the semiclassical to the hydrodynamic description

Thermal distribution of right-coming fermions reservoir 1D channel µLµL µRµR 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

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

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 kT H ≈ mc 2 ?

Thank you for listening ! bosons fermions vs SG, C. Farrell, T. Kiss, and U. Leonhardt, PRA 70, (2004); SG, PRL 94, (2005); SG, JPB 39, S109 (2006). ?