From dynamics of a single From dynamics of a single superfmuid - - PowerPoint PPT Presentation

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From dynamics of a single From dynamics of a single superfmuid - - PowerPoint PPT Presentation

From dynamics of a single From dynamics of a single superfmuid vortex superfmuid vortex to quantum turbulence to quantum turbulence in the unitary Fermi gas: in the unitary Fermi gas: results of time-dependent results of time-dependent


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From dynamics of a single From dynamics of a single superfmuid vortex superfmuid vortex to quantum turbulence to quantum turbulence in the unitary Fermi gas: in the unitary Fermi gas: results of time-dependent results of time-dependent superfmuid superfmuid density functional theory density functional theory

Gabriel Wlazłowski

Warsaw University of T echnology University of Washington In collaboration with: Aurel Bulgac (UW), Michael McNeil Forbes (WSU, INT) Michelle M. Kelley (Urbana-Champaign) Kenneth J. Roche (PNNL,UW)

Quantum Technologies VI, Warsaw, Poland, 22 June 2015

Supported by:

  • Polish National Science

Center (NCN) grant under decision No. DEC- 2014/13/D/ST3/01940.

  • Polish National Science

Center (NCN) grant under decision No. DEC- 2013/08/A/ST3/00708.

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Present challenge for MBT:

Unifjed description of static and dynamic properties of large Fermi systems

Methods:

QMC (static) DFT (static and dynamic) ...(efgective theories)...

Qualitatively and quantitatively accurate

Cold atoms near a Feshbach Cold atoms near a Feshbach resonance = unitary Fermi gas resonance = unitary Fermi gas

System is dilute but... strongly interacting!

Unitary limit: no interaction length scale... Universal physics... Cold atomic gases Neutron matter High-Tc superconductors Simple, but hard to calculate! (Bertsch Many Body X-challenge)

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DFT: workhorse for electronic structure simulations

The Hohenberga-Kohn theorem assures that the theory can reproduce exactly the ground state energy if the “exact” Energy Density Functional (EDF) is provided Often called as ab initio method Extension to Time-Dependent DFT is straightforward Very successful – DFT industry (commercial

codes for quantum chemistry and solid-state physics)

Can be extended to superfluid systems...

(numerical cost increases dramatically) 1990 2012

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EDF for UFG: Superfluid Local Density Approximation (SLDA)

Dimensional arguments, renormalizability, Galilean invariance, and symmetries (translational, rotational, gauge, parity) determine the functional (energy density) Only local densities unique combination of the kinetic and anomalous densities required by the renormalizability of the theory Self-energy term - the only function

  • f the density alone allowed by

dimensional arguments lowest gradient correction- negligible required by Galilean invariance

Review: A. Bulgac, M.M. Forbes, P. Magierski, Lecture Notes in Physics, Vol. 836, Chap. 9, p.305-373 (2012)

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Three dimensionless constants α, β, and γ determining the functional are extracted from QMC results for homogeneous systems

(for example by fjxing the total energy, the pairing gap and the efgective mass.)

NOTE: there is no fjt to experimental results Forbes, Gandolfi, Gezerlis, PRL 106, 235303 (2011) SLDA has been verifjed and validated against a large number of quantum Monte Carlo results for inhomogeneous systems and experimental data as well

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SLIDE 6

6Li atoms near a Feshbach

resonance (N≈106) cooled in harmonic trap Step potential used to imprint a soliton (evolve to π phase shift) Let system evolve... Take picture (subtle imaging with

tomography)

  • Fig. from

Nature 499, 426 (2013)

Validation against dynamical properties of the system

Recent MIT experiments: Nature 499, 426 (2013), PRL 113, 065301(2014)

  • Fig. from

PRL 113, 065301(2014)

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Experimental results

Yefsah et al., Nature 499, 426 (2013)

PRL 113, 065301(2014)

RESULTS: In the final state: Observe an

  • scillating

vortex line with long period Intertial mass 200 times larger than the free fermion mass Precessional motion ...

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Experimental results – Cascade of Solitary Waves

Figures taken from: M. Zwierlein talk, (http://en.sif.it/activities/fermi_school/mmxiv) School of Physics E. Fermi – Quantum Matter at Ultralow Temperatures Varenna, July 9th , 2014

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Experimental results – Cascade of Solitary Waves

Figures taken from: M. Zwierlein talk, (http://en.sif.it/activities/fermi_school/mmxiv) School of Physics E. Fermi – Quantum Matter at Ultralow Temperatures Varenna, July 9th , 2014

Challenge for theory to describe all stages of the cascade!

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What do fully 3D simulations see?

Movie 1 32×32×128, 560 particles 48×48×128, 1270 particles

  • Phys. Rev. Lett. 112, 025301 (2014)

What about Gross-Pitaevskii equation? Movie 1 GP

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Realistic simulation

Trapping potential: The optical trapping potential in the x and y directions is an axially symmetric gaussian altered by gravity in the vertical direction y anisotropy anharmonicity

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What do fully 3D simulations see?

Movie 2 Movie 3

Crossing and reconnection!

  • Phys. Rev. A 91, 031602 (2015)
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T urbulence: classical vs quantum

Leonardo da Vinci (1452-1519)

  • bservation: the

turbulent flow of water had a structure comprised of vortices

  • f different sizes.

However:

  • vortices are not well-defined for a classical

viscous fluid

  • unstable and appear and disappear

repeatedly

  • circulation is not conserved and not

identical for each vortex

But in quantum world... Quantized circulation: vortex of inviscid superflow and thus it cannot decay (topological defect)

Physics Reports 522, 191 (2013)

Basic process: reconnection

  • Phys. Rev. Lett. 97 (2006) 145301

Quantum turbulence: Chaotic dynamics of many quantized vortices

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T

  • wards quantum turbulence...

Tangle of many vortices!

  • Phys. Rev. A 91, 031602 (2015)

How to generate QT state? Our proposition: “phase imprint”

  • f a lattice of vortices

Movie 4

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SLIDE 15

Thank you

CONCLUSIONS:

DFT capable to explain all aspects of the experiment Long periods of oscillation... Vortex alignment... Correctly describes generation, dynamics, evolution, and eventual decay - large number of degrees of freedom in the SLDA permit many mechanisms for superfluid relaxation: various phonon processes, Cooper pair breaking, and Landau damping Validates (TD)DFT... Can be used to engineer interesting scenarios: colliding of vortices, QT, vortex interactions...