Propagation of polariton fluids and its control Tomas Ostatnický, Alexey V. Kavokin.

Slides:



Advertisements
Similar presentations
Introduction Landau Theory Many phase transitions exhibit similar behaviors: critical temperature, order parameter… Can one find a rather simple unifying.
Advertisements

AMS 691 Special Topics in Applied Mathematics Review of Fluid Equations James Glimm Department of Applied Mathematics and Statistics, Stony Brook University.
Content Outline for Physics B and Physics C Content Area A. Kinematics B. Newton's laws of motion C. Work, energy, power D. Systems of particles, Linear.
Vortex instability and the onset of superfluid turbulence
Lecture 15: Capillary motion
An introduction to superfluidity and quantum turbulence
Chemistry 232 Transport Properties.
AME Int. Heat Trans. D. B. GoSlide 1 Non-Continuum Energy Transfer: Overview.
1 Modeling and Simulation of Photonic Devices and Circuits I (Passive Devices and Circuits) A course on: Optical wave and wave propagation Material optical.
Breakdown of the adiabatic approximation in low-dimensional gapless systems Anatoli Polkovnikov, Boston University Vladimir Gritsev Harvard University.
AME Int. Heat Trans. D. B. GoSlide 1 Non-Continuum Energy Transfer: Gas Dynamics.
World of zero temperature --- introduction to systems of ultracold atoms National Tsing-Hua University Daw-Wei Wang.
Stellar Interior. Solar Facts Radius: –R  = 7  10 5 km = 109 R E Mass : –M  = 2  kg –M  = 333,000 M E Density: –   = 1.4 g/cm 3 –(water is.
Stellar Structure Section 4: Structure of Stars Lecture 9 - Improvement of surface boundary conditions (part 1) Definition of optical depth Simple form.
Stability and Symmetry Breaking in Metal Nanowires III: Nonlinear Stability and Structural Dynamics Capri Spring School on Transport in Nanostructures,
Assignments Reading: Homework: Cengel & Turner Section 12-1, 12-2, 9-4
Stellar Structure Section 3: Energy Balance Lecture 4 – Energy transport processes Why does radiation dominate? Simple derivation of transport equation.
Last Time Free electron model Density of states in 3D Fermi Surface Fermi-Dirac Distribution Function Debye Approximation.
Lecture 10 Energy production. Summary We have now established three important equations: Hydrostatic equilibrium: Mass conservation: Equation of state:
Carbon Nanorings, Lattice Gross-Neveu models of Polyacetylene and the Stability of Quantum Information Michael McGuigan Brookhaven National Laboratory.
Conservation Laws for Continua
Chapter 28 Direct Current Circuits 1.R connections in series and in parallel 2.Define DC (direct current), AC (alternating current) 3.Model of a battery.
Unique additive information measures – Boltzmann-Gibbs-Shannon, Fisher and beyond Peter Ván BME, Department of Chemical Physics Thermodynamic Research.
Anes BOUCHENAK-KHELLADI Advisors : - Jérôme Saint-Martin - Philippe DOLLFUS Institut d’Electronique Fondamentale Phonon thermal transport in Nano-transistors.
The Sun and other stars. The physics of stars A star begins simply as a roughly spherical ball of (mostly) hydrogen gas, responding only to gravity and.
Chapter 7 Restructuring 7.1 Different Sequences in Customary Word Combinations Common Expressions iron and steel; plants and animals the north and.
Lecture 3 BEC at finite temperature Thermal and quantum fluctuations in condensate fraction. Phase coherence and incoherence in the many particle wave.
Quantization via Fractional Revivals Quantum Optics II Cozumel, December, 2004 Carlos Stroud, University of Rochester Collaborators:
1 Physics of GRB Prompt emission Asaf Pe’er University of Amsterdam September 2005.
L4 ECE-ENGR 4243/ FJain 1 Derivation of current-voltage relation in 1-D wires/nanotubes (pp A) Ballistic, quasi-ballistic transport—elastic.
Numerical simulations of thermal counterflow in the presence of solid boundaries Andrew Baggaley Jason Laurie Weizmann Institute Sylvain Laizet Imperial.
Optimization Of a Viscous Flow Between Parallel Plates Based On The Minimization Of Entropy Generation Presentation By Saeed Ghasemi.
Hybrid Bose-Fermi systems
Lecture 2. Why BEC is linked with single particle quantum behaviour over macroscopic length scales Interference between separately prepared condensates.
The review of modern physics has given us a description of nature. Waves are described with a wave equation. Particles are described with particle equations.
ELECTRON THEORY OF METALS 1.Introduction: The electron theory has been developed in three stages: Stage 1.:- The Classical Free Electron Theory : Drude.
Confinement-deconfinement Transition in Graphene Quantum Dots P. A. Maksym University of Leicester 1. Introduction to quantum dots. 2. Massless electron.
First step in Understanding the Nature of Fluid Flow…. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Analysis of Simplest Flow.
Lecture 3. Full statistical description of the system of N particles is given by the many particle distribution function: in the phase space of 6N dimensions.
Alberto Amo, C. Adrados, J. Lefrère, E. Giacobino, A. Bramati
Thermal Properties of Materials
Calculation of Excitations of Superfluid Helium Nanodroplets Roman Schmied and Kevin K. Lehmann Department of Chemistry Princeton University 60 th Ohio.
Cold atoms Lecture th November, Preliminary plan/reality in the fall term Lecture 1 … Lecture 2 … Lecture 3 … Lecture 4 … Lecture 5 … Lecture.
modes Atomic Vibrations in Crystals = Phonons Hooke’s law: Vibration frequency   f = force constant, M = mass Test for phonon effects by using isotopes.
Superconductivity and Superfluidity Landau Theory of Phase Transitions Lecture 5 As a reminder of Landau theory, take the example of a ferromagnetic to.
Flow of Compressible Fluids. Definition A compressible flow is a flow in which the fluid density ρ varies significantly within the flowfield. Therefore,
Chapter 1. Essential Concepts
Chapter 7 in the textbook Introduction and Survey Current density:
Thermodynamics and Transport in Iron-based superconductors Maxim G. Vavilov, University of Wisconsin-Madison, DMR Recent discovery of novel iron-pnictide.
Solid state physics is the study of how atoms arrange themselves into solids and what properties these solids have. Calculate the macroscopic properties.
Physics 176: Lecture 2 Tuesday, 1/18/2011 Before you take your seat: Pick up PRS transmitter Pick up 1-min questionnaire.
Superfluidity and Quantum Vortices. Outline of the presentation Bose-Einstein Condensation Superfluidity Quantum Vortix.
Collective Excitations in QCD Plasma
LAWS OF THERMODYNAMICS
Hydrodynamics of slowly miscible liquids
Nonequilibrium statistical mechanics of electrons in a diode
Electrical Properties of Materials
A course on: Optical wave and wave propagation
Fluid kinematics Chapter 3
Imaging exciton polariton transport in MoSe2
Conservation of Momentum (horizontal)
Chapter 1: Statistical Basis of Thermodynamics
Laws of Thermodynamics
Chapter 5 - Phonons II: Quantum Mechanics of Lattice Vibrations
1 a. A machine can never be 100% efficient. The out put energy will always be less than the input energy 1 a. i) see above ANS ii) see above.
Benchmark #1 Review.
Thermomechanical effect
A. Thermodynamics B. Kinetics and Transport
Chapter 2: Energy and the First Law of Thermodynamics
Presentation transcript:

Propagation of polariton fluids and its control Tomas Ostatnický, Alexey V. Kavokin

Motivation Spintronics – information stored in spin Need of spin transport and processing Microcavity polaritons: half-photon, half-exciton combination of both, may carry spin and interact promising for spin-optronic circuits ElectronicsPhotonics DiffusiveBallisticPropagation ResistivityLosses ~ 0Interactions ~ 10  m Spin transport

Theoretical approach: fluids Assume local thermal equilibrium Thermodynamical description Parameters: density, current, entropy Propagation controlled by static potential and chemical potential

Towards superfluidity: multiple fluids Superfluidity in He II explained by L. Landau in terms of two-fluid model Coexistence of two interacting fluids: a normal fraction and a superfluid fraction Mutual interactions much weaker than interactions within fluid fractions

Multiple fluids & polaritons (1) Helium atoms Infinite lifetime Constant density One normal fraction Polaritons Finite lifetime Variable density Multiple normal fractions LA-phonon assisted transition rate (depending on QW width)

Multiple fluids & polaritons (2) Concept of Landau adapted for polaritons Conservation laws + Navier-Stokes equation + friction + lifetime 4 equations for and S: the last equation is the equation of state Determines potential, pressure and temperature Both superfluid (coherent) and normal fractions present in model

Superfluidity of polaritons Expansion of normal componentShock waves in superfluid

Polariton circuits (1) 1D quantum wire with single parabolic band One or Two “sources” on sides Variable potential barrier by electric field

Polariton circuits (2) Steady-state chemical potential – comparison with electrons Lifetime taken to be infinite Source on the left,  0 on the right

Polariton circuits (3) Equilibrium established after t = lifetime Here  = 1 ns

Polariton circuits (4) Variable friction Variable lifetime

Polariton circuits (5) Two normal fluids from two sources with and without mutual friction

Polariton circuits (6) Control by locally applied electric field in normal direction

Conclusions Modelling of polariton fluid propagation Superfluidity and coexistence of both fractions included Results of simulations reveal behaviour of polaritons similar to electronics but with some peculiarities Possibility of construction of circuits with propagating polaritons Possibility of dynamical control by external electric field ElectronicsPhotonicsPolaritons DiffusiveBallistic Propagation ResistivityLifetimeLosses ~ 0Interactions ~ 10  m Spin transport