Supersolids. Bose-Einstein Condensation in Quantum Solids Does it really exist?? W. J. Mullin

Size: px
Start display at page:

Download "Supersolids. Bose-Einstein Condensation in Quantum Solids Does it really exist?? W. J. Mullin"

Transcription

1

2 Supersolids Bose-Einstein Condensation in Quantum Solids Does it really exist?? W. J. Mullin This is a lively controversy in condensed matter physics. Experiment says yes. Theory says no, or at best maybe. I. Superfluidity. Flow without friction. How does that occur? II. Bose-Einstein condensation. What is it? III. Quantum crystals. What makes them quantum? IV. Supersolids. Can superfluidity exist in a crystal?

3 Quantized Energies In QM a particle in a box has only certain allowed frequencies and energies Particles with short wavelengths (high energies) behave like marbles. Particles with long wavelengths (low energies) behave like waves Can t tell one from another. Quantum interference λ= Weird behavior. Energy Low T means long wavelength E 4 E 3 E 2 E 1 E 0 h < p > = h 2 2πmkT DeBroglie or thermal wavelength

4 Temperature Scales

5 The Cryostat -- a big thermos bottle.

6 Two kinds of particles in nature Fermions (Fermi-Dirac statistics) - all spin- particles e, n, p, µ, ν, quarks, and composites of an odd number of fermions Pauli principle- only one Fermion at a time allowed in each state Electrons in the atom, nuclei in the nucleus, white dwarf star Bosons (Bose-Einstein statistics) - all spin 0,1,... particles γ, π, w, z, gluons,.., composites of an even number of fermions. Bose principle -preference for occupation of the same state by more than one particle BEC in trapped gases and in liquid 4 He 1 2

7 2n 2p 4 He e e Superfluids Liquid 4 He first produced in 1908, superfluid studies in 30 s. Weird properties Liquid all the way to T=0K. (Solidifies only under pressure.) Excellent heat conductor (better than copper) Superleak T>2.2K T<2.2K 1n 2p 3 He e e Fictionless flow Persistent currents

8 Phase Diagram of Liquid Helium Andronikashvili's Experiment

9 Bose-Einstein Condensation Einstein (1925) found that at a certain temperature there was a phase transition in a collection of bosons in which a large number of particles fell into the lowest state. The number in that state grows as the temperature drops. Energy T>T c Energy T<T c E 4 E 3 E 2 E 1 E 0 E 4 E 3 E 2 E 1 E 0 N 0 particles N 0 Tc T Bitter theoretical debate between Landau and London over explanation via BEC (40 s, 50 s)

10 Explanation by BEC? Analogy: Bose effect in the laser (photons are bosons) Bosons like to be in the same state All photons have same frequency, same phase. Superfluid: Particles like to move all in the same way, as a group Energy gap gap object moves through liquid without being able to transfer energy no friction

11 Fermions and Superfluidity Superconductivity Metals that conduct electricity without resistance. Metals have transition T c at few Kelvin. Electrons pair up ( Cooper pairs ) coherently and cooperatively below T c. (Electron pairs are bosons, but this is not quite BEC.) Hi- T c superconductivity (>90K) discovered in ceramics. Superfluidity in liquid 3 He Superfluid transition at T=2 mk Three different superfluid phases Osheroff, Lee, and Richardson Nobel Prize in 1996.

12 Bose-Einstein Condensation of Trapped Atoms 7 Li, 23 Na, 87 Rb are Bosons Atoms are cooled to a transition temperature where they suddenly fall into the lowest energy state. Laser cooling plus magnetic evaporation. This is the phase transition predicted by Einstein in 1925! Cornell and Weiman* JILA, CU Rb 20,000 atoms, Tc= 0.2 µk July 95 Ketterle* MIT Na 50,000 to millions 2 µk August 95 Hulet Rice U Li 20,000 atoms 0.2 µk 1996 * Nobel Prize 2001

13 Theory is easy in a weakly interacting dilute gas; agreement with experiment is remarkable. Spectacular experimental possibilities Atom interference Atomic Laser! -- a coherent source of atomic matter waves

14 Quantum Crystals The lightest elements, hydrogen and helium, form crystals at low temperature. They show the effects of quantum mechanics, especially helium Zero-point energy: Particle in a box has a lowest energy E 0 h2 ml 2 N Particles confined in a crystal have smallest energy E N h2 ma 2 where a is interparticle separation.

15 Helium remains a liquid at T = 0 K unless one applies pressure (25 atm). Zero-point energy melts it. When it does form a crystal it is blown up by zero point motion by a factor of 2. Quantum tunneling: Particles easily exchange places. (Overlapping wave functions) Vacancy waves: All crystals have thermally activated vacancies. You have to heat the crystal to make them. Solid helium has vacancy waves. A vacancy is spread out over the whole crystal

16 All vacancies that have been observed directly in solid helium have been of the thermally activated kind. Zero-Point Vacancies??? Suppose delocalized vacancies existed in the crystal even at T = 0 K. Could the vacancies form a BEC and cause particle motion without friction? That would be a superfluid with solid ordering. Such a state was proposed theoretically in the 70 s. Several experiments looked for it but, never saw it.

17 Until last year! Probable observation of a supersolid helium phase E. Kim & M. H. W. Chan Nature 427, 225 (2004) Torsional oscillator--solid 4 He in vycor (hole-filled glass) annulus and without vycor Moses parts the Red Solid?

18 Measure the superfluid fraction ~2% by observing decrease in moment of inertia

19 New York Times article

20 Theory Old theories suggested supersolids in the first place. More recent work: One side: Supersolids cannot exist without zero-point vacancies, which are not observed. So it is something else. Other side: Superfluidity can be carried via exchange without vacancies. Large Monte Carlo simulations are involved on both sides of the argument. Other recent experiments have not found the same super flow as yet. So what have Kim and Chan found?

Nanoelectronics 14. [( ) k B T ] 1. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture.

Nanoelectronics 14. [( ) k B T ] 1. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture. Nanoelectronics 14 Atsufumi Hirohata Department of Electronics 09:00 Tuesday, 27/February/2018 (P/T 005) Quick Review over the Last Lecture Function Fermi-Dirac distribution f ( E) = 1 exp E µ [( ) k B

More information

Workshop on Supersolid August Brief introduction to the field. M. Chan Pennsylvania State University, USA

Workshop on Supersolid August Brief introduction to the field. M. Chan Pennsylvania State University, USA 1959-11 Workshop on Supersolid 2008 18-22 August 2008 Brief introduction to the field M. Chan Pennsylvania State University, USA Superfluid and supersolid An introduction at the ICTP Supersolid 2008 workshop

More information

70 YEAR QUEST ENDS IN SUCCESS BOSE-EINSTEIN CONDENSATION 2001 NOBEL PRIZE IN PHYSICS

70 YEAR QUEST ENDS IN SUCCESS BOSE-EINSTEIN CONDENSATION 2001 NOBEL PRIZE IN PHYSICS 70 YEAR QUEST ENDS IN SUCCESS BOSE-EINSTEIN CONDENSATION 2001 NOBEL PRIZE IN PHYSICS 8.044, LECTURE 33, SPRING 2004 BOSE-EINSTEIN CONDENSATION IS A QUANUM MECHANICAL EFFECT Image removed due to copyright

More information

Quantum Properties of Two-dimensional Helium Systems

Quantum Properties of Two-dimensional Helium Systems Quantum Properties of Two-dimensional Helium Systems Hiroshi Fukuyama Department of Physics, Univ. of Tokyo 1. Quantum Gases and Liquids 2. Bose-Einstein Condensation 3. Superfluidity of Liquid 4 He 4.

More information

Superfluidity and Superconductivity

Superfluidity and Superconductivity Superfluidity and Superconductivity These are related phenomena of flow without resistance, but in very different systems Superfluidity: flow of helium IV atoms in a liquid Superconductivity: flow of electron

More information

Bose-Einstein Condensate: A New state of matter

Bose-Einstein Condensate: A New state of matter Bose-Einstein Condensate: A New state of matter KISHORE T. KAPALE June 24, 2003 BOSE-EINSTEIN CONDENSATE: A NEW STATE OF MATTER 1 Outline Introductory Concepts Bosons and Fermions Classical and Quantum

More information

Introduction to cold atoms and Bose-Einstein condensation (II)

Introduction to cold atoms and Bose-Einstein condensation (II) Introduction to cold atoms and Bose-Einstein condensation (II) Wolfgang Ketterle Massachusetts Institute of Technology MIT-Harvard Center for Ultracold Atoms 7/7/04 Boulder Summer School * 1925 History

More information

Chapter 7: Quantum Statistics

Chapter 7: Quantum Statistics Part II: Applications - Bose-Einstein Condensation SDSMT, Physics 204 Fall Introduction Historic Remarks 2 Bose-Einstein Condensation Bose-Einstein Condensation The Condensation Temperature 3 The observation

More information

Quantum Fluids and Solids. Christian Enss (4He) & Henri Godfrin (3He)

Quantum Fluids and Solids. Christian Enss (4He) & Henri Godfrin (3He) Quantum Fluids and Solids Christian Enss (4He) & Henri Godfrin (3He) What Do We Consider as Quantum Matter? φ Lennard Jones Potential σ ε r De Boer quantum parameter: De Broglie wavelength: Introduction

More information

Revolution in Physics. What is the second quantum revolution? Think different from Particle-Wave Duality

Revolution in Physics. What is the second quantum revolution? Think different from Particle-Wave Duality PHYS 34 Modern Physics Ultracold Atoms and Trappe Ions Today and Mar.3 Contents: a) Revolution in physics nd Quantum revolution b) Quantum simulation, measurement, and information c) Atomic ensemble and

More information

BEC Vortex Matter. Aaron Sup October 6, Advisor: Dr. Charles Hanna, Department of Physics, Boise State University

BEC Vortex Matter. Aaron Sup October 6, Advisor: Dr. Charles Hanna, Department of Physics, Boise State University BEC Vortex Matter Aaron Sup October 6, 006 Advisor: Dr. Charles Hanna, Department of Physics, Boise State University 1 Outline 1. Bosons: what are they?. Bose-Einstein Condensation (BEC) 3. Vortex Formation:

More information

Supersolidity of excitons

Supersolidity of excitons Supersolidity of excitons Michał Matuszewski Institute of Physics, Polish Academy of Sciences, Warsaw Thomas R. Taylor and Alexey V. Kavokin University of Southampton, UK ISNP 2012, Phuket Outline 1. What

More information

Chapter 7: Quantum Statistics

Chapter 7: Quantum Statistics Part II: Applications - Bose-Einstein Condensation SDSMT, Physics 203 Fall Introduction Historic Remarks 2 Bose-Einstein Condensation Bose-Einstein Condensation The Condensation Temperature 3 The observation

More information

Superfluidity and Condensation

Superfluidity and Condensation Christian Veit 4th of June, 2013 2 / 29 The discovery of superfluidity Early 1930 s: Peculiar things happen in 4 He below the λ-temperature T λ = 2.17 K 1938: Kapitza, Allen & Misener measure resistance

More information

Ultra-cold gases. Alessio Recati. CNR INFM BEC Center/ Dip. Fisica, Univ. di Trento (I) & Dep. Physik, TUM (D) TRENTO

Ultra-cold gases. Alessio Recati. CNR INFM BEC Center/ Dip. Fisica, Univ. di Trento (I) & Dep. Physik, TUM (D) TRENTO Ultra-cold gases Alessio Recati CNR INFM BEC Center/ Dip. Fisica, Univ. di Trento (I) & Dep. Physik, TUM (D) TRENTO Lectures L. 1) Introduction to ultracold gases Bosonic atoms: - From weak to strong interacting

More information

Cold atoms. 1: Bose-Einstein Condensation. Emil Lundh. April 13, Department of Physics Umeå University

Cold atoms. 1: Bose-Einstein Condensation. Emil Lundh. April 13, Department of Physics Umeå University 1: Bose-Einstein Condensation Department of Physics Umeå University lundh@tp.umu.se April 13, 2011 Umeå 114 000 inhabitants Average age 37.9 years Cultural capital of Europe 2014 400 km ski tracks 180

More information

The phases of matter familiar for us from everyday life are: solid, liquid, gas and plasma (e.f. flames of fire). There are, however, many other

The phases of matter familiar for us from everyday life are: solid, liquid, gas and plasma (e.f. flames of fire). There are, however, many other 1 The phases of matter familiar for us from everyday life are: solid, liquid, gas and plasma (e.f. flames of fire). There are, however, many other phases of matter that have been experimentally observed,

More information

PHYS 3313 Section 001 Lecture # 24

PHYS 3313 Section 001 Lecture # 24 PHYS 3313 Section 001 Lecture # 24 Wednesday, April 29, Dr. Alden Stradling Equipartition Theorem Quantum Distributions Fermi-Dirac and Bose-Einstein Statistics Liquid Helium Laser PHYS 3313-001, Spring

More information

BEC of 6 Li 2 molecules: Exploring the BEC-BCS crossover

BEC of 6 Li 2 molecules: Exploring the BEC-BCS crossover Institut für Experimentalphysik Universität Innsbruck Dresden, 12.10. 2004 BEC of 6 Li 2 molecules: Exploring the BEC-BCS crossover Johannes Hecker Denschlag The lithium team Selim Jochim Markus Bartenstein

More information

CONDENSED MATTER: towards Absolute Zero

CONDENSED MATTER: towards Absolute Zero CONDENSED MATTER: towards Absolute Zero The lowest temperatures reached for bulk matter between 1970-2000 AD. We have seen the voyages to inner & outer space in physics. There is also a voyage to the ultra-cold,

More information

Introduction to Bose-Einstein condensation 4. STRONGLY INTERACTING ATOMIC FERMI GASES

Introduction to Bose-Einstein condensation 4. STRONGLY INTERACTING ATOMIC FERMI GASES 1 INTERNATIONAL SCHOOL OF PHYSICS "ENRICO FERMI" Varenna, July 1st - July 11 th 2008 " QUANTUM COHERENCE IN SOLID STATE SYSTEMS " Introduction to Bose-Einstein condensation 4. STRONGLY INTERACTING ATOMIC

More information

Cold fermions, Feshbach resonance, and molecular condensates (II)

Cold fermions, Feshbach resonance, and molecular condensates (II) Cold fermions, Feshbach resonance, and molecular condensates (II) D. Jin JILA, NIST and the University of Colorado I. Cold fermions II. III. Feshbach resonance BCS-BEC crossover (Experiments at JILA) $$

More information

3.024 Electrical, Optical, and Magnetic Properties of Materials Spring 2012 Recitation 8 Notes

3.024 Electrical, Optical, and Magnetic Properties of Materials Spring 2012 Recitation 8 Notes Overview 1. Electronic Band Diagram Review 2. Spin Review 3. Density of States 4. Fermi-Dirac Distribution 1. Electronic Band Diagram Review Considering 1D crystals with periodic potentials of the form:

More information

Introduction to Cold Atoms and Bose-Einstein Condensation. Randy Hulet

Introduction to Cold Atoms and Bose-Einstein Condensation. Randy Hulet Introduction to Cold Atoms and Bose-Einstein Condensation Randy Hulet Outline Introduction to methods and concepts of cold atom physics Interactions Feshbach resonances Quantum Gases Quantum regime nλ

More information

Bose Einstein Condensation

Bose Einstein Condensation April 3, 2017 Quantum Physics becomes visible in the cold Quantum Effects in Macroscopic World at Low Temperature Superconductivity Quantum Hall Effect Bose Einstein Condensation Deep down, all matter

More information

CHAPTER 9 Statistical Physics

CHAPTER 9 Statistical Physics CHAPTER 9 Statistical Physics 9.1 Historical Overview 9.2 Maxwell Velocity Distribution 9.3 Equipartition Theorem 9.4 Maxwell Speed Distribution 9.5 Classical and Quantum Statistics 9.6 Fermi-Dirac Statistics

More information

10 Supercondcutor Experimental phenomena zero resistivity Meissner effect. Phys463.nb 101

10 Supercondcutor Experimental phenomena zero resistivity Meissner effect. Phys463.nb 101 Phys463.nb 101 10 Supercondcutor 10.1. Experimental phenomena 10.1.1. zero resistivity The resistivity of some metals drops down to zero when the temperature is reduced below some critical value T C. Such

More information

From laser cooling to BEC First experiments of superfluid hydrodynamics

From laser cooling to BEC First experiments of superfluid hydrodynamics From laser cooling to BEC First experiments of superfluid hydrodynamics Alice Sinatra Quantum Fluids course - Complement 1 2013-2014 Plan 1 COOLING AND TRAPPING 2 CONDENSATION 3 NON-LINEAR PHYSICS AND

More information

Announcement. Station #2 Stars. The Laws of Physics for Elementary Particles. Lecture 9 Basic Physics

Announcement. Station #2 Stars. The Laws of Physics for Elementary Particles. Lecture 9 Basic Physics Announcement Pick up your quiz after this lecture as you leave the lecture hall. Homework#2 due on Thursday No hand-written homework! Please staple them! Put it in the box before the lecture begins! Station

More information

Helium-3, Phase diagram High temperatures the polycritical point. Logarithmic temperature scale

Helium-3, Phase diagram High temperatures the polycritical point. Logarithmic temperature scale Helium-3, Phase diagram High temperatures the polycritical point Logarithmic temperature scale Fermi liquid theory Start with a noninteracting Fermi gas and turn on interactions slowly, then you get a

More information

PHYS 393 Low Temperature Physics Set 1:

PHYS 393 Low Temperature Physics Set 1: PHYS 393 Low Temperature Physics Set 1: Introduction and Liquid Helium-3 Christos Touramanis Oliver Lodge Lab, Office 319 c.touramanis@liverpool.ac.uk Low Temperatures Low compared to what? Many definitions

More information

Supersolid. Yixing Fu 2013/3/14

Supersolid. Yixing Fu 2013/3/14 Supersolid Yixing Fu 2013/3/14 Supersolid "Superfluid-like solid" Intensively discussed by theorists in 1970s Still uncertain 3/14/2013 Yixing Fu - Physics 141A 2 Outline The pre-history of supersolid

More information

Strongly paired fermions

Strongly paired fermions Strongly paired fermions Alexandros Gezerlis TALENT/INT Course on Nuclear forces and their impact on structure, reactions and astrophysics July 4, 2013 Strongly paired fermions Neutron matter & cold atoms

More information

PHYS 393 Low Temperature Physics Set 2: Liquid Helium-4

PHYS 393 Low Temperature Physics Set 2: Liquid Helium-4 PHYS 393 Low Temperature Physics Set 2: Liquid Helium-4 Christos Touramanis Oliver Lodge Lab, Office 319 c.touramanis@liverpool.ac.uk He 4 atom Two protons, two neutrons in nucleus: I=0 Two electrons in

More information

From BEC to BCS. Molecular BECs and Fermionic Condensates of Cooper Pairs. Preseminar Extreme Matter Institute EMMI. and

From BEC to BCS. Molecular BECs and Fermionic Condensates of Cooper Pairs. Preseminar Extreme Matter Institute EMMI. and From BEC to BCS Molecular BECs and Fermionic Condensates of Cooper Pairs Preseminar Extreme Matter Institute EMMI Andre Wenz Max-Planck-Institute for Nuclear Physics and Matthias Kronenwett Institute for

More information

Effective Field Theory and Ultracold Atoms

Effective Field Theory and Ultracold Atoms Effective Field Theory and Ultracold Atoms Eric Braaten Ohio State University support Department of Energy Air Force Office of Scientific Research Army Research Office 1 Effective Field Theory and Ultracold

More information

A Superfluid Universe

A Superfluid Universe A Superfluid Universe Lecture 2 Quantum field theory & superfluidity Kerson Huang MIT & IAS, NTU Lecture 2. Quantum fields The dynamical vacuum Vacuumscalar field Superfluidity Ginsburg Landau theory BEC

More information

Ana Maria Rey. Okinawa School in Physics 2016: Coherent Quantum Dynamics. Okinawa, Japan, Oct 4-5, 2016

Ana Maria Rey. Okinawa School in Physics 2016: Coherent Quantum Dynamics. Okinawa, Japan, Oct 4-5, 2016 Ana Maria Rey Okinawa School in Physics 016: Coherent Quantum Dynamics Okinawa, Japan, Oct 4-5, 016 What can we do with ultra-cold matter? Quantum Computers Lecture II-III Clocks and sensors Synthetic

More information

Lecture 3. Bose-Einstein condensation Ultracold molecules

Lecture 3. Bose-Einstein condensation Ultracold molecules Lecture 3 Bose-Einstein condensation Ultracold molecules 66 Bose-Einstein condensation Bose 1924, Einstein 1925: macroscopic occupation of the lowest energy level db h 2 mk De Broglie wavelength d 1/3

More information

When superfluids are a drag

When superfluids are a drag When superfluids are a drag KITP October 2008 David Roberts Los Alamos National Laboratory In collaboration with Yves Pomeau (ENS), Andrew Sykes (Queensland), Matt Davis (Queensland), What makes superfluids

More information

Reference for most of this talk:

Reference for most of this talk: Cold fermions Reference for most of this talk: W. Ketterle and M. W. Zwierlein: Making, probing and understanding ultracold Fermi gases. in Ultracold Fermi Gases, Proceedings of the International School

More information

Magnetism in ultracold gases

Magnetism in ultracold gases Magnetism in ultracold gases Austen Lamacraft Theoretical condensed matter and atomic physics April 10th, 2009 faculty.virginia.edu/austen/ Outline Magnetism in condensed matter Ultracold atomic physics

More information

The non-interacting Bose gas

The non-interacting Bose gas Chapter The non-interacting Bose gas Learning goals What is a Bose-Einstein condensate and why does it form? What determines the critical temperature and the condensate fraction? What changes for trapped

More information

The physics of cold atoms from fundamental problems to time measurement and quantum technologies. Michèle Leduc

The physics of cold atoms from fundamental problems to time measurement and quantum technologies. Michèle Leduc The physics of cold atoms from fundamental problems to time measurement and quantum technologies Michèle Leduc Lima, 20 October 2016 10 5 Kelvin 10 4 Kelvin Surface of the sun 10 3 Kelvin 10 2 Kelvin earth

More information

BEC AND MATTER WAVES an overview Allan Griffin, University of Toronto

BEC AND MATTER WAVES an overview Allan Griffin, University of Toronto BEC AND MATTER WAVES an overview Allan Griffin, University of Toronto The discovery of Bose-Einstein condensation ( BEC ) in 1995 in dilute, ultracold trapped atomic gases is one of the most exciting developments

More information

ABSOLUTE ZERO Karina Aliaga

ABSOLUTE ZERO Karina Aliaga ABSOLUTE ZERO Karina Aliaga WHAT IS ABSOLUTE ZERO? Temperature is a physical quantity that measures the kinetic energy of particles in matter. It depends on the oscillations of atoms and molecules. As

More information

The amazing story of Laser Cooling and Trapping

The amazing story of Laser Cooling and Trapping The amazing story of Laser Cooling and Trapping following Bill Phillips Nobel Lecture http://www.nobelprize.org/nobel_prizes/physics/ laureates/1997/phillips-lecture.pdf Laser cooling of atomic beams 1

More information

Ultracold molecules - a new frontier for quantum & chemical physics

Ultracold molecules - a new frontier for quantum & chemical physics Ultracold molecules - a new frontier for quantum & chemical physics Debbie Jin Jun Ye JILA, NIST & CU, Boulder University of Virginia April 24, 2015 NIST, NSF, AFOSR, ARO Ultracold atomic matter Precise

More information

A Mixture of Bose and Fermi Superfluids. C. Salomon

A Mixture of Bose and Fermi Superfluids. C. Salomon A Mixture of Bose and Fermi Superfluids C. Salomon Enrico Fermi School Quantum Matter at Ultralow Temperatures Varenna, July 8, 2014 The ENS Fermi Gas Team F. Chevy, Y. Castin, F. Werner, C.S. Lithium

More information

Superflow in Solid Helium

Superflow in Solid Helium Superflow in Solid Helium Abhishek Roy December 16, 2004 Abstract The small mass and significant zero point motion of solid 4 He make it very different from its conventional counterparts. In the seventies

More information

Realization of Bose-Einstein Condensation in dilute gases

Realization of Bose-Einstein Condensation in dilute gases Realization of Bose-Einstein Condensation in dilute gases Guang Bian May 3, 8 Abstract: This essay describes theoretical aspects of Bose-Einstein Condensation and the first experimental realization of

More information

Superfluidity. v s. E. V. Thuneberg Department of Physical Sciences, P.O.Box 3000, FIN University of Oulu, Finland (Dated: June 8, 2012)

Superfluidity. v s. E. V. Thuneberg Department of Physical Sciences, P.O.Box 3000, FIN University of Oulu, Finland (Dated: June 8, 2012) Superfluidity E. V. Thuneberg Department of Physical Sciences, P.O.Box 3000, FIN-90014 University of Oulu, Finland (Dated: June 8, 01) PACS numbers: 67.40.-w, 67.57.-z, 74., 03.75.-b I. INTRODUCTION Fluids

More information

Precision Interferometry with a Bose-Einstein Condensate. Cass Sackett. Research Talk 17 October 2008

Precision Interferometry with a Bose-Einstein Condensate. Cass Sackett. Research Talk 17 October 2008 Precision Interferometry with a Bose-Einstein Condensate Cass Sackett Research Talk 17 October 2008 Outline Atom interferometry Bose condensates Our interferometer One application What is atom interferometry?

More information

Quantum Quantum Optics Optics VII, VII, Zakopane Zakopane, 11 June 09, 11

Quantum Quantum Optics Optics VII, VII, Zakopane Zakopane, 11 June 09, 11 Quantum Optics VII, Zakopane, 11 June 09 Strongly interacting Fermi gases Rudolf Grimm Center for Quantum Optics in Innsbruck University of Innsbruck Austrian Academy of Sciences ultracold fermions: species

More information

Superfluids, Superconductors and Supersolids: Macroscopic Manifestations of the Microworld Laws

Superfluids, Superconductors and Supersolids: Macroscopic Manifestations of the Microworld Laws University of Massachusetts Amherst From the SelectedWorks of Egor Babaev 2008 Superfluids, Superconductors and Supersolids: Macroscopic Manifestations of the Microworld Laws Egor Babaev, University of

More information

Many-Body Physics with Quantum Gases

Many-Body Physics with Quantum Gases Many-Body Physics with Quantum Gases Christophe Salomon Okinawa Summer school on quantum dynamics September 26-October 6, 2017 Ecole Normale Supérieure, Paris Summary of lectures Quantum simulation with

More information

Strongly Correlated Physics With Ultra-Cold Atoms

Strongly Correlated Physics With Ultra-Cold Atoms Strongly Correlated Physics With Ultra-Cold Atoms Predrag Nikolić Rice University Acknowledgments Collaborators Subir Sachdev Eun-Gook Moon Anton Burkov Arun Paramekanti Sponsors W.M.Keck Program in Quantum

More information

Lecture 19: Building Atoms and Molecules

Lecture 19: Building Atoms and Molecules Lecture 19: Building Atoms and Molecules +e r n = 3 n = 2 n = 1 +e +e r y even Lecture 19, p 1 Today Nuclear Magnetic Resonance Using RF photons to drive transitions between nuclear spin orientations in

More information

PHYS-E0551. Low Temperature Physics Basics of Cryoengineering Course 2015:

PHYS-E0551. Low Temperature Physics Basics of Cryoengineering Course 2015: PHYS-E0551 Low Temperature Physics Basics of Cryoengineering Course 2015: 18.9. 4.12. Introduction Short history of cryogenics Some phase diagrams Cryogenic fluids Safety measures 1 Three courses under

More information

April Schafroth s bosons? 2. BCS paired electrons? 3. Lattice Bosons?! -- new paradigm of metallic conductivity

April Schafroth s bosons? 2. BCS paired electrons? 3. Lattice Bosons?! -- new paradigm of metallic conductivity April 2011 1. Schafroth s bosons? 2. BCS paired electrons? 3. Lattice Bosons?! -- new paradigm of metallic conductivity Energy transport solar cells nuclear energy wind energy 15% of electric power is

More information

A Mixture of Bose and Fermi Superfluids. C. Salomon

A Mixture of Bose and Fermi Superfluids. C. Salomon A Mixture of Bose and Fermi Superfluids C. Salomon INT workshop Frontiers in quantum simulation with cold atoms University of Washington, April 2, 2015 The ENS Fermi Gas Team F. Chevy, Y. Castin, F. Werner,

More information

1 Superfluidity and Bose Einstein Condensate

1 Superfluidity and Bose Einstein Condensate Physics 223b Lecture 4 Caltech, 04/11/18 1 Superfluidity and Bose Einstein Condensate 1.6 Superfluid phase: topological defect Besides such smooth gapless excitations, superfluid can also support a very

More information

Quantum Theory of Matter

Quantum Theory of Matter Quantum Theory of Matter Overview Lecture Derek Lee Imperial College London January 2007 Outline 1 Course content Introduction Superfluids Superconductors 2 Course Plan Resources Outline 1 Course content

More information

We already came across a form of indistinguishably in the canonical partition function: V N Q =

We already came across a form of indistinguishably in the canonical partition function: V N Q = Bosons en fermions Indistinguishability We already came across a form of indistinguishably in the canonical partition function: for distinguishable particles Q = Λ 3N βe p r, r 2,..., r N ))dτ dτ 2...

More information

Physics Nov Bose-Einstein Gases

Physics Nov Bose-Einstein Gases Physics 3 3-Nov-24 8- Bose-Einstein Gases An amazing thing happens if we consider a gas of non-interacting bosons. For sufficiently low temperatures, essentially all the particles are in the same state

More information

Quantum Gases. Subhadeep Gupta. UW REU Seminar, 11 July 2011

Quantum Gases. Subhadeep Gupta. UW REU Seminar, 11 July 2011 Quantum Gases Subhadeep Gupta UW REU Seminar, 11 July 2011 Ultracold Atoms, Mixtures, and Molecules Subhadeep Gupta UW REU Seminar, 11 July 2011 Ultracold Atoms High sensitivity (large signal to noise,

More information

Many-Body Problems and Quantum Field Theory

Many-Body Problems and Quantum Field Theory Philippe A. Martin Francois Rothen Many-Body Problems and Quantum Field Theory An Introduction Translated by Steven Goldfarb, Andrew Jordan and Samuel Leach Second Edition With 102 Figures, 7 Tables and

More information

The XY model, the Bose Einstein Condensation and Superfluidity in 2d (I)

The XY model, the Bose Einstein Condensation and Superfluidity in 2d (I) The XY model, the Bose Einstein Condensation and Superfluidity in 2d (I) B.V. COSTA UFMG BRAZIL LABORATORY FOR SIMULATION IN PHYSICS A Guide to Monte Carlo Simulations in Statistical Physics by Landau

More information

BCS everywhere else: from Atoms and Nuclei to the Cosmos. Gordon Baym University of Illinois

BCS everywhere else: from Atoms and Nuclei to the Cosmos. Gordon Baym University of Illinois BCS everywhere else: from Atoms and Nuclei to the Cosmos Gordon Baym University of Illinois October 13, 2007 Wide applications of BCS beyond laboratory superconductors Pairing of nucleons in nuclei Neutron

More information

Superconductivity and Superfluidity

Superconductivity and Superfluidity Superconductivity and Superfluidity Contemporary physics, Spring 2015 Partially from: Kazimierz Conder Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland Resistivity

More information

Ultracold Fermi and Bose Gases and Spinless Bose Charged Sound Particles

Ultracold Fermi and Bose Gases and Spinless Bose Charged Sound Particles October, 011 PROGRESS IN PHYSICS olume 4 Ultracold Fermi Bose Gases Spinless Bose Charged Sound Particles ahan N. Minasyan alentin N. Samoylov Scientific Center of Applied Research, JINR, Dubna, 141980,

More information

Non Classical Rotational Inertia in Two Dimensional 4 He Solid on Graphite

Non Classical Rotational Inertia in Two Dimensional 4 He Solid on Graphite Non Classical Rotational Inertia in Two Dimensional 4 He Solid on Graphite Yoshiyuki Shibayama Department of Physics, Keio University Collaborators Hiroshi Fukuyama The University of Tokyo Keiya Shirahama

More information

Problems with/failures of QM

Problems with/failures of QM CM fails to describe macroscopic quantum phenomena. Phenomena where microscopic properties carry over into macroscopic world: superfluidity Helium flows without friction at sufficiently low temperature.

More information

What are we going to talk about: BEC and Nonlinear Atom Optics

What are we going to talk about: BEC and Nonlinear Atom Optics What are we going to talk about: BEC and Nonlinear Atom Optics Nobel Prize Winners E. A. Cornell 1961JILA and NIST Boulder, Co, USA W. Ketterle C. E. Wieman 19571951MIT, JILA and UC, Cambridge.M Boulder,

More information

Fermi-Dirac and Bose-Einstein

Fermi-Dirac and Bose-Einstein Fermi-Dirac and Bose-Einstein Beg. chap. 6 and chap. 7 of K &K Quantum Gases Fermions, Bosons Partition functions and distributions Density of states Non relativistic Relativistic Classical Limit Fermi

More information

Physics 107 Final Exam May 6, Your Name: 1. Questions

Physics 107 Final Exam May 6, Your Name: 1. Questions Physics 107 Final Exam May 6, 1996 Your Name: 1. Questions 1. 9. 17. 5.. 10. 18. 6. 3. 11. 19. 7. 4. 1. 0. 8. 5. 13. 1. 9. 6. 14.. 30. 7. 15. 3. 8. 16. 4.. Problems 1. 4. 7. 10. 13.. 5. 8. 11. 14. 3. 6.

More information

Modern Physics for Scientists and Engineers International Edition, 4th Edition

Modern Physics for Scientists and Engineers International Edition, 4th Edition Modern Physics for Scientists and Engineers International Edition, 4th Edition http://optics.hanyang.ac.kr/~shsong 1. THE BIRTH OF MODERN PHYSICS 2. SPECIAL THEORY OF RELATIVITY 3. THE EXPERIMENTAL BASIS

More information

CHAPTER 9 Statistical Physics

CHAPTER 9 Statistical Physics CHAPTER 9 Statistical Physics 9.1 9.2 9.3 9.4 9.5 9.6 9.7 Historical Overview Maxwell Velocity Distribution Equipartition Theorem Maxwell Speed Distribution Classical and Quantum Statistics Fermi-Dirac

More information

ICAP Summer School, Paris, Three lectures on quantum gases. Wolfgang Ketterle, MIT

ICAP Summer School, Paris, Three lectures on quantum gases. Wolfgang Ketterle, MIT ICAP Summer School, Paris, 2012 Three lectures on quantum gases Wolfgang Ketterle, MIT Cold fermions Reference for most of this talk: W. Ketterle and M. W. Zwierlein: Making, probing and understanding

More information

Ytterbium quantum gases in Florence

Ytterbium quantum gases in Florence Ytterbium quantum gases in Florence Leonardo Fallani University of Florence & LENS Credits Marco Mancini Giacomo Cappellini Guido Pagano Florian Schäfer Jacopo Catani Leonardo Fallani Massimo Inguscio

More information

From Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules.

From Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules. Today From Last Time Important new Quantum Mechanical Concepts Indistinguishability: Symmetries of the wavefunction: Symmetric and Antisymmetric Pauli exclusion principle: only one fermion per state Spin

More information

Superfluid Helium-3: From very low Temperatures to the Big Bang

Superfluid Helium-3: From very low Temperatures to the Big Bang Superfluid Helium-3: From very low Temperatures to the Big Bang Universität Frankfurt; May 30, 2007 Dieter Vollhardt Contents: The quantum liquids 3 He and 4 He Superfluid phases of 3 He Broken symmetries

More information

Lecture 19: Building Atoms and Molecules

Lecture 19: Building Atoms and Molecules Lecture 19: Building Atoms and Molecules +e r n = 3 n = 2 n = 1 +e +e r ψ even Lecture 19, p 1 Today Nuclear Magnetic Resonance Using RF photons to drive transitions between nuclear spin orientations in

More information

CHAPTER 1 Matter in our Surroundings CONCEPT DETAILS

CHAPTER 1 Matter in our Surroundings CONCEPT DETAILS CHAPTER 1 Matter in our Surroundings CONCEPT DETAILS KEY CONCEPTS : [ *rating as per the significance of concept] 1. Particle nature of Matter *** 2. States of Matter **** 3. Interchange in states of Matter

More information

HW posted on web page HW10: Chap 14 Concept 8,20,24,26 Prob. 4,8. From Last Time

HW posted on web page HW10: Chap 14 Concept 8,20,24,26 Prob. 4,8. From Last Time HW posted on web page HW10: Chap 14 Concept 8,20,24,26 Prob. 4,8 From Last Time Philosophical effects in quantum mechanics Interpretation of the wave function: Calculation using the basic premises of quantum

More information

Bose-Einstein condensates in optical lattices

Bose-Einstein condensates in optical lattices Bose-Einstein condensates in optical lattices Creating number squeezed states of atoms Matthew Davis University of Queensland p.1 Overview What is a BEC? What is an optical lattice? What happens to a BEC

More information

Strongly Correlated Systems:

Strongly Correlated Systems: M.N.Kiselev Strongly Correlated Systems: High Temperature Superconductors Heavy Fermion Compounds Organic materials 1 Strongly Correlated Systems: High Temperature Superconductors 2 Superconductivity:

More information

Fermi gas model. Introduction to Nuclear Science. Simon Fraser University Spring NUCS 342 February 2, 2011

Fermi gas model. Introduction to Nuclear Science. Simon Fraser University Spring NUCS 342 February 2, 2011 Fermi gas model Introduction to Nuclear Science Simon Fraser University Spring 2011 NUCS 342 February 2, 2011 NUCS 342 (Lecture 9) February 2, 2011 1 / 34 Outline 1 Bosons and fermions NUCS 342 (Lecture

More information

Bose-Einstein condensation of lithium molecules and studies of a strongly interacting Fermi gas

Bose-Einstein condensation of lithium molecules and studies of a strongly interacting Fermi gas Bose-Einstein condensation of lithium molecules and studies of a strongly interacting Fermi gas Wolfgang Ketterle Massachusetts Institute of Technology MIT-Harvard Center for Ultracold Atoms 3/4/04 Workshop

More information

STATES OF MATTER NOTES..

STATES OF MATTER NOTES.. STATES OF MATTER NOTES.. While you are reading, answer the following which will help you with the States of Matter Project. What is matter (definition): What are the states of matter and what are the characteristics/properties

More information

Physics Nov Cooling by Expansion

Physics Nov Cooling by Expansion Physics 301 19-Nov-2004 25-1 Cooling by Expansion Now we re going to change the subject and consider the techniques used to get really cold temperatures. Of course, the best way to learn about these techniques

More information

Helium. Characteristics of a cryogenic fluid. Name that man. Spelling Bee

Helium. Characteristics of a cryogenic fluid. Name that man. Spelling Bee Characteristics of a cryogenic fluid Critical, normal boiling, and triple point temperatures of cryogenic fluids 1. Critical, normal boiling, and triple point temperatures of cryogenic fluids. Vapor pressure

More information

Please read the following instructions:

Please read the following instructions: MIDTERM #1 PHYS 33 (MODERN PHYSICS II) DATE/TIME: February 16, 17 (8:3 a.m. - 9:45 a.m.) PLACE: RB 11 Only non-programmable calculators are allowed. Name: ID: Please read the following instructions: This

More information

Directions of Basic Research in Quantum Matter

Directions of Basic Research in Quantum Matter Brief Heirarchical view of physics Where to look for new phases of condensed matter? Outline Directions of Basic Research in Quantum Sciences Ben Simons Cavendish Laboratory Brief Heirarchical view of

More information

BCS-BEC Crossover. Hauptseminar: Physik der kalten Gase Robin Wanke

BCS-BEC Crossover. Hauptseminar: Physik der kalten Gase Robin Wanke BCS-BEC Crossover Hauptseminar: Physik der kalten Gase Robin Wanke Outline Motivation Cold fermions BCS-Theory Gap equation Feshbach resonance Pairing BEC of molecules BCS-BEC-crossover Conclusion 2 Motivation

More information

Introduction. Chapter The Purpose of Statistical Mechanics

Introduction. Chapter The Purpose of Statistical Mechanics Chapter 1 Introduction 1.1 The Purpose of Statistical Mechanics Statistical Mechanics is the mechanics developed to treat a collection of a large number of atoms or particles. Such a collection is, for

More information

Physics 127a: Class Notes

Physics 127a: Class Notes Physics 7a: Class Notes Lecture 4: Bose Condensation Ideal Bose Gas We consider an gas of ideal, spinless Bosons in three dimensions. The grand potential (T,µ,V) is given by kt = V y / ln( ze y )dy, ()

More information

Superfluidity in interacting Fermi gases

Superfluidity in interacting Fermi gases Superfluidity in interacting Fermi gases Quantum many-body system in attractive interaction Molecular condensate BEC Cooper pairs BCS Thomas Bourdel, J. Cubizolles, L. Khaykovich, J. Zhang, S. Kokkelmans,

More information

NanoKelvin Quantum Engineering

NanoKelvin Quantum Engineering NanoKelvin Quantum Engineering Few x 10 5 Yb atoms 250mm 400 nk 250 nk < 200 nk Control of atomic c.m. position and momentum. Today: Bose-Fermi double superfluid Precision BEC interferometry Ultracold

More information

Energy Levels Zero energy. From Last Time Molecules. Today. n- and p-type semiconductors. Energy Levels in a Metal. Junctions

Energy Levels Zero energy. From Last Time Molecules. Today. n- and p-type semiconductors. Energy Levels in a Metal. Junctions Today From Last Time Molecules Symmetric and anti-symmetric wave functions Lightly higher and lower energy levels More atoms more energy levels Conductors, insulators and semiconductors Conductors and

More information