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Helium-4: The Once and Future Supersolid

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... Normal-Supersolid transition accompanied by Commensurate-incommensurate transition Change in local density profile Dai Xi, ... class first order ... rotational ... – PowerPoint PPT presentation

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Title: Helium-4: The Once and Future Supersolid


1
Helium-4The Once and Future Supersolid
  • Michael Ma
  • University of Cincinnati

Hong Kong Forum, 2006
2
Supersolid Solid with Superfluid Properties
Introduction Solids - Quantum or Otherwise
3
Supersolid Solid with Superfluid Properties
Introduction Solids - Quantum or
Otherwise Living in the Past This is the
Moment Days of Future Passed
4
Classical Solid
  • Static density

5
  • ??gaussian like
  • harmonic approximation valid
  • ltu2gt1/2 ltlt a
  • Lindemanns Rule Melts when ltu2gt1/2 0.14a
  • Particles are localized.

6
Quantum Solid
He4 Shallow potential well light mass
large zero point motion
7
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8
Quantum Solid
conventional solid
He4
9
  • Lindemanns Rule does not hold
  • ltu2gt 0.3 a, pressure dependent
  • Short-ranged correlations important
  • Deviation of density from gaussian
  • strong anharmonicity
  • Solid caused by steep repulsive core
  • Particle exchange

Nosanow
10
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11
  • Two-particle exchange not favored due to
    repulsive core
  • Three and Four particle ring exchange
  • Jex mK, Debye T 25 K

12
  • Lindemanns Rule does not hold
  • ltu2gt 0.3 a, pressure dependent
  • Short-ranged correlations important
  • Deviation of density from gaussian
  • strong anharmonicity
  • Solid caused by steep repulsive core
  • Particle exchange

Nosanow
13
  • Intriguing possibility
  • but atoms mobile
  • mobile atoms (bosons) can Bose condense
  • exhibit superfluidity

14
Bose-Einstein condensation - Non-interacting
bosons at low T, n0/N O(1)
  • Bose condensation / Off-diagonal long range order
  • Generalization to interacting bosons by Penrose
    and Onsager
  • Further generalization by Yang as ODLRO
  • Largest eigenvalue of the density matrix O(N)
  • - Applicable for non-translational invariant
    system also
  • Superfluidity
  • zero resistance flow
  • irrotational flow
  • ODLRO sufficient condition for superfluidity

15
PAST
16
A quantum solid may Bose condense and be a
supersolid!
  • Microscopic ring exhange may lead to macroscopic
    exchange
  • Andreev and Lifshitz - quantum fluctuations
  • may favor finite density of vacancies even at
    T0.
  • Vacancies are mobile and can Bose condense.
  • Chester - Jastrow wavefunctions generally have
    ODLRO,
  • including ones describing solid order.
    Speculate due to vacancy
  • condensation.
  • Leggett - Supersolid exhibits non-classical
    rotational inertia.
  • Provided expression for upper bound.

17
Andreev-Lifshitz
  • Vacancy motion is diffusive at high T due to
    scattering off phonons
  • Wave-like at low T --gt tight binding band
  • Delocalization energy may overcome local
    activation E
  • Vacancies spontaneously generated
  • Bose condense at low T

18
Chester
  • Jastrow wavefuntion generically
    has ODLRO (Reatto)
  • Write and
    consider
  • as partition function of a classical system at
    temp Teff
  • Transition from liquid to solid with increasing
    density
  • solid will have ODLRO
  • postulate due to BC of vacancies.

19
Irrotational Flow Meissner Effect
Lab frame
Rotating frame
?
H H - ?L
H
v p/m - A A ? x r
v p/m
  • Meissner effect gt v lt ?r
  • gtmoment of inertia I lt I0
  • Non-classical Rotational Inertia (NCRI)
  • ?I/I0 ?s/?
  • ??I can be measured very accurately from resonant
    frequency

20
For 30years, expt search overwhelmingly negative
Meisel. Physica
21
Expt gt vacancies activated
X-ray data Simmons
data fit to c(T) exp -(f/kT)
Ev 10 K
22
Present
23
Kim and Chan, Science 2004
Detection of NCRI of solid He4 in torsional
oscillator
24
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25
  • Effect goes away if He4 replaced by He3
  • Effect significantly reduced if annulus blocked
  • NCRI also observed by
  • Shirahama group at Keio U
  • Kubota group at U of Tokyo
  • Rittner and Reppy (Cornell)

26
  • Effect goes away if He4 replaced by He3
  • Effect significantly reduced if annulus blocked
  • NCRI also observed by
  • Shirahama group at Keio U
  • Kubota group at U of Tokyo
  • Rittner and Reppy (Cornell)
  • NCRI disappears upon annealing
  • Cubic cell

27
Still No Evidence for Infinite Conductivity
  • Day and Beamish
  • No pressure driven flow
  • vc lt 10-14 m/s
  • Sasaki et al
  • No observed flow
  • without grain boundaries

28
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29
Kim and Chan
Critical velocity single quantum of circulation
30
He3 dependence
31
He3 dependence
32
Bulk EquilBm Supersolid?
  • Pro
  • Phase coherence
  • NCRI does not anneal to 0
  • No difference between bulk and vycor
  • ?s increases with Xtal quality
  • specific heat anomaly
  • Con
  • no evidence of zero resistance
  • NCRI may anneal to 0
  • ?s temp dependence
  • He3 impurities effects
  • geometry dependence
  • tiny entropy, 10-6 kB/He4

33
Commensurate vs. Incommensurate Supersolid
filling
Incomm. SS
MI
Commensurate SS
x
1
KE
Incomm SS
34
Commensurate SS
  • Pro
  • Galli and Reatto
  • (Variational SW)
  • Con
  • Ceperley and Bernu (Ring Exchange)
  • Boninsegni et al (Worm Algorithm)
  • Prokofev and Svistunov (Proof)

35
Incommensurate SS
  • If incommensurate gt SS (Galli and Reatto)
  • Anderson-Brinkman-Huse
  • T7 correction to CV
  • gt ?n T4
  • Commensurate solid metastable

But T7 can be due to anharmonic effect
36
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37
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38
local distortion of lattice and density vacancy
hopping given by (heavy) polaron mass attraction
between vacancies (Troyer)
39
Dai Xi, FCZ, MM HuaiBin Zhuang
  • With finite vacancy density, distortion can be
    static and uniform
  • vacancies have light mass
  • Bose condensation energy can overcome
    activation energy
  • First order transition
  • At T0, nv 0 in normal solid
  • finite in supersolid
  • Normal-Supersolid transition accompanied by
  • Commensurate-incommensurate transition
  • Change in local density profile

40
Change in Local Density Profile
?(r)
?(r)
Supersolid
Normal Solid
41
Qualitative Agreement with Penn State Expts
42
Pressure Dependence of T0 Superfluid Density
43
Finite T Superfluid Density
Finite T
  • data suggests transiton
  • smeared by disorder
  • specific heat shows no
  • critical behavior
  • Two possibilities for pure system
  • second order transition not in X-Y universality
    class
  • first order transition

Transition is first order in our model
44
He3 Impurities
  • Expt, with increasing He3 concentration
  • Tc increases
  • low T ?s decreases
  • NCRI not observeable beyond 0.1 He3
    concentration
  • Qualitative agreement
  • Impurties weaken solid ordering and favors
    defects
  • gt Tc increases
  • Impurities localize vacancies
  • gt reduce ?s and eventually destroys Bose
    condensation
  • (dirty bosons)

45
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46
Future
Is it or isnt it? Smoking gun?
If helium is not SS, is there a deeper reason
than energetics?
47
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48
Thank You!
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