10 pages digest of the works at basel 2014-2015
TRANSCRIPT
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Kouki Nakata
University of Basel Switzerland
Magnon Transport Theory
All the responsibility of this slide rests with `Kouki Nakata' (2016)
10 pages digest of the works at Basel 2014-2015
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Yes !
[Phys. Rev. B 90, 144419 (2014)] [Phys. Rev. B 92, 014422 (2015)] [Phys. Rev. B 92, 134425 (2015)]
We have established it: Magnon counterpart of electron transport
Q. Can we control magnon transport 𝝁𝑩 like electrons 𝒆 ?
FINAL GOAL Establish valid methods to control magnon transport 𝝁𝐁
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Charge transport 𝑒 Magnon transport 𝜇B
Wiedemann-Franz (WF) law [R. Franz and G. Wiedemann,
Annalen der Physik 165, 497 (1853)]
Thermoelectric property
Magnon Wiedemann-Franz law [K. Nakata et al., Phys. Rev. B 92, 134425 (2015)]
Thermomagnetic property
Superconducting state [H. K. Onnes (1911)]
Persistent charge current [M. Buttiker et al. Phys. Lett. A, 96, 365 (1983)]
Magnon-BEC [S. O. Demokritov et al., Nature 443, 430 (2006)]
Persistent magnon-BEC current [K. Nakata et al., Phys. Rev. B 90, 144419 (2014)]
Josephson effect [B. D. Josephson, Phys. Lett. 1, 251 (1962)]
Magnon Josephson effect [K. Nakata et al., Phys. Rev. B 90, 144419 (2014)]
Quantum Hall effect [K. v. Klitzing et al., Phys. Rev. Lett. 45, 494 (1980)]
Magnon quantum Hall effect [K. Nakata & D. Loss, to be submitted (2016)]
Find the counterpart !!
Guiding Principle
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Magnon Wiedemann-Franz Law
VS
(Free electron at low temp.) Low temp.:
Electron (metal) Magnon (FI)
R. Franz and G. Wiedemann [Annalen der Physik 165, 497 (1853)]
K. Nakata and D. Loss [Phys. Rev. B 92, 134425 (2015)]
Fermion Boson Statistics
Lorenz number
WF law (Low temp.)
𝑇-linear behavior = Universal
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1853
[R. Franz and G. Wiedemann, Annalen der Physik 165, 497 (1853)]
Wiedemann-Franz Law for Electron Transport in Metal
Wiedemann-Franz Law for Magnon Transport in FI [K. Nakata and D. Loss, Phys. Rev. B 92, 134425 (2015)]
2015
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Experiment [S. O. Demokritov et al., Nature 443, 430 (2006)]
Quasi-equilibrium Magnon-BEC
Experimental result by [A. A. Serga et al., Nat. commun. 5, 3452 (2014)]
Microwave pumping: Room temperature
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Magnon VS Magnon-BEC
Incoherent spin precession Macroscopic coherent spin precession Macroscopic spins
= Sum of variety kinds of modes Macroscopic number of magnons occupies a single state
Quasi-equilibrium condensation
Part I: Magnon Part II: Magnon-BEC
= Spin-wave ~ Superconducting state of spin-wave
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dc ac : Josephson effect
BEC
BEC
Magnetic field difference:
Part II: Condensed magnon (BEC) Part I: Non-condensed magnon
ac/dc Properties
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J J J
J
J
J
J J
BEC
Magnon-BEC Ring Analogous to superconducting ring
A-C phase Persistent magnon-BEC current
E (A-C phase)
(Note; as long as magnons are in condensation)
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Non-condensed magnon
Cylindrical wire
Condensed magnon
(1) Magnetic current (2) (3)
𝜇B
𝑉m 𝐼m
Electromagnetism by Magnon Current
[D. Loss and P. M. Goldbart, Phys. Lett. A 215, 197 (1996)] [F. Meier and D. Loss, Phys. Rev. Lett. 90, 167204 (2003)]
(Flow of magnetic dipole)
𝐸m
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Magnon Transport Ferromagnetic Insulator
Universal thermomagnetic relation Magnon Seebeck & Peltier effects
III. Measurement II. Magnon-BEC Berry phase Josephson & persistent currents
Electromagnetic control Direct detection
I. Wiedemann-Franz Law for Magnon in FI
SUMMARY
[Phys. Rev. B 90, 144419 (2014)] [Phys. Rev. B 92, 014422 (2015)] [Phys. Rev. B 92, 134425 (2015)]
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Supplemental Material
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Appendix: Part I
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Magnon & Heat Currents
Magnon current
Heat current
: Magnon lifetime (phenomenologically introduced)
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Onsager relation:
Integrating over
Linear response:
Magnon & Heat Currents
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Onsager Matrix Magnon current
Heat current
Onsager coefficient
Onsager relation
Polylogarithm function:
Exponential integral: Euler constant:
Cross-section area of the junction interface:
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Thermal Conductance 𝑲 for Boson
Note: Definition of thermal conductance
with
WF law
Magnon current Heat current
Magnetic conductance: 𝑮
Thermal conductance: 𝑲
for fermions
for bosons (magnons)
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Thermo-electric & –magnetic Effects VS
(Free electron at low temp.) Low temp.:
Electron (metal) Magnon (FI)
R. Franz and G. Wiedemann [Annalen der Physik 165, 497 (1853)]
K. Nakata, P. Simon, and D. Loss [Phys. Rev. B 92, 134425 (2015)]
Fermion Boson Statistics
Onsager relation
Thomson relation
Seebeck & Peltier
Lorenz number
WF law (Low temp.)
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REMARK There was a possibility at low temp.:
Magnon WF law in FI:
𝐾
𝐺= (
𝑘B
𝑔𝜇B)2𝑇 ∙
𝑘B𝑇
𝑔𝜇B𝐵
𝑛−1
∝ 𝑇𝑛
𝐾
𝐺= (
𝑘B
𝑔𝜇B)2𝑇 ∝ 𝑇
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Anisotropic spin 𝜂 ≠ 1 Magnon-magnon interactions
At such low temperatures: Phonon contributions are negligibly small
WF law & Onsager relations: Broken
Contributions of the breakings: Negligibly small at low temperatures 𝒪(10−1)K
WF law & Onsager relations: Approximately satisfied at such low temperatures [Note: Originally (𝜂 = 1), the WF law is realized at such low temperatures]
Broken Relations & Low Temperature
[H. Adachi et al., Appl. Phys. Lett. 97, 252506 (2010)]
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Magnon VS Magnon-BEC
Incoherent spin precession Macroscopic coherent spin precession = Macroscopic spins
= Sum of variety kinds of modes = Macroscopic number of magnons occupies a single state
Quasi-equilibrium condensation
Number density: Number density:
Part I: Magnon Part II: Magnon-BEC
= Spin-wave ~ Superconducting state of spin-wave
Cooper pair: 𝑐𝒌↑𝑐−𝒌↓ BCS ≠ 0
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Appendix: Part II
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Microwave pumping Non-equilibrium steady state
Quasi-equilibrium magnon-BEC = [Metastable state]
≠ [Ground state]
Thermalization
Microwave: Switched off
FMR
B B
Quasi-equilibrium magnon-BEC
[C. D. Batista et al., Rev. Mod. Phys., 86, 563 (2014)]
= Dynamical condensation ≠ Thermal condensation
U(1)-symmetry: Broken U(1)-symmetry: Recovered
Quasi-equilibrium Magnon-BEC
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Quasi-equilibrium Magnon-BEC [C. D. Batista et al., Rev. Mod. Phys., 86, 563 (2014)]
= Dynamical condensation ≠ Thermal condensation
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Magnon-BEC Order Parameter [Textbook by Leggett] BEC: Einstein for free particles (i.e., no interactions)
Single-particle density matrix
𝜌1(𝒓, 𝒓′; 𝑡);
Probability amplitude 𝜌1(𝒓, 𝒓′; 𝑡) ≡ 𝜓 +(𝒓𝑡)𝜓(𝒓′𝑡)
(𝜓: Bose field)
Single eigenvalue Single BEC Several eigenvalues Fragmented BEC
Penrose & Onsager (1956)
lim𝒓−𝒓′→∞
𝜌1 𝒓, 𝒓′; 𝑡 = Ψ∗ 𝒓𝑡 Ψ (𝒓′𝑡)
Ψ(𝒓𝑡) ≡ 𝜓 (𝒓𝑡) : BEC order parameter = Off-diagonal long-range order (ODLRO) Widely used in BEC community
Yang (1962)
Extension of definition including interactions
Quasi-equilibrium magnon-BEC by microwave pumping satisfies this condition Experiment [S. O. Demokritov et al., Nature 443, 430 (2006)]
Quantum ? OR Classical ? [A. Ruckriegel and P. Kopietz, PRL 115, 157203 (2015)]
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Magnetic field difference:
Period of ac Josephson effect:
Parameter values:
Josephson current:
Josephson magnon current:
Adjusting parameters:
10 ns
ac Josephson Effect
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ac Josephson Effect: Nonlinear Effect
Magnon Josephson Eq.:
Josephson current:
Time-evolution of phase:
Nonlinear effect: 𝑧(0) ≠ 0 & Δ𝐵 = 0 ac Josephson effect Period 𝑇~10ns at weak 𝐽ex
Nonlinear effect
Linear effect
Experimental reach 1T/cm: Linear effect ≪ Nonlinear effect
Period 𝑻 of ac Josephson effect:
e.g.:
Within experimental reach
𝑧 0 = 0.6
Initial population imbalance:
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dc Josephson Effect
Electric field Magnetic field
No A-C phase A-C phase
Electromagnetically realizable by applying an increasing magnetic field:
: dc effect ? : dc effect
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Macroscopic Quantum Self-Trapping
MQST
(a)
(b)-(d)
MQST occurs when
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``Direct Observation of Tunneling and Nonlinear Self-Trapping in a Single Bosonic Josephson Junction’’ [M. Albiez et al., PRL 95, 010402 (2005)]
MQST in Cold Atoms Already experimentally observed [M. Albiez et al., PRL 95, 010402 (2005)]
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time (p = 50)
Destabilized deviation: 1/p << 1
Stable
Magnon-BEC Ring
Quantization:
time
1/p
1
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Device for Direct Measurement To detect persistent quantized magnon-BEC current in the ring
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Appendix: Others
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3-dim Cubic Ferromagnet
Holstein-Primakoff (H-P) transformation
Heisenberg spin model:
Standard textbook [K. Kubo] on magnetism tells us:
Fourier transformation:
Parabolic dispersion: → 0 (𝑘 → 0)
Magnon = A kind of Nambu-Goldstone mode
= Massless particle = Non-relativistic magnon
𝜔𝑘
𝑘
Picture from google search
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d-dim Cubic Anti-Ferromagnet (d≥3)
Bogoliubov transformation New Magnon Operators: 𝛼 & 𝛽
Diagonalization:
Linear dispersion: Relativistic magnon = Dirac magnon on d-dim AF
𝑘
𝜔𝑘
Standard textbook [K. Kubo] on magnetism tells us:
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Nambu-Goldstone (NG) Theorem Magnon = A kind of NG mode (particle)
A continuous symmetry is spontaneously broken (SSB) Massless particles = NG boson
Heisenberg model: SSB of SO(3) Magnon = NG mode
B
A
A B
Magnon
[TEXTBOOK by Peskin]
``Rough & intuitive’’ correspondence
(massless)
Picture from wiki.
Picture from Google search
The relation between [# of broken symmetries] & [# of NG particles]: See [Watanabe-Murayama] & [Hidaka]
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Mermin–Wagner–Hohenberg-Coleman theorem:
Continuous symmetries cannot be spontaneously broken (NO SSB):
- 𝑑 ≤ 2 - At finite temperature - Sufficiently short-range interactions
Absence of NG particles (e.g. magnons) on 𝑑 ≤ 2
Why 3-dim ?
See also recent development: [Phys. Rev. Lett. 107, 107201 (2011)] D. Loss, F. L. Pedrocchi, and A. J. Leggett
NOTE: The absence of SSB is valid only in the thermodynamic limit Ordering in finite size at finite temperatures is possible
Picture from Google search
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Lattice structure
Band structure
Dirac Magnon on 2-dim Honeycomb Lattice
Magnon Dirac Eq.
[arXiv:1512.04902] J. Fransson, A. M. Black-Schaffer, and A. V. Balatsky
Dirac Magnon
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AF Dirac Magnon
Dirac magnons are inherent to honeycomb lattice (geometric properties): Ferro or AF does not matter
In sharp contrast to cubic lattice
Ferromagnet Anti-ferromagnet
3-dim cubic lattice Since 1930
𝜔𝑘 ∝ 𝑘2 Non-relativistic
𝜔𝑘 ∝ 𝑘 Relativistic
2-dim honeycomb lattice [arXiv:1512.04902]
𝜔𝑘 ∝ 𝑘 Relativistic
𝜔𝑘 ∝ 𝑘 Relativistic
[arXiv:1512.04902] J. Fransson, A. M. Black-Schaffer, and A. V. Balatsky