klaus richter’s group complex quantum systems, universität ......transport mechanism: elastic...
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THERMOELECTRIC CONVERSION IN DISORDERED NANOWIRES
Complex Quantum Systems, Universität Regensburg
Cosimo Gorini
Mainz, 28 / 01 / 2016 | PAGE 1
Klaus Richter’s group
1-slidehystory ofthermoelectricity
q Thepioneers:Volta(1794),Seebeck (1821),Peltier (1834),Joule(1843),Thomson(1851;later LordKelvin).
q Theoretical formalisation:Onsager (1931).
q Thegolden age:ca.1930– 1960(Ioffe).
q Therebirth:1990’s(Hicks &Dresselhaus).
q Today:energy efficiency concerns.| PAGE 2
Thermoelectric effects: simultaneous charge & energy/heat flows
Siberia can listen to Stalin’s radio (USSR, 1948)Nanostructuration
Thermoelectricity:Rulesofthegame
HOT COLDelectrons
| PAGE 3
J1 = charge current
J2 = heat currentL i j = linear transport
coefficients
Seebeck(thermopower) Figure of merit
Max efficiencyCarnot efficiency Curzon-Ahlborn limit
Efficiency at max power
Thermoelectricity:Rulesofthegame
HOT COLDelectrons
Thermopower(orSeebeck coeff.):
Maximizetheefficiency i.e.thefigureofmerit:
…keepingareasonableelectricaloutputpower(powerfactor):
| PAGE 4
“… fundamental scientific challenges could be overcome by deeper understanding of charge and heat transport”
“… a newly emerging field of low-dimensional thermoelectricity, enabled by materials nanoscience and nanotechnology”
Dresselhaus et al: Adv. Mater. 2007
Majumdar: Science 2004
Whysemiconductornanowires?
SC nanowires
Reduced thermal conductancePhonon vs electrons mean free path, geometrical designs(Hochbaum 2008, Heron 2010)
Enhanced thermopowerField effect transistors (Brovman 2013, Roddaro 2013 & many others)
Scalable output powerArrays of parallel NWs (Pregl 2013, Stranz 2013)
| PAGE 5
Someexperimentalrealizations
Karg et al. (IBM Zurich), 2013
Fan et al. (Berkeley CA), 2008
Shin et al. (Seoul), 2011
Hochbaum et al. (Berkeley CA), 2008
Pregl et al. (TU Dresden), 2013
However à Imbalance between experimental / theoretical works !| PAGE 6
Outline
q Nanowires intheFieldEffect TransistorconfigurationThe1DAndersonModel
q Thermopower ofsingleNW:low Telastic regimeq Thermopower ofsingleNW:inelasticphonon-assisted regimeq Parallel nanowires:scalable power factor andhotspotcoolingq 3-Terminalthermoelectric ratchet (``all-in-one thermocouple’’)
q Conclusions andprospects| PAGE 7
Aller à l’idéal et comprendre le réel.
Jean Jaurès
Field-EffectTransistors(FET)
• Single (or array of) doped nanowire(s) in the FET configuration
• Substrate: Electrically and thermally insulating
• Gate: «back» or «top»
• Heater: for thermoelectric measurements
"Seebeck" configuration: thermal bias
"Peltier" configuration: voltage bias
Π = 𝑆𝑇: equivalent within linear response if time-reversal symmetrypreserved (Kelvin relation)
Goal: effect of gate modulation on the thermopower
Setup used by P. Kim (Columbia) (2013)
| PAGE 8
Vg Impurity band
1DAndersonModel
• 1Delectroniclatticewithon-site(uniform) disorder𝑉' ∈ (-W/2,W/2)
• Allelectronsarelocalizedwithlocalizationlengthξ (E)
• Statesdistributed withinanimpurityband2𝐸+≈4t+W
• Behaviorofthetypicalthermopowerwhenthegatevoltage𝑉, isvaried
µ
E
• Tight-binding Hamiltonian
GateVoltage
2EB
Prototypical model of localized system
| PAGE 9
B.Derrida&E.Gardner,J.Physique45,1283(1984)
"Bulk" formulas:
"Edge" formulas:
Analytical expressionsderived inweakdisorder limit
W=t:bandedge at2t+W/2 2.5t
1Ddensityofstatesν andlocalizationlengthξLocalizationlength
Density
ofstates
| PAGE 10
Outline
ü Nanowires intheFieldEffect TransistorconfigurationThe1DAndersonModel
q Thermopower ofsingleNW:low Telastic regimeq Thermopower ofsingleNW:inelasticphonon-assisted regimeq Parallel Nanowires:scalable power factor andhotspotcoolingq 3-Terminalthermoelectric ratchet
q Conclusions andprospects
| PAGE 11
Elasticregime:Thermopower
LowTemperatures+LinearResponseàMottformula:
Localizedregime:𝜏 decaysexponentiallywithlength
Typical𝜏dependsontheenergy viaξ(E)(localization length)
Theory:
Numerics: RecursiveGreenFunctioncalculationofS
Transportmechanism:elastic(coherent)tunnelling
| PAGE 12
R. Bosisio, G. Fleury, & J.-L. Pichard, New J. Phys. 16:035004 (2014)
Elasticregime:Summary
Enhancement of the thermopower atthe band edges (role of 𝜉(E))
Analytical description of the results
Sommerfeld Expansion (low T)Wiedemann-Franz law à Low S
Very low power factor 𝑄 = 𝐺𝑆4because of the exponential reductionof G at the band edges
Interest: Ultra-low T Peltier cooling?
OR à toward higher temperatures!| PAGE 13
Outline
ü Nanowires intheFieldEffect TransistorconfigurationThe1DAndersonModel
ü Thermopower ofsingleNW:low Telastic regimeq Thermopower ofsingleNW:inelasticphonon-assisted regimeq Parallel Nanowires:scalable power factor andhotspotcoolingq 3-Terminalthermoelectric ratchet
q Conclusions andprospects
| PAGE 14
VariableRangeHopping:TransportMechanism
Mott à competition between tunneling and activated processes
Phonon Bath
kT kTVg
𝛍
ener
gy
position
Variable Range Hopping: phonon-assisted transport à sequence of hopsof variable size
Optimal hop size: Mott hopping length
LM
or Mott hopping energy
i
j
| PAGE 15
TransportMechanisms
Low T:LM>>Là elastic transport
Increasing T: LMLà onset ofinelastic processes (VRH)
Increasing T: LM ξà simple activated transport (NNH)T
Cut-off required by ∆ 𝑇7 = 𝑘+𝑇7 ≤ 2𝐸+
(Ta :onset ofsimple activation in1D(Kurkijärvi 1973,Raikh&Ruzin 1989))
Elastic
VRH
NNH
Mott’s Hopping Energy:finiterange ofstates
contributing totransport
Relevant energy scaleforactivated transport
| PAGE 16
Between leadandlocalized states [Elastic tunnelingrates]
Between localized states[Inelastic hopping rates]
1. Transitionrates(Fermigoldenrule)
Inelastic(Phonon-Assisted)Regime:method
𝛼=L,R
Phonon Bath
𝛍α𝐢
𝐣
Essentialingredients tobuild &solve theRandom Resistor Network
Miller & Abrahams, PR (1960), Ambegaokar, Halperin & Langer PRB (1971), Jiang, Entin-Wohlman & Imry., PRB (2014)
ξ energy dependenceusually neglected!
| PAGE 17
Inelastic(Phonon-Assisted)Regime:method
2.Fermidistributionsatequilibrium (nobias)
3.Occupationprobabilities outofequilibrium
Jiang, Entin-Wohlman & Imry., PRB (2014)
4.Currents
5.Current conservationatevery node i(Kirchoff)Ncoupled equations inNvariables
à 𝛿𝑓'
| PAGE 18
Miller– AbrahamsResistorNetwork
6.Totalparticle/heat currents
7.Transport coefficients
Summing all terms flowingoutfromL(R)terminal
(Having assumed Peltier configuration: T constant everywhere)
Jiang, Entin-Wohlman & Imry., PRB (2014)
Conductance
Peltier coefficient
Thermopower
| PAGE 19
InelasticRegime:Typicalthermopower
Approachingthebandedge(increasingVg)
• Thermopower enhancement when thebandedges areapproached
• Rich behaviour oftheT-dependence ofthethermopower, "reflecting" theshape ofthedensity of statesandlocalization length
S0 vs Temperature
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, New J. Phys. 16:095005 (2014)
Vg=1.5 t
Vg=2.3 t
T-1
| PAGE 20
Inelasticregime:theory
Theory:Percolation approach to solve the RRN:
Ambegaokar, Halperin, Langer à conductance (1971)Zvyaginà thermopower (1973)
thermopower = energy averaged over the percolating path
~𝑇AB:simple activation:energy to «jump»
toward 𝜖E
(inside)
(outside)
~𝑇AB/4:Variable Range Hopping
(Mott)
Integrate between (μ-∆; μ+∆)
| PAGE 21
InelasticRegime:Typicalthermopower
S0 vs Temperature
S0 vs Gate Voltage
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, New J. Phys. 16:095005 (2014)
Electrical Conductance
(inside)
(outside)
| PAGE 22
µ
2∆
InelasticRegime:Mottenergy
Mott’s HoppingEnergy:finiterange ofstates contributing totransport
Sdepends ontheasymmetryofthestates
aroundμwithin[μ-∆, μ+∆]
Integrationinside[μ-∆, μ+∆]
| PAGE 23
Outline
ü Nanowires intheFieldEffect TransistorconfigurationThe1DAndersonModel
ü Thermopower ofsingleNW:low Telastic regimeü Thermopower ofsingleNW:inelasticphonon-assisted regimeq Parallel Nanowires:scalable power factor andhotspotcoolingq 3-Terminalthermoelectric ratchet
q Conclusions andprospects
| PAGE 24
Arraysofparallelnanowires
Suspended Deposited
• Neglect inter-wire hoppingà independent nanowires
• Transport through each NW: VRH / NNH regime (same treatment as before)
Fan et al., 2008Shin et al., 2011
| PAGE 25
Parallelnanowires:powerfactorandfigureofmerit
Rescaled power factor Electronic figure of merit
Scalable Power Factor(without affecting the electronic figure of merit)
Iso-curve S0=2 kB/e
Band edge
Motttemperature
Parameters:
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, Phys. Rev. Applied 3, 054002 (2015)
P μW for 105 NWs (1 cm) and δT10 K| PAGE 26
Parallelnanowires:powerfactorandfigureofmerit
Rescaled power factor Electronic figure of merit
Estimation of the parasitic phononic contribution to ZT
(For doped Si-NWs and SiO2 substrate)
| PAGE 27
Parallelnanowires:HotSpotcooling
Hopping heat current through each localized state i
Ei randomly distributed à Local fluctuations
Λph: inelastic phonon mean free path = thermalization length in the substrate
kT kT
𝛍
| PAGE 28
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, Phys. Rev. Applied 3, 054002 (2015)
Parallelnanowires:HotSpotcooling
Vg=0: band center Vg=2.25 t: band edge
Parameters: (Heat currents in unit of )
Formation of hot and cold spots near the boundaries of the
substrate
Top view of the substrate
| PAGE 29
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, Phys. Rev. Applied 3, 054002 (2015)
Parallelnanowires:HotSpotcooling
Estimation of the cooling power density:
10 W/cm2
at δμ=1mV 7.7 x 10-2 tand T = 75K 0.5t
(still linear response)
Opportunities for heat management in microstructures
E.g.: hot spot cooling in microelectronics: transferring heat some microns away
| PAGE 30
10 μm
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, Phys. Rev. Applied 3, 054002 (2015)
Microprocessors ~ 100 W/cm2
Outline
ü Nanowires intheFieldEffect TransistorconfigurationThe1DAndersonModel
ü Thermopower ofsingleNW:low Telastic regimeü Thermopower ofsingleNW:inelasticphonon-assisted regimeü Parallel Nanowires:scalable power factor andhotspots coolingq 3-Terminalthermoelectric ratchet
q Conclusions andprospects
| PAGE 31
3-Terminalthermoelectricratchet
| PAGE 32
Bosisio, Fleury, Pichard & Gorini, arXiv (2015)
q Microscale heat harvester or coolerq Non – local thermal machine (``all-in-one thermocouple’')q Simple (ideally Si – based)
Sànchez & Büttiker, PRB (2011) à Low T, coherent, feasible but extremely low power
3-Terminalthermoelectricratchet
| PAGE 33
Theend
| PAGE 34
q Variable Range Hopping à inelastic, large window for e-h asymmetry
q Parallel nanowires à high Seebeck AND good power factor Qq Gate-controlled local heat exchanges (hot spots cooling)q 3-Terminal thermoelectric ratchet:
1. Simple setup, energy harvester/cooler2. Good power factor Q and electronic ZT (0.1 - 100)
Riccardo Bosisio Jean-Louis PichardGeneviève Fleury
Aller à l’idéal et comprendre le réel.
Jean Jaurès
Thefuture
Wishlist
• Rigorous treatment of e-ph coupling
• Combining DFT calculations of γe and γep
• Non-linear regime (higher output powers), multi-terminal setups
• Heat-to-spin conversion I: magnetism and/or spin-orbit in wires
• Heat-to-spin conversion II: hot magnon bath
• Time-dependent configurations.
| PAGE 35
InelasticRegime:Thermopower fluctuations
R. Bosisio, C. Gorini, G. Fleury, & J.-L. Pichard, New J. Phys. 16:095005 (2014)
Vg = 0
Vg = 2.2t
Numerical simulationsfor kT=t and W=t
Bulk of the band Band Edge
| PAGE 36
Parallelnanowires:HotSpotcooling
| PAGE 37
ParasiticPhononContributiontoZT
(For doped Si-NWs and SiO2 substrate)
| PAGE 38
Parallelnanowires:addenda
| PAGE 39
DensityofstateswithCoulombgap
∆ ?
| PAGE 40
Thermopower Enhancement:experimentalresults
GroupofPhilipKim(preprint2013)SimilardatainthegroupofF.Giazotto orH.Riel
Largelyenhancedthermopower nearthebandedgeofthenanowire
(Fieldeffect transistordevice configuration)
(ExperimentsmainlycarriedoutatRoomTemperature)| PAGE 41
Linearresponse:Onsagerformalism
(Two-terminal) Coupled 1D charge and heat transport
Fluxes
Affinities (forces)
Positivity of entropy production Onsager relation (TRS)
Transport coefficients & Onsager matrix elements
| PAGE 42
ElasticRegime:validityofSommerfeld expansion
Validity of Sommerfeld Expansion
Q: Validity of the Mott’s formula for S
Wiedemann-Franz (WF) law, Mott’sformula
Sommerfeld temperature isproportional to the mean energy
level spacing in the system:
(Proportionality constant dependson required precision)
Result for a tunnel barrier:
Estimation for Si nanowire: 100 mK| PAGE 43
ElasticRegime:Typicalthermopowerofatunnelbarrier
In the basis
σ = nonvanishingpart of Σ
| PAGE 44
Three-terminalquantumthermalmachines
Efficiency: depends on the sign of the heat currents
Carnot limit
Not a function of the temperatures only !!
Efficiencies at maximum power
Generalized figures of merit
F. Mazza, R. Bosisio, G. Benenti, V. Giovannetti., R. Fazio & F. Taddei, New J. Phys. (2014)| PAGE 45
GATE MODULATED CARRIER DENSITY
ln G(V gate) at three temperatures in a large gate voltage range(details of the conductance pattern are not seen for this gate voltage sampling)
Inset: the same curve in a linear scale. Note the linearity at voltages above the transition.
ConductorAnderson Insulator
Edge of the impurity band = -2,5 V (Complete depletion of the disordered nanowire)
| PAGE 46
CONDUCTANCE FLUCTUATION S INDUCED BY VARYING THE GATE VOLTAGE
Bulk of the impurity band Edge of the impurity band
Mott Formula :
Larger thermopower at the band edges
𝑺 ≈𝝏𝐥𝐧(𝑮)𝝏𝑽𝒈
| PAGE 47