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Low-temperature thermoelectric properties of bilayer graphene Adam Rycerz , Dominik Suszalski, and Grzegorz Rut Marian Smoluchowski Institute of Physics, Jagiellonian University, Kraków, Poland StoCP 2018, Zakopane, Poland, September 16–21, 2018 Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

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Page 1: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

Low-temperature thermoelectric propertiesof bilayer graphene

Adam Rycerz, Dominik Suszalski, and Grzegorz RutMarian Smoluchowski Institute of Physics, Jagiellonian University,

Kraków, Poland

StoCP 2018, Zakopane, Poland, September 16–21, 2018

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 2: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Emergent Dirac fermions in grapheneTunable band gap and trigonal warping in BLGQuantum size effects

Why graphene?

Atomically-thin2D

crystals

Dirac materialsgraphene, silicene(?), ... vdW heterostr.

h-BN, h-AlN(?)MoS2, HfSe2, ...Black-PTiSe2 (CWD+SC!)

Artificial graphenes & analogsTopolog. insulators: HgTe/CdTe,Bi1−xSbx , Bi2Se3, Bi2Te3, ...d-wave superconductorsWeyl semimetals

For a review of the topic, see: Wehling et al., Adv. Phys. 76, 1 (2014).Theory of SC in TiSe2: Chen et al., arXiv:1806.08064.

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 3: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Emergent Dirac fermions in grapheneTunable band gap and trigonal warping in BLGQuantum size effects

Emergent Dirac fermions in graphene

What differs graphene from a collection of carbon atoms?

The valley pseudospin (⇒ fermion doubling)

Time-reversal symmetry breaking at zero magnetic field

Pseudodiffusive charge transport, . . . , SC in twisted-BLG (!)

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 4: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Emergent Dirac fermions in grapheneTunable band gap and trigonal warping in BLGQuantum size effects

Tunable band gap and trigonal warping

E = "L

k`

"L =�1

4

✓�3

�0

◆2

⇡ 1 meV

k` =2p3

�1�3

a�20

⇡ 0.05 nm�1

[ Top: IEEE Spectrum, 2009; bottom: McCann & Koshino, 2013 ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 5: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Emergent Dirac fermions in grapheneTunable band gap and trigonal warping in BLGQuantum size effects

[55] Zhang et al., Phys. Rev. B 78, 235408 (2008).[56] Li et al., Phys. Rev. Lett. 102, 037403 (2009).[67] Dresselhaus & Dresselhaus, Adv. Phys. 51, 1 (2002).[76] Malard et al., Phys. Rev. B 76, 201401(R) (2007).[80] Kuzmenko et al., Phys. Rev. B 80, 165406 (2009).[82] Taychatanapat et al., Nature Phys. 7, 621 (2011).

Yankowitz et al., (2014): γ1 = 0.39 eV, γ4 = 0.22 eV, but γ3 not determined ...

⇒ Novel phenomena governed solely by γ3 desired!

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 6: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Emergent Dirac fermions in grapheneTunable band gap and trigonal warping in BLGQuantum size effects

Where to expect TW effects on transport?

Time-energy uncertainty relation limits the energy resolution:

∆E >~

∆t∼ ~vF

L,

where we set ∆t ∼ tflight ≈ L/vF .�E / 1/L

The condition ∆E . 2εL leads to

L &~vF

2εL=√

3γ3

0

γ1γ23

a ≈ 400 nm,

where γ0 = 3.16 eV, γ1 = 0.38 eV, γ3 = 0.3 eV, a = 0.246 nm.

⇒ Effects of γ3 6= 0 on transport prop-s may depend on thesystem size; the crossover range: 100 nm < L < 1µm.

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 7: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Brief overviewUniversal conductivity of MLGEmergent conductivity of BLG

Electric and thermal currents

where gs = gv = 2 denote spin and valley degeneracies,T (E) ≡ Tr(tt†), and fL, fR are Fermi-Dirac distributions.

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 8: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Brief overviewUniversal conductivity of MLGEmergent conductivity of BLG

Monolayer at the charge-neutrality point

G =2e2

h

∞∑

n=−∞

1cosh2[π(n + α)L/W ]

W�L' 4e2

πhWL,

where α = 12 for the mass confinement (ΨA|y=0 = ΨB|y=0,

ΨA|y=W= −ΨB|y=W ).

The conductivity: σ = GL/W = 4e2/(πh) ≡ σ0 .

Theory: Katsnelson (2006); Tworzydło et al. (2006)Experiment: Miao et al., (2007); Danneau et al., (2008).

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 9: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Brief overviewUniversal conductivity of MLGEmergent conductivity of BLG

Emergent conductivity of BLG

Landauer conductivity [Snyman& Beenakker, 2007], γ3 = γ4 = 0:

σbilayer = GL/W = 2σ0

Kubo conductivity [Cserti et al.,2007], γ3 6= 0:

σbilayer = 6σ0 ( ! )

Experiment: [Mayorov et al.,2011] σbilayer ' 5σ0.

[ with σ0 ≡ (4/π)e2/h – universalconductivity of a monolayer. ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 10: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Brief overviewUniversal conductivity of MLGEmergent conductivity of BLG

EXP: Mayorov et al, 2011(�BLG ⇡ 5�0 )

<latexit sha1_base64="HyCKdNKPWLxmGgR/I3vh85vKi1g=">AAACBnicdVDLSgMxAMzWV62vqkcvwSJUKGV3Xfu4FT3owUMFawvdsmTTtA3NPkiyYln6AV78FS+KJ8Wjv+DfmG3XQ0UHAsPMhGTGDRkVUte/tMzS8srqWnY9t7G5tb2T3927FUHEMWnhgAW84yJBGPVJS1LJSCfkBHkuI213fJ747TvCBQ38GzkJSc9DQ58OKEZSSU6+WLRLtqBDDzmxzT14dnUxtVEY8uA+np6mjm6Xjp18QS/XaxXTqkC9rOtVwzQSYlatEwsaSklQACmaTv7T7gc48ogvMUNCdA09lL0YcUkxI9OcHQkSIjxGQxLPekzhkZL6cBBwdXwJZ+pCDnlCTDxXJT0kR+K3l4h/ed1IDmq9mPphJImP5w8NIgZlAJNRYJ9ygiWbKIIwp+qHEI8QR1iq6XKq+k8/+D9pmeV62bi2Cg0z3SALDsAhKAIDVEEDXIImaAEMHsEzeAPv2oP2pL1or/NoRkvv7IMFaB/fd7CYYA==</latexit><latexit sha1_base64="HyCKdNKPWLxmGgR/I3vh85vKi1g=">AAACBnicdVDLSgMxAMzWV62vqkcvwSJUKGV3Xfu4FT3owUMFawvdsmTTtA3NPkiyYln6AV78FS+KJ8Wjv+DfmG3XQ0UHAsPMhGTGDRkVUte/tMzS8srqWnY9t7G5tb2T3927FUHEMWnhgAW84yJBGPVJS1LJSCfkBHkuI213fJ747TvCBQ38GzkJSc9DQ58OKEZSSU6+WLRLtqBDDzmxzT14dnUxtVEY8uA+np6mjm6Xjp18QS/XaxXTqkC9rOtVwzQSYlatEwsaSklQACmaTv7T7gc48ogvMUNCdA09lL0YcUkxI9OcHQkSIjxGQxLPekzhkZL6cBBwdXwJZ+pCDnlCTDxXJT0kR+K3l4h/ed1IDmq9mPphJImP5w8NIgZlAJNRYJ9ygiWbKIIwp+qHEI8QR1iq6XKq+k8/+D9pmeV62bi2Cg0z3SALDsAhKAIDVEEDXIImaAEMHsEzeAPv2oP2pL1or/NoRkvv7IMFaB/fd7CYYA==</latexit><latexit sha1_base64="HyCKdNKPWLxmGgR/I3vh85vKi1g=">AAACBnicdVDLSgMxAMzWV62vqkcvwSJUKGV3Xfu4FT3owUMFawvdsmTTtA3NPkiyYln6AV78FS+KJ8Wjv+DfmG3XQ0UHAsPMhGTGDRkVUte/tMzS8srqWnY9t7G5tb2T3927FUHEMWnhgAW84yJBGPVJS1LJSCfkBHkuI213fJ747TvCBQ38GzkJSc9DQ58OKEZSSU6+WLRLtqBDDzmxzT14dnUxtVEY8uA+np6mjm6Xjp18QS/XaxXTqkC9rOtVwzQSYlatEwsaSklQACmaTv7T7gc48ogvMUNCdA09lL0YcUkxI9OcHQkSIjxGQxLPekzhkZL6cBBwdXwJZ+pCDnlCTDxXJT0kR+K3l4h/ed1IDmq9mPphJImP5w8NIgZlAJNRYJ9ygiWbKIIwp+qHEI8QR1iq6XKq+k8/+D9pmeV62bi2Cg0z3SALDsAhKAIDVEEDXIImaAEMHsEzeAPv2oP2pL1or/NoRkvv7IMFaB/fd7CYYA==</latexit><latexit sha1_base64="HyCKdNKPWLxmGgR/I3vh85vKi1g=">AAACBnicdVDLSgMxAMzWV62vqkcvwSJUKGV3Xfu4FT3owUMFawvdsmTTtA3NPkiyYln6AV78FS+KJ8Wjv+DfmG3XQ0UHAsPMhGTGDRkVUte/tMzS8srqWnY9t7G5tb2T3927FUHEMWnhgAW84yJBGPVJS1LJSCfkBHkuI213fJ747TvCBQ38GzkJSc9DQ58OKEZSSU6+WLRLtqBDDzmxzT14dnUxtVEY8uA+np6mjm6Xjp18QS/XaxXTqkC9rOtVwzQSYlatEwsaSklQACmaTv7T7gc48ogvMUNCdA09lL0YcUkxI9OcHQkSIjxGQxLPekzhkZL6cBBwdXwJZ+pCDnlCTDxXJT0kR+K3l4h/ed1IDmq9mPphJImP5w8NIgZlAJNRYJ9ygiWbKIIwp+qHEI8QR1iq6XKq+k8/+D9pmeV62bi2Cg0z3SALDsAhKAIDVEEDXIImaAEMHsEzeAPv2oP2pL1or/NoRkvv7IMFaB/fd7CYYA==</latexit>

[ Notation: t⊥ ≡ γ1, t ′ ≡ γ3 ]

Non-cummuting limits:lim

L→∞lim

d→∞σBLG = 2σ0

limd→∞

limL→∞

σBLG = 6σ0 (! )

[ γ1∼γ3∼e−Bd/d0 , εL∼(

e−Bd/d0)3

,and thus εL/γ1 → 0 with d →∞(the interlayer distance) ]

Surprising analogy withsystems showingspontaneous symmetrybreaking !

Grzegorz Rut & AR:⇒ PRB 89, 045421 (2014)⇒ EPL 107, 47005 (2014)

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 11: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Quasiparticles in doped BLG

E/EL

0 0.5 1.0 1.5 2.00

0.5

1.0

DO

S[e

V�

1nm

�2]

mC / |E|

Massless !Dirac!fermions

Massive !chiral!fermions

Hea

vy fe

r-s

In a generic 2D system!

the cyclotronic mass:

mC(E) =

⇡~2

2DOS(E)

me↵ =t?2v2

F

⇡ 0.033 me

Transitions between !different populations !of quasiparticles!should have !signatures !in thermoelectric properties...

!

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 12: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Why thermoelectrics?

The Mott formula for metals [Cutler & Mott, Phys. Rev. (1969)]

S ≈ π2k2BT

3e

[∂ lnσ(E)

∂E

]

E=EF

,

The Drude conductivity: σ = ne2τ/meff ∼ DOS(EF )× kBT(provided that the mobility µ̃(E) ∼ τ/meff ≈ const.).⇒ Any abrupt change in DOS(E) should has some signature in S.

The Goldsmid-Sharp energy gap in semiconductors|S|max ≈ Eg/(2eTmax) allows the thermoelectric-basedband-gap (Eg) determination, instead of employing the familiaractivation formula σ ∼ exp(−Eg/2kBT ).[Goldsmid & Sharp, J. Electron. Mater. (1999)] .

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 13: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Zero-temperature conductivity (µ 6= 0)

0 20 40 60 80

100 120 140

0 0.2 0.4 0.6 0.8 1 1.2

Cond

uctiv

ity [4

e 2/h

]

μ [meV]

0 10 20 30 40 50 0

2

4

6

8

Cond

uctiv

ity [4

e2/h

]

μ [µeV]

t0 =

0.3eV

t0 = 0.2 eV

t0 = 0

6�0<latexit sha1_base64="n/HZEG646XDAVmRDmvhtdR3BMvY=">AAAB5XicdVDLSgMxFL1TX7W+qi7dBIvgasiMQx+7ghuXFRxbaUvJpJk2NPMgyQil9BfcKK4Uf8df8G/MtHVR0QOBwzkn3HtukAquNMZfVmFjc2t7p7hb2ts/ODwqH5/cqySTlPk0EYnsBEQxwWPma64F66SSkSgQrB1MrnO//cik4kl8p6cp60dkFPOQU6KN9FDtKT6KyAAPyhVsN+pV16sibGNcc1wnJ27Nu/KQY5QcFVihNSh/9oYJzSIWayqIUl0Hp7o/I1JzKti81MsUSwmdkBGbLdacowsjDVGYSPNijRbqWo5ESk2jwCQjosfqt5eLf3ndTIf1/ozHaaZZTJeDwkwgnaC8MxpyyagWU0MIldxsiOiYSEK1uUzJVP/ph/4nvms3bOfWqzTrqxsU4QzO4RIcqEETbqAFPlCI4Bne4N0aW0/Wi/W6jBas1Z9TWIP18Q3gMIu9</latexit><latexit sha1_base64="n/HZEG646XDAVmRDmvhtdR3BMvY=">AAAB5XicdVDLSgMxFL1TX7W+qi7dBIvgasiMQx+7ghuXFRxbaUvJpJk2NPMgyQil9BfcKK4Uf8df8G/MtHVR0QOBwzkn3HtukAquNMZfVmFjc2t7p7hb2ts/ODwqH5/cqySTlPk0EYnsBEQxwWPma64F66SSkSgQrB1MrnO//cik4kl8p6cp60dkFPOQU6KN9FDtKT6KyAAPyhVsN+pV16sibGNcc1wnJ27Nu/KQY5QcFVihNSh/9oYJzSIWayqIUl0Hp7o/I1JzKti81MsUSwmdkBGbLdacowsjDVGYSPNijRbqWo5ESk2jwCQjosfqt5eLf3ndTIf1/ozHaaZZTJeDwkwgnaC8MxpyyagWU0MIldxsiOiYSEK1uUzJVP/ph/4nvms3bOfWqzTrqxsU4QzO4RIcqEETbqAFPlCI4Bne4N0aW0/Wi/W6jBas1Z9TWIP18Q3gMIu9</latexit><latexit sha1_base64="n/HZEG646XDAVmRDmvhtdR3BMvY=">AAAB5XicdVDLSgMxFL1TX7W+qi7dBIvgasiMQx+7ghuXFRxbaUvJpJk2NPMgyQil9BfcKK4Uf8df8G/MtHVR0QOBwzkn3HtukAquNMZfVmFjc2t7p7hb2ts/ODwqH5/cqySTlPk0EYnsBEQxwWPma64F66SSkSgQrB1MrnO//cik4kl8p6cp60dkFPOQU6KN9FDtKT6KyAAPyhVsN+pV16sibGNcc1wnJ27Nu/KQY5QcFVihNSh/9oYJzSIWayqIUl0Hp7o/I1JzKti81MsUSwmdkBGbLdacowsjDVGYSPNijRbqWo5ESk2jwCQjosfqt5eLf3ndTIf1/ozHaaZZTJeDwkwgnaC8MxpyyagWU0MIldxsiOiYSEK1uUzJVP/ph/4nvms3bOfWqzTrqxsU4QzO4RIcqEETbqAFPlCI4Bne4N0aW0/Wi/W6jBas1Z9TWIP18Q3gMIu9</latexit><latexit sha1_base64="n/HZEG646XDAVmRDmvhtdR3BMvY=">AAAB5XicdVDLSgMxFL1TX7W+qi7dBIvgasiMQx+7ghuXFRxbaUvJpJk2NPMgyQil9BfcKK4Uf8df8G/MtHVR0QOBwzkn3HtukAquNMZfVmFjc2t7p7hb2ts/ODwqH5/cqySTlPk0EYnsBEQxwWPma64F66SSkSgQrB1MrnO//cik4kl8p6cp60dkFPOQU6KN9FDtKT6KyAAPyhVsN+pV16sibGNcc1wnJ27Nu/KQY5QcFVihNSh/9oYJzSIWayqIUl0Hp7o/I1JzKti81MsUSwmdkBGbLdacowsjDVGYSPNijRbqWo5ESk2jwCQjosfqt5eLf3ndTIf1/ozHaaZZTJeDwkwgnaC8MxpyyagWU0MIldxsiOiYSEK1uUzJVP/ph/4nvms3bOfWqzTrqxsU4QzO4RIcqEETbqAFPlCI4Bne4N0aW0/Wi/W6jBas1Z9TWIP18Q3gMIu9</latexit>

2�0<latexit sha1_base64="0AMYOxZyrfYdJ6GrGWC1XFlvqOA=">AAAB5XicdVDLSsNAFL3xWeur6tLNYBFchSTGPnYFNy4rGFtpS5lMJ+3QmSTMTIRS+gtuFFeKv+Mv+DdO2rqo6IGBwzlnuPfcMOVMacf5stbWNza3tgs7xd29/YPD0tHxvUoySWhAEp7IdogV5SymgWaa03YqKRYhp61wfJ37rUcqFUviOz1JaU/gYcwiRrA20oPXVWwocN/pl8qOXa9VPL+CHNtxqq7n5sSr+pc+co2SowxLNPulz+4gIZmgsSYcK9VxnVT3plhqRjidFbuZoikmYzyk0/maM3RupAGKEmlerNFcXclhodREhCYpsB6p314u/uV1Mh3VelMWp5mmMVkMijKOdILyzmjAJCWaTwzBRDKzISIjLDHR5jJFU/2nH/qfBJ5dt91bv9y4Wt6gAKdwBhfgQhUacANNCICAgGd4g3drZD1ZL9brIrpmLf+cwAqsj2/ZRYu2</latexit><latexit sha1_base64="0AMYOxZyrfYdJ6GrGWC1XFlvqOA=">AAAB5XicdVDLSsNAFL3xWeur6tLNYBFchSTGPnYFNy4rGFtpS5lMJ+3QmSTMTIRS+gtuFFeKv+Mv+DdO2rqo6IGBwzlnuPfcMOVMacf5stbWNza3tgs7xd29/YPD0tHxvUoySWhAEp7IdogV5SymgWaa03YqKRYhp61wfJ37rUcqFUviOz1JaU/gYcwiRrA20oPXVWwocN/pl8qOXa9VPL+CHNtxqq7n5sSr+pc+co2SowxLNPulz+4gIZmgsSYcK9VxnVT3plhqRjidFbuZoikmYzyk0/maM3RupAGKEmlerNFcXclhodREhCYpsB6p314u/uV1Mh3VelMWp5mmMVkMijKOdILyzmjAJCWaTwzBRDKzISIjLDHR5jJFU/2nH/qfBJ5dt91bv9y4Wt6gAKdwBhfgQhUacANNCICAgGd4g3drZD1ZL9brIrpmLf+cwAqsj2/ZRYu2</latexit><latexit sha1_base64="0AMYOxZyrfYdJ6GrGWC1XFlvqOA=">AAAB5XicdVDLSsNAFL3xWeur6tLNYBFchSTGPnYFNy4rGFtpS5lMJ+3QmSTMTIRS+gtuFFeKv+Mv+DdO2rqo6IGBwzlnuPfcMOVMacf5stbWNza3tgs7xd29/YPD0tHxvUoySWhAEp7IdogV5SymgWaa03YqKRYhp61wfJ37rUcqFUviOz1JaU/gYcwiRrA20oPXVWwocN/pl8qOXa9VPL+CHNtxqq7n5sSr+pc+co2SowxLNPulz+4gIZmgsSYcK9VxnVT3plhqRjidFbuZoikmYzyk0/maM3RupAGKEmlerNFcXclhodREhCYpsB6p314u/uV1Mh3VelMWp5mmMVkMijKOdILyzmjAJCWaTwzBRDKzISIjLDHR5jJFU/2nH/qfBJ5dt91bv9y4Wt6gAKdwBhfgQhUacANNCICAgGd4g3drZD1ZL9brIrpmLf+cwAqsj2/ZRYu2</latexit><latexit sha1_base64="0AMYOxZyrfYdJ6GrGWC1XFlvqOA=">AAAB5XicdVDLSsNAFL3xWeur6tLNYBFchSTGPnYFNy4rGFtpS5lMJ+3QmSTMTIRS+gtuFFeKv+Mv+DdO2rqo6IGBwzlnuPfcMOVMacf5stbWNza3tgs7xd29/YPD0tHxvUoySWhAEp7IdogV5SymgWaa03YqKRYhp61wfJ37rUcqFUviOz1JaU/gYcwiRrA20oPXVWwocN/pl8qOXa9VPL+CHNtxqq7n5sSr+pc+co2SowxLNPulz+4gIZmgsSYcK9VxnVT3plhqRjidFbuZoikmYzyk0/maM3RupAGKEmlerNFcXclhodREhCYpsB6p314u/uV1Mh3VelMWp5mmMVkMijKOdILyzmjAJCWaTwzBRDKzISIjLDHR5jJFU/2nH/qfBJ5dt91bv9y4Wt6gAKdwBhfgQhUacANNCICAgGd4g3drZD1ZL9brIrpmLf+cwAqsj2/ZRYu2</latexit>

Fabry-Perrot resonances: ∆E ≈ 2π(~vF/L)√|E |/t⊥ for t ′ = 0, or

∆E ∼ π~v3/L = 2π(~vF/L)√

EL/t⊥ for t ′ 6= 0.Above: L = 104l⊥ = 17.7µm. [ Suszalski, Rut, AR, PRB (2018) ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 14: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

In the linear-responce regime:

with Ln given by

The Lorentz number

[LWF ≡ 13π

2 (kB/e)2 ⇔ T (E) =const;a model T (E) ∝ |E | ⇔ Lmax ≈ 2.37LWF.]

[ Suszalski, Rut, AR, PRB (2018) ]

0.8

1.2

1.6

2

2.4

0.30.60.91.21.5

T [K

]

0.0

0.2

0.4

0.6

0.8

1.0

1.2

0 0.2 0.4 0.6 0.8 1 1.2

0 0.3 0.6 0.9 1.2EL [meV]

S [k

B/e]

[meV]μ

L/L W

F

T=

2K

T = 0.515K

T = 0.2K

T = 80mK

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 15: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

⇒ One does not necessarily need to include interactions tounderstand some experimental data!

Lmax ⇡ 2.37 LWF<latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit><latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit><latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit><latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit>

Lmax ⇡ 2.37 LWF<latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit><latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit><latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit><latexit sha1_base64="YZTnSqhVJaxct3vzIcd4+w2X5EE=">AAACDHicdVDLSgMxAMzWV62vqkcvwSJ4kGV3W/q4FQTx4KGCtYVuWbJptg3NPkiy0rLsN3jxV7wonhTxF/wbs21FKjoQGGYmJDNuxKiQhvGp5VZW19Y38puFre2d3b3i/sGtCGOOSRuHLORdFwnCaEDakkpGuhEnyHcZ6bjj88zv3BEuaBjcyGlE+j4aBtSjGEklOUU9sTFi8Cp1Epv70EeT1EZRxMNJklp6uWaf/QQ6F6lTLBl6o161KlVo6IZRMy0zI1atUq5AUykZSmCBllP8sAchjn0SSMyQED3TiGQ/QVxSzEhasGNBIoTHaEiSWZsUnihpAL2QqxNIOFOXcsgXYuq7KukjORK/vUz8y+vF0qv3ExpEsSQBnj/kxQzKEGbTwAHlBEs2VQRhTtUPIR4hjrBUAxZU9e9+8H/StvSGbl5XSk1rsUEeHIFjcApMUANNcAlaoA0weABP4BW8affao/asvcyjOW1x5xAsQXv/ApQ9mzQ=</latexit>

[ EXP: Crossno et al, Science (2016) ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 16: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Chemical potential µ is not a directly-measurable quantity, but itis monotonically-dependent on the carrier density n.

Characteristic temperatures, at which the secondarymaximum of S (minimum of L) vanishes are:

T S? = 0.050× EL/kB,

TL? = 0.118× EL/kB.

(For t ′ = 0.3 eV, EL/kB ≈ 10 K.)

Also, a global maximum ofS corresponds to

T Smax = 0.20× EL/kB.

[ Suszalski, Rut, AR, PRB (2018) ]

0.0

0.1

0.2

0.3

0 0.5 1 1.5

μ max

[m

eV]

T [K]

0

20

40

60

80

(n-p

) max

[μm

-2]

0

20

40

60

80

(n-p

) max

[μm

-2]

0

20

40

60

80

(n-p

) max

[μm

-2]

0.7

0.8

0.9

1.0

1.1

S max

[k B

/e]

0 0.5 1 1.5 2

0.00

0.03

0.06

0.09

0.12

0.15

ZTm

ax

T [K]t0 =0

t0 =0.2 e

V

t0 =

0.3eV

(a)

(b)

(c)

(d)

Z T ( μ m

ax )

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 17: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Remarks on intrinsic gap in BLG (1)

Free-standing (suspended) BLG:

[Credit: Lau lab, UC Riverside]

Width of resistivity peak matches the self-consistent(mean-field) gap:

∆i (T ) = ∆i (0) tanh

(1.74

√Tc

T− 1

)for T ≤ Tc ,

with ∆i (0) ≈ 1.5 meV, Tc ≈ 12 K (∆i (0)/kBTc ≈ 1.5).[Nam et al., 2D Mater 2016; Morpurgo, Graph. Week 2018]

BLG in v.d. Walls heterostructures (vdWH):No signatures of∆i >0 found as yet (!)

[Kraft et al., Nat. Comm 2018]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 18: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Remarks on intrinsic gap in BLG (2)

Possible explanations of the presentce/absence of ∆iin free-standing BLG / vdWH containing BLG:

Self-consistent gap strongly depends on effectiveHubbard-U: ∆i ∼ t0 exp(−const/Ueff) [Hirsch, 1985].

Supression of Ueff due to dielectric constant maydramatically reduce ∆i and Tc .

Lattice mismatch between BLG and h-BN induces aneffective potential (Moiré pattern) destabilizing quasi-longrange order (?)

. . . ?

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 19: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

The nonzero gap case (∆ > 0)

-0.05 0.00 0.05 0.10 0.150.0

1.0

2.0

3.0

G/W

[g0/µm

]

μ-Δ/2 [meV]

(e)

(a)

(b)

{µL, TL}

VI

=)IQ

{µR, TR}

=)IQ

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0 3 6 9 120

6

12

18

μ [meV]

G/W

[g0/µ

m]

0

5

10

15

20

S[k

B/e

]

(c)

(d)

U=

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U=20

meV

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U=

10m

eV

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U =150meV

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[ Rut, Suszalski, AR, in preparation ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 20: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Red solid line:Approx/asymptoticexpression [,T (E) / ⇥(|E|� 1

2�)]

|S|max = |S|GSmax�(kB/e)⇥

⇥12 ln x + ln 2 � 1

2 + O(x�1)⇤, with x = �/2kBT � 1.

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Dotted line:The reference(Goldsmid-Sharp)value:

|S|GSmax = �

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|S|G

Sm

ax�

|S| m

ax

[kB

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<latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit><latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit><latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit><latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit>

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<latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit><latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit><latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit><latexit sha1_base64="KSGBZTJvfc/4ccuvBiKsL1DuvLc=">AAACFHicbVDLSgMxAMz6rPW16tFLahE8aN0tih6LHvRYqX1Ad12yabYNzT5IsmLZ7m948Ve8iAii4N2/MW330taBwDAzIZlxI0aFNIxfbWFxaXllNbeWX9/Y3NrWd3YbIow5JnUcspC3XCQIowGpSyoZaUWcIN9lpOn2r0d+85FwQcPgXg4iYvuoG1CPYiSV5Ojnw9rQSSzuQx89pQ/JmFrHN7U0tQonVmHKtmC771ydEtvRi0bJGAPOEzMjRZCh6uifVifEsU8CiRkSom0akbQTxCXFjKR5KxYkQriPuiQZl0rhoZI60Au5OoGEY3Uqh3whBr6rkj6SPTHrjcT/vHYsvUs7oUEUSxLgyUNezKAM4Wgh2KGcYMkGiiDMqfohxD3EEZZqx7yqbs4WnSeNcsk0SubdWbFSzkbIgX1wAI6ACS5ABdyCKqgDDF7AG/gC39qz9qq9ax+T6IKW3dkDU9B+/gCufp2k</latexit>

0

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�3 ⌘ t0 = 0.3 eV<latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit><latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit><latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit><latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit>

�3 ⌘ t0 = 0.3 eV<latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit><latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit><latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit><latexit sha1_base64="v8M4KGTmQhq+41cyA3u1iRrJAxA=">AAAB/3icbVBNS8MwAE3n15xfVY9eokP0IKN1gvMgDLx4nGC3wTpKmqVbWNLUJB2O0osX/4oXxZPiP/Av+G/stl42fRB4vPdC8p4fMaq0Zf0YhaXlldW14nppY3Nre8fc3WsqEUtMHCyYkG0fKcJoSBxNNSPtSBLEfUZa/vBm4rdGRCoqwns9jkiXo35IA4qRziTPPHT7iHPkVV3yENNRkuqTa6tSdc9c7ovHhDRTzyxbFWsK+JfYOSmDHA3P/HZ7AsechBozpFTHtiLdTZDUFDOSltxYkQjhIeqTZFoghceZ1IOBkNkJNZyqcznElRpzP0typAdq0ZuI/3mdWAe1bkLDKNYkxLOHgphBLeBkDdijkmDNxhlBWNLshxAPkERYZ5uVsur2YtG/xDmvXFXsu4tyvZZvUAQH4AicAhtcgjq4BQ3gAAyewSv4AJ/Gk/FivBnvs2jByO/sgzkYX79YaZWP</latexit>

T = 1K<latexit sha1_base64="9ruOToFeRGKbw8XDYfczG8P7rkU=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiBetCKLgR3FRobKEJZTKdtEMnmTgzEUvoT7hRXCn+jL/g3zhts2nrgYHDOWe499wg4Uxp2/61CmvrG5tbxe3Szu7e/kH58OhRiVQS6hLBhewEWFHOYupqpjntJJLiKOC0HYxup377mUrFRNzS44T6ER7ELGQEayP5rRvHu/CiQLxk95NeuWJX7RnQKnFyUoEczV75x+sLkkY01oRjpbqOnWg/w1Izwumk5KWKJpiM8IBms1Un6MxIfRQKaV6s0UxdyOFIqXEUmGSE9VAte1PxP6+b6rDuZyxOUk1jMh8Uphxpgaa9UZ9JSjQfG4KJZGZDRIZYYqLNdUqmurNcdJW4l9XrqvNQqzTq+Q2KcAKncA4OXEED7qAJLhB4gjf4hC+LW6/Wu/Uxjxas/M8xLMD6/gM72I0Q</latexit><latexit sha1_base64="9ruOToFeRGKbw8XDYfczG8P7rkU=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiBetCKLgR3FRobKEJZTKdtEMnmTgzEUvoT7hRXCn+jL/g3zhts2nrgYHDOWe499wg4Uxp2/61CmvrG5tbxe3Szu7e/kH58OhRiVQS6hLBhewEWFHOYupqpjntJJLiKOC0HYxup377mUrFRNzS44T6ER7ELGQEayP5rRvHu/CiQLxk95NeuWJX7RnQKnFyUoEczV75x+sLkkY01oRjpbqOnWg/w1Izwumk5KWKJpiM8IBms1Un6MxIfRQKaV6s0UxdyOFIqXEUmGSE9VAte1PxP6+b6rDuZyxOUk1jMh8Uphxpgaa9UZ9JSjQfG4KJZGZDRIZYYqLNdUqmurNcdJW4l9XrqvNQqzTq+Q2KcAKncA4OXEED7qAJLhB4gjf4hC+LW6/Wu/Uxjxas/M8xLMD6/gM72I0Q</latexit><latexit sha1_base64="9ruOToFeRGKbw8XDYfczG8P7rkU=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiBetCKLgR3FRobKEJZTKdtEMnmTgzEUvoT7hRXCn+jL/g3zhts2nrgYHDOWe499wg4Uxp2/61CmvrG5tbxe3Szu7e/kH58OhRiVQS6hLBhewEWFHOYupqpjntJJLiKOC0HYxup377mUrFRNzS44T6ER7ELGQEayP5rRvHu/CiQLxk95NeuWJX7RnQKnFyUoEczV75x+sLkkY01oRjpbqOnWg/w1Izwumk5KWKJpiM8IBms1Un6MxIfRQKaV6s0UxdyOFIqXEUmGSE9VAte1PxP6+b6rDuZyxOUk1jMh8Uphxpgaa9UZ9JSjQfG4KJZGZDRIZYYqLNdUqmurNcdJW4l9XrqvNQqzTq+Q2KcAKncA4OXEED7qAJLhB4gjf4hC+LW6/Wu/Uxjxas/M8xLMD6/gM72I0Q</latexit><latexit sha1_base64="9ruOToFeRGKbw8XDYfczG8P7rkU=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiBetCKLgR3FRobKEJZTKdtEMnmTgzEUvoT7hRXCn+jL/g3zhts2nrgYHDOWe499wg4Uxp2/61CmvrG5tbxe3Szu7e/kH58OhRiVQS6hLBhewEWFHOYupqpjntJJLiKOC0HYxup377mUrFRNzS44T6ER7ELGQEayP5rRvHu/CiQLxk95NeuWJX7RnQKnFyUoEczV75x+sLkkY01oRjpbqOnWg/w1Izwumk5KWKJpiM8IBms1Un6MxIfRQKaV6s0UxdyOFIqXEUmGSE9VAte1PxP6+b6rDuZyxOUk1jMh8Uphxpgaa9UZ9JSjQfG4KJZGZDRIZYYqLNdUqmurNcdJW4l9XrqvNQqzTq+Q2KcAKncA4OXEED7qAJLhB4gjf4hC+LW6/Wu/Uxjxas/M8xLMD6/gM72I0Q</latexit>

T = 5K<latexit sha1_base64="RJWpAWqPADdEfRm1qsDliJZHJRc=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiinUhFNwIbio0ttCEMplO2qGTTJyZiCX0J9worhR/xl/wb5y22bT1wMDhnDPce26QcKa0bf9ahZXVtfWN4mZpa3tnd6+8f/CoRCoJdYngQrYDrChnMXU105y2E0lxFHDaCoa3E7/1TKViIm7qUUL9CPdjFjKCtZH85s2ld+ZFgXjJ7sfdcsWu2lOgZeLkpAI5Gt3yj9cTJI1orAnHSnUcO9F+hqVmhNNxyUsVTTAZ4j7NpquO0YmReigU0rxYo6k6l8ORUqMoMMkI64Fa9Cbif14n1WHNz1icpJrGZDYoTDnSAk16ox6TlGg+MgQTycyGiAywxESb65RMdWex6DJxz6vXVefholKv5TcowhEcwyk4cAV1uIMGuEDgCd7gE74sbr1a79bHLFqw8j+HMAfr+w9B5I0U</latexit><latexit sha1_base64="RJWpAWqPADdEfRm1qsDliJZHJRc=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiinUhFNwIbio0ttCEMplO2qGTTJyZiCX0J9worhR/xl/wb5y22bT1wMDhnDPce26QcKa0bf9ahZXVtfWN4mZpa3tnd6+8f/CoRCoJdYngQrYDrChnMXU105y2E0lxFHDaCoa3E7/1TKViIm7qUUL9CPdjFjKCtZH85s2ld+ZFgXjJ7sfdcsWu2lOgZeLkpAI5Gt3yj9cTJI1orAnHSnUcO9F+hqVmhNNxyUsVTTAZ4j7NpquO0YmReigU0rxYo6k6l8ORUqMoMMkI64Fa9Cbif14n1WHNz1icpJrGZDYoTDnSAk16ox6TlGg+MgQTycyGiAywxESb65RMdWex6DJxz6vXVefholKv5TcowhEcwyk4cAV1uIMGuEDgCd7gE74sbr1a79bHLFqw8j+HMAfr+w9B5I0U</latexit><latexit sha1_base64="RJWpAWqPADdEfRm1qsDliJZHJRc=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiinUhFNwIbio0ttCEMplO2qGTTJyZiCX0J9worhR/xl/wb5y22bT1wMDhnDPce26QcKa0bf9ahZXVtfWN4mZpa3tnd6+8f/CoRCoJdYngQrYDrChnMXU105y2E0lxFHDaCoa3E7/1TKViIm7qUUL9CPdjFjKCtZH85s2ld+ZFgXjJ7sfdcsWu2lOgZeLkpAI5Gt3yj9cTJI1orAnHSnUcO9F+hqVmhNNxyUsVTTAZ4j7NpquO0YmReigU0rxYo6k6l8ORUqMoMMkI64Fa9Cbif14n1WHNz1icpJrGZDYoTDnSAk16ox6TlGg+MgQTycyGiAywxESb65RMdWex6DJxz6vXVefholKv5TcowhEcwyk4cAV1uIMGuEDgCd7gE74sbr1a79bHLFqw8j+HMAfr+w9B5I0U</latexit><latexit sha1_base64="RJWpAWqPADdEfRm1qsDliJZHJRc=">AAAB6XicbVDLSsNAFL2pr1pfVZduBovgQkoiinUhFNwIbio0ttCEMplO2qGTTJyZiCX0J9worhR/xl/wb5y22bT1wMDhnDPce26QcKa0bf9ahZXVtfWN4mZpa3tnd6+8f/CoRCoJdYngQrYDrChnMXU105y2E0lxFHDaCoa3E7/1TKViIm7qUUL9CPdjFjKCtZH85s2ld+ZFgXjJ7sfdcsWu2lOgZeLkpAI5Gt3yj9cTJI1orAnHSnUcO9F+hqVmhNNxyUsVTTAZ4j7NpquO0YmReigU0rxYo6k6l8ORUqMoMMkI64Fa9Cbif14n1WHNz1icpJrGZDYoTDnSAk16ox6TlGg+MgQTycyGiAywxESb65RMdWex6DJxz6vXVefholKv5TcowhEcwyk4cAV1uIMGuEDgCd7gE74sbr1a79bHLFqw8j+HMAfr+w9B5I0U</latexit>

T = 10K<latexit sha1_base64="DqCo4FZpD1QjVQIm0KVncI/gf0Q=">AAAB6nicbVDLSgMxFL3js9ZX1aWbYBFcSJkRwboQCm4ENxU6ttCpJZNm2tBkMiQZsQz9CjeKK8WP8Rf8G9N2Nm09EDicc8K954YJZ9q47q+zsrq2vrFZ2Cpu7+zu7ZcODh+1TBWhPpFcqlaINeUspr5hhtNWoigWIafNcHg78ZvPVGkm44YZJbQjcD9mESPYWOmpceO5wXkgQvmS3Y+7pbJbcadAy8TLSRly1Luln6AnSSpobAjHWrc9NzGdDCvDCKfjYpBqmmAyxH2aTXcdo1Mr9VAklX2xQVN1LoeF1iMR2qTAZqAXvYn4n9dOTVTtZCxOUkNjMhsUpRwZiSbFUY8pSgwfWYKJYnZDRAZYYWLseYq2urdYdJn4F5XrivdwWa5V8xsU4BhO4Aw8uIIa3EEdfCCg4A0+4csRzqvz7nzMoitO/ucI5uB8/wGqG41K</latexit><latexit sha1_base64="DqCo4FZpD1QjVQIm0KVncI/gf0Q=">AAAB6nicbVDLSgMxFL3js9ZX1aWbYBFcSJkRwboQCm4ENxU6ttCpJZNm2tBkMiQZsQz9CjeKK8WP8Rf8G9N2Nm09EDicc8K954YJZ9q47q+zsrq2vrFZ2Cpu7+zu7ZcODh+1TBWhPpFcqlaINeUspr5hhtNWoigWIafNcHg78ZvPVGkm44YZJbQjcD9mESPYWOmpceO5wXkgQvmS3Y+7pbJbcadAy8TLSRly1Luln6AnSSpobAjHWrc9NzGdDCvDCKfjYpBqmmAyxH2aTXcdo1Mr9VAklX2xQVN1LoeF1iMR2qTAZqAXvYn4n9dOTVTtZCxOUkNjMhsUpRwZiSbFUY8pSgwfWYKJYnZDRAZYYWLseYq2urdYdJn4F5XrivdwWa5V8xsU4BhO4Aw8uIIa3EEdfCCg4A0+4csRzqvz7nzMoitO/ucI5uB8/wGqG41K</latexit><latexit sha1_base64="DqCo4FZpD1QjVQIm0KVncI/gf0Q=">AAAB6nicbVDLSgMxFL3js9ZX1aWbYBFcSJkRwboQCm4ENxU6ttCpJZNm2tBkMiQZsQz9CjeKK8WP8Rf8G9N2Nm09EDicc8K954YJZ9q47q+zsrq2vrFZ2Cpu7+zu7ZcODh+1TBWhPpFcqlaINeUspr5hhtNWoigWIafNcHg78ZvPVGkm44YZJbQjcD9mESPYWOmpceO5wXkgQvmS3Y+7pbJbcadAy8TLSRly1Luln6AnSSpobAjHWrc9NzGdDCvDCKfjYpBqmmAyxH2aTXcdo1Mr9VAklX2xQVN1LoeF1iMR2qTAZqAXvYn4n9dOTVTtZCxOUkNjMhsUpRwZiSbFUY8pSgwfWYKJYnZDRAZYYWLseYq2urdYdJn4F5XrivdwWa5V8xsU4BhO4Aw8uIIa3EEdfCCg4A0+4csRzqvz7nzMoitO/ucI5uB8/wGqG41K</latexit><latexit sha1_base64="DqCo4FZpD1QjVQIm0KVncI/gf0Q=">AAAB6nicbVDLSgMxFL3js9ZX1aWbYBFcSJkRwboQCm4ENxU6ttCpJZNm2tBkMiQZsQz9CjeKK8WP8Rf8G9N2Nm09EDicc8K954YJZ9q47q+zsrq2vrFZ2Cpu7+zu7ZcODh+1TBWhPpFcqlaINeUspr5hhtNWoigWIafNcHg78ZvPVGkm44YZJbQjcD9mESPYWOmpceO5wXkgQvmS3Y+7pbJbcadAy8TLSRly1Luln6AnSSpobAjHWrc9NzGdDCvDCKfjYpBqmmAyxH2aTXcdo1Mr9VAklX2xQVN1LoeF1iMR2qTAZqAXvYn4n9dOTVTtZCxOUkNjMhsUpRwZiSbFUY8pSgwfWYKJYnZDRAZYYWLseYq2urdYdJn4F5XrivdwWa5V8xsU4BhO4Aw8uIIa3EEdfCCg4A0+4csRzqvz7nzMoitO/ucI5uB8/wGqG41K</latexit>

�3 ⌘ t0 = 0<latexit sha1_base64="oI2GJniA5NkbcumT+2F6Za9h3Kk=">AAAB8nicbVDLSsNAFJ3UV62v+Ni5GSyiq5KoYF0IBTcuKxhbaEqYTKft0Jkkztwp1NAvcaO4UvwQf8G/MW2zaeuBgcM5Z7j3njARXIPj/FqFldW19Y3iZmlre2d3z94/eNKxUZR5NBaxaoZEM8Ej5gEHwZqJYkSGgjXCwd3EbwyZ0jyOHmGUsLYkvYh3OSWQSYF95PeIlCS49Nmz4cN0DGe3TmCXnYozBV4mbk7KKEc9sH/8TkyNZBFQQbRuuU4C7ZQo4FSwcck3miWEDkiPpdOdx/g0kzq4G6vsRYCn6lyOSK1HMsySkkBfL3oT8T+vZaBbbac8SgywiM4GdY3AEONJAbjDFaMgRhkhVPFsQ0z7RBEKWU2l7HR38dBl4l1Ubiruw1W5Vs07KKJjdILOkYuuUQ3dozryEEUv6A19oi/LWK/Wu/Uxixas/M8hmoP1/QcXN5Bf</latexit><latexit sha1_base64="oI2GJniA5NkbcumT+2F6Za9h3Kk=">AAAB8nicbVDLSsNAFJ3UV62v+Ni5GSyiq5KoYF0IBTcuKxhbaEqYTKft0Jkkztwp1NAvcaO4UvwQf8G/MW2zaeuBgcM5Z7j3njARXIPj/FqFldW19Y3iZmlre2d3z94/eNKxUZR5NBaxaoZEM8Ej5gEHwZqJYkSGgjXCwd3EbwyZ0jyOHmGUsLYkvYh3OSWQSYF95PeIlCS49Nmz4cN0DGe3TmCXnYozBV4mbk7KKEc9sH/8TkyNZBFQQbRuuU4C7ZQo4FSwcck3miWEDkiPpdOdx/g0kzq4G6vsRYCn6lyOSK1HMsySkkBfL3oT8T+vZaBbbac8SgywiM4GdY3AEONJAbjDFaMgRhkhVPFsQ0z7RBEKWU2l7HR38dBl4l1Ubiruw1W5Vs07KKJjdILOkYuuUQ3dozryEEUv6A19oi/LWK/Wu/Uxixas/M8hmoP1/QcXN5Bf</latexit><latexit sha1_base64="oI2GJniA5NkbcumT+2F6Za9h3Kk=">AAAB8nicbVDLSsNAFJ3UV62v+Ni5GSyiq5KoYF0IBTcuKxhbaEqYTKft0Jkkztwp1NAvcaO4UvwQf8G/MW2zaeuBgcM5Z7j3njARXIPj/FqFldW19Y3iZmlre2d3z94/eNKxUZR5NBaxaoZEM8Ej5gEHwZqJYkSGgjXCwd3EbwyZ0jyOHmGUsLYkvYh3OSWQSYF95PeIlCS49Nmz4cN0DGe3TmCXnYozBV4mbk7KKEc9sH/8TkyNZBFQQbRuuU4C7ZQo4FSwcck3miWEDkiPpdOdx/g0kzq4G6vsRYCn6lyOSK1HMsySkkBfL3oT8T+vZaBbbac8SgywiM4GdY3AEONJAbjDFaMgRhkhVPFsQ0z7RBEKWU2l7HR38dBl4l1Ubiruw1W5Vs07KKJjdILOkYuuUQ3dozryEEUv6A19oi/LWK/Wu/Uxixas/M8hmoP1/QcXN5Bf</latexit><latexit sha1_base64="oI2GJniA5NkbcumT+2F6Za9h3Kk=">AAAB8nicbVDLSsNAFJ3UV62v+Ni5GSyiq5KoYF0IBTcuKxhbaEqYTKft0Jkkztwp1NAvcaO4UvwQf8G/MW2zaeuBgcM5Z7j3njARXIPj/FqFldW19Y3iZmlre2d3z94/eNKxUZR5NBaxaoZEM8Ej5gEHwZqJYkSGgjXCwd3EbwyZ0jyOHmGUsLYkvYh3OSWQSYF95PeIlCS49Nmz4cN0DGe3TmCXnYozBV4mbk7KKEc9sH/8TkyNZBFQQbRuuU4C7ZQo4FSwcck3miWEDkiPpdOdx/g0kzq4G6vsRYCn6lyOSK1HMsySkkBfL3oT8T+vZaBbbac8SgywiM4GdY3AEONJAbjDFaMgRhkhVPFsQ0z7RBEKWU2l7HR38dBl4l1Ubiruw1W5Vs07KKJjdILOkYuuUQ3dozryEEUv6A19oi/LWK/Wu/Uxixas/M8hmoP1/QcXN5Bf</latexit>

[ Rut, Suszalski, AR, in preparation ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 21: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Thermoelectric figure of merit

ZT =σS2Tκel + κph

,

where σ is the electrical conductivity, S-the Seebeck coefficient, κel(κph) - electronic (phononic) part of the thermal conductivity.

In the linear-responce regime, one can roughly approximate themaximal energy conversion efficiency

η =Pel

IQ≈ 1

4ZT

∆TT

(=

ZT4η?

)

(for ∆T � T ), with Pel – the maximal (usefull) electric power and IQ –the thermal current [see: Kim et al., PNAS 112, 8205 (2015)].

For instance, ZT =3, ∆T =100 K and T =300 K gives η ≈ 0.25,comparable with η? = 0.33 for a perfect Carnot engine.

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 22: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

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0 2 4 6 8 10

ZT

µ [meV]

ZTmax

ZTmax

0.04

0.08

0.12

0.

ZT

0.

0.4

0.8

1.2 (a)

(b)

(c)

(d)

LA+TA

LA+TA

LA+TA+ZA

U=0

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LA+TA+ZA

0.0

1.0

2.0

3.0

0 50 100 150 2000.0

0.2

0.4

0.6

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T=5 K

T=1 K T=1 K

T=5 K

ZT = S2σT/κ , with κ = κel + κph. We have µZTmax ≈ ∆/2; in contrast:

µSmax ≈ 1

2 kBT ln(2∆/kBT )� ∆/2. In effect, ZTmax is sensitive to T (E)

details near the band boundary and does not grow monotonicallywith ∆ (like |S|max). Instead, ZT reaches a global maximum for∆max∼102kBT . [ Rut, Suszalski, AR, in preparation ]

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .

Page 23: Low-temperature thermoelectric properties of bilayer grapheneth.if.uj.edu.pl › ~adamr › presentations › talk_StoCP2018.pdf · Thermoelectric properties Emergent Dirac fermions

IntroductionLandauer-Büttiker formalism

Thermoelectric properties

Quasiparticles in doped BLGSeebeck coefficient and Lorentz numberGapless vs gapped BLG

Acknowlegments

The group:

Grzegorz Rut Dominik Suszalski

Former collaboration: Anton Akhmerov,Jens Bardarson, Carlo Beenakker, PatrikRecher, Klaus Richter, Björn Trauzettel,Jakub Tworzydło, Michael Wimmer, . . .

Funding:

Project web site: http://th.if.uj.edu.pl/∼adamr/sonata.html

See also: Suszalski et al., POSTER NO. 15Rut et al., POSTER NO. 13

THANK YOU!

Rycerz, Suszalski, Rut, Low-temperature thermoelectric properties . . .