presentaciรณn de powerpointย ยท thermoelectric power generation. thermoelectric cooling....
TRANSCRIPT
M.R. Ibarra
Institute of Nanosciencie of AragรณnLaboratory of Advanced MicroscopiesCondensed Matter Physics Department
Outline
โข The concept of spin currrentsโข The thermoelectric conversionโข Introduction to Thermospin effectsโข SSE effects in [Fe3O4/Pt]n multilayersโข Spin Peltier effect in [Fe3O4/Pt]n multilayersโข Thermoelectric power: thermopilesโข Conclusions
Charge and spin currents
JS = 0
Jc
Jc = 0
JS JS
Jc = 0
Jc: charge current JS: spin current
Conduction-electronspin current
Spin wave (magnons)spin current
Pure Spin Currents
Net electron spin flow
Non-magneticMetal
MagneticInsulator
Magnon flow
Spin Hall effect (SHE)Interconversion of charge โ spin currents in materials with high spin orbit coupling (high Z)(Dyakanov & Parel 1971,Hirch 1999)
(Js) Spin (Jc) Charge
Jc
JS
US-L US-L
Inverse Spin Hall effect (ISHE)Interconversion of spin currents โ charge currents in non-magnetic metals with high spin orbit coupling (high Z)
(JS) Spin (Jc) Charge
Jc
JS US-L
Saitoh, E., Ueda, M., Miyajima, H., & Tatara, G. (2006). Conversion of spin current into charge current at room temperature: Inverse spin-Hall effect. Applied Physics Letters, 88(2006), 1โ4.
Thermoelectric effects
Seebeck effect: ๐๐ = ๐ธ๐ธ๐ป๐ป๐ป๐ป
๐ต๐ต๐ต๐ต
๐ฌ๐ฌ๐ฝ๐ฝ = ๐๐(๐ธ๐ธ โ ๐๐ ๐ป๐ป๐ป๐ป) = 0
Peltier effect: ฮ = ๐๐ ๐ป๐ป
๐ต๐ต๐ต๐ต
+
Thermoelectric power generation Thermoelectric cooling
๐๐๐ป๐ป =๐๐2๐๐๐ ๐
๐ป๐ป
๐ ๐ = ๐ ๐ ๐๐ + ๐ ๐ ๐๐ ๐ ๐ ๐๐ = ๐ฟ๐ฟ๐๐๐ป๐ป
๐ฟ๐ฟ =๐๐2
3๐๐๐ต๐ต๐๐
2
= 2.44 ร 10โ8 ๏ฟฝ๐๐ฮฉ๐พ๐พ2
Figure of merit
๐ต๐ต๐ฝ๐ฝ
Would it be posible thermoelectriceffect due to spin?
๐ต๐ต๐ต๐ต
๐ต๐ต๐ต๐ต
JS
Spin Peltier Effect (SPE)Spin Seebeck Effect (SSE)
JS
Heat vs. Electricity
To get Electricity To get Heat
Charge
Spin
Seebeck effect Peltier effect
Spin Seebeck effect
Uchida 2008
Spin Peltier effectFlipse 2014
Daimon 2016
Spin Seebeck effect effect: Spin current generation by heat
)( NFB
SS TTkGI โโ=
H. Adachi et al. PRB 83, 094410 (2011), Rep. Prog. Phys. 76, 036501 (2013)
J. Xiao et al. PRB 81, 214418 (2010)
Spintronics
Spin Seebeck
Effect
SeebeckEffect
16
Longitudinal spin Seebeck effect (LSSE)
Longitudinal SSE setup
paramagnet
ferromagnet
Inverse spin Hall effect:
K. Uchida et al.,Appl. Phys. Lett. 97, 172505 (2010).
EISHE = ฮธSHฯ(JS ร ฯ)
Spin Seebeck basic principles
โข Spin current proportional to applied thermal gradient
โข Injected spin current converted in electric voltage by the inverse spin Hall effect
H. Adachi et al. Phys. Rev. B 83, 094410,& Rep. Prog. Phys. 76, (2013) 036501
๐ธ๐ธ๐ผ๐ผ๐ผ๐ผ๐ผ๐ผ๐ธ๐ธ =๐๐๐ผ๐ผ๐ผ๐ผ๐๐๐ด๐ด
2๐๐โ
๐ฝ๐ฝ๐ผ๐ผ ร ๏ฟฝโ๏ฟฝ๐
๐ผ๐ผ๐ผ๐ผ = โ๐บ๐บ๐ผ๐ผ๐๐๐ต๐ตโ
(๐ป๐ป๐น๐น โ ๐ป๐ป๐๐)
J. Xiao et al. Phys. Rev. B 81, 214418
Magnon emission associatedwith spin accumulation at themetal-ferromagnet interface (Takahasi et al ICM 2009)
Spin angular momentumtransfer at the interface:Magnon and elecronspin currentinterconversion(Steven et al. PRB 86 (2012) 214424)
SPIN CURRENT AT THE INTERFACES
Fe3O4
Pt
Fe3O4
SSE in [F/N]n multilayers
Pt
Combined PLD & Sputtering
KrF Laser (ฮป = 248 nm)
PLD-sputtering (Neocera Llc) P180-sys
(Neocera Llc)
Sputtering module
21
Atomic resolution morphological characterization
MgO/(Fe3O4/Pt)
STEM-HAADF image
0,21 nm MgO
Fe3O4
Interface Fe3O4/MgO
0,39 nm
Pt
a~ 0,83 nm
Fe3O4
Pt
Fe3O4
50 nm
MgO
Fe3O4
Pt
FIB-Pt-C
23Atomic resolution chemical mapping of the interfaces
SSE vs number of Fe3O4/Pt bilayers
-8 -6 -4 -2 0 2 4 6 8-10
-5
0
5
10
V ML /
โT
(ยตV/
K)
H (kOe)
n = 1 n = 2 n = 3 n = 6
T = 300 K
n = 1
n = 6
SSE voltage enhancement with incresing number of Fe3O4/Ptbilayers
50 nmMgO
Fe3O4
Pt
50 nm
Ramos et al. Phys. Rev. B 92, 220407(Rap. Comm.) (2015)
-6 -4 -2 0 2 4 6
-0.5
0.0
0.5
1 x Pt/Fe3O4(tF), 300K
tF = 40 nm
(Vy/โ
T) (L
z/Ly)
(ยตV
/K)
H (kOe)
tF = 160 nm
tFPt
Fe3O4MgO
-6 -4 -2 0 2 4 6
-0.5
0.0
0.5 n = 4
H (kOe)
(Vy/โ
T)(L
z/Ly)
(ยตV/
K)
n = 1
n x Pt/Fe3O4(40), T=300 K
PtFe3O4
MgO
4 x
Fe3O4
Pt (15 nm)t (nm)
2mm
7mm
SSE dependence on Fe3O4 thickness
A. Anadรณn et al. 2016) APL (2016)
Dependence of SSE versus metal/insulator interlayer
Spin current across the multilayer must be considered
-8 -6 -4 -2 0 2 4 6 8-30
-20
-10
0
10
20
30
V ML /
โT
(ยตV/
K)
H (kOe)
n x Fe3O4/Pt(tN) n = 1 n = 6
GSSE
T = 300 K
Pt 15 nm
Pt 7 nm
Optimized configuration
-8 -6 -4 -2 0 2 4 6 8
-30
-20
-10
0
10
20
30 n = 12n = 6
V ML/โ
T (ยต
V/K)
H (kOe)
T = 300 K
n = 1
[Fe3O4(23)/Pt(7)]n
Largest SSE voltage measured in a thin film based structure!!
VML โ 28 ยตV/ K !!
29
Mechanism of LSSE enhancement in multilayer systems
Essence of LSSE enhancement: Boundary conditions for spin currents flowing normal to P/F interfaces
(i) spin currents must disappear at the top and bottom surfaces(ii) spin currents are continuous at the interfaces
Spin
cur
rent
PtFe3O4 Fe3O4
T = 300 K
z
PtFe3O4
Magnon spin current
Electron spin current
Qualitative agreement with experimental results
0 1 2 3 4 5 6 70
2
4
6
8
10
experiment
T = 300 K
S SSE (ยตV
/K)
Number of Fe3O4/Pt bilayers (n)
0.00
0.02
0.04
0.06
0.08
0.10
model
<JS>
Average SSE voltage measured:
๐ฝ๐ฝ๐ผ๐ผ =1๐ก๐ก๐๐๐๐
๏ฟฝ๐๐=1
๐๐๏ฟฝ
๐ง๐ง๐๐=0
๐ก๐ก๐๐
๐๐๐๐ ๐ฝ๐ฝ๐ ๐ (๐๐)(๐๐)
Maximum spin current at central interlayers
Envelope curve(JS(z)):
Ramos et al. Phys. Rev. B 92, 220407(Rap. Comm.) (2015)
(Ilustration from Graham Jones)
K. Uchida et al. Phys. Rev.B 95, 184437 (2017)
Spin peltier effect
K. Uchida et al. Phys. Rev.B 95, 184437 (2017)
Strong enhancement of the spin peltier effect in multiple bilayers
Spin Seebeck device
Wide area, low cost thermoelectric devices
Conventional charge thermoelectric device:
Many thermocouples necessaryHigh cost, difficulty in integration
T-gradient over centimeter scale neededThin film device difficult
Spin-Seebeck thermoelectric device
Many thermocouples unnecessaryLow cost, ultimate integration
T-gradient over nanometer scale is sufficientThin film device possible
(IMR, Tohoku Univ. / NEC / ASRC, JAEA/Zaragoza)
SSE thermopilesBilayer Multilayer
TP2TP1
Spin current conversiรณn at the interfaces F/N gives rise to anstrong enhancement of the thermospin effects in multiplebilayers and constitutes an excellent play ground for thestudy of new physical phenomena and promising for devicesapplication
K. Uchida et al. review Proceedings of the IEEE 104, 1499 (2016)
LSSE Termopower LSSE power factor
Monographic issue in Journal PhysD: Applied Physics on
CALORITRONICS to appear soon
Enhanced thermo-spin effects in iron-oxide/metal multilayers
R Ramos1, I. Lucas2,3,4, P. A. Algarabel4,5, L. Morellรณn2,3,4,K. Uchida6,7,8, E. Saitoh1,8,9,10 and M. R. Ibarra2,3,4,11
Development of thin-film thermoelectric SSE baseddevices
Strategic Japanese-Spanish Cooperative Research Program Nanotechnologies and new materials for environmental
challenges