Oxide Films & Nanostructures on Silicon for Thermal Energy Harvesting in Microelectronic Devices

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Oxide Films & Nanostructures on Silicon for Thermal Energy Harvesting in Microelectronic Devices R. Bachelet R. Moalla, A. Carretero-Genevrier, L. Mazet, L. Louahadj, J. Penuelas, B. Vilquin, C. Dubourdieu, G. Saint-Girons

Outline I. Intro: Context & INL presentation II. Thin films: n-type doped d SrTiO 3 III. Nanowires: Hollandites (BaMn 8 O 16 ) IV. Pyroelectric epitaxial thin films IV. Conclusions

Context: nanostructured materials for TE Material challenges/requirements: G.J. Snyder et al., Nat. Mat. 7, 105 (2008) C.J. Vineis et al., Adv. Mat. 22, 3970 (2010) K. Koumoto et al., J. Am. Ceram. Soc. 96, 1 (2013) ZT = S 2 T / (K e +K l ) ZT > 1 Semi-conductor materials Nanostructured => large, S => Decrease L Efficiency / Reliability (oxidation/intermixing ) Non toxic / Abundant elements Integration

Scientific and application fields 250 people (130 permanent) 7 900 m 2 NanoLyon platform 500 m 2 clean room Information technologies Hetero and Nano-structures Energy «Green technologies» Nanophotonics Nanomaterials Functionnal materials Photonics Photovoltaics Solar cells Nanocaracterisation Microtechnologies NANOLYON Technological Platform MOEMS Labs-on-a-chip Nanodevices MEMS-NEMS Electronics Heterogeneous design Biotechnologies Health Sensors Biochips Life science/ health care Technologies

NANOLYON technological platform A«proximity» platform for Micro- & Nano-Technologies To develop novel (nano)materials & novel concepts of devices & characterizations New clean rooms in 2013 (500 m 2 ) MBE Sputtering Sol-gel Lithography

III-V Nanostructures Semiconductor nanostructures: reducing dimensions at the nanoscale 2D: SLs & QWs 1D: NWs InP InAlAsP 200 nm 0D: QDs Works led by P. Regreny and Michel Gendry, H&N team, INL

Oxide Films and Nanostructures /Si 1. Thin films: n-type doped SrTiO 3 BaMn 2. Nanowires: Hollandites (BaMn O ) 8 O 16 8 16) 10 µm Si (Substrat) 3. Pyroelectric epitaxial thin films

1. n-type doped SrTiO 3 /Si SrTiO 3 : a model for oxide electronics Tuning (& S) By doping Doped by aliovalent cations La-STO: (La [3+],Sr [2+] )TiO 3 Doped by oxygen vacancies: T = 300 K G. Herranz et al. PRL 98, 216803 (2007) B. Jalan & S. Stemmer, APL 97, 042106 (2010)

1. n-type doped SrTiO 3 /Si Increasing interfaces at the nanoscale Superlattices (Nano)Polycrystalline Nb-STO: Sr(Ti [4+],Nb [5+] )O 3 ZT 300K > 1 with K min 1.4 W.m -1.K -1 S bulk = 61 V.K -1 ; n = 2-4 10 21 cm -3 ; n undoped < 10 15 cm -3 H. Ohta et al., Nat. Mat. 6, 129 (2007) S. Ohta et al., APL 87, 092108 (2005) K. Koumoto et al., J. Am. Ceram. Soc. 96, 1 (2013)

1. n-type doped SrTiO 3 /Si Epitaxial SrTiO 3 /Si 14 ML Doped by oxygen vacancies 1000 STO(110) (a) 100 W SrTiO 3- Int. (c cps) 100 10 (b) 200 W 20 30 40 50 60 70 2 ( ) nsity (a.u..) Inte (c) 300 W (d) 400 W SrTiO 3 G. Niu et al. APL 2009 L. Louahadj et al. 034 0,34 035 0,35 036 0,36 037 0,37 038 0,38 q // (Å -1 )

1. n-type doped SrTiO 3 /Si Electrical measurements (I-V) on p-type Si(001): => p-n junction Superlattices and 2DEGs LAO/STO SLs LaAlO 3 TE measurements: in progress STiO SrTiO 3 (, S, K) LaAlO 3 Collab: Fransisco Rivadulla (CIQUS, Spain) SrTiO 3 (Univ. Santiago de Compostela) Perspectives: - Full TE measures - SL polycristalline - doped / undoped O. Marty INL(UCBL) - p-type thin films C. Merckling et al. 4 nm

2. Oxide Nanowires of Hollandites Integration of 1D oxide nanowires in confined geometries (CSD) 1. Synthesis: track-etched polymer template assisted elaboration Pore size from 10 nm Precursor solution (sol gel) 700 1000 C Silicon A. Carretero-Genevrier et al., Chem. Soc. Rev. (2013)

2. Oxide Nanowires of Hollandites 2. Some results A. Carretero-Genevrier et al., Chem. Soc. Rev. (2013) Chem. Mater (2013) S 300K = 20 μv/k PF K 2 75K = 30 W/cm.K n=10 22 cm 3 Phys.Rev. B 79 085207 (2009

2. Oxide Nanowires of Hollandites 3. Perspectives Measuring TE parameters Composite materials (NWs + SC Matrix) n-& p-type materials Integration in modules (structuring, contacts, )

3. Pyroelectric epitaxial thin films Thermal energy harvesting for electrical conversion With Thermoelectrics I = f ( T) With Pyroelectrics (b) Electrode PE P s Pt BST PZT PMN PT I = f(dt/dt) Electrode Buffer SRO La STO LNO STO Si(001) Si SOI GaAs

3. Pyroelectric epitaxial thin films P (b) Electrode P s PE Electrode Buffer Pt BST PZT PMN PT SRO La STO LNO STO Si(001) Si SOI GaAs Polycristalline Single-crystalline Bulk materials ref + Thin films + ++? >1 mw/cm 3 for temperature variations of 10 C PhD thesis starting (R. Moalla): Collab. with LGEF-INSA (G. Sebald, D. Guyomar) S.B. Lang, Phys. Today 58, 31 (2005) G. Sebald et al., Smart Mater. Struct. 18, 125006 (2009)

3. Pyroelectric epitaxial thin films Ferroelectric ABO 3 /SrTiO 3 /Si PFM (Collab. B. Gautier, INL): P In progress: L. Mazet et al. R. Moalla et al. Material challenge: - High Pyroelectric coef. - High P - Out-of-plane P - Low leakage currents S. Yin et al., Thin Solid Films 520, 4572 (2012) G. Niu et al.,, Thin Sol. Films 520,, 4595 (2012) G. Niu et al., Microelec. Eng. 88, 1232 (2011) => BST, PZT, PMN-PT BST/SRO/STO/Si

Conclusions SrTiO 3 -based TE thin films by physical method 3 control of, S by doping & reducing K L by nanostructuring Hollandites Nanowires by original i chemical method control of density, diameter, chemical composition.. Need of full TE characterizations Alternatively, promising single-crystalline Pyroelectric films