1 / 44

Process Development for ZnO-based Devices

Process Development for ZnO-based Devices. Kelly Ip PhD Defense ~ July 1, 2005 ~ University of Florida ~ Materials Science and Enginering. Outline. Introduction Inductively-coupled plasma (ICP) etching Hydrogen in ZnO Contact metallization Ohmic contacts Schottky contacts

brice
Télécharger la présentation

Process Development for ZnO-based Devices

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Process Development for ZnO-based Devices Kelly Ip PhD Defense ~ July 1, 2005 ~ University of Florida ~ Materials Science and Enginering

  2. Outline • Introduction • Inductively-coupled plasma (ICP) etching • Hydrogen in ZnO • Contact metallization • Ohmic contacts • Schottky contacts • p-n junction diode • Conclusions

  3. Introduction GaNZnO Bandgap (eV)3.43.3 µe (cm2/V-sec)220200 µh (cm2/V-sec)105-50 me0.27mo0.24mo mh0.8mo0.59mo Exciton binding28 60 energy (meV) • Direct, wide bandgap • Bulk ZnO (n-type) commercially available • Grown on inexpensive substrates at low temperatures • High exciton binding energy • Heterojunction by substitution in Zn-site • Cd ~ 3.0 eV • Mg ~ 4.0 eV • Nanostructures demonstrated • Ferromagnetism at practical Tc when doped with transition metals • Obstacle: good quality, reproducible p-type Potential Applications UV/Blue optoelectronics Transparent transistors Nanoscale detectors Spintronic devices

  4. ICP Etching • Wet etching • HCl, HNO3, NH4Cl, and HF • Generally isotropic with limited resolution and selectivity • High-density plasma etching • Anisotropic with high resolution • Favored by modern manufacturing environment • Bulk, wurtzite (0001) ZnO from Eagle-Picher • Gas chemistry: • Cl2/Ar (10/5 sccm) & CH4/H2/Ar (3/8/5 sccm) • Constant ICP source power at 500W and process pressure at 1 mTorr • Varied rf chuck power: 50 – 300W

  5. ICP Etching - Etch Rates CH4/H2/Ar ~3000 Å/min Cl2/Ar ~1200 Å/min

  6. ICP Etching - Etch Mechanism Ion-Assisted Etch Mechanism ER  E0.5-ETH0.5 ETH ~ 96 eV for CH4/H2/Ar Vapor pressure of etch products: (CH4)2Zn 301 mTorr at 20°C ZnCl2 1 mTorr at 428 °C

  7. ICP Etching - Photoluminescence Optical degradation even at the lowest rf power

  8. ICP - AFM Control 100 W rf 50 W rf 200 W rf 300 W rf Zn and O etch products removed at same rate

  9. ICP Etching - AES and SEM Control O Zn CH4/H2/Ar 200W rf O Zn

  10. ICP Etching - Summary • Dry etching is possible with practical etch rates using CH4/H2/Ar • Surface is smooth and stoichiometric • Anisotropic sidewalls • Optical quality is sensitive to ion energy and flux

  11. Hydrogen in ZnO • Hydrogen • Predicted role as shallow donor • Introduced from growth ambient • Present in optimal plasma etch chemistry • Understand diffusion behavior and thermal stability • Bulk, wurtzite (0001) ZnO, undoped (n~1017cm-3) from Eagle-Picher • Hydrogen incorporation • Ion Implantation of 2H or 1H (100keV, 1015 - 1016 cm-2) • 2H plasma exposure in PECVD at 100-300°C, 30 mins • Post-annealing: 500 - 700°C

  12. Hydrogen in ZnO - Implanted - SIMS Removal of 2H below SIMS limit at 700°C Thermally less stable than GaN (>900ºC)

  13. Hydrogen in ZnO - Implanted - RBS/C Minimal affect on BS yield near surface Small increase in scattering peak (6.5% of the random level before implantation and 7.8% after implantation)  the nuclear energy loss profile of 100keV H+ is max

  14. Hydrogen in ZnO - Implanted - PL Severe optical degradation even after 700ºC anneal Point defect recombination centers dominate

  15. Hydrogen in ZnO - Plasma - SIMS Large diffusion depth 2H diffuses as an interstitial, with little trapping by the lattice elements or by defects or impurities

  16. Hydrogen in ZnO - Plasma/annealed - SIMS 2H completely evolve out of the crystal at 500°C

  17. Hydrogen in ZnO - Plasma - CV • Effects 2H plasma treatment • Passivate the compensating acceptor impurities • Induces a donor state and increases the free electron concentration Suggest H from growth process n-type conductivity probably arises from multiple impurity sources

  18. Hydrogen in ZnO Implanted Plasma exposure Implanted 2H is slightly more thermally stable: trapping at residual damage in the ZnO by the nuclear stopping process

  19. Hydrogen in ZnO - Summary • Thermal stability and diffusion behavior of hydrogen in ZnO • T  700 °C completely evolved the implanted H from ZnO • Residual implant-induced defects severely degrade optical properties and minimal affect crystal structure • Plasma: incorporation depths of about 30 m for 0.5 hr at 300°C • T  500 °C to remove H introduced by plasma exposure • Thermal stability of the hydrogen retention : • direct implantation > plasma exposure • Trapping at residual implant damage

  20. Ohmic Contacts • Require low specific contact resistance • Surface treatments • As-received • Organic solvents (trichloroethylene, methanol, acetone, 3 mins each) • H plasma • Ti/Al/Pt/Au metal scheme on n-type ZnO • Bulk • PLD films • Au/Ni/Au and Au on p-type ZnMgO

  21. Ohmic Contacts - Ti/Al/Pt/Au on Bulk Cross-sectional view of circular TLM Metals RO R1 Bulk n-ZnO C = RS LT2 Marlow and Das, Solid-State Electron. 25 91 (1982) ρc lowest at 250 °C anneal ρc ~ 610-4 cm2 Severe contact degradation after 600 °C anneal

  22. Ohmic Contacts - Ti/Al/Pt/Au on Bulk - AES

  23. Ohmic Contacts - Ti/Al/Pt/Au on Bulk - SEM

  24. Ohmic Contacts - Growth: n-type ZnO:P Films Hall Hall Post-growth Post-growth Carrier conc Carrier conc mobility mobility Resistivity Resistivity Anneal T Anneal T 3 3 2 2 W W (°C) (°C) (#/cm (#/cm ) ) ( ( cm) cm) (cm (cm /Vs) /Vs) 20 20 ´ ´ 1.5 1.5 10 10 30 30 0.002 0.002 18.5 18.5 19 19 ´ ´ 6 10 6 10 425 425 0.013 0.013 7.8 7.8 18 18 ´ ´ 2.4 2.4 10 10 450 450 1.3 1.3 1.9 1.9 17 17 ´ ´ 3.2 3.2 10 10 500 500 12.8 12.8 1.5 1.5 15 15 ´ ´ 7.5 7.5 10 10 600 600 463 463 1.8 1.8 • N-type phosphorus-doped ZnO film on (0001) Al2O3 grown by PLD • Post-growth annealing • Increase anneal temperature • Decrease carrier concentration and Hall mobility • Increase resistivity • Reduction of shallow state density • P dopants activation as acceptors in O site Heo et al APL 83 1128 (2003)

  25. Ohmic Contacts - Ti/Al/Pt/Au ZnO:P Films Ti/Al/Pt/Au (200/800/400/800)Å on PLD ZnO:P films Nonalloyed: n = 1.5  1020 cm-3 c = 8.7  10-7 -cm2 Annealed: Measured at RT: n = 6.0  1019 cm-3 c = 3.9  10-7 -cm2 Measured at 200 °C n = 2.4  1018 cm-3 c = 2.2  10-8 -cm2

  26. Ohmic Contacts - p-type ZnMgO Films • Ohmic behavior after annealing  500 °C • Ti/Au more thermally stable than Ni/Au contacts • Severe degradation of Ni/Au after 600 °C anneal S. Kim et al APL 84 1904 (2004)

  27. Ohmic Contacts - p-type ZnMgO Films Specific contact resistance after 600 °C anneal Au: 2.5  10-5 cm2 Au/Ni/Au: 7.6  10-6 cm2

  28. Ohmic Contacts - Au/ZnMgO

  29. Ohmic Contacts - Au/Ni/Au/ZnMgO

  30. Ohmic Contacts - Summary • Ti/Al/Pt/Au to n-type ZnO (bulk, thin film) • No significant improvement from H2 plasma treatment or organic solvent cleaning • AES revealed Ti-O interfacial reactions and intermixing between Al and Pt layers T250°C • Au/Ni/Au to p-type ZnMgO: lower C than Au alone

  31. Schottky Contacts Previous Works • Metals: Au, Ag, Pd • Schottky barriers heights ~ 0.6-0.8 eV • Barrier heights not following the difference in the work function value  interface defect states determine contact characteristics • Au is unstable even at 60°C This Work • Investigate the effect of UV surface cleaning • Metal schemes: • PLD n-type film: Pt • Bulk: Pt, W, W2B, W2B5, CrB2

  32. Schottky Contacts - Pt/Au on Bulk • No ozone treatment: Linear I-V • Ozone treatment: • B = 0.696 eV •  = 1.49 • Js = 6.17  10-6 A-cm-2

  33. Schottky Contacts - UV Ozone - AFM No Ozone Treatment 30 min Ozone Treatment

  34. Schottky Contacts - UV Ozone - XPS Desorption of surface C contaminants

  35. Schottky Contacts - W/Pt/Au on Bulk Sputter-induced damages • Non-rectifying for 250 °C and 500 °C anneal • Rectifying after 700 °C anneal

  36. Schottky Contacts - W/Pt/Au - AES • Post-deposition annealing  500 °C: no detectable intermixing • 700 C anneal: Zn diffused out to the Au-Pt interface, independent of whether the samples had been exposed to ozone

  37. Schottky Contacts - W2B5 vs. W2B W2B5/Pt/Au as deposited W2B/Pt/Au as deposited W2B5/Pt/Au 600ºC annealed W2B/Pt/Au 600ºC annealed

  38. Schottky Contacts - Summary • Ozone treatment removes surface C contamination • Pt contacts: ozone treatment produces transition from ohmic to rectifying behavior • W contacts: require annealing T  700°C to repair sputter-induced damages • AES revealed intermixing of metal layers and out-diffusion of Zn to Au-Pt interface • Low barrier heights for boride contacts • W2B showed good thermal stability  high temperature ohmic contacts

  39. p-n Junction Diode - Growth and Structure Circular ohmic contact (50 to 375 m diameter) Zn0.9Mg0.1O: P0.02 PLD film (~1.4 m) Buffer n-ZnO PLD film (~0.8 m) Bulk ZnO (0.5 mm, n ~ 1017 cm-3) Full backside ohmic contact • Pulsed laser deposition (PLD) • (0001) bulk ZnOsubstrate • Zn0.9Mg0.01O:P0.02 target • KrF excimer laser ablation source • Laser repetition rate: 1 Hz • Laser pulse energy density: 3 J-cm-2 • Growth: 400 °C, O2 overpressure of 20 mTorr Undoped buffer layer necessary for good rectifying behavior • Ohmic contacts: • p-ZnMgO: Pt/Au (200/800Å) • n-ZnO: Ti/Al/Pt/Au 200/400/200/800Å) • Annealed at 200 °C, 1 min, N2 ambient

  40. p-n Junction Diode - IV Characteristics Measured at room temp: VRB –9.0 V Js 4.610-9 A·cm-2 Vf 4.0 V RON 14.5 m ·cm-2

  41. p-n Junction Diode - Reverse Breakdown Temperature coefficient: Slightly negative ~ .1 to .2 V/K Presence of defects Non-optimized growth and processing

  42. p-n Junction Diode - Summary • Demonstrated ZnO-based p-n junctions • ZnMgO/ZnO heterostructure system • n-type ZnO buffer on the ZnO substrate is critical in achieving acceptable rectification in the junctions • Important step in realizing minority carrier devices in the ZnO system

  43. Conclusions • ICP etching • Methane-based chemistry • Practical etch rate but optical degradation • H in ZnO • Much less thermally stable than GaN • Completely evolve out by 700°C anneals • Ohmic contacts to ZnO • Straightforward n-type • Rapidly improving for p-type • Schottky contacts to ZnO • Low B for both n-type and p-type • Surface states dominate transport mechanism • p-n junction diode using ZnMgO/ZnO demonstrated

  44. Acknowledgements • Committee members: • Prof. Stephen Pearton, Chair • Prof. Cammy Abernathy • Prof. David Norton • Prof. Rajiv Singh • Prof. Fan Ren, External • Contributors:

More Related