Fabrication of ZnO Nanowire Arrays for Hybrid Photovoltaic ... ZnO MRS Poster.pdfNov 15, 2012  ·...

1
Experimental Setup Effect of Growth Conditions Conclusions Fabrication of ZnO Nanowire Arrays for Hybrid Photovoltaic Applications Joshua A. Taillon, Luz J. Martínez-Miranda, and Lourdes G. Salamanca-Riba University of Maryland, Department of Materials Science and Engineering, College Park, MD 20742 Primary goals: Controlled fabrication of uniform ZnO nanowire arrays on Si substrates via chemical vapor deposition with vapor-liquid-solid (VLS) mechanism Optimization of growth parameters Fabrication of hybrid photovoltaic cells using ZnO and smectic octylcyanobiphenyl (8CB) liquid crystals Summary of work: Achieved reproducible growth of ZnO nanowire arrays on Si in horizontal tube furnace Determined effect of various growth parameters on resulting arrays Observed enhanced optical absorption when nanowires and liquid crystal are combined Nanowires seem to grow by non-VLS mechanism Goals and Summary References This work was supported in part by the National Science Foundation under the University of Maryland MRSEC DMR 05-20471. We acknowledge the support of the Maryland NanoCenter and its FabLab in the fabrication of the nanowire arrays, including Thomas Loughran and Jonathan Hummel. We also acknowledge the support of the Maryland Nanocenter and its NispLab. The NispLab is supported in part by the NSF as a MRSEC Shared Experimental Facility. Acknowledgments Motivation Methods & Experimental Parameters Creating offspring from parent structures [4] GA creating convex hull for binary alloy system [4] Common Nanowire Array Growth Morphologies Reflectivity: Nanowires with Liquid Crystal Alternate Synthesis Design Joshua A. Taillon Materials Science and Engineering University of Maryland College Park 1240 Jeong H. Kim Engineering Building 225 College Park, MD 20742 USA Contact Horizontal tube furnace (: 1 atm) Source Zn and substrates in alumina boats Au thin film catalyst layer (2 nm) Si (001) wafer with native SiO 2 oxide layer Inert Ar carrier gas = 700 − 850°C Future Work Setup reproducibly grows ZnO nanowire arrays Vertical alignment needs improvement VLS mechanism not active Growth results are heavily dependent on a wide range of experimental parameters Localized conditions greatly affect results, e.g., Zn vapor pressure, O 2 partial pressure Most promising conditions: Lowest possible flow rates (less turbulence) Lowest 2 (lowers oxidation rate) Earlier O 2 release (steady state conditions) Less Zn source (reduces Zn vapor saturation) Approaching optimized conditions for VLS growth “Showerhead” O 2 delivery shows great promise Optical absorption is higher when nanowires are combined with liquid crystal Further investigation of new furnace geometry Characterize effect of other growth parameters: Total chamber pressure Substrate/source temperature Distance between source and substrate Growth time and furnace heating rate Fabricate proof-of-concept devices Measure photoconductivity of ZnO nanowires with liquid crystal Characterize liquid crystal orientation effect of nanowires relative to ZnO nanoparticles [1] M. Grätzel, Inorganic Chemistry 44, 6841 (2005). [2] H.E. Unalan, P. Hiralal, D. Kuo, B. Parekh, G. Amaratunga, and M. Chhowalla, Journal of Materials Chemistry 18, 5909 (2008). [3] L. Schmidt-Mende, A. Fechtenkötter, K. Müllen, E. Moons, R.H. Friend, and J.D. MacKenzie, Science (New York, N.Y.) 293, 1119 (2001). [4] L.J. Martínez-Miranda, K.M. Traister, I. Meléndez-Rodríguez, and L. Salamanca-Riba, Applied Physics Letters 97, 223301 (2010). [5] R.S. Wagner and W.C. Ellis, Applied Physics Letters 4, 89–90 (1964). [6] M.H. Huang,Y. Wu, H. Feick, N. Tran, E. Weber, and P.Yang, Advanced Materials 13, 113 (2001). [7] Y.-T.Yin,Y.-Z. Chen, C.-H. Chen, and L.-Y. Chen, Journal of the Chinese Chemical Society 58, (2011). [8] A.B. Djurišić, A.M.C. Ng, and X.Y. Chen, Progress in Quantum Electronics 34, 191 (2010). [9] J. Park, H.-H. Choi, K. Siebein, and R.K. Singh, Journal of Crystal Growth 258, 342 (2003). Email: [email protected] Website: http://www.joshuataillon.com W: (301) 405-3314 Hybrid Photovoltaic Design Nanowire Array Crystallinity Combination of inorganic nanostructures and organic material can improve absorption and mechanical properties Dye-sensitized solar cells [1] Flexible ZnO/P3HT bulk heterojunctions [2] Liquid crystal photovoltaics can self-organize, enhancing charge transfer along axis of orientation [3] Incorporating ZnO nanoparticles enhances order of liquid crystal, greatly improving hole mobility [4] ITO ITO Liquid Crystal ZnO Could a continuous inorganic pathway (nanowires) have the same effect? Enhanced hole conduction from liquid crystals Enhanced electron conduction in nanowires Can we control the morphology of ZnO nanowire arrays? Use smectic octylcyanobiphenol (8CB) to investigate ordering between liquid crystal and nanowires Compare to ordering with nanoparticles ITO Au Catalyst n-Si Substrate ZnO Liquid Crystal 2.25 eV 8CB 2.3 eV ZnO 4.2 eV 3.7 eV Expected band structure ZnO: electron conductor 8CB: hole conductor Schematic of VLS growth [5] Vapor-liquid-solid nanowire growth method [5] Chemical vapor deposition technique Catalyst metal thin film Metal droplet acts as seed for nanowire Has been used successfully for ZnO aligned nanowire array synthesis [6,7] Zn powder and O 2 gas source materials Results are strongly dependent on experimental conditions and particular sample geometry [8] Growth parameters investigated in this study: Total gas flow rate (O 2 + Ar carrier gas) Relative gas flow rates (Ar:O 2 ratio) Timing of gas release Mass of Zn source powder Geometry of interior components Affects substrate temperature and local 2 and A. Uniform diameters; narrow wires grow from textured ZnO film B. Tetrapod “overgrowth” extended above nanowire growth HRTEM and XRD: Nanowires are high quality and single-crystalline Grow along [0001] direction Fairly uniform diameter No evidence for VLS growth (metal at tip) C. Thicker diameters; inferior alignment; non- uniform shape and size D. Mix of “nanobelts,” “nanorods,” tetrapods, and “nanoribbons” Preliminary reflectivity measurements Using poorly-aligned but uniform 200 nm diameter array Measure pure liquid crystal and hybrid system Witnessed decreased reflection reflection = absorption Both liquid crystal and nanowires contribute to photoabsorption 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 299 382 464 545 624 702 Reflectivity Wavelength (nm) NW + liquid crystal Liquid crystal only Total Gas Flow: Lower flow rates decreases branching and allows for more controlled growth Relative Gas Flow Ratio: Lower oxygen partial pressure suppresses tetrapod overgrowth and encourages vertical wire alignment Oxygen Gas Release Time: Earlier gas release improves uniformity and nanowire shape/alignment steady state growth Oxidation of source before melting can prevent Zn vapor formation if not enough Zn source used Zn Source Mass: Reduced source mass discourages top-level overgrowth and improves uniformity, to a point Too little Zn source can cause early oxidation and prevent evaporation into Zn vapor 110 sccm 55 sccm 22 sccm Ar:O 2 = 10:1 T = 700 C Zn mass = 0.4 g Ar:O 2 = 20:4 Total flow: 21 – 24 sccm T = 700 C Zn mass = 0.4 g Ar:O 2 = 20:1 Ar:O 2 = 20:2 O 2 on at 700°C Ar:O 2 = 20:2 T = 700 C Zn mass = 0.4 g O 2 on at 400°C O 2 on at 20°C Zn = 0.4 g Ar:O 2 = 20:2 T= 700 C Zn mass = 0.4-0.1 g Zn = 0.2 g Zn = 0.1 g When using low source mass (0.2 g and below) and earlier O 2 gas release, Zn source has tendency to oxidize with a skin, preventing evaporation Introducing O 2 directly at substrate allows for finer control of growth conditions: Geometry and local 2 can be finely controlled Oxidation of source is prevented Greater flexibility in localized conditions Design after J. Park et al. [9]: “Showerhead” O 2 delivery Releases O 2 immediately to substrate Preliminary Results: Showerhead prevents source oxidation Did not immediately observe VLS as in [9] Changing internal geometry significantly affected growth results (need further optimization)

Transcript of Fabrication of ZnO Nanowire Arrays for Hybrid Photovoltaic ... ZnO MRS Poster.pdfNov 15, 2012  ·...

  • Experimental Setup Effect of Growth Conditions

    Conclusions

    Fabrication of ZnO Nanowire Arrays for Hybrid Photovoltaic Applications

    Joshua A. Taillon, Luz J. Martínez-Miranda, and Lourdes G. Salamanca-Riba

    University of Maryland, Department of Materials Science and Engineering, College Park, MD 20742

    Primary goals:• Controlled fabrication of uniform ZnO nanowire

    arrays on Si substrates via chemical vapor deposition with vapor-liquid-solid (VLS) mechanism

    • Optimization of growth parameters • Fabrication of hybrid photovoltaic cells using ZnO

    and smectic octylcyanobiphenyl (8CB) liquid crystals

    Summary of work:• Achieved reproducible growth of ZnO nanowire

    arrays on Si in horizontal tube furnace• Determined effect of various growth parameters on

    resulting arrays• Observed enhanced optical absorption when

    nanowires and liquid crystal are combined• Nanowires seem to grow by non-VLS mechanism

    Goals and Summary

    References

    • This work was supported in part by the National Science Foundation under the University of Maryland MRSEC DMR 05-20471.

    • We acknowledge the support of the Maryland NanoCenter and its FabLab in the fabrication of the nanowire arrays, including Thomas Loughran and Jonathan Hummel.

    • We also acknowledge the support of the Maryland Nanocenter and its NispLab. The NispLab is supported in part by the NSF as a MRSEC Shared Experimental Facility.

    Acknowledgments

    Motivation

    Methods &Experimental Parameters

    Creating offspring from parent structures [4]

    GA creating convex hull for binary alloy system

    [4]

    Common Nanowire ArrayGrowth Morphologies

    Reflectivity: Nanowires with Liquid Crystal

    Alternate Synthesis Design

    Joshua A. Taillon• Materials Science and Engineering• University of Maryland College

    Park• 1240 Jeong H. Kim Engineering• Building 225• College Park, MD 20742 USA

    Contact

    • Horizontal tube furnace (𝑃: 1 atm)

    • Source Zn and substrates in alumina boats

    • Au thin film catalyst layer (2 nm)

    • Si (001) wafer with native SiO2 oxide layer

    • Inert Ar carrier gas

    • 𝑇 = 700 − 850°C

    Future Work

    • Setup reproducibly grows ZnO nanowire arrays

    • Vertical alignment needs improvement

    • VLS mechanism not active

    • Growth results are heavily dependent on a wide

    range of experimental parameters

    • Localized conditions greatly affect results,

    e.g., Zn vapor pressure, O2 partial pressure

    • Most promising conditions:

    • Lowest possible flow rates (less turbulence)

    • Lowest 𝑃𝑂2 (lowers oxidation rate)

    • Earlier O2 release (steady state conditions)

    • Less Zn source (reduces Zn vapor saturation)

    • Approaching optimized conditions for VLS growth

    • “Showerhead” O2 delivery shows great

    promise

    • Optical absorption is higher when nanowires are

    combined with liquid crystal

    • Further investigation of new furnace geometry

    • Characterize effect of other growth parameters:

    • Total chamber pressure

    • Substrate/source temperature

    • Distance between source and substrate

    • Growth time and furnace heating rate

    • Fabricate proof-of-concept devices

    • Measure photoconductivity of ZnO nanowires

    with liquid crystal

    • Characterize liquid crystal orientation effect of

    nanowires relative to ZnO nanoparticles

    [1] M. Grätzel, Inorganic Chemistry 44, 6841 (2005).

    [2] H.E. Unalan, P. Hiralal, D. Kuo, B. Parekh, G. Amaratunga, and

    M. Chhowalla, Journal of Materials Chemistry 18, 5909

    (2008).

    [3] L. Schmidt-Mende, A. Fechtenkötter, K. Müllen, E. Moons, R.H.

    Friend, and J.D. MacKenzie, Science (New York, N.Y.) 293,

    1119 (2001).

    [4] L.J. Martínez-Miranda, K.M. Traister, I. Mele ́ndez-Rodríguez,

    and L. Salamanca-Riba, Applied Physics Letters 97, 223301

    (2010).

    [5] R.S. Wagner and W.C. Ellis, Applied Physics Letters 4, 89–90

    (1964).

    [6] M.H. Huang, Y. Wu, H. Feick, N. Tran, E. Weber, and P. Yang,

    Advanced Materials 13, 113 (2001).

    [7] Y.-T. Yin, Y.-Z. Chen, C.-H. Chen, and L.-Y. Chen, Journal of the

    Chinese Chemical Society 58, (2011).

    [8] A.B. Djurišić, A.M.C. Ng, and X.Y. Chen, Progress in Quantum

    Electronics 34, 191 (2010).

    [9] J. Park, H.-H. Choi, K. Siebein, and R.K. Singh, Journal of

    Crystal Growth 258, 342 (2003).

    Email: [email protected]: http://www.joshuataillon.com

    W: (301) 405-3314

    Hybrid Photovoltaic DesignNanowire Array

    Crystallinity

    • Combination of inorganic nanostructures and

    organic material can improve absorption and

    mechanical properties

    • Dye-sensitized solar cells [1]

    • Flexible ZnO/P3HT bulk heterojunctions [2]

    • Liquid crystal photovoltaics

    can self-organize, enhancing

    charge transfer along axis of

    orientation [3]

    • Incorporating ZnO

    nanoparticles enhances

    order of liquid crystal,

    greatly improving hole

    mobility [4]

    ITO

    ITOLiquid

    Crystal

    ZnO

    • Could a continuous inorganic pathway

    (nanowires) have the same effect?

    • Enhanced hole conduction from liquid crystals

    • Enhanced electron conduction in nanowires

    • Can we control the morphology of ZnO

    nanowire arrays?

    • Use smectic

    octylcyanobiphenol (8CB)

    to investigate ordering

    between liquid crystal and

    nanowires

    • Compare to ordering

    with nanoparticles

    ITO

    Au Catalyst

    n-Si Substrate

    ZnOLiquid Crystal

    2.25 eV

    8CB

    ∼2.3 eVZnO4.2 eV

    3.7 eV

    • Expected band

    structure

    • ZnO: electron

    conductor

    • 8CB: hole

    conductor

    Schematic of VLS growth [5]

    • Vapor-liquid-solid nanowire

    growth method [5]

    • Chemical vapor

    deposition technique

    • Catalyst metal thin film

    • Metal droplet acts as

    seed for nanowire

    • Has been used successfully for ZnO aligned

    nanowire array synthesis [6,7]

    • Zn powder and O2 gas source materials

    • Results are strongly dependent on experimental

    conditions and particular sample geometry [8]

    • Growth parameters investigated in this study:

    • Total gas flow rate (O2 + Ar carrier gas)

    • Relative gas flow rates (Ar:O2 ratio)

    • Timing of gas release

    • Mass of Zn source powder

    • Geometry of interior components

    • Affects substrate temperature and

    local 𝑃𝑂2 and 𝑃𝑍𝑛 𝑣

    A. Uniform diameters;

    narrow wires grow from

    textured ZnO film

    B. Tetrapod “overgrowth”

    extended above

    nanowire growth

    • HRTEM and XRD:

    • Nanowires are high quality and single-crystalline

    • Grow along [0001] direction

    • Fairly uniform diameter

    • No evidence for VLS growth (metal at tip)

    C. Thicker diameters;

    inferior alignment; non-

    uniform shape and size

    D. Mix of “nanobelts,”

    “nanorods,” tetrapods,

    and “nanoribbons”

    • Preliminary reflectivity measurements

    • Using poorly-aligned but uniform 200 nm

    diameter array

    • Measure pure liquid crystal and hybrid system

    • Witnessed decreased reflection

    • ↓ reflection = ↑ absorption• Both liquid crystal and nanowires contribute to

    photoabsorption

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    299 382 464 545 624 702

    Refl

    ecti

    vit

    y

    Wavelength (nm)

    NW + liquid crystal

    Liquid crystal only

    Total Gas Flow:

    • Lower flow rates decreases branching and allows for more controlled growth

    Relative Gas Flow Ratio:

    • Lower oxygen partial pressure suppresses tetrapod overgrowth and encourages vertical wire alignment

    Oxygen Gas Release Time:

    • Earlier gas release improves uniformity and

    nanowire shape/alignment → steady state growth

    • Oxidation of source before melting can prevent Zn vapor formation if not enough Zn source used

    Zn Source Mass:

    • Reduced source mass discourages top-level overgrowth and improves uniformity, to a point

    • Too little Zn source can cause early oxidation and prevent evaporation into Zn vapor

    110 sccm

    55 sccm

    22 sccm

    Ar:O2 = 10:1T = 700 C

    Zn mass = 0.4 g

    Ar:O2 = 20:4

    Total flow: 21 – 24 sccm

    T = 700 C

    Zn mass = 0.4 g

    Ar:O2 = 20:1

    Ar:O2 = 20:2

    O2 on at 700°C

    Ar:O2 = 20:2

    T = 700 C

    Zn mass = 0.4 g

    O2 on at 400°C

    O2 on at 20°C

    Zn = 0.4 g

    Ar:O2 = 20:2

    T= 700 C

    Zn mass = 0.4-0.1 g

    Zn = 0.2 g

    Zn = 0.1 g

    • When using low source mass (0.2 g and below)

    and earlier O2 gas release, Zn source has tendency

    to oxidize with a skin, preventing evaporation

    • Introducing O2 directly at substrate allows for

    finer control of growth conditions:

    • Geometry and local 𝑃𝑂2can be finely controlled

    • Oxidation of source is prevented

    • Greater flexibility in localized conditions

    • Design after J. Park et al. [9]:

    • “Showerhead” O2 delivery

    • Releases O2 immediately to substrate

    Preliminary Results:

    • Showerhead prevents source oxidation

    • Did not immediately observe VLS as in [9]

    • Changing internal geometry significantly

    affected growth results (need further

    optimization)

    mailto:[email protected]://www.joshuataillon.com/