Thermal Conductivity Comparison of Indium Gallium Zinc Oxide Thin

Mar 9, 2016 - †Graduate Program in Applied Physics, ‡Department of Electrical Engineering and Computer Science, §Department of Material Science a...
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Thermal Conductivity Comparison of Indium-Gallium-Zinc-Oxide Thin Films: Dependence on Temperature, Crystallinity, and Porosity Boya Cui, Li Zeng, Denis T. Keane, Michael J. Bedzyk, D. Bruce Buchholz, Robert P. H. Chang, Xinge Yu, Jeremy Smith, Tobin J. Marks, Yu Xia, Antonio F. Facchetti, Julia E. Medvedeva, and Matthew Grayson J. Phys. Chem. C, Just Accepted Manuscript • DOI: 10.1021/acs.jpcc.5b12105 • Publication Date (Web): 09 Mar 2016 Downloaded from http://pubs.acs.org on March 11, 2016

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Thermal Conductivity Comparison of Indium-Gallium-Zinc-Oxide Thin Films: Dependence on Temperature, Crystallinity, and Porosity

Boya Cui,

†, ‡

Li Zeng,



Robert P. H. Chang,

Denis Keane,

†, ¶

Xinge Yu,

Antonio F. Facchetti,

†Graduate

k, ⊥

¶,§ k

Michael J. Bedzyk,

Jeremy Smith,

k

Julia E. Medvedeva,

†, ¶

D. Bruce Buchholz,

Tobin J. Marks,

#

k

and M. Grayson

Xia Yu,





∗,†,‡

Program in Applied Physics, Northwestern University, Evanston, IL 60208, USA

‡Department

of Electrical Engineering and Computer Science, Northwestern University, Evanston, IL 60208, USA

¶Department

of Material Science and Engineering, Northwestern University, Evanston, IL 60208, USA

§Northwestern kDepartment

Synchrotron Research Center, Argonne, IL 60439

of Chemistry, Northwestern University, Evanston, IL 60208, USA

⊥Polyera #Department

Corporation, Skokie, IL 60077, USA

of Physics, Missouri University of Science and Technology, Rolla, MO 65409, USA

E-mail: [email protected].

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Abstract The cross-plane thermal conductivity of InGaZnO (IGZO) thin lms was measured using the 3ω technique from 18 K to 300 K. The studied morphologies include amorphous (a-IGZO), semicrystalline (semi-c-IGZO), and c-axis-aligned single-crystal-like IGZO (c-IGZO) grown by pulsed laser deposition (PLD), as well as a-IGZO deposited by sputtering and by solution combustion processing. The atomic structures of the amorphous and crystalline lms were simulated within ab-initio molecular dynamics. The lm quality and texturing information was assessed by X-ray diraction and grazing incidence wide-angle X-ray scattering. X-ray reectivity was also conducted to quantify lm densities and porosities. All the high-density lms exhibit an empirical power-law temperature dependence of the thermal conductivity κ ∼ T 0.6 in the specied temperature range. Among the PLD dense lms, semi-c-IGZO exhibits the highest thermal conductivity, remarkably exceeding both lms with more order (c-IGZO) and with less order (a-IGZO) by a factor of 4. The less dense combustion-synthesized lms, on the other hand, exhibited lower thermal conductivity, quantitatively consistent with a porous lm using either an eective medium or percolation model. All samples are consistent with the porosity-adapted Cahill-Pohl (p-CP) model of minimum thermal conductivity.

1 Introduction Indium gallium zinc oxide (IGZO) thin lms have attracted scientic and technological attention due to their high carrier mobility, low intrinsic carrier concentration, good optical transparency, and consistent uniformity over large areas. for device applications

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These IGZO properties are useful

such as display backplanes, smart windows, and low-cost exible

transparent electronics. Single-crystalline IGZO was rst proposed to be a high-performance active channel material in transparent eld-eect transistors since electron mobilities as high as

µ≈

2 1 80 cm /(V·s) were reported. Furthermore, amorphous phase a-IGZO is also useful

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for exible electronics owing to the ability to process at room-temperature mobilities

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and achieve

2 2 cm /(V·s) far exceeding that of amorphous silicon (a-Si:H). Most studies

µ >10

have focused on characterizing and optimizing electrical and optical properties, however, a careful study of the thermal properties has been lacking.

Such a study of IGZO thermal

conductivity is useful for eective thermal management in IGZO devices, such as thin-lm transistors in display backplanes.

Knowledge of the thermal conductivity helps to model

heat generation within that active layer and the thermal distribution throughout the device.

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Additionally, IGZO has been proposed as a thermoelectric candidate, in a similar fashion to other transparent oxides such as gure of merit

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10

InZnO. IGZO may have a competitive thermoelectric

compared with other oxide materials, suggesting the intriguing possibility

of invisible thermoelectric devices" made with transparent oxides.

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Furthermore, the

large-area capabilities might allow for integration into solar panels for photovoltaic/thermal hybrid systems

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to generate power from unavoidable waste heat. It might also act as the n-

type layer of the recently proposed p ×n -type transverse thermoelectrics

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for novel thermal

management geometries. Moreover, an understanding of thermal transport in a-IGZO may yield clues to dierentiate various fabrication methods, linking the thermal properties to the lm structure and fabrication technique and eventually identifying strategies for improving electron mobility. To our knowledge, there are only a few prior studies on IGZO thermal conductivity and those were conducted at room temperature, only. Seo et al.

12

κ,

studied the thermoelectric

performance of sputtered IGZO thin lms and reported that, remarkably, the more ordered crystalline lm has a factor of 7 lower thermal conductivity than the less ordered polycrystalline lm.

This counter-intuitive variation of thermal conductivity on morphology

begs conrmation, as well as motivating a more detailed temperature-dependent study to achieve a better understanding of the underlying physics. Thermal conductivity for sputtered a-IGZO thin lms

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was also reported, but again only at room temperature, thereby limiting

the utility in comparing with theory.

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This work will examine the temperature-dependent thermal conductivity of IGZO thin lms fabricated with dierent techniques that are systematically analyzed and compared. Growth methods for comparison include pulsed laser deposition (PLD), sputtering, and spray-

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and spin-combustion

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solution processing. Among the PLD lms, a series was grown

under dierent conditions to vary the crystallinity, from amorphous (a-), to semi-crystalline (semi-c-), to single-crystal-like (c-) phases. Ab-initio molecular dynamics is also employed to determine the local structure of amorphous IGZO and to compare the room-temperature atomic displacements in a- and c-IGZO. X-ray studies, including X-ray diraction (XRD), grazing incidence wide angle scattering (GIWAXS) and X-ray reectivity (XRR), complement the thermal conductivity studies to assess the lm density, porosity, crystallinity, and crystal orientation of the lms processed by various means.

The temperature-dependent

thermal conductivity of IGZO thin lms is characterized from 18 K to 300 K using the 3 ω technique. Following the theoretical literature, we will adopt the term "vibrons"

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to refer to the

generic vibrational modes responsible for thermal transport, since phonons represent relevant modes of heat propagation only in crystalline materials. We note that in all morphologies, the heat is primarily conducted through vibrons rather than electrons, because even for highly doped IGZO lms with electrical conductivity the thermal conductivity is only

σ = 100

σe = 7.3 × 10−2

S/cm the electronic contribution to

W/(m · K) according to Wiedemann −Franz

law  less than 10 % of even the poorest thermally conducting PLD lm. conductivity

σ

of IGZO can be tuned in a wide range

6



= 10−3 ∼ 102

The electrical

S/cm) to target

various applications, but all the lms under study were grown to have relatively low

5 × 10−1

S/cm to guarantee negligible electron contribution.

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σ