Time-domain thermoreflectance (TDTR) measurements of anisotropic thermal conductivity using a variable spot size approach
Open accessAbstract
It is challenging to characterize thermal conductivity of materials with strong anisotropy. In this work, we extend the time-domain thermoreflectance (TDTR) method with a variable spot size approach to simultaneously measure the in-plane (Kr) and the through-plane (Kz) thermal conductivity of materials with strong anisotropy. We first determine Kz from the measurement using a larger spot size, when the heat flow is mainly one-dimensional along the through-plane direction, and the measured signals are only sensitive to Kz. We then extract the in-plane thermal conductivity Kr from a second measurement using the same modulation frequency but with a smaller spot size, when the heat flow becomes three-dimensional, and the signal is sensitive to both Kr and Kz. By choosing the same modulation frequency for the two sets of measurements, we can avoid potential artifacts introduced by the frequency-dependent Kz, which we have found to be non-negligible, especially for some two-dimensional layered materials like MoS2. After careful evaluation of the sensitivity of a series of hypothetical samples, we provided guidelines on choosing the most appropriate laser spot size and modulation frequency that yield the smallest uncertainty, and established a criterion for the range of thermal conductivity that can be measured reliably using our proposed variable spot size TDTR approach. We have demonstrated this variable spot size TDTR approach on samples with a wide range of in-plane thermal conductivity, including fused silica, rutile titania (TiO2 [001]), zinc oxide (ZnO [0001]), molybdenum disulfide (MoS2), hexagonal boron nitride (h-BN), and highly ordered pyrolytic graphite.
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TDTR has been applied to measure materials with thermal conductivity values ranging from about 2000 W m−1 K−1 (e.g., diamond and graphite) to as low as 0.03 W m−1 K−1 (e.g., disordered WSe2 films).
“In particular, time-domain thermoreflectance (TDTR) technique has been applied for measuring materials with thermal conductivity values ranging from a high end at ~2000 W m -1 K -1 (like diamond 36 and graphite 24, 37 ) to as low as 0.03 W m -1 K -1 (e.g., disordered WSe2 films 26 ).”
From Tutorial: Time-domain thermoreflectance (TDTR) for thermal property characterization of bulk and thin film materials (2018) · cites this paper as [37]
Results and Discussions (p. 19) says TDTR has been applied to measure through-plane conductivity from about 2000 W m−1 K−1 in diamond to about 0.03 W m−1 K−1 in disordered layered crystals and fullerene derivatives. The paper also reports an in-plane measurement near 2000 W m−1 K−1 for highly ordered pyrolytic graphite (table, p. 22). Our copy does not identify the low-conductivity material as disordered WSe2 films. (LLM, conf=0.86)
Experimental — accuracy not yet measuredVariable spot size TDTR can measure both in-plane and through-plane thermal conductivities by changing the relative size of the laser spot compared to the thermal penetration depth.
“By changing the relative size of laser spot as compared to the thermal penetration depth, as illustrated in Figure 18(a), TDTR can measure both the in-plane and the through-plane thermal conductivities.”
From Tutorial: Time-domain thermoreflectance (TDTR) for thermal property characterization of bulk and thin film materials (2018) · cites this paper as [37]
The Kc of ZnO determined from the elliptical-beam method (56 W m-1 K-1) is slightly lower than a first-principles calculation in literature (62 W m-1 K-1) but is consistent with another TDTR measurement of Kz of ZnO [0001] (55 W m-1 K-1).
“The Kc of ZnO determined from the elliptical-beam method (56 W m -1 K -1 ) is slightly lower than a first-principles calculation in literature (62 W m -1 K -1 ) 195 but is consistent with another TDTR measurement of Kz of ZnO [0001] (55 W m -1 K -1 ) 37 , which has its c -axis along the through-plane direction.”
From Tutorial: Time-domain thermoreflectance (TDTR) for thermal property characterization of bulk and thin film materials (2018) · cites this paper as [37]
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Thermoelectric effect and devices on IVA and VA Xenes
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Monolithic-3D Integration with 2D Materials: Toward Ultimate Vertically-Scaled 3D-ICs
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Self-citationPhonon and Thermal Properties of Thin Films Made from WS2 Mono- and Few-Layer Flakes
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Anisotropic Thermal Diffusivity Measurement of Thin Films: From a Few to Hundreds of Microns
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Thermal transport property of boron nitride nanosheets
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Thermal transport in metal halide perovskites and other third-generation photovoltaic materials
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A review of molecular dynamic simulation on polymer electrolyte membrane fuel cell
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Strained Polymer Thermal Conductivity Enhancement Counteracted by Additional Off-Axis Strain
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- Authors
- Jiang, P., Qian, X., & Yang, R.
- Affiliations
- University of Colorado Boulder (US)
- Venue
- Review of Scientific Instruments
- Publisher
- AIP Publishing
- Published
- 2017-07-01
- Volume
- 88
- Issue
- 7
- Pages
- 074901-074901
- ISSN
- 0034-6748 (ISSN-L)
- 1089-7623
- OpenAlex
- W2605963437
- Cited by
- 175
- References
- 49
- Citations by year
- 2026: 19 · 2025: 23 · 2024: 25 · 2023: 22 · 2022: 18 · 2021: 25 · 2020: 14 · 2019: 12 · 2018: 13 · 2017: 4
- FWCI
- 4.97
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Review of Scientific Instruments (publishedVersion)
- PubMed (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- arXiv (Cornell University)
- Funders
- National Science Foundation (1511195)
- Defense Advanced Research Projects Agency (FA8650-15-1-7524)
- Topics
- Physical Sciences › Materials Science › Materials Chemistry › Thermal properties of materials
- Physical Sciences › Engineering › Mechanics of Materials › Thermography and Photoacoustic Techniques
- Physical Sciences › Engineering › Mechanical Engineering › Mechanical and Thermal Properties Analysis
- Keywords
- time-domain thermoreflectance, anisotropic thermal conductivity, in-plane thermal conductivity, through-plane thermal conductivity, MoS2, hexagonal boron nitride, pyrolytic graphite, rutile TiO2, zinc oxide, fused silica, measurement uncertainty
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