Steady-State ThermoReflectance Fiberoptics (SSTR-F)

Steady-State ThermoReflectance Fiberoptics (SSTR-F) combines the technological power of laser based thermoreflectance experiments with the proven measurement capabilities of steady state thermal measurements that can accommodate sample sizes as small as a few hundred microns.

Best For Liquids, and Pastes

80K – 600K

Temperature
Range

Up to 100 microns

Spot Size

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Steady-State ThermoReflectance Fiberoptics

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    Features
    SSTR-F features
    SSTR-F
    • Absolute measurement of thermal conductivity
    • Thin films and coatings (> 1 micron)
    • Effective boundary resistance (thickness <1 micron)
    • Auto-scanning for thermal conductivity mapping
    • No inputs (i.e. heat capacity)
    FDTR
    • Multi-Thermophysical Properties
    • Thin films and coatings (> 5 nm)
    • Thermal Boundary Resistances
    SSTR-F measures thermal conductivity using the combination of laser based thermoreflectance techniques with traditional steady-state thermal testing concepts using the Hopkins Analysis. Harnessing decades of knowledge regarding the relationship between temperature and the thermoreflectance of metals, laser heating of a thin metal film on a material of interest allows for determination of the thermal conductivity of the underlying material without knowledge of the material’s heat capacity by probing the response of the metal due to the pump. These concepts, laser based pumpprobe experiments, have been utilized for decades to measure various optical, mechanical, and thermal properties of materials.

    Unlike most traditional free-space (exposed laser beams) pump-probe experiments, SSTR-F incorporates all of its active and passive components in fiber-optic leading to a compact, simple system with increased safety, no need for prior optical experience, and
    streamlined high throughput measurements.

    The technique works in principle by inducing a steady-state temperature rise in a material via long enough exposure to heating from a pump laser. A probe beam is then used to detect the resulting change in reflectance, which is proportional to the change in temperature at the sample surface. Increasing the power of the pump beam to induce larger temperature rises, Fourier’s law is used to determine the thermal conductivity.

    For expanded capabilities, the FDTR Testing Module may be added to the basic SSTR system. A key upgrade is the ability to measure thermal conductance and heat capacity of ultra-thin films – coatings down to a few nanometers thick. Understanding of the intrinsic and interface resistances between layers on a nano-scale, is a valued measurement for investigating the heat transfer efficiency of micro-electronics and related fields.

    Specification
    SSTR-F Specification
    Materials Solids and Liquids
    Thermal Conductivity Range 0.05 to 2500 W/m•K
    Directional Measurement Through-thickness and In-plane
    Spot Size Up to 100 microns
    Temperature Range 80K – 600K
    Accuracy 5%
    Repeatability 2%
    FDTR Specification
    Thermal Conductivity Range 0.05 to 2500 W/m•K
    Directional Measurement Through-thickness and In-plane
    Thin-film Thickness > 5 nm
    Sample Measurements
    the sample
    The Sample

    Samples of interest and sapphire sample are coated with a thin metal layer and sapphire sample is tested to determine the gamma coefficient.

    Approximate Time: 1 minute

    place the sample
    Place Sample

    Place sample on stage, specify number of tests, and specify spacing. Based on Z direction, the sample stage auto-focuses the laser.

    Approximate Time: 1 minute

    Run Experiment
    Run Experiment

    The scan routine starts with autofocus at every point and runs user specified number of tests.

    Approximate Time: < 2 minute

    Export Results to excel
    Exporting Results

    Calculations of thermal conductivity with associated error are computed and reported.

    Approximate Time: 1 minute

    Applications
    Bulk High Thermal Conductivity Small Samples
    SSTR-F Application

    Single Crystal silicon carbide (4H-SiC) wafer pieces of 2 mm diameter x 0.5 mm thickness were measured for thermal conductivity. SSTR-F testing results of 335 W/m·K +/- 28 W/m·K, correlated well with literature values (364 W/m·K) and traditional Time-domain Thermoreflectance (TDTR) measurements of 324 W/m·K.

    High Thermal Conductivity Coatings
    SSTR-F Application

    High-purity aluminum nitride (AIN) coatings were grown on sapphire wafers at thickness of 6 μm. This coating was measured with test spot of 20 μm and 40 μm, and values were within +/- 5% of each other. The measured AIN in-plane thermal conductivity was measured at average of 283.7 W/m·K across multiple sample locations. Thermal conductivity values were observed to vary widely (+/- 36.3 W/m·K) due to micro-structure, grain size and defect concentrations. Additional measurement of bulk thermal conductivity on coatings as thin as 1 μm are also possible with SSTR-F.

    High Resolution Thermal Mapping
    Thermal Diffusivity of Water

    Using the SSTR-F and automated X-Y movement testing stage, users are able to thermally map their samples for thermal conductivity. The testing spot size can be changed via varying objectives from 1 to 100 microns for sensitivity tuning, while the step size can be optimized to match the micro-structural length scales of a sample.

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      Featured Webinar

      Thermal Conductivity of cutting fluids with the Transient Hot Wire

      Depending on the context and on which type of cutting fluid is being considered, these fluids may be referred to as cutting fluid, cutting oil, cutting compound, coolant, or lubricant. The main purposes of these fluids are to keep the object being cut at a stable temperature, maximize the life of the cutting tip, and prevent rust on machine parts and cutters.

      December 8, 2021

      speakers

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      speakers

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