2016
DOI: 10.1103/physrevb.93.035309
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Thermal interface conductance across metal alloy–dielectric interfaces

Abstract: We present the first measurements of thermal interface conductance as a function of metal alloy composition. Composition spread alloy films of

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Cited by 20 publications
(17 citation statements)
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“…Kapitza conductance is extremely dependent on the structural details of the interface at the nanoscale since the characteristic dimensions are comparable to or less than the vibrational mean‐free paths. Nanostructuring at the interface has been efficiently used to tune the energy transport pathways across interfacial regions either by introducing roughness, nonplanar features, interface mixing, or by functionalizing the interface to alter the stiffness of the bonds …”
Section: Effect Of Nanostructuring and Surface Functionalizationmentioning
confidence: 99%
“…Kapitza conductance is extremely dependent on the structural details of the interface at the nanoscale since the characteristic dimensions are comparable to or less than the vibrational mean‐free paths. Nanostructuring at the interface has been efficiently used to tune the energy transport pathways across interfacial regions either by introducing roughness, nonplanar features, interface mixing, or by functionalizing the interface to alter the stiffness of the bonds …”
Section: Effect Of Nanostructuring and Surface Functionalizationmentioning
confidence: 99%
“…As shown in Figure 19, the TDTR signal is dominantly determined by the interfacial thermal conductance when delay time is longer than 2 ns. TDTR technique is therefore implemented extensively to study the thermal transport mechanisms across interfaces, including the effect of surface chemistry on interfacial thermal conductance across functionalized liquid-solid boundary [95,117,118] and solid-solid interfaces [119], interfacial thermal conductance between metals and dielectrics, [120][121][122][123][124] and interface between low dimensional materials and bulk substrates [125][126][127] Let's consider bulk materials first to introduce the physical picture we based on to determine heat capacity and thermal conductivity simultaneously. Under periodic laser heating, the penetration depth is defined as a characteristic length which describes the depth of temperature gradient penetrates into the sample can be written as , = √2 / 0 where 0 is the modulation frequency, is volumetric heat capacity and the index of directions corresponds to in-plane ( = ) and cross-plane ( = ) respectively.…”
Section: Transient Thermoreflectance Techniquementioning
confidence: 99%
“…where the constants are [7]. Following Jeong et al's approach to calculating G for adhesion layers, we treat phonon wavelengths smaller than the thickness of the adhesion layer as being transmitted from the adhesion layer to the dielectric, and larger wavelengths as being transmitted from the Au layer directly into the Al 2 O 3 [2].…”
Section: A Interdiffusion Composition Modellingmentioning
confidence: 99%
“…Adding as little as 1. interfaces, the value of G decreases as the Au content, x, increases [7]. While those two works quantify G at the extremes of interdiffusion (no interdiffusion and complete interdiffusion), it is unknown how an intermediate value of interdiffusion would affect G, despite its potential to compromise the thermal benefits of adhesion layers over the lifetime of a device.…”
Section: Introductionmentioning
confidence: 99%