From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: Cross-sectional diagram of a superconductor-normal metal-superconductor Josephson junction. The electrodes are typically made of Nb, which become superconducting at temperatures below approximately 9K. The barrier is a normal metal.

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: Predicted and experimentally determined critical power of Nb-MoSi-Nb Josephson junctions. The data are from Chong . Two types of junctions with different bottom electrode-substrate interfaces are studied. The silicon substrates were maintained at 4K.

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: Predicted electron and phonon temperature profiles in the metal layer for three cases with different values of Lm∕δ

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: Predicted out-of-plane thermal resistance of Au films sandwiched between two dielectric materials at room temperature. The dashed line is obtained using the present two-fluid heat conduction model and the sold line using the conventional heat conduction model.

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: The thermal resistance of SiOx films near room temperature reported in the literature as a function of thickness. The y intercept is commonly interpreted as the thermal interface resistance.

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: Geometry and thermal boundary conditions used to analyze heat conduction across a metal layer sandwiched between two amorphous dielectric layers as part of a nanolaminate

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: The thermal resistance per unit thickness of W-AlOx nanolaminates at room temperature. The symbols are experimental data , the dotted line is the prediction of the conventional continuum heat conduction model, and the solid line is the prediction of the present two-fluid model. The nanolaminates were synthesized using the atomic layer deposition (ALD) technique at two different temperatures or using the magnetron sputtering technique (Magnetron) as described in .

From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces Date of download: 10/15/2017 Copyright © ASME. All rights reserved. From: Nanoscale Heat Conduction Across Metal-Dielectric Interfaces J. Heat Transfer. 2006;128(9):919-925. doi:10.1115/1.2241839 Figure Legend: The effective thermal conductivity of Ta∕TaOx nanolaminates plotted as a function of interface density at room temperature. The symbols are experimental data and the dotted line is the prediction of the present two-fluid model.