Apr 25, 2024
2:45pm - 3:00pm
Room 327, Level 3, Summit
Marat Khafizov1,Vinay Chauhan1,Hao Ma2,Zilong Hua3,Azat Abdullaev4,Shadman Priam1,Saqeeb Adnan1,Erika Nosal1,Michael Manley2,Zhandos Utegulov4,Lingfeng He5,David Hurley3
The Ohio State University1,Oak Ridge National Laboratory2,Idaho National Laboratory3,Nazarbayev University4,North Carolina State University5
Marat Khafizov1,Vinay Chauhan1,Hao Ma2,Zilong Hua3,Azat Abdullaev4,Shadman Priam1,Saqeeb Adnan1,Erika Nosal1,Michael Manley2,Zhandos Utegulov4,Lingfeng He5,David Hurley3
The Ohio State University1,Oak Ridge National Laboratory2,Idaho National Laboratory3,Nazarbayev University4,North Carolina State University5
We demonstrate utilization of energetic particle to introduce few nanometer-sized features in crystalline solids leading to changes in thermal transport. This integrated analysis includes ion irradiation, microstructure characterization using transmission electron microscopy, measurement of thermal conductivity tensor using spatial domain thermoreflectance, and modeling of thermal conductivity accounting for observed nanostructure. In cubic CeO<sub>2</sub> bombarded with 2 MeV energy protons faulted dislocation loops are formed. These loops have long range strain field resulting in significant reduction of thermal conductivity. Aligned ion tracks in Al<sub>2</sub>O<sub>3</sub> generated by bombardment with 167 MeV xenon ions modify its thermal conductivity anisotropy, where thermal conductivity along direction perpendicular to ion channels exhibits larger conductivity reduction compared to direction parallel to the channels. Lastly, we show modification of conductivity anisotropy in hexagonal delta-phase U-Zr alloy, caused by formation of platelet nanoprecipitates. For the latter case, the anisotropic modification is also observed in phonon lifetimes measured using inelastic X-ray scattering.