Kento Katagiri1,Leora Dresselhaus-Marais1,Tatiana Pikuz2,Genki Kamimura2,Hirotaka Nakamura2,Gooru Masaoka2,Ryosuke Kodama2,Masato Ota2,Shunsuke Egashira2,Youichi Sakawa2,Takayoshi Sano2,Frank Schoofs3,Michel Koenig4,Bruno Albertazzi4,Gabriel Rigon5,Lichao Fang1,Zoe Smith1,Yuichi Inubushi6,Kohei Miyanishi7,Keiichi Sueda7,Tadashi Togashi6,Makina Yabashi6,Toshinori Yabuuchi6,Norimasa Ozaki2
Stanford University1,Osaka University2,UK Atomic Energy3,LULI, CNRS, CEA, Ecole Polytechnique4,Nagoya University5,JASRI6,RIKEN7
Kento Katagiri1,Leora Dresselhaus-Marais1,Tatiana Pikuz2,Genki Kamimura2,Hirotaka Nakamura2,Gooru Masaoka2,Ryosuke Kodama2,Masato Ota2,Shunsuke Egashira2,Youichi Sakawa2,Takayoshi Sano2,Frank Schoofs3,Michel Koenig4,Bruno Albertazzi4,Gabriel Rigon5,Lichao Fang1,Zoe Smith1,Yuichi Inubushi6,Kohei Miyanishi7,Keiichi Sueda7,Tadashi Togashi6,Makina Yabashi6,Toshinori Yabuuchi6,Norimasa Ozaki2
Stanford University1,Osaka University2,UK Atomic Energy3,LULI, CNRS, CEA, Ecole Polytechnique4,Nagoya University5,JASRI6,RIKEN7
Since plastic deformation of crystals is primarily driven by the motion of dislocations (line defects), it is necessary to understand how fast they can propagate in order to describe the deformation dynamics of solids compressed at highest strain rates. Although many models predict the upper bound of dislocation velocities to lie between the longitudinal and transverse acoustic velocities, experimentally capturing the ultrafast dislocation motion under high strain-rate deformation remains elusive. We present our recent experimental results of <i>in-situ </i>X-ray radiography of laser-shocked single crystal diamonds. By using the ultra-bright femtosecond-duration pulses available at the SACLA X-ray Free Electron Laser facility, we imaged inelastic shock waves in diamond that propagated with a velocity comparable to the bulk sound velocity of diamond (≥ 11 µm/ns). For these waves, we observed shock-induced stacking faults form along diamond’s {111} slip planes via imaging, at velocities that indicate that the dislocations leading the stacking fault formation propagate transonically (<i>i.e</i>., with a speed between the transverse and longitudinal wave velocities of the crystal). Our advanced characterization of transonic dislocation motion gives new insights into the fundamental behavior of the dislocation propagation in crystals.