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Excitations of Quasi-Particles in Nanostructured Systems University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 5-2017 Excitations of Quasi-Particles in Nanostructured Systems Jingxuan Ge University of Tennessee, Knoxville, [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Other Materials Science and Engineering Commons Recommended Citation Ge, Jingxuan, "Excitations of Quasi-Particles in Nanostructured Systems. " PhD diss., University of Tennessee, 2017. https://trace.tennessee.edu/utk_graddiss/4461 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Jingxuan Ge entitled "Excitations of Quasi- Particles in Nanostructured Systems." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Doctor of Philosophy, with a major in Materials Science and Engineering. Gerd Duscher, Major Professor We have read this dissertation and recommend its acceptance: Ramki Kalyanaraman, Haixuan Xu, Dibyendu Mukherjee Accepted for the Council: Dixie L. Thompson Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Excitations of Quasi-Particles in Nanostructured Systems A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Jingxuan Ge May 2017 Dedications To my father, my parents in-law, my husband, and my son. ii Acknowledgements I would like to gratefully and sincerely thank my committee members, my friends, and my family for their guidance, help, and support during my graduate studies at University of Tennessee. I would never have been able to finish my dissertation without the excellent atmosphere they provided to me. First and foremost, I offer my sincerest gratitude to my supervisor, Dr. Gerd Duscher, for his guidance, patience, enthusiasm, encouragement, and support throughout my PhD study. He has been opening my minds and enlightening me in many aspects of my daily life and academic life. I feel very lucky that my excellent mentor in scientific research is also an open minded, bright, and humorous friend of mine in daily life. He offers me endless helps in our academic life and daily life. This indeed makes my life as a graduate student much more colorful and memorable. I am grateful to Dr. Ramakrishnan Kalyanaraman as my co-advisor, who is one of the best leaders I have ever seen. He provides me continuous support, guidance, help, and most importantly, patience to my research. His insightful comments and suggestions during the discussion always inspired me to seek more sources or alternative approach to resolve the issue I had during the research. I am thankful to Dr. Haixuan Xu and Dr. Dibyendu Mukherjee for being interested in my research and serving on my committees. And I am also grateful to Dr. John Dunlap for his kind help in the laboratory. I owe my deepest gratitude to my husband, Mengkun Tian, who helps me in my academic and takes care of my life. I am grateful to my parents –in-law, who take care of my son. Thanks Annette Farah, Humaira Taz and Abhinav Malasi who synthesized samples in my research; Thanks Ritesh Sachan, who discovered the ferroplasmon and led me to this field. Thanks my collaborator Dr. Hans-peter Wagner who guidance, help, and most importantly, patience to my iii research; Thanks my friend Dr. Guoliang Li, who helps me in my academic. Thanks Chenze Liu, who help me in writing my dissertation; Thanks my groupmates and friends Dr. Peizhi Liu, Dr. Ondrej Dyck, Nicholas Cross, Ting Wu, Prasad, Yueying Wu, Yucheng Fang, Qingya Zeng, Hengxing Xu, Shuying Chen, Youxiong Ye, Rui Feng and Yuan Li who have been one of the most important parts of my life. Thanks to the sponsorship from the Materials Sciences and Basic Energy Sciences, Office of Science, U.S. Department of Energy & Department of Defense and Center for Materials Processing, UTK. We thank the Joint Institute of Advanced Materials for microscopy access. iv Abstract The excitation of quasiparticles, like the investigated excitons and plasmons here, are the optically most prominent responses of materials. In nanostructured system, the sample quality is crucial for quantitative investigations of these optical excitations. We used electron beam evaporation, nano-second laser dewetting, and electron metalorganic chemical vapor deposition techniques to prepare well-defined and “clean” transmission electron microscopy (TEM) samples. Electron energy-loss microscopy (EELS) performed in STEM mode was employed to investigate the structural and electro-optical properties. Quantifit software was used to analyze the EELS spectra quantitatively in terms of inelastic scattering probability, energy and lifetime. We found that the ferroplasmon originates from induced excitation by the Ag’s intrinsic dipole mode at low energy, and it has a redshift with increasing particle size. Because the bimetallic system is associated with one dipole mode only, the ferroplasmons is strongly dependent on geometry. Disc-skirt AgCo nanostructures also show ferroplasmons because plasmon excitation mode of Ag disc is similar in geometry to Ag spherical, while the nanotriangles and nanobowties did not show a ferroplasmon. The bulk plasmon (BP) did not have a significate change from the pure metals to the metals in the bimetallic systems, indicating that the electron density did not change through the contact of the metals. In semiconductors, high binding energy excitons were detected universally at room temperature by EELS for the first time. The states associated with these excitons were identified as molecular states. The singlet S0 state can be directly excited to the triplet T1 state by electrons, even though the transition is forbidden optically. The conclusion on molecular states was based on the fact that this excitation can be bleached with time, and recovered in minutes. Band- bending was observed when the semiconductor is in contacting with Au nanoparticles. This exciton has a signal reduction and blue shift introduced by the band bending. The higher energy exciton can be excited from the S0 state to the singlet S1 state when the band bending is large v enough. The distribution of the point defects can be mapped with high precision through mapping the intensity of the exciton. Key words: Quasi-Particles, Ferroplasmons, Excitons, EELS, Excitation vi Table of Contents Chapter 1 Introduction ................................................................................................................ 1 1.1 Plasmons ......................................................................................................................... 1 1.1.1 Localized surface plasmon ........................................................................................ 1 1.1.2 Bulk plasmons (BPs) ................................................................................................. 7 1.1.3 TEM sample preparation ........................................................................................... 8 1.2 Excitons ........................................................................................................................... 9 1.2.1 Singlet/Triplet Molecular States ................................................................................. 9 1.2.2 Point Defect States in GaAs .....................................................................................10 1.3 Motivation and overview ..................................................................................................11 1.3.1 Motivation I ...............................................................................................................11 1.3.2 Motivation II ..............................................................................................................12 Chapter 2 Experimental Method ................................................................................................14 2.1 TEM sample preparation .................................................................................................14 2.1.1 Metallic NPs synthesis and TEM sample preparation ...............................................14 2.1.3 NWs TEM sample preparation ..................................................................................26 2.2 Characterization ..............................................................................................................31 2.2.1 STEM image .............................................................................................................32 2.2.2 Monochromated EELS in STEM mode .....................................................................34 2.3 Analysis method ..............................................................................................................38 2.3.1 ZLP and Low loss spectra quantification ...................................................................38 2.3.2 Core loss spectra quantification ................................................................................41 vii Chapter 3 Ferroplasmon results and discussion ........................................................................45
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