Optical and Electrical Properties of Organic Semiconductors: Experiment and Simulation
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Dicke Superradiance in Solids [Invited]
C80 Vol. 33, No. 7 / July 2016 / Journal of the Optical Society of America B Review Dicke superradiance in solids [Invited] 1 1 2 1 2 KANKAN CONG, QI ZHANG, YONGRUI WANG, G. TIMOTHY NOE II, ALEXEY BELYANIN, AND 1,3,4, JUNICHIRO KONO * 1Department of Electrical and Computer Engineering, Rice University, Houston, Texas 77005, USA 2Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843, USA 3Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA 4Department of Materials Science and NanoEngineering, Rice University, Houston, Texas 77005, USA *Corresponding author: [email protected] Received 18 February 2016; revised 7 April 2016; accepted 7 April 2016; posted 8 April 2016 (Doc. ID 259437); published 13 May 2016 Recent advances in optical studies of condensed matter systems have led to the emergence of a variety of phenomena that have conventionally been studied in the realm of quantum optics. These studies have not only deepened our understanding of light–matter interactions but have also introduced aspects of many-body corre- lations inherent in optical processes in condensed matter systems. This paper is concerned with the phenomenon of superradiance (SR), a profound quantum optical process originally predicted by Dicke in 1954. The basic concept of SR applies to a general N body system, where constituent oscillating dipoles couple together through interaction with a common light field and accelerate the radiative decay of the whole system. Hence, the term SR ubiquitously appears in order to describe radiative coupling of an arbitrary number of oscillators in many situations in modern science of both classical and quantum description. -
Structural Characterization Studies on Semiconducting Znsnn2 Films Using Synchrotron X-Ray Diffraction
Structural Characterization Studies on Semiconducting ZnSnN2 Films using Synchrotron X-ray Diffraction by Nancy Senabulya A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Applied Physics) in The University of Michigan 2017 Doctoral Committee: Professor Roy Clarke, Chair Professor Steven M. Durbin Assistant Professor Emmanouil Kioupakis Professor Cagliyan Kurdak [email protected] ORCID ID: 0000-0002-3394-5452 © Nancy Senabulya All Rights Reserved To Andrew, Jordan and Elise ii ACKNOWLEDGEMENTS I would like to thank my mom who sacrificed everything for my siblings and I to get the best education in Uganda. For some reason, she always believed I would get a PhD and I never believed her until now. Her love and support helping me look after our kids in the first six months of their lives, when I had them in graduate school is the reason I could complete this PhD in record time. My sister and friend Donna has been an important source of inspiration for me since childhood. Her passion for Math and Science and subsequent successful career in Telecommunications Engineering have allowed me to dream beyond my wildest dreams the things I could accomplish as a woman from a developing country. Thank you, Donna, for not allowing to be limited by circumstances. You worked hard and set a good example for all of us to follow. I am proud to be your sister. Diana, Ivan, Penny, Jenna, Martin, I love you guys so much. Thanks for rooting for me throughout this whole process, I have enjoyed our conversations on skype and been so proud of all you have accomplished the last few years. -
5. Atomic Radiation Processes
5. Atomic radiation processes Einstein coefficients for absorption and emission oscillator strength line profiles: damping profile, collisional broadening, Doppler broadening continuous absorption and scattering 1 2 A.A. LineLine transitionstransitions Einstein coefficients probability that a photon in frequency interval in the solid angle range is absorbed by an atom in the energy level El with a resulting transition El Eu per second: abs dω dw (ν, ω,l,u)=Blu Iν(ω) ϕ(ν)dν 4π atomic property ~ no. of incident probability for probability for photons absorption of with photon with probability for absorption transition l u profile Blu : Einstein coefficient for absorption 3 Einstein coefficients similarly for stimulated emission st dω dw (ν,ω,l,u)=Bul Iν (ω) ϕ(ν)dν 4π Bul : Einstein coefficient for stimulated emission and for spontaneous emission sp dω dw (ν, ω,l,u)=Aul ϕ(ν)dν 4π Aul : Einstein coefficient for spontaneous emission 4 st dω abs dω dw (ν,ω,l,u)=Bul Iν (ω) ϕ(ν)dν 4π dw (ν, ω,l,u)=Blu Iν(ω) ϕ(ν)dν 4π Einstein coefficients, absorption and emission coefficients Number of absorptions & stimulated emissions dF dV = dF ds Iν in dV per second: abs st ds nl dw dV, nu dw dV absorbed energy in dV per second: abs abs st stimulated emission counted dE = nl hν dw dV nu hν dw dV ν − as negative absorption and also (using definition of intensity): abs L dEν = κν Iν ds dω dν dF Absorption and emission coefficients are a function of Einstein coefficients, occupation numbers and line broadening hν κL = ϕ(ν)[n B n B ] ν 4π l lu − u ul L hν for -
Equation Chapter 1 Section 1
Fundamentals of Spectroscopy and Laser Physics In this chapter we present the fundamental physical definitions and theoretically de- rived relations that underlie practical laser theory and engineering, and indeed, much of linear optical spectroscopy. Our purpose, however, is not to offer a comprehensive treatment of this topic (see the references for recommended reading) but rather to de- velop essential understanding in an economical format. To this end, such basic concepts as radiative lifetime, absorption, and polarization dephasing will be initially developed from first principles by using a classical model of the atom. Quantum mechanical as- pects of the radiation problem will then be introduced as needed in order to polish the classical results into their useful or more appropriate modern forms. Copyright © 2002, Timothy R. Gosnell 1 Table of Contents 1 CLASSICAL CHARGED-PARTICLE OSCILLATOR 3 1.1 Damped, Undriven Oscillator 3 1.2 Driven, Damped Oscillator 6 1.2.1 Absorption Cross Section 8 1.2.2 Oscillator Strength 9 1.3 Collisions: Inelastic and Elastic Relaxation 10 1.4 Oscillator Ensembles 12 1.4.1 Homogeneous Broadening 12 1.4.2 Inhomogeneous Broadening 13 2 QUANTUM THEORY OF RESONANT ABSORPTION AND STIMULATED EMISSION 14 2.1 The Quantum Two-Level System 15 2.1.1 Basic Properties 15 2.1.2 Electric Dipole Moment Operator 16 2.1.3 Radiative Damping of the Undriven Two-Level System 18 2.2 Semiclassical RadiationTheory 20 2.2.1 The Density Matrix 20 2.2.2 Damping in the Semiclassical Equations of Motion 23 2.2.3 Solutions of the