Terahertz Quantum Cascade Lasers Benjamin S. Williams
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RADAR POLARIZATION PROPERTIES AND LUNAR SECONDARY CRATERING A Dissertation Presented to the Faculty of the Graduate School of Cornell University In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy by Kassandra Martin-Wells January 2013 © 2013 Kassandra Martin-Wells RADAR POLARIZATION PROPERTIES AND LUNAR SECONDARY CRATERING Kassandra Martin-Wells, Ph. D. Cornell University 2013 Age dating of planetary surfaces relies on an accurate correlation between lunar crater size-frequency distributions and radiometric ages of samples returned from the Moon. For decades, it has been assumed that cratering records are dominated by “primary” impacts of interplanetary bolides [McEwen et al., 2005]. Unlike primary craters, secondary craters, which originate as ejecta from large primary events, occur in large clusters in both space and time. It was long believed that the majority of secondary craters formed at low velocities near their parent crater, resulting in a class of craters with morphologies which are easily distinguished from primary craters of a similar size [McEwen et al., 2005]. However, recent work by Bierhaus et al. (2005), McEwen et al. (2005) argues that cratering records in the Solar System may be strongly contaminated by hard-to-identify secondary craters. They advise caution when relying on counts at small diameters [McEwen et al., 2005; Bierhaus et al., 2005]. Despite the difficulties, something must be done to improve the accuracy of age dates derived from size-frequency distributions of small craters. In this thesis, a method of secondary crater identification based on radar circular polarization properties is presented. The radar polarization and photographic studies of lunar secondary craters in this thesis reveal that secondary cratering is a widespread phenomenon on the lunar surface. -
Federico Capasso “Physics by Design: Engineering Our Way out of the Thz Gap” Peter H
6 IEEE TRANSACTIONS ON TERAHERTZ SCIENCE AND TECHNOLOGY, VOL. 3, NO. 1, JANUARY 2013 Terahertz Pioneer: Federico Capasso “Physics by Design: Engineering Our Way Out of the THz Gap” Peter H. Siegel, Fellow, IEEE EDERICO CAPASSO1credits his father, an economist F and business man, for nourishing his early interest in science, and his mother for making sure he stuck it out, despite some tough moments. However, he confesses his real attraction to science came from a well read children’s book—Our Friend the Atom [1], which he received at the age of 7, and recalls fondly to this day. I read it myself, but it did not do me nearly as much good as it seems to have done for Federico! Capasso grew up in Rome, Italy, and appropriately studied Latin and Greek in his pre-university days. He recalls that his father wisely insisted that he and his sister become fluent in English at an early age, noting that this would be a more im- portant opportunity builder in later years. In the 1950s and early 1960s, Capasso remembers that for his family of friends at least, physics was the king of sciences in Italy. There was a strong push into nuclear energy, and Italy had a revered first son in En- rico Fermi. When Capasso enrolled at University of Rome in FREDERICO CAPASSO 1969, it was with the intent of becoming a nuclear physicist. The first two years were extremely difficult. University of exams, lack of grade inflation and rigorous course load, had Rome had very high standards—there were at least three faculty Capasso rethinking his career choice after two years. -
Glossary Glossary
Glossary Glossary Albedo A measure of an object’s reflectivity. A pure white reflecting surface has an albedo of 1.0 (100%). A pitch-black, nonreflecting surface has an albedo of 0.0. The Moon is a fairly dark object with a combined albedo of 0.07 (reflecting 7% of the sunlight that falls upon it). The albedo range of the lunar maria is between 0.05 and 0.08. The brighter highlands have an albedo range from 0.09 to 0.15. Anorthosite Rocks rich in the mineral feldspar, making up much of the Moon’s bright highland regions. Aperture The diameter of a telescope’s objective lens or primary mirror. Apogee The point in the Moon’s orbit where it is furthest from the Earth. At apogee, the Moon can reach a maximum distance of 406,700 km from the Earth. Apollo The manned lunar program of the United States. Between July 1969 and December 1972, six Apollo missions landed on the Moon, allowing a total of 12 astronauts to explore its surface. Asteroid A minor planet. A large solid body of rock in orbit around the Sun. Banded crater A crater that displays dusky linear tracts on its inner walls and/or floor. 250 Basalt A dark, fine-grained volcanic rock, low in silicon, with a low viscosity. Basaltic material fills many of the Moon’s major basins, especially on the near side. Glossary Basin A very large circular impact structure (usually comprising multiple concentric rings) that usually displays some degree of flooding with lava. The largest and most conspicuous lava- flooded basins on the Moon are found on the near side, and most are filled to their outer edges with mare basalts. -
DESIGN and FABRICATION of Gan-BASED HETEROJUNCTION BIPOLAR TRANSISTORS
DESIGN AND FABRICATION OF GaN-BASED HETEROJUNCTION BIPOLAR TRANSISTORS By KYU-PIL LEE A DISSERTATION PRESENTED TO THE GRADUATE SCHOOL OF THE UNIVERSITY OF FLORIDA IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY UNIVERSITY OF FLORIDA 2003 In his heart a man plans his course, But, the LORD determines his steps. Proverbs 16:9 ACKNOWLEDGMENTS First and foremost, I would like to express great appreciation with all my heart to Professor Pearton and Professor Ren for their expert advice, guidance, and instruction throughout the research. I also give special thanks to members of my committee (Professor Abernathy, Professor Norton, and Professor Singh) for their professional input and support. Additional special thanks are reserved for the people of our research group (Kwang-hyun, Kelly, Ben, Jihyun, and Risarbh) for their assistance, care, and friendship. I am very grateful to past group members (Sirichai, Pil-yeon, David, Donald and Bee). 1 also give my thanks to P. Mathis for her endless help and kindness; and to Mr. Santiago who is network assistant in the Chemical Engineering Department, because of his great help with my simulation. I also thank my discussion partners about material growth technologies, Dr. B. Gila, Dr. M. Overberg, Jerry and Dr. Kang-Nyung Lee. I would like to give my thanks to my friends (especially Kyung-hoon, Young-woo, Se-jin, Byeng-sung, Yong-wook, and Hyeng-jin). Even when they were very busy, they always helped my research work without hesitation. I cannot forget Samsung's vice president Dr. Jong-woo Park’s devoted help, and the steadfast support from Samsung Electronics. -
Based Vertical Double Heterojunction Bipolar Transistors with High Current Amplification
COMMUNICATION Heterojunction Bipolar Transistor www.advelectronicmat.de 2D Material-Based Vertical Double Heterojunction Bipolar Transistors with High Current Amplification Geonyeop Lee, Stephen J. Pearton, Fan Ren, and Jihyun Kim* been applied to various types of semicon- The heterojunction bipolar transistor (HBT) differs from the classical homo- ductor devices, such as lasers, solar cells, junction bipolar junction transistor in that each emitter-base-collector layer high electron mobility transistors, and het- [3–6] is composed of a different semiconductor material. 2D material (2DM)- erojunction bipolar transistors (HBTs). Notably, with a bipolar junction transistor, based heterojunctions have attracted attention because of their wide range which is a three-terminal transistor fabri- of fundamental physical and electrical properties. Moreover, strain-free cated by connecting two P–N homojunc- heterostructures formed by van der Waals interaction allows true bandgap tion diodes, there is a trade-off between engineering regardless of the lattice constant mismatch. These characteristics the current gain and high-frequency ability [3,7] make it possible to fabricate high-performance heterojunction devices such because of these problems. In sharp contrast, HBTs realized using the hetero- as HBTs, which have been difficult to implement in conventional epitaxy. structure can avoid these trade-offs and Herein, NPN double HBTs (DHBTs) are constructed from vertically stacked improve device performance.[8] HBTs, due 2DMs (n-MoS2/p-WSe2/n-MoS2) using dry transfer technique. The forma- to their high power efficiency, uniformity tion of the two P–N junctions, base-emitter, and base-collector junctions, of threshold voltage, and low 1/f noise in DHBTs, was experimentally observed. -
Quantum Dot and Electron Acceptor Nano-Heterojunction For
www.nature.com/scientificreports OPEN Quantum dot and electron acceptor nano‑heterojunction for photo‑induced capacitive charge‑transfer Onuralp Karatum1, Guncem Ozgun Eren2, Rustamzhon Melikov1, Asim Onal3, Cleva W. Ow‑Yang4,5, Mehmet Sahin6 & Sedat Nizamoglu1,2,3* Capacitive charge transfer at the electrode/electrolyte interface is a biocompatible mechanism for the stimulation of neurons. Although quantum dots showed their potential for photostimulation device architectures, dominant photoelectrochemical charge transfer combined with heavy‑metal content in such architectures hinders their safe use. In this study, we demonstrate heavy‑metal‑free quantum dot‑based nano‑heterojunction devices that generate capacitive photoresponse. For that, we formed a novel form of nano‑heterojunctions using type‑II InP/ZnO/ZnS core/shell/shell quantum dot as the donor and a fullerene derivative of PCBM as the electron acceptor. The reduced electron–hole wavefunction overlap of 0.52 due to type‑II band alignment of the quantum dot and the passivation of the trap states indicated by the high photoluminescence quantum yield of 70% led to the domination of photoinduced capacitive charge transfer at an optimum donor–acceptor ratio. This study paves the way toward safe and efcient nanoengineered quantum dot‑based next‑generation photostimulation devices. Neural interfaces that can supply electrical current to the cells and tissues play a central role in the understanding of the nervous system. Proper design and engineering of such biointerfaces enables the extracellular modulation of the neural activity, which leads to possible treatments of neurological diseases like retinal degeneration, hearing loss, diabetes, Parkinson and Alzheimer1–3. Light-activated interfaces provide a wireless and non-genetic way to modulate neurons with high spatiotemporal resolution, which make them a promising alternative to wired and surgically more invasive electrical stimulation electrodes4,5. -
17 Band Diagrams of Heterostructures
Herbert Kroemer (1928) 17 Band diagrams of heterostructures 17.1 Band diagram lineups In a semiconductor heterostructure, two different semiconductors are brought into physical contact. In practice, different semiconductors are “brought into contact” by epitaxially growing one semiconductor on top of another semiconductor. To date, the fabrication of heterostructures by epitaxial growth is the cleanest and most reproducible method available. The properties of such heterostructures are of critical importance for many heterostructure devices including field- effect transistors, bipolar transistors, light-emitting diodes and lasers. Before discussing the lineups of conduction and valence bands at semiconductor interfaces in detail, we classify heterostructures according to the alignment of the bands of the two semiconductors. Three different alignments of the conduction and valence bands and of the forbidden gap are shown in Fig. 17.1. Figure 17.1(a) shows the most common alignment which will be referred to as the straddled alignment or “Type I” alignment. The most widely studied heterostructure, that is the GaAs / AlxGa1– xAs heterostructure, exhibits this straddled band alignment (see, for example, Casey and Panish, 1978; Sharma and Purohit, 1974; Milnes and Feucht, 1972). Figure 17.1(b) shows the staggered lineup. In this alignment, the steps in the valence and conduction band go in the same direction. The staggered band alignment occurs for a wide composition range in the GaxIn1–xAs / GaAsySb1–y material system (Chang and Esaki, 1980). The most extreme band alignment is the broken gap alignment shown in Fig. 17.1(c). This alignment occurs in the InAs / GaSb material system (Sakaki et al., 1977). -
July 2020 in This Issue Online Readers, ALPO Conference November 6-7, 2020 2 Lunar Calendar July 2020 3 Click on Images an Invitation to Join ALPO 3 for Hyperlinks
A publication of the Lunar Section of ALPO Edited by David Teske: [email protected] 2162 Enon Road, Louisville, Mississippi, USA Recent back issues: http://moon.scopesandscapes.com/tlo_back.html July 2020 In This Issue Online readers, ALPO Conference November 6-7, 2020 2 Lunar Calendar July 2020 3 click on images An Invitation to Join ALPO 3 for hyperlinks. Observations Received 4 By the Numbers 7 Submission Through the ALPO Image Achieve 4 When Submitting Observations to the ALPO Lunar Section 9 Call For Observations Focus-On 9 Focus-On Announcement 10 2020 ALPO The Walter H. Haas Observer’s Award 11 Sirsalis T, R. Hays, Jr. 12 Long Crack, R. Hill 13 Musings on Theophilus, H. Eskildsen 14 Almost Full, R. Hill 16 Northern Moon, H. Eskildsen 17 Northwest Moon and Horrebow, H. Eskildsen 18 A Bit of Thebit, R. Hill 19 Euclides D in the Landscape of the Mare Cognitum (and Two Kipukas?), A. Anunziato 20 On the South Shore, R. Hill 22 Focus On: The Lunar 100, Features 11-20, J. Hubbell 23 Recent Topographic Studies 43 Lunar Geologic Change Detection Program T. Cook 120 Key to Images in this Issue 134 These are the modern Golden Days of lunar studies in a way, with so many new resources available to lu- nar observers. Recently, we have mentioned Robert Garfinkle’s opus Luna Cognita and the new lunar map by the USGS. This month brings us the updated, 7th edition of the Virtual Moon Atlas. These are all wonderful resources for your lunar studies. -
Heterojunction Quantum Dot Solar Cells
Heterojunction Quantum Dot Solar Cells by Navid Mohammad Sadeghi Jahed A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Doctor of Philosophy in Electrical and Computer Engineering Waterloo, Ontario, Canada, 2016 © Navid Mohammad Sadeghi Jahed 2016 I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. ii Abstract The advent of new materials and application of nanotechnology has opened an alternative avenue for fabrication of advanced solar cell devices. Before application of nanotechnology can become a reality in the photovoltaic industry, a number of advances must be accomplished in terms of reducing material and process cost. This thesis explores the development and fabrication of new materials and processes, and employs them in the fabrication of heterojunction quantum dot (QD) solar cells in a cost effective approach. In this research work, an air stable, highly conductive (ρ = 2.94 × 10-4 Ω.cm) and transparent (≥85% in visible range) aluminum doped zinc oxide (AZO) thin film was developed using radio frequency (RF) sputtering technique at low deposition temperature of 250 °C. The developed AZO film possesses one of the lowest reported resistivity AZO films using this technique. The effect of deposition parameters on electrical, optical and structural properties of the film was investigated. Wide band gap semiconductor zinc oxide (ZnO) films were also developed using the same technique to be used as photo electrode in the device structure. -
Facts & Features Lunar Surface Elevations Six Apollo Lunar
Greek Mythology Quadrants Maria & Related Features Lunar Surface Elevations Facts & Features Selene is the Moon and 12 234 the goddess of the Moon, 32 Diameter: 2,160 miles which is 27.3% of Earth’s equatorial diameter of 7,926 miles 260 Lacus daughter of the titans 71 13 113 Mare Frigoris Mare Humboldtianum Volume: 2.03% of Earth’s volume; 49 Moons would fit inside Earth 51 103 Mortis Hyperion and Theia. Her 282 44 II I Sinus Iridum 167 125 321 Lacus Somniorum Near Side Mass: 1.62 x 1023 pounds; 1.23% of Earth’s mass sister Eos is the goddess 329 18 299 Sinus Roris Surface Area: 7.4% of Earth’s surface area of dawn and her brother 173 Mare Imbrium Mare Serenitatis 85 279 133 3 3 3 Helios is the Sun. Selene 291 Palus Mare Crisium Average Density: 3.34 gm/cm (water is 1.00 gm/cm ). Earth’s density is 5.52 gm/cm 55 270 112 is often pictured with a 156 Putredinis Color-coded elevation maps Gravity: 0.165 times the gravity of Earth 224 22 237 III IV cresent Moon on her head. 126 Mare Marginis of the Moon. The difference in 41 Mare Undarum Escape Velocity: 1.5 miles/sec; 5,369 miles/hour Selenology, the modern-day 229 Oceanus elevation from the lowest to 62 162 25 Procellarum Mare Smythii Distances from Earth (measured from the centers of both bodies): Average: 238,856 term used for the study 310 116 223 the highest point is 11 miles. -
Band Alignment and Graded Heterostructures
Band Alignment and Graded Heterostructures Guofu Niu Auburn University Outline • Concept of electron affinity • Types of heterojunction band alignment • Band alignment in strained SiGe/Si • Cusps and Notches at heterojunction • Graded bandgap • Impact of doping on equilibrium band diagram in graded heterostructures Reference • My own SiGe book – more on npn SiGe HBT base grading • The proc. Of the IEEE review paper by Nobel physics winner Herb Kromer – part of this lecture material came from that paper • The book chapter of Prof. Schubert of RPI – book can be downloaded online from docstoc.com • http://edu.ioffe.ru/register/?doc=pti80en/alfer_e n.tex - by Alfreov, who shared the noble physics prize with Kroemer for heterostructure laser work 3 Band alignment • So far I have intentionally avoided the issue of band alignment at heterojunction interface • We have simply focused on – ni^2 change due to bandgap change for abrupt junction – Ec or Ev gradient produced by Ge grading • We have seen in our Sdevice simulation that the final band diagrams actually depend on doping – A Ec gradient favorable for electron transport is obtained for forward Ge grading in p-type (npn HBT) – A Ev gradient favorable for hole transport is obtained for forward Ge grading in n-type (pnp HBT) Electron Affinity – rough picture • Neglect interface between vacuum and semiconductor, vacuum level is drawn to be position independent • The energy needed to move an electron from Ec to vacuum level is called electron affinity. 5 Electron Affinity Model • The electron affinity model is the oldest model invoked to calculate the band offsets in semiconductor heterostructures (Anderson, 1962). -
Heterojunction Engineering for Next Generation Hybrid II-VI Materials
City University of New York (CUNY) CUNY Academic Works All Dissertations, Theses, and Capstone Projects Dissertations, Theses, and Capstone Projects 9-2017 Heterojunction Engineering for Next Generation Hybrid II-VI Materials Thor Garcia The Graduate Center, City University of New York How does access to this work benefit ou?y Let us know! More information about this work at: https://academicworks.cuny.edu/gc_etds/2385 Discover additional works at: https://academicworks.cuny.edu This work is made publicly available by the City University of New York (CUNY). Contact: [email protected] HETEROJUNCTION ENGINEERING FOR NEXT GENERATION HYBRID II-VI MATERIALS by THOR AXTMANN GARCIA A dissertation submitted to the Graduate Faculty in chemistry in partial fulfillment of the requirements for the degree of Doctor of Philosophy, The City University of New York 2017 © 2017 THOR AXTMANN GARCIA All Rights Reserved ii Heterojunction Engineering for Next Generation Hybrid II-VI Materials by Thor Axtmann Garcia This manuscript has been read and accepted for the Graduate Faculty in chemistry in satisfaction of the dissertation requirement for the degree of Doctor of Philosophy. Date Professor Maria C. Tamargo Chair of Examining Committee Date Professor Brian R. Gibney Executive Officer Supervisory Committee: Professor Aidong Shen Professor Igor L. Kuskovsky Professor Glen Kowach THE CITY UNIVERSITY OF NEW YORK iii ABSTRACT Heterojunction Engineering for Next Generation Hybrid II-VI Materials by Thor Axtmann Garcia Advisor: Professor Maria C. Tamargo Molecular Beam Epitaxy(MBE) is a versatile thin film growth technique with monolayer control of crystallization. The flexibility and precision afforded by the technique allows for unique control of interfaces and electronic structure of the films grown.