Quantum Enhanced Microscopy, Equs Annual Workshop, Noosa, AUS, December 2016 - Poster Accompanied by Abstract
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Wien Peaks, Planck Distribution Function and Its Decomposition, The
Applied Physics Research; Vol. 12, No. 4; 2020 ISSN 1916-9639 E-ISSN 1916-9647 Published by Canadian Center of Science and Education How to Understand the Planck´s Oscillators? Wien Peaks, Planck Distribution Function and Its Decomposition, the Bohm Sheath Criterion, Plasma Coupling Constant, the Barrier of Determinacy, Hubble Cooling Constant. (24.04.2020) Jiří Stávek1 1 Bazovského 1228, 163 00 Prague, Czech republic Correspondence: Jiří Stávek, Bazovského 1228, 163 00 Prague, Czech republic. E-mail: [email protected] Received: April 23, 2020 Accepted: June 26, 2020 Online Published: July 31, 2020 doi:10.5539/apr.v12n4p63 URL: http://dx.doi.org/10.5539/apr.v12n4p63 Abstract In our approach we have combined knowledge of Old Masters (working in this field before the year 1905), New Masters (working in this field after the year 1905) and Dissidents under the guidance of Louis de Broglie and David Bohm. Based on the great works of Wilhelm Wien and Max Planck we have presented a new look on the “Wien Peaks” and the Planck Distribution Function and proposed the “core-shell” model of the photon. There are known many “Wien Peaks” defined for different contexts. We have introduced a thermodynamic approach to define the Wien Photopic Peak at the wavelength λ = 555 nm and the Wien Scotopic Peak at the wavelength λ = 501 nm to document why Nature excellently optimized the human vision at those wavelengths. There could be discovered many more the so-called Wien Thermodynamic Peaks for other physical and chemical processes. We have attempted to describe the so-called Planck oscillators as coupled oscillations of geons and dyons. -
Sir Arthur Eddington and the Foundations of Modern Physics
Sir Arthur Eddington and the Foundations of Modern Physics Ian T. Durham Submitted for the degree of PhD 1 December 2004 University of St. Andrews School of Mathematics & Statistics St. Andrews, Fife, Scotland 1 Dedicated to Alyson Nate & Sadie for living through it all and loving me for being you Mom & Dad my heroes Larry & Alice Sharon for constant love and support for everything said and unsaid Maggie for making 13 a lucky number Gram D. Gram S. for always being interested for strength and good food Steve & Alice for making Texas worth visiting 2 Contents Preface … 4 Eddington’s Life and Worldview … 10 A Philosophical Analysis of Eddington’s Work … 23 The Roaring Twenties: Dawn of the New Quantum Theory … 52 Probability Leads to Uncertainty … 85 Filling in the Gaps … 116 Uniqueness … 151 Exclusion … 185 Numerical Considerations and Applications … 211 Clarity of Perception … 232 Appendix A: The Zoo Puzzle … 268 Appendix B: The Burying Ground at St. Giles … 274 Appendix C: A Dialogue Concerning the Nature of Exclusion and its Relation to Force … 278 References … 283 3 I Preface Albert Einstein’s theory of general relativity is perhaps the most significant development in the history of modern cosmology. It turned the entire field of cosmology into a quantitative science. In it, Einstein described gravity as being a consequence of the geometry of the universe. Though this precise point is still unsettled, it is undeniable that dimensionality plays a role in modern physics and in gravity itself. Following quickly on the heels of Einstein’s discovery, physicists attempted to link gravity to the only other fundamental force of nature known at that time: electromagnetism. -
Optics Terminology Resource Optics Terminology Resource Version 1.0 (Last Updated: 2019-03-30)
- Institute for scientific and technical information - Optics terminology resource Optics terminology resource Version 1.0 (Last updated: 2019-03-30) Terminology resource used for indexing bibliographical records dealing with “Optics” in the PASCAL database, until 2014. French, Spanish and German versions of this vocabulary are also available. This vocabulary is browsable online at: https://www.loterre.fr Legend • Syn: Synonym. • → : Corresponding Preferred Term. • FR: French Preferred Term. • ES: Spanish Preferred Term. • DE: German Preferred Term. • NT: Narrower Term. • BT: Broader Term. • RT: Related Term. • URI: Concept's URI (link to the online view). This resource is licensed under a Creative Commons Attribution 4.0 International license: TABLE OF CONTENTS Alphabetical Index 4 Terminological entries 5 List of entries 243 Alphabetical index from 1/f noise to 1/f noise p. 7 -7 from 2R signal regeneration to 2R signal regeneration p. 8 -8 from 3R signal regeneration to 3R signal regeneration p. 9 -9 from ABCD matrix to azo dye p. 10 -22 from backlighting to Butterworth filter p. 26 -30 from cadmium alloy to Czochralski method p. 36 -46 from dark cloud to dysprosium barium cuprate p. 50 -55 from EBIC to eye tracking p. 59 -66 from F2 laser to fuzzy logic p. 70 -76 from g-factor to gyrotron p. 78 -83 from H-like ion to hysteresis loop p. 87 -90 from ice to IV-VI semiconductor p. 99 -100 from Jahn-Teller effect to Josephson junction p. 101 -101 from Kagomé lattice to Kurtosis parameter p. 102 -103 from lab-on-a-chip to Lyot filter p. -
Vocabulaire D'optique Vocabulaire D'optique Version 1.0 (Dernière Mise À Jour : 2019-03-30)
- Institut de l'information scientifique et technique - Vocabulaire d'optique Vocabulaire d'optique Version 1.0 (dernière mise à jour : 2019-03-30) Vocabulaire utilisé pour l’indexation des références bibliographiques de la base de données PASCAL jusqu’en 2014, dans le domaine de l'optique. Des versions de cette ressource en anglais, espagnol et allemand sont également disponibles. La ressource est en ligne sur le portail terminologique Loterre : https://www.loterre.fr Légende • Syn : Synonyme. • → : Renvoi vers le terme préférentiel. • EN : Préférentiel anglais. • ES : Préférentiel espagnol. • DE : Préférentiel allemand. • TS : Terme spécifique. • TG : Terme générique. • TA : Terme associé. • URI : URI du concept (cliquer pour le voir en ligne). Cette ressource est diffusée sous licence Creative Commons Attribution 4.0 International : TABLE DES MATIÈRES Index alphabétique 4 Entrées terminologiques 5 Liste des entrées 240 Index alphabétique de aberration chromatique à axicon p. 7 -22 de balayage en Z à bruit quantique p. 23 -26 de calcul bidimensionnel à cytométrie en flux p. 27 -49 de décharge capillaire à dynamique spatio-temporelle p. 50 -65 de EBIC à extensométrie p. 66 -80 de fabrication à fusion superficielle p. 81 -91 de gain optique à gyrotron p. 92 -97 de halogénure à hyperpolarisabilité électrique p. 98 -101 de illusion de Müller-Lyer à isotope du carbone p. 102 -112 de jauge de contrainte à jonction supraconductrice p. 113 -113 de KGW à krypton p. 114 -114 de L-alanine à luminescence p. 129 -130 de macroparticule à myopie p. 131 -154 de nano-aimant à nuage sombre p. 155 -158 de objet de phase à ozone p. -
University of Oklahoma Graduate College
UNIVERSITY OF OKLAHOMA GRADUATE COLLEGE THEORETICAL STUDIES OF MULTI-MODE NOON STATES FOR APPLICATIONS IN QUANTUM METROLOGY AND PROPOSALS OF EXPERIMENTAL SETUPS FOR THEIR GENERATION A DISSERTATION SUBMITTED TO THE GRADUATE FACULTY in partial fulfillment of the requirements for the Degree of DOCTOR OF PHILOSOPHY By LU ZHANG Norman, Oklahoma 2018 THEORETICAL STUDIES OF MULTI-MODE NOON STATES FOR APPLICATIONS IN QUANTUM METROLOGY AND PROPOSALS OF EXPERIMENTAL SETUPS FOR THEIR GENERATION A DISSERTATION APPROVED FOR THE SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING BY Dr. Kam Wai Clifford Chan, Chair Dr. Pramode Verma Dr. Alberto Marino Dr. Samuel Cheng Dr. Gregory MacDonald Dr. Robert Huck 1 c Copyright by LU ZHANG 2018 All Rights Reserved. Acknowledgements I would like to express my deepest appreciation to my committee chair Dr. Kam Wai Cliff Chan, who has been a supportive and accommodating advisor to me. For the past five years, we have been working together on multiple projects in the field of quantum metrology, in which he has valuable insight, and always provides helpful comments and suggestions. With his help, I learned time management skills to work more efficiently, how to think like a scientist, and how to become a researcher. I truly appreciate his trust in me and the financial support from him and Dr. Verma, which made it possible for me to complete my doctorate degree. I am also extremely grateful of all the other committee members, Dr. Pramode Verma, Dr. Alberto Marino, Dr. Samuel Cheng, Dr. Gregory MacDonald, and Dr. Robert Huck, for their help over the past few years and precious comments on the dissertation. -
Quantum State Entanglement Creation, Characterization, and Application
“When two systems, of which we know the states by their respective representatives, enter into temporary physical interaction due to known forces between them, and when after a time of mutual influence the systems separate again, then they can no longer be described in the same way as before, viz. by endowing each of them with a representative of its own. I would not call that one but rather the characteristic trait of quantum mechanics, the one that enforces its entire departure from classical lines of thought. By the interaction, the two representatives (or ψ-functions) have become entangled.” —Erwin Schrödinger (1935) 52 Los Alamos Science Number 27 2002 Quantum State Entanglement Creation, characterization, and application Daniel F. V. James and Paul G. Kwiat ntanglement, a strong and tious technological goal of practical two photons is denoted |HH〉,where inherently nonclassical quantum computation. the first letter refers to Alice’s pho- Ecorrelation between two or In this article, we will describe ton and the second to Bob’s. more distinct physical systems, was what entanglement is, how we have Alice and Bob want to measure described by Erwin Schrödinger, created entangled quantum states of the polarization state of their a pioneer of quantum theory, as photon pairs, how entanglement can respective photons. To do so, each “the characteristic trait of quantum be measured, and some of its appli- uses a rotatable, linear polarizer, a mechanics.” For many years, entan- cations to quantum technologies. device that has an intrinsic trans- gled states were relegated to being mission axis for photons. For a the subject of philosophical argu- given angle φ between the photon’s ments or were used only in experi- Classical Correlation and polarization vector and the polariz- ments aimed at investigating the Quantum State Entanglement er’s transmission axis, the photon fundamental foundations of physics. -
Abstract Book
Sunday Afternoon, January 19, 2020 PCSI insights into the electronic properties, we perform angle resolved Room Canyon/Sugarloaf - Session PCSI-1SuA photoemission spectroscopy (ARPES) after each thermal annealing step. The ARPES data show how graphene's doping changes upon thermal 2D Heterostructure Design annealing, signature of a different interaction with the Ge substrate. Moderator: Edward Yu, The University of Texas at Austin [1] J. Lee, Science, 344(2014). 2:35pm PCSI-1SuA-2 Optical Properties of Semiconducting Moiré Crystals, [2] J. Tesch, Carbon, 122(2017). Xiaoqin Elaine Li, Univ of Texas at Austin INVITED [3] G.P. Campbell, Phys. Rev. Mater., 2(2018). In van der Waals (vdW) heterostructures formed by stacking two [4] J. Tesch, Nanoscale, 10(2018). monolayers, lattice mismatch or rotational misalignment introduces an in- plane moiré superlattice. The periodic atomic alignment variations [5] D. Zhou, J. Phys. Chem. C., 122(2018). between the two layers impose both an energy and optical selection rule [6] H.W. Kim, J. Phys. Chem. Lett., 9(2018). modulations as illustrated in Fig. 1A-B. Optical properties of such moiré [7] B. Kiraly, Appl. Phys. Lett., 113(2018). superlattices have just begun to be investigated experimentally [1-5]. In this talk, I will discuss how the properties of the interlayer excitons in a twisted transition metal dichalcogenide (TMD) heterobilayer are modified PCSI by the moiré potential. Specifically, we studied MoSe2/Wse2 bilayers with small twist angles, where electrons mostly reside in the MoSe2 and holes Room Canyon/Sugarloaf - Session PCSI-2SuA nominally in the Wse2 monolayer because of the type-II band alignment. -
The Second Quantum Revolution
10.1098/rsta.2003.1227 Quantumtechnology: the second quantumrevolution ByJonathanP.Dowling 1 andGerardJ.M ilburn 2 1QuantumComputing T echnologies Group,Section 367, Jet PropulsionLaboratory, Pasadena, CA91109,USA 2Departmentof Applied Mathematics andTheoretic al Physics, University ofCambridge, Wilberforce Road,Cambridge CB3 0WA,UK and Centre forQuantum Computer T echnology, The University ofQueensland, StLucia, QLD 4072, Australia Publishedonline 20 June2003 Weare currently in the midst of a second quantumrevolution .The ¯rst quantum revolution gave usnew rules that govern physical reality.The second quantum revo- lution will take these rules and use them to develop new technologies. In this review wediscuss the principles upon which quantum technology is based and the tools required to develop it. Wediscuss anumber of examples of research programs that could deliver quantum technologies in coming decades including: quantum informa- tion technology,quantum electromechanical systems, coherent quantum electronics, quantum optics and coherent matter technology. Keywords: quantum technology;quantum information; nanotechnology, quantum optics, mesoscopics; atom optics 1.Introduction The ¯rst quantumrevolution occurred at the turn of the last century,arising out theoretical attempts to explain experiments on blackbody radiation. From that the- ory arose the fundamental idea of wave{particle duality: in particular the idea that matter particles sometimes behaved like waves, and that light waves sometimes acted like particles. This simple idea -
Violation of Heisenberg's Uncertainty Principle
Violation of Heisenberg’s uncertainty principle Koji Nagata1 and Tadao Nakamura2 1Department of Physics, Korea Advanced Institute of Science and Technology, Daejeon 305-701, Korea E-mail: ko mi [email protected] 2Department of Information and− Computer− Science, Keio University, 3-14-1 Hiyoshi, Kohoku-ku, Yokohama 223-8522, Japan E-mail: [email protected] ( Dated: July 28, 2015) Recently, violation of Heisenberg’s uncertainty relation in spin measurements is discussed [J. Erhart et al., Nature Physics 8, 185 (2012)] and [G. Sulyok et al., Phys. Rev. A 88, 022110 (2013)]. We derive the optimal limitation of Heisenberg’s uncertainty principle in a specific two-level system (e.g., electron spin, photon polarizations, and so on). Some physical situation is that we would measure σx and σy, simultaneously. The optimality is certified by the Bloch sphere. We show that a violation of Heisenberg’s uncertainty principle means a violation of the Bloch sphere in the specific case. Thus, the above experiments show a violation of the Bloch sphere when we use 1 as measurement outcome. This conclusion agrees with recent researches [K. Nagata, Int. J. Theor.± Phys. 48, 3532 (2009)] and [K. Nagata et al., Int. J. Theor. Phys. 49, 162 (2010)]. PACS numbers: 03.65.Ta, 03.67.-a I. INTRODUCTION position σx and the standard deviation of momentum σp was derived by Earle Hesse Kennard [18] later that year The quantum theory (cf. [1—5]) gives accurate and at- and by Hermann Weyl [19] in 1928. times-remarkably accurate numerical predictions. Much Recently, Ozawa discusses universally valid reformu- experimental data has fit to quantum predictions for long lation of the Heisenberg uncertainty principle on noise time. -
Book of Abstracts
CPAD Instrumentation Frontier Workshop 2021 Thursday 18 March 2021 - Monday 22 March 2021 Stony Brook, NY Book of Abstracts Contents Welcome and Introduction ................................... 1 Summary of the BRN for Detectors .............................. 1 Higgs and Energy Frontier ................................... 1 Dark Matter ........................................... 1 Cosmic Acceleration ...................................... 1 2021 DPF Instrumentation Award - Early Career ....................... 1 2020 GIRA Award - Runner up ................................. 1 Blue Sky presentation - 5’ flash talks ............................. 2 Early Career Plenary ...................................... 2 The Electron Ion Collider: Physics, Accelerator and Detector Technologies . 2 EIC Detector Needs - Discussion ................................ 2 Development of the Mu2e electromagnetic calorimeter mechanical structures . 2 Metastable Liquids: Breakthrough Technologies for Dark Matter and Neutrinos . 3 Development of the Mu2e electromagnetic calorimeter front-end and readout electronics 3 Mu2e TDAQ and slow control systems ............................ 4 DPF Instrumentation Awards ................................. 5 Neutrinos ............................................ 5 Explore the Unknown ...................................... 5 Closing Remarks and Road Ahead ............................... 5 Summary of Quantum Sensors ................................. 5 Summary of Noble Elements .................................. 5 Summary of Calorimetry -
Some Study Materials on Quantum Mechanics Part of Paper C9t (Vu Physics Hons
SOME STUDY MATERIALS ON QUANTUM MECHANICS PART OF PAPER C9T (VU PHYSICS HONS. CBCS 4TH SEMESTER) DEBASISH AICH VU CBCS Semester-IV 2019: Planck’s quantum, Planck’s constant and light as a collection of photons; Blackbody Radiation: Quantum theory of Light; Photo-electric effect and Compton scattering. De Broglie wavelength and matter waves; Davisson-Germer experiment. Wave description of particles by wave packets. Group and Phase velocities and relation between them. Two-Slit experiment with electrons. Probability. Wave amplitude and wave functions. Historical Note 1. Situation towards the end of the 19th century and the beginning of the 20th century 1.1 Advancement in Physics: Classical mechanics: Newtonian Mechanics (Principia 1687-1713-1726; Sir Isaac Newton, English, 1643-1727) > Lagrangian Formulation (1750s) (Joseph-Louis Lagrange, Italian-French, 1736-1813) > Hamiltonian Formulation (1833) (William Rowan Hamilton, Irish, 1805-1865) Electrodynamics: Maxwell’s (James Clerk Maxwell, Scottish, 1831-1879) Equations of Electromagnetic waves [1861]. [In present form by Oliver Heaviside (English), Josiah W Gibbs (American), Heinrich Hertz (German, 1857-1894) in 1884] Lorentz (Dutch, 1853-1928) Force Equation [1861 Maxwell > 1881J. J. Thomson1 (English) > 1884 Heaviside > 1895 Lorentz] Thermodynamics: Carnot Theorem (1824) [Nicolas Leonard Carnot, French 1796-1832], Maxwell-Boltzmann (Ludwig Eduard Boltzmann, German, 1844-1906) Statistics (1868). 1.2. Major unsolved Questions: Energy Distribution [푢(휈)푑휈 표푟 푢(휆)푑휆] of Blackbody Radiation. Photo electric effect: Experiment by Hertz in 1887. Stability of Rutherford’s (New Zealand-born British) atom (1911 Gold Foil Expt.). Existence of aether: Michelson (American) –Morley (American) Experiment (1887, at Western Reserve University, Ohio). Atomic Spectra: Balmer (Swiss Mathematician) series: Balmer formula (1885) 휆 = 퐵 = 퐵 Rydberg (Swedish Physicist) Formula (1888) 휈̅ = = − = 푅 − With 푅 = 1.09737309 × 10 푚 . -
Unit – I - Physics for Engineers-Spha1101
Basic Quantum Physics SCHOOL OF SCIENCE AND HUMANITIES DEPARTMENT OF PHYSICS UNIT – I - PHYSICS FOR ENGINEERS-SPHA1101 1 Basic Quantum Physics UNIT 1 BASIC QUANTUM PHYSICS 1.0 INTRODUCTION Quantum theory is the theoretical basis of modern physics that explains the behaviour of matter and energy on the scale of atoms and subatomic particles / waves where classical physics does not always apply due to wave-particle duality and the uncertainty principle. In 1900, physicist Max Planck presented his quantum theory to the German Physical Society. Planck had sought to discover the reason that radiation from a glowing body changes in color from red, to orange, and, finally, to blue as its temperature rises. The Development of Quantum Theory In 1900, Planck made the assumption that energy was made of individual units, or quanta. In 1905, Albert Einstein theorized that not just the energy, but the radiation itself was quantizedin the same manner. In 1924, Louis de Broglie proposed the wave nature of electrons and suggested that all matter has wave properties. This concept is known as the de Broglie hypothesis, an example of wave–particle duality, and forms a central part of the theory of quantum mechanics. In 1927, Werner Heisenberg proposed uncertainty principle. It states that the more precisely the position of some particle is determined, the less precisely its momentum can be known, and vice versa. The formal inequality relating 2 Basic Quantum Physics the standard deviation of position σx and the standard deviation of [3] momentum σp was derived by Earle Hesse Kennard later that year and by Hermann Weyl in 1928 ℎ ≥ 푥 푦 4 where ħ is the reduced Planck constant, h/(2π).