Tddft Derivative Couplings and Other Topics in Quantum Chemistry
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The Geometrie Phase in Quantum Systems
A. Bohm A. Mostafazadeh H. Koizumi Q. Niu J. Zwanziger The Geometrie Phase in Quantum Systems Foundations, Mathematical Concepts, and Applications in Molecular and Condensed Matter Physics With 56 Figures Springer Table of Contents 1. Introduction 1 2. Quantal Phase Factors for Adiabatic Changes 5 2.1 Introduction 5 2.2 Adiabatic Approximation 10 2.3 Berry's Adiabatic Phase 14 2.4 Topological Phases and the Aharonov—Bohm Effect 22 Problems 29 3. Spinning Quantum System in an External Magnetic Field 31 3.1 Introduction 31 3.2 The Parameterization of the Basis Vectors 31 3.3 Mead—Berry Connection and Berry Phase for Adiabatic Evolutions Magnetic Monopole Potentials 36 3.4 The Exact Solution of the Schrödinger Equation 42 3.5 Dynamical and Geometrical Phase Factors for Non-Adiabatic Evolution 48 Problems 52 4. Quantal Phases for General Cyclic Evolution 53 4.1 Introduction 53 4.2 Aharonov—Anandan Phase 53 4.3 Exact Cyclic Evolution for Periodic Hamiltonians 60 Problems 64 5. Fiber Bundles and Gauge Theories 65 5.1 Introduction 65 5.2 From Quantal Phases to Fiber Bundles 65 5.3 An Elementary Introduction to Fiber Bundles 67 5.4 Geometry of Principal Bundles and the Concept of Holonomy 76 5.5 Gauge Theories 87 5.6 Mathematical Foundations of Gauge Theories and Geometry of Vector Bundles 95 Problems 102 XII Table of Contents 6. Mathematical Structure of the Geometric Phase I: The Abelian Phase 107 6.1 Introduction 107 6.2 Holonomy Interpretations of the Geometric Phase 107 6.3 Classification of U(1) Principal Bundles and the Relation Between the Berry—Simon and Aharonov—Anandan Interpretations of the Adiabatic Phase 113 6.4 Holonomy Interpretation of the Non-Adiabatic Phase Using a Bundle over the Parameter Space 118 6.5 Spinning Quantum System and Topological Aspects of the Geometric Phase 123 Problems 126 7. -
Geometric Phase from Aharonov-Bohm to Pancharatnam–Berry and Beyond
Geometric phase from Aharonov-Bohm to Pancharatnam–Berry and beyond Eliahu Cohen1,2,*, Hugo Larocque1, Frédéric Bouchard1, Farshad Nejadsattari1, Yuval Gefen3, Ebrahim Karimi1,* 1Department of Physics, University of Ottawa, Ottawa, Ontario, K1N 6N5, Canada 2Faculty of Engineering and the Institute of Nanotechnology and Advanced Materials, Bar Ilan University, Ramat Gan 5290002, Israel 3Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel *Corresponding authors: [email protected], [email protected] Abstract: Whenever a quantum system undergoes a cycle governed by a slow change of parameters, it acquires a phase factor: the geometric phase. Its most common formulations are known as the Aharonov-Bohm, Pancharatnam and Berry phases, but both prior and later manifestations exist. Though traditionally attributed to the foundations of quantum mechanics, the geometric phase has been generalized and became increasingly influential in many areas from condensed-matter physics and optics to high energy and particle physics and from fluid mechanics to gravity and cosmology. Interestingly, the geometric phase also offers unique opportunities for quantum information and computation. In this Review we first introduce the Aharonov-Bohm effect as an important realization of the geometric phase. Then we discuss in detail the broader meaning, consequences and realizations of the geometric phase emphasizing the most important mathematical methods and experimental techniques used in the study of geometric phase, in particular those related to recent works in optics and condensed-matter physics. Published in Nature Reviews Physics 1, 437–449 (2019). DOI: 10.1038/s42254-019-0071-1 1. Introduction A charged quantum particle is moving through space. -
The Quantum Geometric Phase As a Transformation Invariant
PRAMANA © Printed in India Vol. 49, No. 1, --journal of July 1997 physics pp. 33--40 The quantum geometric phase as a transformation invariant N MUKUNDA* Centre for Theoretical Studies and Department of Physics, Indian Institute of Science, Bangalore 560012, India * Honorary Professor, Jawaharlal Nehru Centre for Advanced Scientific Research, Jakkur, Bangalore 560 064, India Abstract. The kinematic approach to the theory of the geometric phase is outlined. This phase is shown to be the simplest invariant under natural groups of transformations on curves in Hilbert space. The connection to the Bargmann invariant is brought out, and the case of group representations described. Keywords. Geometric phase; Bargmann invariant. PACS No. 03.65 1. Introduction Ever since Berry's important work of 1984 [1], the geometric phase in quantum mechanics has been extensively studied by many authors. It was soon realised that there were notable precursors to this work, such as Rytov, Vladimirskii and Pancharatnam [2]. Considerable activity followed in various groups in India too, notably the Raman Research Institute, the Bose Institute, Hyderabad University, Delhi University, the Institute of Mathematical Sciences to name a few. IIn the account to follow, a brief review of Berry's work and its extensions will be given [3]. We then turn to a description of a new approach which seems to succeed in reducing the geometric phase to its bare essentials, and which is currently being applied in various situations [4]. Its main characteristic is that one deals basically only with quantum kinematics. We define certain simple geometrical objects, or configurations of vectors, in the Hilbert space of quantum mechanics, and two natural groups of transformations acting on them. -
Basic Principles and Analytical Application of Derivative Spectrophotometry
13 Basic Principles and Analytical Application of Derivative Spectrophotometry Joanna Karpinska Institute of Chemistry, University of Bialystok, Bialystok Poland 1. Introduction Analytical methods based on measurements of UV or visible light absorption belong to the most popular and most often used in laboratory practice. Commercially available apparatuses are cheap and easy for operation. Spectrophotometric procedures usually are not time- and labour-consuming. The economical aspects of UV-Vis techniques is worth of emphasize too. It is one of the cheapest technique, so spectrophotometers are basic equipment of every laboratory. The main disadvantage and limitation of the spectrophotometry is its low selectivity. The measurement of absorbance is burden by interferences derived from others components of sample. A recorded UV-Vis spectrum is the sum of absorbances of analyte and matrix. Usually, recorded bands are well-defined but more or less distorted by a background. As the background is called absorbance exhibited by matrix (reagents or accompanied compounds). The problem with specific or nonspecific background can be omitted by measurements versus blank. Such procedure can be successfully applied only in the case of simple samples, which composition is stable and well known or when highly selective reagents are used. An isolation of an analyte from matrix is another solution for increasing the selectivity of assay. But every additional operation introduced into sample preparation procedure extents time and costs of single analysis and increases risk of loss or contamination of the analyte. One of the simplest method for an increasing a selectivity is derivatisation of spectra. This operation allows to remove spectral interferences and as a consequence leads to increase selectivity of assay. -
Geometry in Quantum Mechanics: Basic Training in Condensed Matter Physics
Geometry in Quantum Mechanics: Basic Training in Condensed Matter Physics Erich Mueller Lecture Notes: Spring 2014 Preface About Basic Training Basic Training in Condensed Matter physics is a modular team taught course offered by the theorists in the Cornell Physics department. It is designed to expose our graduate students to a broad range of topics. Each module runs 2-4 weeks, and require a range of preparations. This module, \Geometry in Quantum Mechanics," is designed for students who have completed a standard one semester graduate quantum mechanics course. Prior Topics 2006 Random Matrix Theory (Piet Brouwer) Quantized Hall Effect (Chris Henley) Disordered Systems, Computational Complexity, and Information Theory (James Sethna) Asymptotic Methods (Veit Elser) 2007 Superfluidity in Bose and Fermi Systems (Erich Mueller) Applications of Many-Body Theory (Tomas Arias) Rigidity (James Sethna) Asymptotic Analysis for Differential Equations (Veit Elser) 2008 Constrained Problems (Veit Elser) Quantum Optics (Erich Mueller) Quantum Antiferromagnets (Chris Henley) Luttinger Liquids (Piet Brouwer) 2009 Continuum Theories of Crystal Defects (James Sethna) Probes of Cold Atoms (Erich Mueller) Competing Ferroic Orders: the Magnetoelectric Effect (Craig Fennie) Quantum Criticality (Eun-Ah Kim) i 2010 Equation of Motion Approach to Many-Body Physics (Erich Mueller) Dynamics of Infectious Diseases (Chris Myers) The Theory of Density Functional Theory: Electronic, Liquid, and Joint (Tomas Arias) Nonlinear Fits to Data: Sloppiness, Differential Geometry -
Nomenclature of Carboxylic Acids • Select the Longest Carbon Chain Containing the Carboxyl Group
Chapter 5 Carboxylic Acids and Esters Carboxylic Acids • Carboxylic acids are weak organic acids which Chapter 5 contain the carboxyl group (RCO2H): Carboxylic Acids and Esters O C O H O RCOOH RCO2H Chapter Objectives: O condensed ways of • Learn to recognize the carboxylic acid, ester, and related functional groups. RCOH writing the carboxyl • Learn the IUPAC system for naming carboxylic acids and esters. group a carboxylic acid C H • Learn the important physical properties of the carboxylic acids and esters. • Learn the major chemical reaction of carboxylic acids and esters, and learn how to O predict the products of ester synthesis and hydrolysis reactions. the carboxyl group • Learn some of the important properties of condensation polymers, especially the polyesters. Mr. Kevin A. Boudreaux • The tart flavor of sour-tasting foods is often caused Angelo State University CHEM 2353 Fundamentals of Organic Chemistry by the presence of carboxylic acids. Organic and Biochemistry for Today (Seager & Slabaugh) www.angelo.edu/faculty/kboudrea 2 Nomenclature of Carboxylic Acids • Select the longest carbon chain containing the carboxyl group. The -e ending of the parent alkane name is replaced by the suffix -oic acid. • The carboxyl carbon is always numbered “1” but the number is not included in the name. • Name the substituents attached to the chain in the Nomenclature of usual way. • Aromatic carboxylic acids (i.e., with a CO2H Carboxylic Acids directly connected to a benzene ring) are named after the parent compound, benzoic acid. O C OH 3 -
1 Geometric Phases in Quantum Mechanics Y.BEN-ARYEH Physics
Geometric phases in Quantum Mechanics Y.BEN-ARYEH Physics Department , Technion-Israel Institute of Technology , Haifa 32000, Israel Email: [email protected] Various phenomena related to geometric phases in quantum mechanics are reviewed and explained by analyzing some examples. The concepts of 'parallelisms', 'connections' and 'curvatures' are applied to Aharonov-Bohm (AB) effect, to U(1) phase rotation, to SU (2) phase rotation and to holonomic quantum computation (HQC). The connections in Schrodinger equation are treated by two alternative approaches. Implementation of HQC is demonstrated by the use of 'dark states' including detailed calculations with the connections, for implementing quantum gates. 'Anyons' are related to the symmetries of the wave functions, in a two-dimensional space, and the use of this concept is demonstrated by analyzing an example taken from the field of Quantum Hall effects. 1.Introduction There are various books treating advanced topics of geometric phases [1-3]. The solutions for certain problems in this field remain , however, not always clear. The purpose of the present article is to explain various phemomena related to geometric phases and demonstrate the explanations by analyzing some examples. In a previous Review [4] the use of geometric phases related to U(1) phase rotation [5] has been described. The geometric phases have been related to topological effects [6], and an enormous amount of works has been reviewed, including both theoretical and experimental results. The aim of the present article is to extend the previous treatment [4] so that it will include now more fields , in which concepts of geometric phases are applied. -
Quantum Adiabatic Theorem and Berry's Phase Factor Page Tyler Department of Physics, Drexel University
Quantum Adiabatic Theorem and Berry's Phase Factor Page Tyler Department of Physics, Drexel University Abstract A study is presented of Michael Berry's observation of quantum mechanical systems transported along a closed, adiabatic path. In this case, a topological phase factor arises along with the dynamical phase factor predicted by the adiabatic theorem. 1 Introduction In 1984, Michael Berry pointed out a feature of quantum mechanics (known as Berry's Phase) that had been overlooked for 60 years at that time. In retrospect, it seems astonishing that this result escaped notice for so long. It is most likely because our classical preconceptions can often be misleading in quantum mechanics. After all, we are accustomed to thinking that the phases of a wave functions are somewhat arbitrary. Physical quantities will involve Ψ 2 so the phase factors cancel out. It was Berry's insight that if you move the Hamiltonian around a closed, adiabatic loop, the relative phase at the beginning and at the end of the process is not arbitrary, and can be determined. There is a good, classical analogy used to develop the notion of an adiabatic transport that uses something like a Foucault pendulum. Or rather a pendulum whose support is moved about a loop on the surface of the Earth to return it to its exact initial state or one parallel to it. For the process to be adiabatic, the support must move slow and steady along its path and the period of oscillation for the pendulum must be much smaller than that of the Earth's. -
Functional Group Transformations in Derivatives Of
Article pubs.acs.org/joc Functional Group Transformations in Derivatives of 1,4- Dihydrobenzo[1,2,4]triazinyl Radical † § † ∥ † ‡ † ⊥ Agnieszka Bodzioch, , Minyan Zheng, , Piotr Kaszynski,́ *, , and Greta Utecht , † Organic Materials Research Group Department of Chemistry, Vanderbilt University, Nashville, Tennessee 37235, United States ‡ Faculty of Chemistry, University of Łodź,́ Tamka 12, 91403 Łodź,́ Poland *S Supporting Information ABSTRACT: Transformations of functional groups OCOPh, ’ − OCH2Ph, I, NO2, and CO2Me in Blatter s radical derivatives 1 5 were investigated in order to develop synthetic tools for incorporation of the benzo[1,2,4]triazinyl system into complex molecular architectures. Thus, basic hydrolysis of OCOPh or Pd-catalyzed debenzylation of OCH2Ph gave phenol functionality, which was acylated and alkylated. Pd-catalyzed Suzuki, Negishi, Sonogashira, and Heck C−C cross-coupling reactions of iodo derivatives 1c, 1d, and 2d ffi were also successful and e cient. Reduction of NO2 in 1e led to aniline derivative 1t, which was reductively alkylated with hexanal and coupled to L-proline. Selected benzo[1,2,4]triazinyl radicals were characterized by EPR and electronic absorption spectroscopy, and the results were analyzed in tandem with DFT computational methods. Lastly, the mechanism for formation of the 1,4- dihydrobenzo[1,2,4]triazine ring was investigated using the B3LYP/6-31G(2d,p) method. ■ INTRODUCTION little attention, and only a handful of derivatives have been Stable π-delocalized radicals are becoming important structural reported in the literature. This situation changed several years elements of materials for solar cells,1 energy storage,2 ago when Koutentis began systematic development of synthetic − electronic,3,4 and biological5 8 applications.9,10 Their incorpo- access to this class of radicals. -
Geometric Phases Without Geometry
Geometric phases without geometry Amar Vutha∗ and David DeMille Department of Physics, Yale University, New Haven, CT 06520, USA Geometric phases arise in a number of physical situations and often lead to systematic shifts in frequencies or phases measured in precision experiments. We describe, by working through some simple examples, a method to calculate geometric phases that relies only on standard quantum mechanical calculations of energy level shifts. This connection between geometric phases and off- resonant energy shifts simplifies calculation of the effect in certain situations. More generally, it also provides a way to understand and calculate geometric phases without recourse to topology. PACS numbers: 03.65.Vf, 32.60.+i I. INTRODUCTION A geometric phase, often also referred to as an adiabatic phase or Berry's phase, is a real, physical phase shift that can lead to measurable effects in experiments ([1, 2, 3] are some examples). In the classic version of this effect, the state of a particle with a magnetic moment is modified under the influence of a magnetic field which undergoes a slow change in its direction. The motion of the field leads to a phase shift accumulated between the quantum states of the particle, in addition to the dynamical phase due to the Larmor precession of the magnetic moment around the magnetic field. This extra phase is termed a geometric phase because it has a simple interpretation in terms of the geometry traced out by the system's Hamiltonian as it evolves in its parameter space. We point the interested reader to [4] and references within for an excellent account of the geometric approach to calculating geometric phases, and its various connections with the topology of the parameter space. -
Anticipations of the Geometric Phase
ANTICIPATIONS OF THE GEOMETRIC PHASE The notion that a quantum system's wovefunction may not return to its original phase after its parameters cycle slowly around a circuit had many precursors—in polarized light, radio waves, molecules, matrices and curved surfaces. Michael Berry In science we like to emphasize the novelty and originality A physical example of this "global change without of our ideas. This is harmless enough, provided it does not local change" is the Foucault pendulum (figure 1), whose blind us to the fact that concepts rarely arise out of direction of swing, described by a unit vector e, is slaved to nowhere. There is always a historical context, in which the local vertical, described by the radial unit vector r. isolated precursors of the idea have already appeared. The slaving law is parallel transport, which means that What we call "discovery" sometimes looks, in retrospect, the direction of swing does not rotate about the vertical— more like emergence into the air from subterranean that is, e has no component of angular velocity along r. intellectual currents. However, in spite of never being rotated, e does not return The geometric phase, whose discovery I reported early to its original value when, after a day, r has completed a in 1983, is no exception to this rule.1 The paper was about circuit C (here a circle of latitude). The anholonomy is the quantum systems forced round a cycle by a slow circuit of angle between the initial and final swing directions e, and parameters that govern them; it gave rise to a number of is equal to the solid angle subtended at the Earth's center applications and several generalizations, documented in a byC. -
Topological Transition in Measurement-Induced Geometric Phases
Topological transition in measurement-induced geometric phases Valentin Gebharta,b,1, Kyrylo Snizhko b,1 , Thomas Wellensa, Andreas Buchleitnera, Alessandro Romitoc, and Yuval Gefenb,2 aPhysikalisches Institut, Albert-Ludwigs-Universitat¨ Freiburg, 79104 Freiburg, Germany; bDepartment of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel; and cDepartment of Physics, Lancaster University, Lancaster LA1 4YB, United Kingdom Edited by Yakir Aharonov, Chapman University, Orange, CA, and approved February 4, 2020 (received for review July 10, 2019) The state of a quantum system, adiabatically driven in a cycle, may the Pancharatnam phase is equal to the Berry phase associated acquire a measurable phase depending only on the closed trajec- with the trajectory that connects the states j k i by the shortest tory in parameter space. Such geometric phases are ubiquitous geodesics in Hilbert space (6, 16). and also underline the physics of robust topological phenom- The Pancharatnam phase can quite naturally be interpreted ena such as the quantum Hall effect. Equivalently, a geometric as a result of a sequence of strong (projective) measurements phase may be induced through a cyclic sequence of quantum acting on the system and yielding specific measurement read- measurements. We show that the application of a sequence of outs (17). This interpretation is valid for optical experiments weak measurements renders the closed trajectories, hence the observing the Pancharatnam phase induced with sequences of geometric phase, stochastic. We study the concomitant probabil- polarizers (18). Such a phase can be consistently defined despite ity distribution and show that, when varying the measurement the fact that measurements (typically considered an incoher- strength, the mapping between the measurement sequence and ent process) are involved.