Beyond Born-Oppenheimer Design of Thermally Activated Delayed Fluorescence Emitters. Tom Penfold
|
|
- Eustace Brooks
- 5 years ago
- Views:
Transcription
1 Beyond Born-Oppenheimer Design of Thermally Activated Delayed Fluorescence Emitters Tom Penfold
2 Outline Introduction to Solving the Time-Dependent Schrödinger Equation What Problem are we trying to solve? How can we use theory? What are the different levels of theory 2 Solving the Time-Dependent Schrödinger Equation II How to use quantum dynamics The MDH Method Developing a Model Potential Energy Surface. Beyond Born-Oppenheimer Design of Thermally Activated Delayed Fluorescence Emitters The role of molecular vibrations in TADF The effect of Nonadiabatic Coupling Perspectives
3 Schematic for TADF S ΔE S-T k nr k isc k risc k risc k isc exp(-δe S-T /k b T) T k nr k f k ph S 0 Or
4 What are the problems? Rate calculated using Fermi Golden rule is far smaller than experimentally observed rates.
5 Clues from Experiment Switching TADF to RTP.. Ward, JS., et al. Chem. Comm. 52 (206):
6 Setting Up the Hamiltonian Ĥ HFI& =&0.2&cm *& Ĥ SOC =&2&cm *& Ĥ vib& &65&cm *& LE Pictorial Representation Matrix Representation
7 Dynamics ISC Dynamics a. Black: Hamiltonian as described. b. Red: Increased nonadiabatic coupling. c. Blue: Smaller energy gap. risc Dynamics a. Density Matrix simulations to address risc at 00 K. b. ISC and risc are connected. c. No nonadiabatic coupling -> Very slow rate. ChemPhysChem 7 (9),
8 Ĥ HFI& =&0.2&cm *& Ĥ SOC =&2&cm *& Ĥ vib& &65&cm *& LE What is the mechanism? Clearly two state are insufficient and so must move past first order perturbation theory. First step is a internal conversion between the triplet states. Allowed transition and therefore its fast. Second step:
9 The effect of the embedding environment (a) (b) k risc& (c) k risc& LE LE k risc& LE a! b! Changing the polarity shifts the states but not the LE.! M Etherington Nat Commun. 206; 7: 680.
10 What about D-A-D D-A (C s ) D-A-D (C 2v )! (A ) (A ) (B ) (A 2 ) (A 2 ) (B ) LE (A ) LE (B ) LE (A 2 )
11 How to think about the mechanism? Ĥ HFI& =&0.2&cm *& Ĥ SOC =&2&cm *& Ĥ vib& &65&cm *& LE - LE In reality the interchangeability depends upon the strength of the coupling. Slightly different mechanism Marian et al. [Journal of Physical Chemistry C 20 (206): ], but overall message- mixing and vibrations are important.
12 The extended picture of TADF. S k nr k isc ΔE S-T2 T 2 k risc T 2 ΔE S-T T k f k nr k ph T k ic/ric S 0 Kinetically, because the T-T2 conversion is so fast, its appears as a equilibrium and therefore the state model behaves in a similar fashion to the 2 state model. 2 This is not limited to states, there can be many more involved.
13 The effect of nonadiabatic coupling. Physical Chemistry Chemical Physics 9, (207)
14 k risc as a function of the energy gaps k risc shown as a function of the two energy gaps present in the state model. Unsurprisingly the rate is largest when the energy gap is smallest. As ΔE S-T is increased, the rate decreases. The opposite behavior is seen for ΔE T-T2, suggesting the importance of this energy gap, which is coupled by nonadiabatic coupling.
15 Non-Arrhenius TADF Ĥ HFI& =&0.2&cm *& Ĥ SOC =&2&cm *& Ĥ vib& &65&cm *& LE Non-adiabatic coupling results in mixingpopulation transfer without temperature. Physical Chemistry Chemical Physics 9, (207)
16 Regio- and Stereoselectivity The structure plays a big role and can be interconverted. 0. ev energy above S minimum is sufficient to convert. Nat Commun :4987
17 A different approach to design. LE LE (a) Present TADF Limited to small radiative rates. (b) Ideal TADF Large radiative rates achievable. Within the present approach, the nonadiabatic coupling mechanism doesn t lead to any significant advances. We propose an alternative approach
18 Considerations for TADF OLEDs Molecular Vibrations Aligning Energy Levels High Performing TADF OLEDs Effect of Embedding Environment Molecular Structure Need to marry detailed studies and high throughput!
19 Conclusions and Outlook Insight into Theory What Problem are we trying to solve? How can we use theory? What are the different levels of theory? 2 Insight into TADF Mechanism How to use quantum dynamics The MDH Method Developing a Model Potential Energy Surface. What needs to be done? The role of molecular vibrations in TADF The effect of Nonadiabatic Coupling Perspectives
Introduction to Solving the Time- Dependent Schrödinger Equation. Tom Penfold
Introduction to Solving the Time- Dependent Schrödinger Equation Tom Penfold Outline 1 Introduction to Solving the Time-Dependent Schrödinger Equation What problems are we trying to solve? How can we use
More informationThe Role of Molecular Structure And Conformation in TADF
II The Role of Molecular Structure And Conformation in TADF Physics Fernando Dias Paloma dos Santo Lays Marc Etherington Heather Cole Przemyslaw Data David Graves Chemistry Martin Bryce Jonathan Ward Vandana
More informationCHEM3023: Spins, Atoms and Molecules
CHEM3023: Spins, Atoms and Molecules Lecture 3 The Born-Oppenheimer approximation C.-K. Skylaris Learning outcomes Separate molecular Hamiltonians to electronic and nuclear parts according to the Born-Oppenheimer
More informationHelsinki Winterschool in Theoretical Chemistry 2013
Helsinki Winterschool in Theoretical Chemistry 2013 Prof. Dr. Christel M. Marian Institute of Theoretical and Computational Chemistry Heinrich-Heine-University Düsseldorf Helsinki, December 2013 C. M.
More informationMarcus Theory for Electron Transfer a short introduction
Marcus Theory for Electron Transfer a short introduction Minoia Andrea MPIP - Journal Club -Mainz - January 29, 2008 1 Contents 1 Intro 1 2 History and Concepts 2 2.1 Frank-Condon principle applied to
More informationarxiv: v2 [physics.chem-ph] 8 Apr 2016
Rates and singlet/triplet ratios from TADF transients Mitchell C. Nelson (Dated: 15 March 2016) arxiv:1603.08998v2 [physics.chem-ph] 8 Apr 2016 Thermally activated delayed fluorescence has been reported
More informationPHOTOCHEMISTRY NOTES - 1 -
- 1 - PHOTOCHEMISTRY NOTES 1 st Law (Grotthus-Draper Law) Only absorbed radiation produces chemical change. Exception inelastic scattering of X- or γ-rays (electronic Raman effect). 2 nd Law (Star-Einstein
More informationDiatomic Molecules. 7th May Hydrogen Molecule: Born-Oppenheimer Approximation
Diatomic Molecules 7th May 2009 1 Hydrogen Molecule: Born-Oppenheimer Approximation In this discussion, we consider the formulation of the Schrodinger equation for diatomic molecules; this can be extended
More informationClass 24: Density of States
Class 24: Density of States The solution to the Schrödinger wave equation showed us that confinement leads to quantization. The smaller the region within which the electron is confined, the more widely
More informationElectronic Supplementary Information
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2016 Electronic Supplementary Information Understanding the efficiency drooping
More information23 The Born-Oppenheimer approximation, the Many Electron Hamiltonian and the molecular Schrödinger Equation M I
23 The Born-Oppenheimer approximation, the Many Electron Hamiltonian and the molecular Schrödinger Equation 1. Now we will write down the Hamiltonian for a molecular system comprising N nuclei and n electrons.
More informationLuminescence. Photoluminescence (PL) is luminescence that results from optically exciting a sample.
Luminescence Topics Radiative transitions between electronic states Absorption and Light emission (spontaneous, stimulated) Excitons (singlets and triplets) Franck-Condon shift(stokes shift) and vibrational
More informationQuantum Master Equations for the Electron Transfer Problem
20/01/2010 Quantum Master Equations for the Electron Transfer Problem Seminarvortrag Dekohaerenz und Dissipation in Quantensystemen Antonio A. Gentile The general transport problem in micro/mesoscopic
More informationRotations and vibrations of polyatomic molecules
Rotations and vibrations of polyatomic molecules When the potential energy surface V( R 1, R 2,..., R N ) is known we can compute the energy levels of the molecule. These levels can be an effect of: Rotation
More informationWhat dictates the rate of radiative or nonradiative excited state decay?
What dictates the rate of radiative or nonradiative excited state decay? Transitions are faster when there is minimum quantum mechanical reorganization of wavefunctions. This reorganization energy includes
More informationAnharmonic energy in periodic systems
Anharmonic energy in periodic systems Bartomeu Monserrat University of Cambridge Electronic Structure Discussion Group 13 March 213 Vibrational properties overview Harmonic phonons are a very good approximation.
More informationLaser Induced Control of Condensed Phase Electron Transfer
Laser Induced Control of Condensed Phase Electron Transfer Rob D. Coalson, Dept. of Chemistry, Univ. of Pittsburgh Yuri Dakhnovskii, Dept. of Physics, Univ. of Wyoming Deborah G. Evans, Dept. of Chemistry,
More informationAn Introduction to Quantum Chemistry and Potential Energy Surfaces. Benjamin G. Levine
An Introduction to Quantum Chemistry and Potential Energy Surfaces Benjamin G. Levine This Week s Lecture Potential energy surfaces What are they? What are they good for? How do we use them to solve chemical
More informationThe linear electron-phonon coupling model for molecular nonadiabatic ET. Simple derivations of the electron transfer rate
The linear ectron-phonon coupling mod for molecular nonadiabatic T Simple derivations of the ectron transfer rate Spiros S. Sourtis epartment of Physics, University of Cyprus Nicosia Cyprus Ph Course CN
More informationHarmonic Oscillator with raising and lowering operators. We write the Schrödinger equation for the harmonic oscillator in one dimension as follows:
We write the Schrödinger equation for the harmonic oscillator in one dimension as follows: H ˆ! = "!2 d 2! + 1 2µ dx 2 2 kx 2! = E! T ˆ = "! 2 2µ d 2 dx 2 V ˆ = 1 2 kx 2 H ˆ = ˆ T + ˆ V (1) where µ is
More informationH + HCO H + HCO 1 A2 1 A 1 CO + H 2
Chemistry 6 Molecular Spectra & Molecular Structure Week # 6 Electronic Spectroscopy and Non-Radiative Processes As was noted briefly last week, the ultraviolet spectroscopy of formaldehyde (specifically
More informationIntroduction to Hartree-Fock Molecular Orbital Theory
Introduction to Hartree-Fock Molecular Orbital Theory C. David Sherrill School of Chemistry and Biochemistry Georgia Institute of Technology Origins of Mathematical Modeling in Chemistry Plato (ca. 428-347
More informationTheoretical Photochemistry WiSe 2017/18
Theoretical Photochemistry WiSe 2017/18 Lecture 7 Irene Burghardt (burghardt@chemie.uni-frankfurt.de) http://www.theochem.uni-frankfurt.de/teaching/ Theoretical Photochemistry 1 Topics 1. Photophysical
More informationDesign of organic TADF molecules. The role of E(S 1 -T 1 ): From fluorescence to TADF and beyond - towards the fourth generation OLED mechanism.
Design of organic TADF molecules. The role of E(S -T ): From fluorescence to TADF and beyond - towards the fourth generation OLED mechanism. H. Yersin, L. Mataranga-Popa, R. Czerwieniec University of Regensburg,
More informationTheoretical Photochemistry WiSe 2016/17
Theoretical Photochemistry WiSe 2016/17 Lecture 8 Irene Burghardt burghardt@chemie.uni-frankfurt.de) http://www.theochem.uni-frankfurt.de/teaching/ Theoretical Photochemistry 1 Topics 1. Photophysical
More informationElectronic Structure Methodology 1
Electronic Structure Methodology 1 Chris J. Pickard Lecture Two Working with Density Functional Theory In the last lecture we learnt how to write the total energy as a functional of the density n(r): E
More informationVibronic quantum dynamics of exciton relaxation/trapping in molecular aggregates
Symposium, Bordeaux Vibronic quantum dynamics of exciton relaxation/trapping in molecular aggregates Alexander Schubert Institute of Physical and Theoretical Chemistry, University of Würzburg November
More information12.2 MARCUS THEORY 1 (12.22)
Andrei Tokmakoff, MIT Department of Chemistry, 3/5/8 1-6 1. MARCUS THEORY 1 The displaced harmonic oscillator (DHO) formalism and the Energy Gap Hamiltonian have been used extensively in describing charge
More informationChem 442 Review for Exam 2. Exact separation of the Hamiltonian of a hydrogenic atom into center-of-mass (3D) and relative (3D) components.
Chem 44 Review for Exam Hydrogenic atoms: The Coulomb energy between two point charges Ze and e: V r Ze r Exact separation of the Hamiltonian of a hydrogenic atom into center-of-mass (3D) and relative
More informationΨ t = ih Ψ t t. Time Dependent Wave Equation Quantum Mechanical Description. Hamiltonian Static/Time-dependent. Time-dependent Energy operator
Time Dependent Wave Equation Quantum Mechanical Description Hamiltonian Static/Time-dependent Time-dependent Energy operator H 0 + H t Ψ t = ih Ψ t t The Hamiltonian and wavefunction are time-dependent
More informationOrganic Photochemistry and Pericyclic Reactions Prof. N.D. Pradeep Singh Department of Chemistry Indian Institute of Technology Kharagpur
Organic Photochemistry and Pericyclic Reactions Prof. N.D. Pradeep Singh Department of Chemistry Indian Institute of Technology Kharagpur Lecture No. #01 Introduction to Organic Photochemistry (Refer Slide
More informationSelected Publications of Prof. Dr. Wenjian Liu
Selected Publications of Prof. Dr. Wenjian Liu College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China 1 Fundamentals of relativistic molecular quantum mechanics 1. Handbook
More informationVibrations and Rotations of Diatomic Molecules
Chapter 6 Vibrations and Rotations of Diatomic Molecules With the electronic part of the problem treated in the previous chapter, the nuclear motion shall occupy our attention in this one. In many ways
More informationQuantum dynamics in complex environments towards biological and nanostructured systems
Quantum dynamics in complex environments towards biological and nanostructured systems Chris Engelbrecht Summer School on Quantum Biology Lecture 4 Irene Burghardt Department of Physical and Theoretical
More informationTheory of electron transfer. Winterschool for Theoretical Chemistry and Spectroscopy Han-sur-Lesse, Belgium, December 2011
Theory of electron transfer Winterschool for Theoretical Chemistry and Spectroscopy Han-sur-Lesse, Belgium, 12-16 December 2011 Electron transfer Electrolyse Battery Anode (oxidation): 2 H2O(l) O2(g) +
More informationChemistry 2. Lecture 1 Quantum Mechanics in Chemistry
Chemistry 2 Lecture 1 Quantum Mechanics in Chemistry Your lecturers 8am Assoc. Prof Timothy Schmidt Room 315 timothy.schmidt@sydney.edu.au 93512781 12pm Assoc. Prof. Adam J Bridgeman Room 222 adam.bridgeman@sydney.edu.au
More informationAyan Chattopadhyay Mainak Mustafi 3 rd yr Undergraduates Integrated MSc Chemistry IIT Kharagpur
Ayan Chattopadhyay Mainak Mustafi 3 rd yr Undergraduates Integrated MSc Chemistry IIT Kharagpur Under the supervision of: Dr. Marcel Nooijen Associate Professor Department of Chemistry University of Waterloo
More informationPath integrals and the classical approximation 1 D. E. Soper 2 University of Oregon 14 November 2011
Path integrals and the classical approximation D. E. Soper University of Oregon 4 November 0 I offer here some background for Sections.5 and.6 of J. J. Sakurai, Modern Quantum Mechanics. Introduction There
More informationCHEM-UA 127: Advanced General Chemistry I
1 CHEM-UA 127: Advanced General Chemistry I I. OVERVIEW OF MOLECULAR QUANTUM MECHANICS Using quantum mechanics to predict the chemical bonding patterns, optimal geometries, and physical and chemical properties
More informationMixed quantum-classical dynamics. Maurizio Persico. Università di Pisa Dipartimento di Chimica e Chimica Industriale
Mixed quantum-classical dynamics. Maurizio Persico Università di Pisa Dipartimento di Chimica e Chimica Industriale Outline of this talk. The nuclear coordinates as parameters in the time-dependent Schroedinger
More informationAndré Schleife Department of Materials Science and Engineering
André Schleife Department of Materials Science and Engineering Yesterday you (should have) learned this: http://upload.wikimedia.org/wikipedia/commons/e/ea/ Simple_Harmonic_Motion_Orbit.gif 1. deterministic
More information11.1. FÖRSTER RESONANCE ENERGY TRANSFER
11-1 11.1. FÖRSTER RESONANCE ENERGY TRANSFER Förster resonance energy transfer (FRET) refers to the nonradiative transfer of an electronic excitation from a donor molecule to an acceptor molecule: D *
More informationIntroduction to Theories of Chemical Reactions. Graduate Course Seminar Beate Flemmig FHI
Introduction to Theories of Chemical Reactions Graduate Course Seminar Beate Flemmig FHI I. Overview What kind of reactions? gas phase / surface unimolecular / bimolecular thermal / photochemical What
More informationQuantum Quenches in Extended Systems
Quantum Quenches in Extended Systems Spyros Sotiriadis 1 Pasquale Calabrese 2 John Cardy 1,3 1 Oxford University, Rudolf Peierls Centre for Theoretical Physics, Oxford, UK 2 Dipartimento di Fisica Enrico
More informationThe Potential Energy Surface (PES) Preamble to the Basic Force Field Chem 4021/8021 Video II.i
The Potential Energy Surface (PES) Preamble to the Basic Force Field Chem 4021/8021 Video II.i The Potential Energy Surface Captures the idea that each structure that is, geometry has associated with it
More informationAdiabatic quantum computation a tutorial for computer scientists
Adiabatic quantum computation a tutorial for computer scientists Itay Hen Dept. of Physics, UCSC Advanced Machine Learning class UCSC June 6 th 2012 Outline introduction I: what is a quantum computer?
More informationCharge and Energy Transfer Dynamits in Molecular Systems
Volkhard May, Oliver Kühn Charge and Energy Transfer Dynamits in Molecular Systems Second, Revised and Enlarged Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Contents 1 Introduction 19 2 Electronic
More informationBorn-Oppenheimer Approximation
Born-Oppenheimer Approximation Adiabatic Assumption: Nuclei move so much more slowly than electron that the electrons that the electrons are assumed to be obtained if the nuclear kinetic energy is ignored,
More informationAb initio Molecular Dynamics Born Oppenheimer and beyond
Ab initio Molecular Dynamics Born Oppenheimer and beyond Reminder, reliability of MD MD trajectories are chaotic (exponential divergence with respect to initial conditions), BUT... With a good integrator
More informationLecture 08 Born Oppenheimer Approximation
Chemistry II: Introduction to Molecular Spectroscopy Prof. Mangala Sunder Department of Chemistry and Biochemistry Indian Institute of Technology, Madras Lecture 08 Born Oppenheimer Approximation Welcome
More informationMolecular energy levels
Molecular energy levels Hierarchy of motions and energies in molecules The different types of motion in a molecule (electronic, vibrational, rotational,: : :) take place on different time scales and are
More informationg, 2.5 mol%) were placed in a sealed tube and then N-methylpyrrolidone (NMP) (1.00 ml)
Supporting Information Molecular Design of Highly Efficient Thermally Activated Delayed Fluorescence Hosts for Blue Phosphorescent and Fluorescent Organic Light-Emitting Diodes Chih-Chun Lin,, Min-Jie
More informationFluorescence (Notes 16)
Fluorescence - 2014 (Notes 16) XV 74 Jablonski diagram Where does the energy go? Can be viewed like multistep kinetic pathway 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet
More informationDihedral Angle Control of Blue Thermally-
Supplementary Information Dihedral Angle Control of Blue Thermally- Activated Delayed Fluorescent Emitters through Donor Substitution Position for Efficient Reverse Intersystem Crossing Chan Seok Oh 1,
More information5.80 Small-Molecule Spectroscopy and Dynamics
MIT OpenCourseWare http://ocw.mit.edu 5.80 Small-Molecule Spectroscopy and Dynamics Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. LECTURE
More informationFirst-principles modeling: The evolution of the field from Walter Kohn s seminal work to today s computer-aided materials design
First-principles modeling: The evolution of the field from Walter Kohn s seminal work to today s computer-aided materials design Peter Kratzer 5/2/2018 Peter Kratzer Abeokuta School 5/2/2018 1 / 34 Outline
More informationOptics and Response Functions
Theory seminar: Electronic and optical properties of graphene Optics and Response Functions Matthias Droth, 04.07.2013 Outline: Light absorption by Dirac fermions Intro: response functions The optics of
More informationUV-vis (Electronic) Spectra Ch.13 Atkins, Ch.19 Engel
XV 74 UV-vis (Electronic) Spectra-2014 -Ch.13 Atkins, Ch.19 Engel Most broadly used analytical tech / especially bio-applic. inexpensive optics / solvent & cell usually not problem intense transitions
More informationHigh-efficiency diphenylsulfon derivatives-based organic lightemitting. diode exhibiting thermally activated delayed fluorescence
High-efficiency diphenylsulfon derivatives-based organic lightemitting diode exhibiting thermally activated delayed fluorescence *, ** Geon Hyeong Lee* and Young Sik Kim *Department of Information Display,
More informationExp. 4. Quantum Chemical calculation: The potential energy curves and the orbitals of H2 +
Exp. 4. Quantum Chemical calculation: The potential energy curves and the orbitals of H2 + 1. Objectives Quantum chemical solvers are used to obtain the energy and the orbitals of the simplest molecules
More information2.4. Quantum Mechanical description of hydrogen atom
2.4. Quantum Mechanical description of hydrogen atom Atomic units Quantity Atomic unit SI Conversion Ang. mom. h [J s] h = 1, 05459 10 34 Js Mass m e [kg] m e = 9, 1094 10 31 kg Charge e [C] e = 1, 6022
More informationDevelopment and application for X-ray excited optical luminescence (XEOL) technology at STXM beamline of SSRF
Development and application for X-ray excited optical luminescence (XEOL) technology at STXM beamline of SSRF Content Introduction to XEOL Application of XEOL Development and Application of XEOL in STXM
More informationNon Adiabatic Transitions near Avoided Crossings: Theory and Numerics
Non Adiabatic Transitions near Avoided Crossings: Theory and Numerics Raoul Bourquin a, Vasile Gradinaru a, George A. Hagedorn b April 8, 2011 Abstract We present a review of rigorous mathematical results
More informationCHEMISTRY Topic #1: Bonding What Holds Atoms Together? Spring 2012 Dr. Susan Lait
CHEMISTRY 2000 Topic #1: Bonding What Holds Atoms Together? Spring 2012 Dr. Susan Lait Why Do Bonds Form? An energy diagram shows that a bond forms between two atoms if the overall energy of the system
More informationVisit for more fantastic resources. OCR. A Level. A Level Physics. Quantum Physics (Answers) Name: Total Marks: /30
Visit http://www.mathsmadeeasy.co.uk/ for more fantastic resources. OCR A Level A Level Physics Quantum Physics (Answers) Name: Total Marks: /30 Maths Made Easy Complete Tuition Ltd 2017 1. Numerous models
More informationWhen are electrons fast and are Born and Oppenheimer correct?
When are electrons fast and are Born and Oppenheimer correct? Wim J. van der Zande Department of Molecular and Laser Physics University of Nijmegen Han-Sur-Lesse, Winter 2003 Contents of the Lectures 0.
More informationVALENCE Hilary Term 2018
VALENCE Hilary Term 2018 8 Lectures Prof M. Brouard Valence is the theory of the chemical bond Outline plan 1. The Born-Oppenheimer approximation 2. Bonding in H + 2 the LCAO approximation 3. Many electron
More informationNonradiative relaxation processes in condensed phases: Quantum versus classical baths
JOURNAL OF CHEMICAL PHYSICS VOLUME 11, NUMBER 11 15 MARCH 1999 Nonradiative relaxation processes in condensed phases: Quantum versus classical baths S. A. Egorov Theoretical Chemistry Institute and Department
More information221B Lecture Notes Many-Body Problems II Molecular Physics
1 Molecules 221B Lecture Notes Many-Body Problems II Molecular Physics In this lecture note, we discuss molecules. I cannot go into much details given I myself am not familiar enough with chemistry. But
More informationTransition probabilities and couplings
L6 Transition probabilities and couplings Mario Barbatti A*Midex Chair Professor mario.barbatti@univ amu.fr Aix Marseille Université, Institut de Chimie Radicalaire LIGT AND Fermi s golden rule LIGT AND
More informationQuantum Theory of Matter
Imperial College London Department of Physics Professor Ortwin Hess o.hess@imperial.ac.uk Quantum Theory of Matter Spring 014 1 Periodic Structures 1.1 Direct and Reciprocal Lattice (a) Show that the reciprocal
More informationSupporting Information
Supporting Information Mulifunctional Dendritic Emitter: Aggregation-Induced Emission Enhanced, Thermally Activated Delayed Fluorescent Material for Solution- Processed Multilayered Organic Light-Emitting
More informationMolecular Dynamics. Park City June 2005 Tully
Molecular Dynamics John Lance Natasa Vinod Xiaosong Dufie Priya Sharani Hongzhi Group: August, 2004 Prelude: Classical Mechanics Newton s equations: F = ma = mq = p Force is the gradient of the potential:
More informationQuantum Mechanical Simulations
Quantum Mechanical Simulations Prof. Yan Wang Woodruff School of Mechanical Engineering Georgia Institute of Technology Atlanta, GA 30332, U.S.A. yan.wang@me.gatech.edu Topics Quantum Monte Carlo Hartree-Fock
More informationStructure of diatomic molecules
Structure of diatomic molecules January 8, 00 1 Nature of molecules; energies of molecular motions Molecules are of course atoms that are held together by shared valence electrons. That is, most of each
More information2. The Schrödinger equation for one-particle problems. 5. Atoms and the periodic table of chemical elements
1 Historical introduction The Schrödinger equation for one-particle problems 3 Mathematical tools for quantum chemistry 4 The postulates of quantum mechanics 5 Atoms and the periodic table of chemical
More informationQuantum Physics II (8.05) Fall 2002 Outline
Quantum Physics II (8.05) Fall 2002 Outline 1. General structure of quantum mechanics. 8.04 was based primarily on wave mechanics. We review that foundation with the intent to build a more formal basis
More informationPhonon wavefunctions and electron phonon interactions in semiconductors
Phonon wavefunctions and electron phonon interactions in semiconductors Bartomeu Monserrat bm418@cam.ac.uk University of Cambridge Quantum Monte Carlo in the Apuan Alps VII QMC in the Apuan Alps VII Bartomeu
More informationTheoretical investigation of internal conversion in chromyl chloride
Proc. Indian Acad. Sci. (Chem. Sci.), Vol. 103, No. 3, March 1991, pp. 369-373. 9 Printed in India. Theoretical investigation of internal conversion in chromyl chloride S RASHEV Institute of Solid State
More informationIntroduction to Computational Chemistry
Introduction to Computational Chemistry Vesa Hänninen Laboratory of Physical Chemistry Chemicum 4th floor vesa.hanninen@helsinki.fi September 10, 2013 Lecture 3. Electron correlation methods September
More informationAtomic Structure and Processes
Chapter 5 Atomic Structure and Processes 5.1 Elementary atomic structure Bohr Orbits correspond to principal quantum number n. Hydrogen atom energy levels where the Rydberg energy is R y = m e ( e E n
More informationControlled collisions of a single atom and an ion guided by movable trapping potentials
Controlled collisions of a single atom and an ion guided by movable trapping potentials Zbigniew Idziaszek CNR-INFM BEC Center, I-38050 Povo (TN), Italy and Center for Theoretical Physics, Polish Academy
More informationr R A 1 r R B + 1 ψ(r) = αψ A (r)+βψ B (r) (5) where we assume that ψ A and ψ B are ground states: ψ A (r) = π 1/2 e r R A ψ B (r) = π 1/2 e r R B.
Molecules Initial questions: What are the new aspects of molecules compared to atoms? What part of the electromagnetic spectrum can we probe? What can we learn from molecular spectra? How large a molecule
More informationPhysical Chemistry Lab II CHEM 4644 Spring 2011 Final Exam 5 questions at 3 points each equals 15 total points possible.
Physical Chemistry Lab II Name: KEY CHEM 4644 Spring 2011 Final Exam 5 questions at 3 points each equals 15 total points possible. Constants: c = 3.00 10 8 m/s h = 6.63 10-34 J s 1 Hartree = 4.36 10-18
More informationIntroduction to Computational Chemistry
Introduction to Computational Chemistry Vesa Hänninen Laboratory of Physical Chemistry room B430, Chemicum 4th floor vesa.hanninen@helsinki.fi September 3, 2013 Introduction and theoretical backround September
More informationLecture 9: Molecular Orbital theory for hydrogen molecule ion
Lecture 9: Molecular Orbital theory for hydrogen molecule ion Molecular Orbital Theory for Hydrogen Molecule Ion We have seen that the Schrödinger equation cannot be solved for many electron systems. The
More informationWhat are molecular orbitals? QUANTUM MODEL. notes 2 Mr.Yeung
What are molecular orbitals? QUANTUM MODEL notes 2 Mr.Yeung Recall, the quantum model is about electrons behaving both a wave and a particle. Electrons are in areas of calculated probability, these are
More informationFinite-size corrections to Fermi s golden rule
Hokkaido University E-mail: ishikawa@particle.sci.hokudai.ac.jp Yutaka Tobita Hokkaido University E-mail: tobita@particle.sci.hokudai.ac.jp The transition process in quantum mechanics has been studied
More informationPreliminary Quantum Questions
Preliminary Quantum Questions Thomas Ouldridge October 01 1. Certain quantities that appear in the theory of hydrogen have wider application in atomic physics: the Bohr radius a 0, the Rydberg constant
More informationConical Intersections. Spiridoula Matsika
Conical Intersections Spiridoula Matsika The Born-Oppenheimer approximation Energy TS Nuclear coordinate R ν The study of chemical systems is based on the separation of nuclear and electronic motion The
More informationAtomic and Molecular Orbitals
7 Atomic and Molecular Orbitals Chemists have developed a variety of methods for describing electrons in molecules. Lewis structures are the most familiar. These drawings assign pairs of electrons either
More informationBrief review of Quantum Mechanics (QM)
Brief review of Quantum Mechanics (QM) Note: This is a collection of several formulae and facts that we will use throughout the course. It is by no means a complete discussion of QM, nor will I attempt
More informationLecture 6: Fluctuation-Dissipation theorem and introduction to systems of interest
Lecture 6: Fluctuation-Dissipation theorem and introduction to systems of interest In the last lecture, we have discussed how one can describe the response of a well-equilibriated macroscopic system to
More informationQuantum Physics III (8.06) Spring 2007 FINAL EXAMINATION Monday May 21, 9:00 am You have 3 hours.
Quantum Physics III (8.06) Spring 2007 FINAL EXAMINATION Monday May 21, 9:00 am You have 3 hours. There are 10 problems, totalling 180 points. Do all problems. Answer all problems in the white books provided.
More informationAdvanced Quantum Mechanics
Advanced Quantum Mechanics University of York Lecturer: Rex Godby Notes by Victor Naden Robinson Lecture 1: TDSE Lecture 2: TDSE Lecture 3: FMG Lecture 4: FMG Lecture 5: Ehrenfest s Theorem and the Classical
More informationAN ACCELERATED SURFACE-HOPPING METHOD FOR COMPUTATIONAL SEMICLASSICAL MOLECULAR DYNAMICS. Laren K. Mortensen
AN ACCELERATED SURFACE-HOPPING METHOD FOR COMPUTATIONAL SEMICLASSICAL MOLECULAR DYNAMICS by Laren K. Mortensen A senior thesis submitted to the faculty of Brigham Young University in partial fulfillment
More informationd 3 r d 3 vf( r, v) = N (2) = CV C = n where n N/V is the total number of molecules per unit volume. Hence e βmv2 /2 d 3 rd 3 v (5)
LECTURE 12 Maxwell Velocity Distribution Suppose we have a dilute gas of molecules, each with mass m. If the gas is dilute enough, we can ignore the interactions between the molecules and the energy will
More informationVibrational Spectra (IR and Raman) update Tinoco has very little, p.576, Engel Ch. 18, House Ch. 6
Vibrational Spectra (IR and Raman)- 2010 update Tinoco has very little, p.576, Engel Ch. 18, House Ch. 6 Born-Oppenheimer approx. separate electron-nuclear Assume elect-nuclear motion separate, full wave
More informationChemistry 2. Molecular Photophysics
Chemistry 2 Lecture 12 Molecular Photophysics Assumed knowledge Electronic states are labelled using their spin multiplicity with singlets having all electron spins paired and triplets having two unpaired
More information2m 2 Ze2. , where δ. ) 2 l,n is the quantum defect (of order one but larger
PHYS 402, Atomic and Molecular Physics Spring 2017, final exam, solutions 1. Hydrogenic atom energies: Consider a hydrogenic atom or ion with nuclear charge Z and the usual quantum states φ nlm. (a) (2
More information