Can we build individual molecules atom by atom? Lecture 2.

Slides:



Advertisements
Similar presentations
Chemical bonding in molecules
Advertisements

Cavity cooling of a single atom James Millen 21/01/09.
Journal Club: Introduction to Fluorescence Spectroscopy and Microscopy Avtar Singh 4/5/11.
Chemistry 2 Lecture 2 Particle in a box approximation.
OPTICAL ABSORPTION.
Introduction to Molecular Orbitals
Chemistry 2 Lecture 1 Quantum Mechanics in Chemistry.
Solving Equations = 4x – 5(6x – 10) -132 = 4x – 30x = -26x = -26x 7 = x.
Lecture 36 Electronic spectroscopy (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been developed.
Lecture 23 Born-Oppenheimer approximation (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been developed.
Chemistry 2 Lecture 10 Vibronic Spectroscopy. Learning outcomes from lecture 9 Excitations in the visible and ultraviolet correspond to excitations of.
1 Cold molecules Mike Tarbutt. 2 Outline Lecture 1 – The electronic, vibrational and rotational structure of molecules. Lecture 2 – Transitions in molecules.
Separating Electronic and Nuclear Motions The Born-Oppenheimer Approximation All Computational Chemistry rests on a fundamental assumption called.
Laser cooling of molecules. 2 Why laser cooling (usually) fails for molecules Laser cooling relies on repeated absorption – spontaneous-emission events.
Lecture 5 The Simple Harmonic Oscillator
1 Molecular Hamiltonians and Molecular Spectroscopy.
Quantum Computing with Trapped Ion Hyperfine Qubits.
Energy Kinetic Energy: energy in the form of motion –Individual Motion (e.g., batted baseball) –Thermal Energy: energy of particles in random motion Potential.
METO 621 LESSON 7. Vibrating Rotator If there were no interaction between the rotation and vibration, then the total energy of a quantum state would be.
MOLECULAR STRUCTURE CHAPTER 14 Experiments show O 2 is paramagnetic.
1 Advanced Chemical Physics. 2 Advanced Physical Chemistry Spectroscopy –Electronic spectroscopy (basics in quantum mechanics) –Vibrational spectroscopy.
Introduction to Infrared Spectrometry Chap 16. Infrared Spectral Regions Table 16-1 Most used – 15.
Quantum Computation Using Optical Lattices Ben Zaks Victor Acosta Physics 191 Prof. Whaley UC-Berkeley.
Rotational Spectroscopy Born-Oppenheimer Approximation; Nuclei move on potential defined by solving for electron energy at each set of nuclear coordinates.
METO 637 LESSON 3. Photochemical Change A quantum of radiative energy is called a photon, and is given the symbol h Hence in a chemical equation we.
Spin-motion coupling in atoms Cooling to motional ground states and Quantum logic spectroscopy.
Basic Ideas Concerning MOs Copyright © 2011 Pearson Canada Inc. Slide 1 of 57General Chemistry: Chapter 11 1.Number of MOs = Number of AOs. 2.Bonding (lower.
DeMille Group Dave DeMille, E. Altuntas, J. Ammon, S.B. Cahn, R. Paolino* Physics Department, Yale University *Physics Department, US Coast Guard Academy.
Lecture 17 Hydrogenic atom (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been developed and made.
Lecture 34 Rotational spectroscopy: intensities. Rotational spectroscopy In the previous lecture, we have considered the rotational energy levels. In.
Determination of fundamental constants using laser cooled molecular ions.
Laser Molecular Spectroscopy CHE466 Fall 2009 David L. Cedeño, Ph.D. Illinois State University Department of Chemistry Electronic Spectroscopy.
Can we build individual molecules atom by atom? Mikkel F. Andersen Jack Dodd Centre for Quantum Technology, Department of Physics, University of Otago.
CHE Inorganic, Physical & Solid State Chemistry Advanced Quantum Chemistry: lecture 2 Rob Jackson LJ1.16,
Ch ; Lecture 26 – Quantum description of absorption.
Optical Zeeman Spectroscopy of the (0,0) bands of the B 3  -X 3  and A 3  -X 3  Transitions of Titanium Monoxide, TiO Wilton L. Virgo, Prof. Timothy.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics &
Chapter 35 Quantum Mechanics of Atoms. S-equation for H atom 2 Schrödinger equation for hydrogen atom: Separate variables:
Quantum Chemistry: Our Agenda (along with Engel)
1.5 Population inversion and laser operation
C We have to solve the time independent problem H o  o = E o  o Harry Kroto 2004.
Lecture 10. Chemical Bonding. H 2 Molecule References Engel, Ch. 12 Ratner & Schatz, Ch. 10 Molecular Quantum Mechanics, Atkins & Friedman (4th ed. 2005),
Lecture 7. Many-Electron Atoms. Pt.5. Good quantum numbers (Terms & Levels) & the Zeeman effect References Ratner Ch , , Engel Ch.11, Pilar.
Chemistry 8.1.
Lecture 11. Hydrogen Atom References Engel, Ch. 9
Lecture 8. Chemical Bonding
1 Tentative content material to be covered for Exam 2 (Wednesday, November 2, 2005) Chapter 16Quantum Mechanics and the Hydrogen Atom 16.1Waves and Light.
Last hour: Total WF: In the BOA, the electronic WF uses R only as a parameter  separation of variables, treating degrees of freedom for nuclear and electronic.
Lecture 34 Rotational spectroscopy: intensities (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been.
Physics I: Fall 2009 Room 123 Dr. Pasquini Mr. Hansen.
Algebra Review. Systems of Equations Review: Substitution Linear Combination 2 Methods to Solve:
Chapter 8. Molecular Motion and Spectroscopy
Fundamentals of Organic Chemistry Chapter 1. What is Organic Chemistry? Old Timers View: Something with vital forces! Now: Chemistry of carbon-containing.
Why do molecules form? Molecular bonds Rotations Vibrations Spectra Complex planar molecules Molecules CHAPTER 9 Molecules Johannes Diderik van der Waals.
Today in Algebra 2 Get a calculator. Go over homework Notes: –Solving Systems of Equations using Elimination Homework.
Lecture 15 Time-dependent perturbation theory
Ultraviolet–visible spectroscopy UV
The Zero Product Property
Chemistry 8.1.
Ultrafast processes in molecules
Lecture 3 Particle on a ring approximation
Rotational and Vibrational Spectra
Lesson 1 LT: I can balance and solve for unknowns in a nuclear equation.
Intermolecular Forces
I = μr2 μ = m1m2/(m1+m2) I (uÅ2) = / B(cm-1)
PHY 752 Solid State Physics
Stored energy due to position
DEPARTMENT OF CHEMISTRY
Molecular Spectra By – P.V.Koshti.
Consider the transition Ar (3p)6, 1S0 → Ar (3p)5 (4p), 1P1
Presentation transcript:

Can we build individual molecules atom by atom? Lecture 2

Yesterday we Talked about two-level atoms in light Optical trapping of atoms Laser cooling of atoms Dave explained how to cool all the way to the ground state (Same thing works for a single neutral atom in an optical micro-trap) Found that the students do not participate much in the lectures This provide the initialisation step of our atoms.

What is the difference between molecular physics and chemistry?

Basic molecular physics

The Hamiltonian

Nuclear equation

Separate S. E. Equations Nuclear motion: Electrons. For all R solve:

Basic molecular physics

We start from

A bit of algebra

We arrive at

Two conclusions Di-atomic molecules are indeed “physics” But the physics is very rich

Dipole operator for molecule

Selection rules for transitions that do not change electronic state: Hetero nuclear: Homo nuclear: No allowed transitions

Franck-Condon Principle Different electronic states