Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics &

Slides:



Advertisements
Similar presentations
Chapter 30 Light Emission
Advertisements

Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
Development and brief application of Raman selection rules Alex Kitt.
Journal Club: Introduction to Fluorescence Spectroscopy and Microscopy Avtar Singh 4/5/11.
© 2010 Pearson Education, Inc. PowerPoint ® Lectures for College Physics: A Strategic Approach, Second Edition Chapter 29 Atoms and Molecules.
Lecture 36 Electronic spectroscopy (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been developed.
Optical Engineering for the 21st Century: Microscopic Simulation of Quantum Cascade Lasers M.F. Pereira Theory of Semiconductor Materials and Optics Materials.
An STM Measures I(r) Tunneling is one of the simplest quantum mechanical process A Laser STM for Molecules Tunneling has transformed surface science. Scanning.
Generation of short pulses
Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators
Femtochemistry: A theoretical overview Mario Barbatti VI – Transition probabilities This lecture can be downloaded at
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.
PG lectures Spontaneous emission. Outline Lectures 1-2 Introduction What is it? Why does it happen? Deriving the A coefficient. Full quantum description.
CHEM 515 Spectroscopy Lecture # 1.
Chem 122 Molecular Spectroscopy Spring 2008 Professor Ronald Cohen GSI Drew Rollins.
Simulation of X-ray Absorption Near Edge Spectroscopy (XANES) of Molecules Luke Campbell Shaul Mukamel Daniel Healion Rajan Pandey.
PG lectures Spontaneous emission. Outline Lectures 1-2 Introduction What is it? Why does it happen? Deriving the A coefficient. Full quantum description.
Laser Induced Fluorescence Structural information about the ground and excited states of molecules. Excitation experiments  Excited state information.
Photochemistry Lecture 1 Electronic excitation of atoms and molecules.
Can we build individual molecules atom by atom? Lecture 2.
Lecture 4 Intramolecular energy transfer
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 1 (1/13/2014) Slide Introduction to Quantum Optics.
1 Part III Physical Chemistry III Points and credit: Approximately 20% for quiz & homework 80% final examination Note*Extra.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
Precise Measurement of Vibrational Transition Frequency of Optically Trapped molecules NICT Masatoshi Kajita TMU G. Gopakumar, M. Abe, M. Hada We propose.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 5 (2/3/2014) Slide Introduction to Quantum Optics &
SPECTROSCOPY COURSE In spectroscopy, interaction of electromagnetic radiations and matter is involved.
Electronic Spectroscopy
Photoassociation Spectroscopy of Ultracold Molecules Liantuan XIAO State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser.
Experiments with ultracold RbCs molecules Peter Molony Cs Rb.
Ch ; Lecture 26 – Quantum description of absorption.
How Do Materials Emit Light? Incandescence Atomic Emission Molecular Fluorescence Phosphorescence Photoluminescence.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
1 Controlling spontaneous emission J-J Greffet Laboratoire Charles Fabry Institut d’Optique, CNRS, Université Paris Sud Palaiseau (France)
Electronic Transition of Ruthenium Monoxide Na Wang, Y. W. Ng and A. S.-C. Cheung Department of Chemistry The University of Hong Kong.
Electronic Spectroscopy of Palladium Dimer (Pd 2 ) 68th OSU International Symposium on Molecular Spectroscopy Yue Qian, Y. W. Ng and A. S-C. Cheung Department.
Fang Wang & Timothy C. Steimle Dept. Chem. & BioChem., Arizona State University, Tempe, AZ,USA The 65 th International Symposium on Molecular Spectroscopy,
Fluorescence Spectroscopy
Trap loss of spin-polarized 4 He* & He* Feshbach resonances Joe Borbely ( ) Rob van Rooij, Steven Knoop, Wim Vassen.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 3 (1/27/2014) Slide Introduction to Quantum Optics.
Max-Planck-Institut für Plasmaphysik CRP on ‘Atomic and Molecular Data for Plasma Modelling’, IAEA, Vienna26-28 September 2005 Compilation and Extension.
Of all the transitions that are allowed, how do I figure out intensities?
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
Jablonski Diagram electronic ground state A F P energy IC ISC IC S0S0 S1S1 S2S2 SnSn (ro)-vibrational states of el. excited states T1T1 T2T2 A = photon.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 10 (2/16/2014) Slide Introduction to Quantum Optics.
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
An analytical potential for the for the a 3  + state of KLi, (derived from observations of the upper vibrational levels only) Houssam Salami, Amanda Ross,
Purdue University Spring 2014 Prof. Yong P. Chen Lecture 16 (3/31/2014) Slide Introduction to Quantum Optics.
Spectroscopy 2: Electronic Transitions CHAPTER 14.
Lecture 36 Electronic spectroscopy. Electronic spectroscopy Transition energies between electronic states fall in the range of UV/vis photons. UV/vis.
Ionization in atomic and solid state physics. Paul Corkum Joint Attosecond Science Lab University of Ottawa and National Research Council of Canada Tunneling.
Purdue University Spring 2016 Prof. Yong P. Chen Lecture 18 (3/24/2016) Slide Introduction to Quantum Photonics.
Solid state physics is the study of how atoms arrange themselves into solids and what properties these solids have. Calculate the macroscopic properties.
PHYS 172: Modern Mechanics Lecture 14 – Energy Quantization Read Summer 2012.
Lecture 6 Radiative Transition in Atoms, Molecules & Insulators/Semiconductors Read: FQ 4, FS 3.
Ultrafast Spectroscopy
Ultrafast processes in molecules
Lecture 19 Inelastic Light Scattering (Raman) cont. Photon Statistics
Lecture 4 Intramolecular energy transfer
Today’s Plan Review 2-level system (Schordinger eq, Rabi, Bloch)
PHY 752 Solid State Physics
Perturbation Theory Lecture 5.
Illustration of Jablonski Diagram
Quantum Mechanical Treatment of The Optical Properties
Overview of spectroscopy transitions
Recall that the vibrational eigenfunctions of a harmonic oscillator are orthogonal: If yj and yk belong to different electronic states as shown here, is.
Perturbation Theory Lecture 5.
Consider the experimental evidence you just saw,
PHY Statistical Mechanics 12:00* -1:45 PM TR Olin 107
Presentation transcript:

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Lecture 7 Light-Matter Interaction 1: Radiative Transitions (Atoms & Molecules) Reminder: HWK2 due Lecture notes taker

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Course Outline Part 1: basic review: Optics+Quantum; Part 2: Basic Light- matter interaction; laser; Part 3: Quantum Optics of photons Part 4: More advanced light-matter interaction Part 5: Quantum information/photonics/ applications Subject to change; Check updates on course web/wiki

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) This Lecture Radiative transition in atom (2-level) (FQ Chap ; also helpful: FS Appendix B) Transitions on Molecules (FS Chap 8.2)

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Classical & Semiclassical L-M interaction 00 Classical Semi-Classical (Lorentz)dipole oscillator model

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) “Driven damped Harmonic Oscillator” Powerful mechanical analogue of L-M interaction γ

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) γ “Driven damped Harmonic Oscillator”

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) (FS Chap 1)

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) +

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”)

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Now move on to quantum (semiclassical) Last quiz: average 30% molecule

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Semiclassical Light-Matter interaction: Einstein Coefficients (Planck blackbody) (FQ Ch4/FS App-B)

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Radiative Transition Rates Fermi Golden Rule (DOS of final state: light (photon) +matter [neglect if discrete]) X-polarized:

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Selection Rules (even/odd)(orbital)

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) “forbidden” transition Metastable state Fluorescence phosphorescence Transition matrix element

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Also can engineer DOS g to control transition rates! cavityPhotonic crystal (bandgap)/ Metamaterials …

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Molecules & molecular solids

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Jablonski Diagram Singlet Triplet SO coupling

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) (X) 1 Σ (2) 1 Σ (2) 3 Σ (1) 3 Σ (3) 1 Σ LIF excitation

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Heaters Li 550 ̊ C Rb 300 ̊ C Rb 300 ̊ C Cooling water PMT Monochromator λ -meter Molecular Spectroscopy in a heat-pipe ( 7 Li 85 Rb) (A) Laser Induced Fluorescence (LIF) (B) Excitation Spectroscopy Laser LIF Laser

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Korek et al., Chem Phys Laser Induced Fluorescence (LIF) Dutta et al., Chem Phys Lett (2011), doi: /j.cplett From low v’ levels of B 1 Π state

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Fluorescence from successively higher vib. (1) 1 П states PR v PR

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Franck-Condon Overlap of Vibronic state

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Photo-association laser

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) PA rate of 7 Li near FR a > 0a < 0 I = 1.65 W/cm 2 v’’ = 83 T ~ 10  K v’’ = 84 v’’ = 83 v’’ = 82 ~10 4 M.Junker et al., PRL 2008

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) v’’ r r E RcRc 2S 1/2 + 2S 1/2 2S 1/2 + 2P 1/2 Why the zero? f(R c )R~ 2 big small Rate depends on ground state wavefunction (Franck- Condon) Bohn and Julienne PRA 60, 414 (1999).

Purdue University Spring 2014 Prof. Yong P. Chen Lecture 6 (2/5/2014) Slide Introduction to Quantum Optics & Quantum Photonics PHYS522 ECE695 (“Coherent Optics & Quantum Electronics”) Next Lecture (8): Light Matter Interaction --- Solids (interband transition) FS Chap 3.