Noisy Light Spectroscopy Darin J. Ulness Department of Chemistry Concordia College, Moorhead, MN.

Slides:



Advertisements
Similar presentations
Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
Advertisements

U Toronto, February 18, 2011Darin J. Ulness, Concordia College 1 Noisy Light Spectroscopy Noisy Light Spectroscopy: Putting noise to good use Darin J.
INTERFEROMETER TO MEASURE DISPERSION Michelson Interferometer response.
Raman Spectroscopy Laser 4880 Å. Raman Spectroscopy.
Halogen Bonding Darin J. Ulness Department of Chemistry Concordia College, Moorhead, MN.
Homo-halogen Bonding in 2-iodo-perfluoroalkane Darin J. Ulness Department of Chemistry Concordia College, Moorhead, MN.
Quantum Coherent Control with Non-classical Light Department of Physics of Complex Systems The Weizmann Institute of Science Rehovot, Israel Yaron Bromberg,
Broadband Cavity Enhanced Absorption Spectroscopy With a Supercontinuum Source Paul S. Johnston Kevin K. Lehmann Departments of Chemistry & Physics University.
Yoan Léger Laboratory of Quantum Opto-electronics Ecole Polytechnique Fédérale de Lausanne Switzerland.
Nonlinear Spectroscopy: Diagrammatic Perturbation Theory Andrei Tokmakoff MIT Department of Chemistry 2009.
Transient Four-Wave Mixing Spectroscopy on PbS Quantum Dots Kevin Blondino (Florida State University) Advisors: Dr. Denis Karaiskaj, USF (faculty) Jason.
Scott Flancher.  Review of halogen bonding  σ -hole  Applications  Homo-halogen bonding hypothesis  Experiments / Data  Kinetics  19 F-NMR  IR.
NMR Nuclear Magnetic Resonance. 1 H, 13 C, 15 N, 19 F, 31 P.
Single Shot Combined Time Frequency Four Wave Mixing Andrey Shalit, Yuri Paskover and Yehiam Prior Department of Chemical Physics Weizmann Institute of.
TWO-PHOTON ABSORPTION IN SEMICONDUCTORS Fabien BOITIER, Antoine GODARD, Emmanuel ROSENCHER Claude FABRE ONERA Palaiseau Laboratoire Kastler Brossel Paris.
Raman Spectroscopy Laser 4880 Å. Raman Spectroscopy.
Narrow transitions induced by broad band pulses  |g> |f> Loss of spectral resolution.
Ultrafast Spectroscopy
X-ray Free-Electron Lasers: Challenges for Theory, Cambridge, Massachusetts, USA, June 19, 2006 Infrared X-ray pump-probe spectroscopy Hans Ågren Department.
References Acknowledgements This work is funded by EPSRC 1.Paul Siddons, Charles S. Adams, Chang Ge & Ifan G. Hughes, “Absolute absorption on rubidium.
References Acknowledgements This work is funded by EPSRC 1.R. P. Abel, U. Krohn, P. Siddons, I. G. Hughes & C. S. Adams, Opt Lett (2009). 2.A.
Those Interfering Signals Modes and Dispersion in Fibers.
First year talk Mark Zentile
Pump-Probe Spectroscopy Chelsey Dorow Physics 211a.
Introduction to Infrared Spectrometry Chap 16. Quantum Mechanical Treatment of Vibrations Required to include quantized nature of E From solving the wave.
Lecture 3 INFRARED SPECTROMETRY
Nonlinear Spectroscopy: Characterizing Fluctuations Andrei Tokmakoff MIT Department of Chemistry 2009.
HIGH-RESOLUTION COHERENT THREE-DIMENSIONAL SPECTROSCOPY OF IODINE
Quantum Beating In Photosynthetic Systems using Noisy Light Darin Ulness Department of Chemistry Concordia College, Moorhead, MN.
David Wilcox Purdue University Department of Chemistry 560 Oval Dr. West Lafayette, IN
Spectroscopic Line Shapes Of Broad Band Sum Frequency Generation Himali Jayathilake Igor Stiopkin, Champika Weeraman, Achani Yatawara and Alexander Benderskii.
RamanRaman. Scattering Tyndall scattering – if small particles are present During Rayleigh scattering (interaction of light with relatively small molecules)
OSU 06/19/08 Ultrabroadband Rotational Spectroscopy: Novel Applications of a Shape Sensitive Detector BRIAN C. DIAN Purdue University Department of Chemistry.
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
Fourier theory We know a lot about waves at a single  : n( , v p ( , R(  absorption(  … Analyze arbitrary in terms of these, because Fourier.
Che 440/540 2D-NMR
Lecture 33 Rotational spectroscopy: energies (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been.
The Nobel Prize in Physics 1930 "for his work on the scattering of light and for the discovery of the effect named after him" Sir Chandrasekhara Venkata.
Shaping Pulses Before They are Born Avi Pe’er Physics Department and BINA center for nano-technology, Bar Ilan University FRISNO 11 Shai Yefet, Naaman.
Systems (filters) Non-periodic signal has continuous spectrum Sampling in one domain implies periodicity in another domain time frequency Periodic sampled.
INTERFERENCE AND QUANTIZATION IN SEMICLASSICAL VIBRATIONAL RESPONSE FUNCTIONS Scott Gruenbaum Department of Chemistry and Chemical Biology Cornell University.
Interaction of laser pulses with atoms and molecules and spectroscopic applications.
Raman Effect The Raman Effect is the phnomenon of scattering of light, one of the most convincing proofs of the quantum theory Was discovered in 1928 Raman.
Terahertz Applications by THz Time Domain Spectroscopy
Augustana, March 2, 2007Darin J. Ulness, Concordia College 1 Noisy Light Spectroscopy Noisy Light Spectroscopy: Putting noise to good use Darin J. Ulness.
Lecture 11 (end of) Fourier Transforms Remember Phils Problems and your notes = everything Today Finish Fourier.
Two Dimensional Coherent Double Resonance Electronic Spectroscopy Ohio State University Molecular Spectroscopy Conference June 20, 2008 Peter C. Chen Department.
Noisy Light Spectroscopy A science story Darin J. Ulness Department of Chemistry Concordia College, Moorhead, MN.
Lecture 31 General issues of spectroscopies. I. General issues of spectroscopies In this lecture, we have an overview of spectroscopies: Photon energies.
NDSU, October 4, 2007Hydrogen Bonding and PyridineDarin J. Ulness, Concordia College 1 Effects of Hydrogen Bonding on the Ring Stretching Modes of Pyridine.
The Academic Experience At Concordia. Influencing the world by becoming responsibly engaged in it The Big Picture.
Broadband High-resolution Spectroscopy with Fabry-Perot Quantum Cascade Lasers Yin Wang and Gerard Wysocki Department of Electrical Engineering Princeton.
Lecture 34 Rotational spectroscopy: intensities (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been.
Complex nanostructures promise to provide a platform for dramatically increasing the efficiency of solar energy conversion into the power and fuels needed.
Introduction to Laser Spectroscopic Techniques for Condensed Matter.
1 Scattering of Light: Raman Spectroscopy Deanna O’Donnell Informal P-Chem Review June 4 th, 2009.
Combined Time Frequency Detection (TFD) by Single Shot Four Wave Mixing Yehiam Prior and Andrey Shalit Department of Chemical Physics Weizmann Institute.
Generation of intense few-cycle pulses from the visible to the mid-IR Josh Nelson 1 Danny Todd 2 Adam Summers 3 Derrek Wilson 3 Dr. Carlos Trallero 3 1.
Optical Characterization Techniques
Optical Coherence Tomography
Water Structure around Hydrophobic Solutes
Water Structure around Hydrophobic Solutes
Noisy Light Spectroscopy
Homo-halogen Bonding in 2-iodo-perfluoroalkane
MICHELSON AND WHITE LIGHT INTERFEROMETRY
Spectroscopy of ultracold bosons by periodic lattice modulations
Ultrafast Proton Dynamics During Proton-Coupled-Electron-Transfer and Excited-State-Proton-Transfer Andrei Tokmakoff, Department of Chemistry, Massachusetts.
And their applications
Sapun H. Parekh, Young Jong Lee, Khaled A. Aamer, Marcus T. Cicerone 
NMR Nuclear Magnetic Resonance Dr. A.G. Nikalje
Presentation transcript:

Noisy Light Spectroscopy Darin J. Ulness Department of Chemistry Concordia College, Moorhead, MN

Noisy Light Spectroscopy What is noisy light? History Theory Experiment Applications and results Context The future of noisy light spectroscopy

What is Noisy Light? Broadband Phase incoherent Quasi continuous wave Noisy Light Spectrum Frequency Time resolution on the order of the correlation time,  c

What is Noisy Light? Ultrashort pulse Short Pulse Spectrum Frequency Time resolution on the order of the pulse width Coherent Phase locked Time Broadband Phase incoherent Quasi continuous wave

What is Noisy Light? Noisy Light Spectrum Frequency Incoherent Phase unlocked Time

What is Noisy Light? Noisy Light Spectrum Frequency Incoherent Phase unlocked Time Color locked!

What is Noisy Light? Time Beam B

What is Noisy Light? Time Beam B Beam B’

What is Noisy Light? Time  Beam B Beam B’

What is Noisy Light? Time  Beam B Beam B’ Compare  with  c

History Morita, Asaka, Hartmann develop the photon echo Dugan develops Spectrally resolved CARS Most noisy light papers published between 1986 and Many counter parts to short pulse methods. FTC diagrams invented Higher dimensional spectroscopy Noisy light focused on application of CARS. Very few groups working with noisy light from 1996 on. Exciton quantum beats

Foundations of Noisy Light Optical coherence theory Perturbation theory: Density operator Noisy Light Spectroscopy

Nonlinear Spectroscopy P=  E Signal Material Light field Perturbation series approximation P(t) = P (1) + P (2) + P (3) … P (1) =  (1) E, P (2) =  (2) EE, P (3) =  (3) EEE

CARS Coherent Anti-Stokes Raman Scattering  1 -  2 =  R  CARS =  1 +  R RR 11 11  2  CARS

Bichromophoric Model   Noisy light P(t)P(t) (3) P(s)P(s) (3) *

Theoretical Challenges Complicated Mathematics Complicated Physical Interpretation Difficulty The cw nature requires all field action permutations. The light is always on. The proper treatment of the noise cross-correlates chromophores.

FTC Diagram Analysis Set of intensity level terms (pre-evaluated) Set of evaluated intensity level terms Messy integration and algebra Set of FTC diagrams Construction Rules Evaluation Rules Physics hard easy

FTC Diagram Analysis   P(t,{t i }) P(s,{s i }) B B’ B’* B*     P(t,{t i }) P(s,{s i }) = +

FTC Diagram Analysis   P(t,{t i }) P(s,{s i }) arrow segments:  -dependent correlation line segments:  -independent correlation

Indirect Correlation   

   Dynamics on  are probed!

I (2) CARS: Experiment Monochromator Narrowband Source Broadband Source Lens Sample Interferometer t B B’ M I (2) CARS Computer CCD Signal is dispersed onto the CCD Entire Spectrum is taken at each delay 2D data set: the Spectrogram

I (2) CARS: Experiment Great sensitivity to vibrational shifts and dephasing changes Ring breathing mode of benzene in hexane

I (2) CARS: Data Processing Fourier Transformation X-Marginal

I (2) CARS: Hydrogen Bonding FT Neat Pyridine Pyridine/ Water X w = 0.55

I (2) CARS: Hydrogen Bonding

Network model Thermalized distribution model Etc. Fileti, E.E.; Countinho, K.; Malaspina, T.; Canuto, S. Phys. Rev. E. 2003, 67,

Halogen Bonding Electropositve  -hole Test Charge Electroneutral “ring” Electronegative “belt”

I (2) CARS: Halogen Bonding

Exciton Quantum Beats

Future of Noisy Light Spectroscopy I (4) 2DES Theory I (4) 2DES Experiment I (2) CARS Experiment Information Processing Dendritic Integration Indirect correlation in systems Applied Mathematics Group Theory Graph Theory Braid Theory

Acknowledgements Students Theory Jahan Dawlaty Dan Biebighauser John Gregiore Duffy Turner (M) Kurt Haag Issac Heath Carena Daniels Other Group Members Dr. Mark Gealy, Department of Physics Dr. Eric Booth, Post-doctoral researcher Dr. Haiyan Fan, Post-doctoral researcher Funding NSF CAREER Grant CHE Henry Dreyfus Teacher/Scholar program Concordia Chemistry Research Fund Method Development Pye Phyo Aung Tanner Schulz (M) Lindsay Weisel Krista Cosert Perrie Cole (M) Alex Harsh Britt Berger Zach Johnson Thao Ta Hydrogen/Halogen bonding Eric Berg Jeff Eliason (M) Diane Moliva Jason Olson Scott Flancher Danny Green Exciton Beats Erika Sutor Becca Hendrickson (M) Meghan Knudtzon (M) Dylan Howie (M) Bobby Spoja