Optical Spectroscopy. Steady State and Time Dependent Fluorescence Measurements. Kai Wen Teng. October 8 th PHYS 403 Fall 2013
|
|
- Horace Collins
- 5 years ago
- Views:
Transcription
1 Optical Spectroscopy Steady State and Time Dependent Fluorescence Measurements Kai Wen Teng October 8 th 2013 PHYS 403 Fall 2013
2 EM Spectrum of molecules Rotational Energy Infrared Vibrational Energy Near Infrared Electronic Energy Visible and Ultra-Violet r v Diagram from Diagram by Robert Clegg in Photosynth Res Aug- Sep;101(2-3):
3 Types of Fluorescent Molecules Synthetic Organic: Fluorescein Semiconductor Nanocrystal: Crystals: Naturally Occuring: Ruby and assorted mineral From mineralman.net Fluorescent Nanodiamonds Fluorescent Proteins: Green Fluorescent Protein Image from Zrazhevskiy et al Nano Lett., 2010, 10 (9), pp DOI: /nl
4 Perrin-Jablonski energy diagram (S0, S1 and S2 transitions) Alexander Jablonski Diagram by Ulai Noomnarm in Photosynth Res Aug-Sep;101(2-3):
5 Absorption (S 0 -S 1 ) l? Beer-Lambert s Law log(i 0 ) log(i) cl Extinction coefficient: Concentration
6 Steady State Measurements: Absorbance One of the very first commercially available instrument that measures absorbance was the Beckman DU Machine nowadays that utilizes diffraction grating and diode array detector can acquire an absorbance spectra in less than 10 seconds.
7 Organic dye: Fluorescence (S 1 -S 0 ) Solvent Effect: Ruby:
8 Time-Dependent Fluorescence: Fluorescence Lifetime Fluorescence Lifetime: The average amount of time a molecule stays in excited state Probability of being in the excited state kf = rate constant for leaving excited state while emitting a photon ki = rate constant for leaving excited state through other means (ie. Dynamic quenching, Energy Transfer, etc) Excited State kf ki ki Diagram by Robert Clegg in Photosynth Res Aug-Sep;101(2-3): Fluorescence Lifetime: i 1 ki Lifetime is sensitive to other decaying pathway present!
9 Measuring the Depletion of the excited state * * kf kt t # x # xo e # F * x k Intensity that you = measure [x] * KF is rate constant of fluorescence Intensity measured is proportional to the # of molecules in the excited state!
10 Measuring Lifetime: Time Domain nsec What do you need? -Collect signal fast enough -Fitting
11 Measuring Lifetime: Frequency Domain E(t) = E o + Eωcos ωet + φe F(t) = F + F cos ω t + φ - φ o ω E E tan ω E F F 1 ω o M = = Eω Eo 1+ ωτ Mod 2 What do you need? -Intensity modulators -Synchronization
12 Samples Described by Multiple Lifetimes I(t) = i a e i -t τ i Some Examples: -ECFP (Enhanced Cyan Fluorescent Protein (FP)) -mcherry -Teal FP a τ F(t) = E a τ + E cos(ω t - (φ - φ )) i i o i i ω 2 E i E i i 1+ (ωeτ i ) You still can only measure M,φ E α F(t) = 1+ ω i cos(ω 2 E t - (φ i - φ E )) Fo Eo i 1+ (ωeτ i ) F(t) = 1+ F o E E ω o Mcos(ω t - (φ - φ)) E i
13 Mixing is used in commercial instruments [G(t)*F(t)]= DC+ Terms with frequencies GE 2 ω ω + M (ω E,ω G,ω E +ω G cos((ωg - ω E )t + φg - φ E + φ) ) Images from Molecular Fluorescence by Bernard Valeur
14 AOMs Intensity Modulator Annals of the New York Academy of Sciences Vol. 158 pp , modulation frequency limited by resonance frequency of the acoustooptic cell -variations in the intensity modulation caused by temperature
15 Pockels Cell Biophysical Journal Vol. 44 (1983) pp Hecht Optics
16 Directly Modulated Diode System in ESB Laser Diodes -> (405nm,436nm,473nm,635nm,690nm,780nm,830nm) LEDs -> (280nm,300nm,335nm,345nm,460nm,500nm,520nm)
17 ISS SLM Phoenix Upgrade Original System New Upgrades PMT Housing New Acquisition Box Stepper Motor Controller -photon counting -Measures nanosecond lifetime
18 Champaign, Illinois Domain of FD FLIM Robert Clegg UIUC Full-Field FLIM Enrico Gratton UIUC Scanning Confocal FLIM (FLIMBox) Beniamino Barbieri ISS Inc. Commercialization of FD FLIM
19 Msin(φ) The Polar Plot Msin(φ) φ Mcos(φ) Mcos(φ) Vectors on the Polar Plot R = Mcos(φ)x ˆ+ Msin(φ)y ˆ R=αiR i + α jrj R= α M cos(φ )+ α M cos(φ ) xˆ i i i j j j + α M sin(φ )+ α M sin(φ ) yˆ i i i j j j -movement of the vector depends on the emitted intensity of each species (i)
20 Msin(Ф) Emission Spectral Analysis on the SLM Msin(Ф) Fluorescein 4.3ns Measured Data (60MHz) RhodB 1.7ns Simulated Data (60MHz) Fluorescein 4.3ns RhodB 1.7ns Mcos(Ф) Mcos(Ф) Measured Spectrum Wavelength (nm)
21 Intensity Intensity Intensity Quantum Yield/FRET D FRET R A D A Wavelength Donor Exc. Donor Em. Acceptor Exc. Acceptor Em. D A Wavelength Wavelength Quantum Yield of Energy Transfer = Rate of Energy Transfer Total deexcitation rate 1 1 DA D = 1 = 1 D DA D
22 Top of cell: Intensity Msinφ Top of cell: Lifetimes Msinφ Optical Sections Rendered by Lifetime 0µm 0.5µm 1.0µm 1.5µm 2.0µm 2.5µm 3.0µm 3.5µm 4.0µm 4.5µm 5.0µm 5.5µm 6.0µm 6.5µm 7.0µm 7.5µm 8.0µm 8.5µm 9.0µm 9.5µm 10.0µm 10.5µm 4.5µm ns ns 1 4 ns 3 ns 4 ns 3 ns 2 #1 #2 0 Mcosφ Images courtesy of John Eichorst Mcosφ 1.0
Fluorescence Spectroscopy
Fluorescence Spectroscopy Steady State and Time Dependent Fluorescence Measurements Kai Wen Teng PHYS 403 Fall 15 EM Spectrum of molecules Rotational Energy Infrared Vibrational Energy Near Infrared Electronic
More informationFluorescence Spectroscopy
Fluorescence Spectroscopy Steady State and Time Dependent Fluorescence Measurements Kai Wen Teng PHYS 403 Summer 2014 EM Spectrum of molecules Rotational Energy Infrared Vibrational Energy Near Infrared
More informationLABORATORY OF ELEMENTARY BIOPHYSICS
LABORATORY OF ELEMENTARY BIOPHYSICS Experimental exercises for III year of the First cycle studies Field: Applications of physics in biology and medicine Specialization: Molecular Biophysics Fluorescence
More information1. Transition dipole moment
1. Transition dipole moment You have measured absorption spectra of aqueous (n=1.33) solutions of two different chromophores (A and B). The concentrations of the solutions were the same. The absorption
More informationWhat the Einstein Relations Tell Us
What the Einstein Relations Tell Us 1. The rate of spontaneous emission A21 is proportional to υ 3. At higher frequencies A21 >> B(υ) and all emission is spontaneous. A 21 = 8π hν3 c 3 B(ν) 2. Although
More informationSupplementary Materials
Supplementary Materials Sample characterization The presence of Si-QDs is established by Transmission Electron Microscopy (TEM), by which the average QD diameter of d QD 2.2 ± 0.5 nm has been determined
More informationsingle-molecule fluorescence resonance energy transfer
single-molecule fluorescence resonance energy transfer (2) determing the Förster radius: quantum yield, donor lifetime, spectral overlap, anisotropy michael börsch 26/05/2004 1 fluorescence (1) absorbance
More informationFluorescence Resonance Energy Transfer (FRET) Microscopy
Fluorescence Resonance Energy Transfer () Microscopy Mike Lorenz Optical Technology Development mlorenz@mpi-cbg.de -FLM course, May 2009 What is fluorescence? Stoke s shift Fluorescence light is always
More informationAbsorption spectrometry summary
Absorption spectrometry summary Rehearsal: Properties of light (electromagnetic radiation), dual nature light matter interactions (reflection, transmission, absorption, scattering) Absorption phenomena,
More informationLecture 5. Anisotropy decay/data analysis. Enrico Gratton
Lecture 5. Anisotropy decay/data analysis Enrico Gratton Anisotropy decay Energy-transfer distance distributions Time resolved spectra Excited-state reactions Basic physics concept in polarization The
More informationTime resolved optical spectroscopy methods for organic photovoltaics. Enrico Da Como. Department of Physics, University of Bath
Time resolved optical spectroscopy methods for organic photovoltaics Enrico Da Como Department of Physics, University of Bath Outline Introduction Why do we need time resolved spectroscopy in OPV? Short
More information10. 6 Photochemistry. Out-class reading: Levine, pp photochemistry
Out-class reading: Levine, pp. 800-804 photochemistry 6.1 Brief introduction of light 1) Photochemistry The branch of chemistry which deals with the study of chemical reaction initiated by light. 2) Energy
More informationMeasurement Examples. Excitation and Emission Scans. Steady State Fluorescence Anisotropy. Kinetic Measurements
Measurement Examples A division of Edinburgh Instruments Ltd. Excitation and Emission Scans Excitation and emission spectra are standard measurements in fluorescence spectroscopy. The figure demonstrates
More informationn ( λ ) is observed. Further, the bandgap of the ZnTe semiconductor is
Optical Spectroscopy Lennon O Naraigh, 0000 Date of Submission: 0 th May 004 Abstract: This experiment is an exercise in the principles and practice of optical spectroscopy. The continuous emission spectrum
More informationOptics and Spectroscopy
Introduction to Optics and Spectroscopy beyond the diffraction limit Chi Chen 陳祺 Research Center for Applied Science, Academia Sinica 2015Apr09 1 Light and Optics 2 Light as Wave Application 3 Electromagnetic
More informationFluorescence Spectroscopy
Fluorescence Spectroscopy Frequency and time dependent emission Emission and Excitation fluorescence spectra Stokes Shift: influence of molecular vibrations and solvent Time resolved fluorescence measurements
More informationLecture 3: Light absorbance
Lecture 3: Light absorbance Perturbation Response 1 Light in Chemistry Light Response 0-3 Absorbance spectrum of benzene 2 Absorption Visible Light in Chemistry S 2 S 1 Fluorescence http://www.microscopyu.com
More informationUsing Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging
TECHNICAL NOTE Using Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging Shih-Chu Liao, Yuansheng Sun, Ulas Coskun ISS, Inc. Introduction The advantages of multiphoton excitation
More informationChapter 6 Photoluminescence Spectroscopy
Chapter 6 Photoluminescence Spectroscopy Course Code: SSCP 4473 Course Name: Spectroscopy & Materials Analysis Sib Krishna Ghoshal (PhD) Advanced Optical Materials Research Group Physics Department, Faculty
More informationConfocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup
1 Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup Abstract Jacob Begis The purpose of this lab was to prove that a source of light can be
More informationBecause light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.
Light We can use different terms to describe light: Color Wavelength Frequency Light is composed of electromagnetic waves that travel through some medium. The properties of the medium determine how light
More informationReference literature. (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters )
September 17, 2018 Reference literature (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters 13-14 ) Reference.: https://slideplayer.com/slide/8354408/ Spectroscopy Usual Wavelength Type of Quantum
More informationChemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES
Chemistry 524--Final Exam--Keiderling May 4, 2011 3:30 -?? pm -- 4286 SES Please answer all questions in the answer book provided. Calculators, rulers, pens and pencils are permitted. No open books or
More informationModel Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy
Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Section I Q1. Answer (i) (b) (ii) (d) (iii) (c) (iv) (c) (v) (a) (vi) (b) (vii) (b) (viii) (a) (ix)
More informationSolution set for EXAM IN TFY4265/FY8906 Biophysical microtechniques
ENGLISH NORWEGIAN UNIVERSITY OF SCIENCE AND TECHNOLOGY DEPARTMENT OF PHYSICS Contact during exam: Magnus Borstad Lilledahl Telefon: 73591873 (office) 92851014 (mobile) Solution set for EXAM IN TFY4265/FY8906
More informationPhys 2310 Fri. Dec. 12, 2014 Today s Topics. Begin Chapter 13: Lasers Reading for Next Time
Phys 2310 Fri. Dec. 12, 2014 Today s Topics Begin Chapter 13: Lasers Reading for Next Time 1 Reading this Week By Fri.: Ch. 13 (13.1, 13.3) Lasers, Holography 2 Homework this Week No Homework this chapter.
More informationBMB Class 17, November 30, Single Molecule Biophysics (II)
BMB 178 2018 Class 17, November 30, 2018 15. Single Molecule Biophysics (II) New Advances in Single Molecule Techniques Atomic Force Microscopy Single Molecule Manipulation - optical traps and tweezers
More informationSpectral Resolution. Spectral resolution is a measure of the ability to separate nearby features in wavelength space.
Spectral Resolution Spectral resolution is a measure of the ability to separate nearby features in wavelength space. R, minimum wavelength separation of two resolved features. Delta lambda often set to
More informationAbsorption photometry
The light Absorption photometry Szilvia Barkó University of Pécs, Faculty of Medicines, Dept. Biophysics February 2011 Transversal wave E Electromagnetic wave electric gradient vector wavelength The dual
More informationLecture 0. NC State University
Chemistry 736 Lecture 0 Overview NC State University Overview of Spectroscopy Electronic states and energies Transitions between states Absorption and emission Electronic spectroscopy Instrumentation Concepts
More informationCHEM Outline (Part 15) - Luminescence 2013
CHEM 524 -- Outline (Part 15) - Luminescence 2013 XI. Molecular Luminescence Spectra (Chapter 15) Kinetic process, competing pathways fluorescence, phosphorescence, non-radiative decay Jablonski diagram
More informationSupporting Information
Supporting Information Study of Diffusion Assisted Bimolecular Electron Transfer Reactions: CdSe/ZnS Core Shell Quantum Dot acts as an Efficient Electron Donor as well as Acceptor. Somnath Koley, Manas
More informationtwo slits and 5 slits
Electronic Spectroscopy 2015January19 1 1. UV-vis spectrometer 1.1. Grating spectrometer 1.2. Single slit: 1.2.1. I diffracted intensity at relative to un-diffracted beam 1.2.2. I - intensity of light
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 informationSupporting Information
Supporting Information Cyclodextrin Supramolecular Complex as Water Soluble Ratiometric Sensor for ferric Ion Sensing Meiyun Xu, Shuizhu Wu,* Fang Zeng, Changmin Yu College of Materials Science & Engineering,
More informationEnergy transfer and optical gain studies of FDS: Rh B dye mixture investigated under CW laser excitation
Energy transfer and optical gain studies of FDS: Rh B dye mixture investigated under CW laser excitation M. Kailasnath *a, G. Ajith Kumar, V.P.N Nampoori b International School of Photonics, Cochin University
More informationChapter 17: Fundamentals of Spectrophotometry
Chapter 17: Fundamentals of Spectrophotometry Spectroscopy: the science that deals with interactions of matter with electromagnetic radiation or other forms energy acoustic waves, beams of particles such
More informationLaboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching
Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching Jonathan Papa 1, * 1 Institute of Optics University of Rochester, Rochester,
More informationElectronic Supplementary Information
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2017 Electronic Supplementary Information Polymorphism and microcrystal shape
More informationSinglet. Fluorescence Spectroscopy * LUMO
Fluorescence Spectroscopy Light can be absorbed and re-emitted by matter luminescence (photo-luminescence). There are two types of luminescence, in this discussion: fluorescence and phosphorescence. A
More informationFluorescence Workshop UMN Physics June 8-10, 2006 Quantum Yield and Polarization (1) Joachim Mueller
Fluorescence Workshop UMN Physics June 8-10, 2006 Quantum Yield and Polarization (1) Joachim Mueller Quantum yield, polarized light, dipole moment, photoselection, dipole radiation, polarization and anisotropy
More informationSurvey on Laser Spectroscopic Techniques for Condensed Matter
Survey on Laser Spectroscopic Techniques for Condensed Matter Coherent Radiation Sources for Small Laboratories CW: Tunability: IR Visible Linewidth: 1 Hz Power: μw 10W Pulsed: Tunabality: THz Soft X-ray
More informationWhat is spectroscopy?
Absorption Spectrum What is spectroscopy? Studying the properties of matter through its interaction with different frequency components of the electromagnetic spectrum. With light, you aren t looking directly
More informationChem Homework Set Answers
Chem 310 th 4 Homework Set Answers 1. Cyclohexanone has a strong infrared absorption peak at a wavelength of 5.86 µm. (a) Convert the wavelength to wavenumber.!6!1 8* = 1/8 = (1/5.86 µm)(1 µm/10 m)(1 m/100
More informationR O Y G B V. Spin States. Outer Shell Electrons. Molecular Rotations. Inner Shell Electrons. Molecular Vibrations. Nuclear Transitions
Spin States Molecular Rotations Molecular Vibrations Outer Shell Electrons Inner Shell Electrons Nuclear Transitions NMR EPR Microwave Absorption Spectroscopy Infrared Absorption Spectroscopy UV-vis Absorption,
More informationWavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p
Introduction to Spectroscopy (Chapter 6) Electromagnetic radiation (wave) description: Wavelength λ Velocity v Electric Field Strength 0 Amplitude A Time t or Distance x Period p Frequency ν time for 1
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 informationEffects of Temperature and Concentration on the Rate of Photo-bleaching of Erythrosine in Water
Supporting Information for: Effects of Temperature and Concentration on the Rate of Photo-bleaching of Erythrosine in Water Joshua K. G. Karlsson, Owen J. Woodford, Roza Al-Aqar and Anthony Harriman* Molecular
More informationChapter 17: Fundamentals of Spectrophotometry
Chapter 17: Fundamentals of Spectrophotometry Spectroscopy: the science that deals with interactions of matter with electromagnetic radiation or other forms energy acoustic waves, beams of particles such
More informationPhys 2310 Mon. Dec. 4, 2017 Today s Topics. Begin supplementary material: Lasers Reading for Next Time
Phys 2310 Mon. Dec. 4, 2017 Today s Topics Begin supplementary material: Lasers Reading for Next Time 1 By Wed.: Reading this Week Lasers, Holography 2 Homework this Week No Homework this chapter. Finish
More informationLinear and nonlinear spectroscopy
Linear and nonlinear spectroscopy We ve seen that we can determine molecular frequencies and dephasing rates (for electronic, vibrational, or spin degrees of freedom) from frequency-domain or timedomain
More informationSpectroscopy of. Semiconductors. Luminescence OXFORD IVAN PELANT. Academy ofsciences of the Czech Republic, Prague JAN VALENTA
Luminescence Spectroscopy of Semiconductors IVAN PELANT Institute ofphysics, v.v.i. Academy ofsciences of the Czech Republic, Prague JAN VALENTA Department of Chemical Physics and Optics Charles University,
More informationCHAPTER 5 SPECTRAL CHARACTERISTICS OF NONLINEAR DYES IN LIQUID MEDIUM
90 CHAPTER 5 SPECTRAL CHARACTERISTICS OF NONLINEAR DYES IN LIQUID MEDIUM 5.1 INTRODUCTION The new nonlinear optical (NLO) materials with high optical nonlinearities are gaining interest both in research
More informationP. Lambrev October 10, 2018
TIME-RESOLVED OPTICAL SPECTROSCOPY Petar Lambrev Laboratory of Photosynthetic Membranes Institute of Plant Biology The Essence of Spectroscopy spectro-scopy: seeing the ghosts of molecules Kirchhoff s
More informationFluorescence Polarization Anisotropy FPA
Fluorescence Polarization Anisotropy FPA Optics study of light Spectroscopy = light interacts the study of the interaction between matter & electro-magnetic radiation matter Spectroscopy Atomic Spectroscopy
More informationNanoscale confinement of photon and electron
Nanoscale confinement of photon and electron Photons can be confined via: Planar waveguides or microcavities (2 d) Optical fibers (1 d) Micro/nano spheres (0 d) Electrons can be confined via: Quantum well
More informationFROM LOCALIZATION TO INTERACTION
EPFL SV PTBIOP FROM LOCALIZATION TO INTERACTION BIOP COURSE 2015 COLOCALIZATION TYPICAL EXAMPLE EPFL SV PTBIOP Vinculin Alexa568 Actin Alexa488 http://www.olympusconfocal.com/applications/colocalization.html
More informationMolecular spectroscopy
Molecular spectroscopy Origin of spectral lines = absorption, emission and scattering of a photon when the energy of a molecule changes: rad( ) M M * rad( ' ) ' v' 0 0 absorption( ) emission ( ) scattering
More informationLaboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching
Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Jose Alejandro Graniel Institute of Optics University of Rochester,
More informationUltraviolet-Visible and Infrared Spectrophotometry
Ultraviolet-Visible and Infrared Spectrophotometry Ahmad Aqel Ifseisi Assistant Professor of Analytical Chemistry College of Science, Department of Chemistry King Saud University P.O. Box 2455 Riyadh 11451
More informationDEVELOPMENT OF NANO PARTICLE SIZING SYSTEM USING FLUORESCENCE POLARIZATION
XX IMEKO World Congress Metrology for Green Growth September 9 14, 2012, Busan, Republic of Korea DEVELOPMENT OF NANO PARTICLE SIZING SYSTEM USING FLUORESCENCE POLARIZATION Terutake Hayashi, Masaki Michihata,
More informationAnalytical Chemistry II
Analytical Chemistry II L4: Signal processing (selected slides) Computers in analytical chemistry Data acquisition Printing final results Data processing Data storage Graphical display https://www.creativecontrast.com/formal-revolution-of-computer.html
More informationEinführung in die Photonik II
Einführung in die Photonik II ab 16.April 2012, Mo 11:00-12:30 Uhr SR 218 Lectures Monday, 11:00 Uhr, room 224 Frank Cichos Molecular Nanophotonics Room 322 Tel.: 97 32571 cichos@physik.uni-leipzig.de
More informationAnalytical Spectroscopy Review
Analytical Spectroscopy Review λ = wavelength ν = frequency V = velocity = ν x λ = 2.998 x 10 8 m/sec = c (in a vacuum) ν is determined by source and does not change as wave propogates, but V can change
More informationImagent for fnirs and EROS measurements
TECHNICAL NOTE Imagent for fnirs and EROS measurements 1. Brain imaging using Infrared Photons Brain imaging techniques can be broadly classified in two groups. One group includes the techniques that have
More informationDynamic population gratings in highly doped erbium fibers
Dynamic population gratings in highly doped erbium fibers Sonia Melle, Oscar G. Calderón, Z. C. Zhuo, M. A. Antón, F. Carreño Lasers, Quantum Optics and Non-linear Optics Group Complutense University of
More informationChemistry 524--Final Exam--Keiderling Dec. 12, pm SES
Chemistry 524--Final Exam--Keiderling Dec. 12, 2002 --4-8 pm -- 238 SES Please answer all questions in the answer book provided. Calculators, rulers, pens and pencils are permitted plus one 8.5 x 11 sheet
More informationFluorescence Quenching
Summary Fluorescence Quenching The emission of light from the excited state of a molecule (fluorescence or phosphorescence) can be quenched by interaction with another molecule. The stationary and time-dependent
More informationSUPPLEMENTARY INFORMATION
DOI: 10.1038/NPHOTON.2013.97 Supplementary Information Far-field Imaging of Non-fluorescent Species with Sub-diffraction Resolution Pu Wang et al. 1. Theory of saturated transient absorption microscopy
More informationLuminescence spectroscopy
Febr. 203 Luminescence spectroscopy Biophysics 2 nd semester Józse Orbán University o Pécs, Department o Biophysics Deinitions, laws FUNDAMENTALS o SPECTROSCY review - Spectral types (absorbtion/emission
More informationSupporting Information for. Near infrared-to-blue photon upconversion by exploiting direct. S-T absorption of a molecular sensitizer
Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2017 Supporting Information for Near infrared-to-blue photon upconversion by
More informationSupplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures
Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures Andreas W. Schell, 1, a) Johannes Kaschke, 2 Joachim Fischer,
More informationIncreasing your confidence Proving that data is single molecule. Chem 184 Lecture David Altman 5/27/08
Increasing your confidence Proving that data is single molecule Chem 184 Lecture David Altman 5/27/08 Brief discussion/review of single molecule fluorescence Statistical analysis of your fluorescence data
More informationTIME-RESOLVED OPTICAL SPECTROSCOPY
TIME-RESOLVED OPTICAL SPECTROSCOPY Petar Lambrev Laboratory of Photosynthetic Membranes Institute of Plant Biology The Essence of Spectroscopy spectro-scopy: seeing the ghosts of molecules Kirchhoff s
More informationChemistry Instrumental Analysis Lecture 5. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 5 Light Amplification by Stimulated Emission of Radiation High Intensities Narrow Bandwidths Coherent Outputs Applications CD/DVD Readers Fiber Optics Spectroscopy
More informationSupplementary Figures
Supplementary Figures Supplementary Figure. X-ray diffraction pattern of CH 3 NH 3 PbI 3 film. Strong reflections of the () family of planes is characteristics of the preferred orientation of the perovskite
More informationAnswers to questions on exam in laser-based combustion diagnostics on March 10, 2006
Answers to questions on exam in laser-based combustion diagnostics on March 10, 2006 1. Examples of advantages and disadvantages with laser-based combustion diagnostic techniques: + Nonintrusive + High
More informationSemiconductor quantum dots
Semiconductor quantum dots Quantum dots are spherical nanocrystals of semiconducting materials constituted from a few hundreds to a few thousands atoms, characterized by the quantum confinement of the
More informationSingle Emitter Detection with Fluorescence and Extinction Spectroscopy
Single Emitter Detection with Fluorescence and Extinction Spectroscopy Michael Krall Elements of Nanophotonics Associated Seminar Recent Progress in Nanooptics & Photonics May 07, 2009 Outline Single molecule
More informationRadiation-matter interaction.
Radiation-matter interaction Radiation-matter interaction Classical dipoles Dipole radiation Power radiated by a classical dipole in an inhomogeneous environment The local density of optical states (LDOS)
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION Electroluminescence from a single nanotube-molecule-nanotube junction Christoph W. Marquardt, Sergio Grunder, Alfred Błaszczyk, Simone Dehm, Frank Hennrich, Hilbert v. Löhneysen,
More informationFluorescence 2009 update
XV 74 Fluorescence 2009 update 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 informationInfluence of Plasmonic Array Geometry on Energy Transfer from a. Quantum Well to a Quantum Dot Layer
Electronic Supplementary Material (ESI) for Nanoscale. This journal is The Royal Society of Chemistry 2016 Influence of Plasmonic Array Geometry on Energy Transfer from a Quantum Well to a Quantum Dot
More informationEngineering Medical Optics BME136/251 Winter 2017
Engineering Medical Optics BME136/251 Winter 2017 Monday/Wednesday 2:00-3:20 p.m. Beckman Laser Institute Library, MSTB 214 (lab) Teaching Assistants (Office hours: Every Tuesday at 2pm outside of the
More informationApplication of time resolved area normalized emission spectroscopy to multicomponent systems
JOURNAL OF CHEMICAL PHYSICS VOLUME 115, NUMBER 15 15 OCTOBER 2001 Application of time resolved area normalized emission spectroscopy to multicomponent systems A. S. R. Koti and N. Periasamy a) Department
More informationSpectroscopy: Introduction. Required reading Chapter 18 (pages ) Chapter 20 (pages )
Spectroscopy: Introduction Required reading Chapter 18 (pages 378-397) Chapter 20 (pages 424-449) Spectrophotometry is any procedure that uses light to measure chemical concentrations Properties of Light
More informationFluorescence Spectroscopy
Fluorescence Spectroscopy Thomas Schmidt Department of Biophysics Leiden University, The Netherlands tschmidt@biophys.leidenuniv.nl www.biophys.leidenuniv.nl/research/fvl Biophysical Structural Biology
More informationFederal University of São Carlos Physics Department. Time Resolved Measurement System MUE: 2014/
Federal University of São Carlos Physics Department Semiconductor Nanostructure Group Optical Properties, Vibrational, Spin and Transport Time Resolved Measurement System MUE: 2014/07375-2 Young Investigator:
More informationLAB 3: Confocal Microscope Imaging of single-emitter fluorescence. LAB 4: Hanbury Brown and Twiss setup. Photon antibunching. Roshita Ramkhalawon
LAB 3: Confocal Microscope Imaging of single-emitter fluorescence LAB 4: Hanbury Brown and Twiss setup. Photon antibunching Roshita Ramkhalawon PHY 434 Department of Physics & Astronomy University of Rochester
More informationBlending conjugated polymers without phase separation for fluorescent colour tuning of polymeric materials through FRET
Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2014 Supplementary Information Blending conjugated polymers without phase separation for fluorescent
More informationZiessel a* Supporting Information (75 pages) Table of Contents. 1) General Methods S2
S1 Chemistry at Boron: Synthesis and Properties of Red to Near-IR Fluorescent Dyes based on Boron Substituted Diisoindolomethene Frameworks Gilles Ulrich, a, * Sebastien Goeb a, Antoinette De Nicola a,
More informationSmall Signal Gain in DPAL Systems
Physical Sciences Inc. VG11-010 Small Signal Gain in DPAL Systems Kristin L. Galbally-Kinney, Daniel L. Maser, William J. Kessler, Wilson T. Rawlins, and Steven J. Davis 20 New England Business Center
More informationIntroduction to Sources: Radiative Processes and Population Inversion in Atoms, Molecules, and Semiconductors Atoms and Molecules
OPTI 500 DEF, Spring 2012, Lecture 2 Introduction to Sources: Radiative Processes and Population Inversion in Atoms, Molecules, and Semiconductors Atoms and Molecules Energy Levels Every atom or molecule
More informationLaser Detection Techniques
Laser Detection Techniques K.-H. Gericke Institute for Physical Chemistry University Braunschweig E 2 E 1 = hn, λ = c /n Lambert-Beer Law Transmittance of the sample:: T = I / I 0 T = e -snl = e -α, where
More informationSingle Photon detectors
Single Photon detectors Outline Motivation for single photon detection Semiconductor; general knowledge and important background Photon detectors: internal and external photoeffect Properties of semiconductor
More information1 Fluorescence Resonance Energy Transfer
1 Fluorescence Resonance Energy Transfer FRET is nominally the non-radiative transfer of energy from a donor molecule to the acceptor molecule, therefore the signature of FRET is quenching of the low energy
More informationInstrumental Analysis: Spectrophotometric Methods
Instrumental Analysis: Spectrophotometric Methods 2007 By the end of this part of the course, you should be able to: Understand interaction between light and matter (absorbance, excitation, emission, luminescence,fluorescence,
More informationChemistry 304B, Spring 1999 Lecture 5 1. UV Spectroscopy:
Chemistry 304B, Spring 1999 Lecture 5 1 Ultraviolet spectroscopy; UV Spectroscopy: Infrared spectroscopy; Nuclear magnetic resonance spectroscopy General basis of spectroscopy: Shine light at a collection
More informationCD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray
CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray crystallography An example of the use of CD Modeling
More informationChapter 29 Molecular and Solid-State Physics
Chapter 29 Molecular and Solid-State Physics GOALS When you have mastered the content of this chapter, you will be able to achieve the following goals: Definitions Define each of the following terms, and
More information