Fluorescence Resonance Energy Transfer (FRET) Microscopy

Size: px
Start display at page:

Download "Fluorescence Resonance Energy Transfer (FRET) Microscopy"

Transcription

1 Fluorescence Resonance Energy Transfer () Microscopy Mike Lorenz Optical Technology Development -FLM course, May 2009

2 What is fluorescence? Stoke s shift Fluorescence light is always redshifted!!! fluorescence rel. intensity absorption wavelength / nm Quantum yield Ratio of emitted to absorbed photons Lifetime Average time the fluorophore remains in the excited state

3 Spectroscopic principles of E = k k + k f + k x = R R R 6 1,0 R 1948 / ( Q J n ) 1 κ ( 6 Å 0 = 9790 D λ) n: refraction index Φ D : donor quantum efficiency J: spectral overlap integral κ: dipole orientation factor efficiency E 0,8 0,6 0,4 0,2 0,0 ½ R 0 R 0 1½ R 0 dye-to-dye distance 2 R 0

4 Förster distance R 0 R ( 2 4 κ Q J ( n ) Å D ) = λ 1 6 κ 2 Q D donor-acceptor orientation factor donor quantum yield J(λ) overlap integral n refraction index 100 ECFP EYFP J wavelength / nm 4 ( λ ) D ( λ) = F ( λ) ε ( λ) 0 dλ D 2 κ = θ θ A T θ D A ( cosθ 3cosθ cosθ ) 2 T D A D A: D A: random: 2 κ 2 κ 2 κ = 4 = 0 = 2 / 3 For most D-A pairs is R 0 = nm

5 can be measured via ntensity in both channels Fluorescence lifetime of the donor τ τ D DA = k f = k f 1 + k x + k 1 + x k E = 1 D => E τ =1 τ D

6 Requirements for a good pair Maximal overlap of donor emission and acceptor excitation CFP GFP High quantum yield of the donor Good spectral separation norm. intensity Minimal direct excitation of the acceptor at the excitation maximum of the donor Minimal emission of the donor with the acceptor fluorescence (bleed-through) norm. intensity wavelength [nm] CFP YFP wavelength [nm]

7 Common donor/acceptor pairs Donor (Em.) Acceptor (Exc.) R 0 (κ 2 =2/3) FTC (520 nm) TRTC (550 nm) ~ 5 nm Cy3 (566 nm) Cy5 (649 nm) ~ 5.7 nm EGFP (508 nm) Cy3 (554 nm) CFP (477 nm) YFP (514 nm) ~ 5 nm EGFP (508 nm) YFP (514 nm) ~ 5.7 nm EGFP (508 nm) Cherry (588 nm) ~ 5.3 nm

8 DNA bending measured by

9 Microscopy R ~ 2-8 n m R > 10 n m!!! CFP ex em YFP ex em 1 kt ( R0 / R ) = τd optical resolution ~ nm λ χ 0.61 NA 0.6 efficiency Wavelength / nm R06 kt E= = 6 k D + kt R0 + R 6

10 Applications of microscopy

11 detection methods Donor Photobleaching Acceptor Photobleaching => fixed samples Sensitized Emission Ratio maging Fluorescence Lifetime => in vivo Polarization / Anisotropy

12 by Acceptor Photobleaching Prebleach mage Acceptor Bleaching (RO) Postbleach mage Filtering Bkg correction Adjust PMT variations Calculate 405 or or or efficiency E = 1 prepb D postpb D Acquisition Processing

13 CFP-YFP: An excellent pair for CLSM All laser scanning microscopes have the necessary laser lines for CFP and CFP YFP (458 & 514 nm Argon-Laser). YFP 514 nm excites the acceptor only allowing a selective photobleaching norm. intensity Tuneable emission filters can collect most of the CFP fluorescnce without any contribution of the acceptor YFP ( nm) wavelength [nm] Recommended CLSM: Leica SP2 or SP5 (with AOBS) Olympus FV1000 Zeiss LSM 710

14 Problems with CFP-YFP in pb?

15 Can green-red work as a pair? Cherry GFP R 0 ~ 5.3 nm norm. intensity wavelength [nm] Cherry YFP R 0 ~ 5.7 nm norm. intensity wavelength [nm]

16 by Acceptor Photobleaching 1. Take donor & acceptor image 2. partially pb acceptor 3. Take donor image Microscope: Confocal Advantages: Can be used for all experiments Easy quantitative measurements E ~ 0.13 Disadvantages: Destructive Fixed samples only

17 by Sensitized Emission CFP-PTB PTB nf = DA YFP-Raver1 D DA D Donor Donor A A Acceptor DA Acceptor Ex: CFP YFP CFP Em: CFP YFP YFP corrected CFP YFP ex em ex em Microscope: Widefield / Confocal Advantages: Non-destructive => live cell imaging Wavelength / nm Disadvantages: Not quantitative Requires correction for bleedthrough etc. Sensitive to photobleaching

18 by Sensitized Emission nf can be affected by several factors: Donor and acceptor intensity (or concentration) of the pixels efficiency Ratio of complexes to free donor and acceptor => nf should be normalized to be intensity independent Normalization 1. nf Donor 2. Gordon et al. (1998) N = nf Donor Acceptor Normalization by Gordon (2) is not intensity independent 3. Xia & Liu (2001) N = Donor nf Acceptor (1) and (3) are, but only Xia takes both concentrations into account

19 by Donor-Acceptor Ratio maging ratio = Donor Ch Ch 435nm CRB WH1 V V CA 470nm 530nm

20 by Donor-Acceptor Ratio maging ratio = Donor Ch Ch 435nm CDC42 CRB WH1 V V C A 470nm

21 by Donor-Acceptor Ratio maging Microscope: ratio Widefield / Confocal Lorenz et al., Curr Biol, 2004 Advantages: Non-destructive => live cell imaging Easy qualitative measurements mages can be taken simultaneously Disadvantages: Limited for biosensors

22 J Cell Sci Mar 15;117(Pt 8):

23 by Anisotropy (Homotransfer) rotational correlation time (~18 ns) >> fluorescence lifetime (<3 ns) Emission light is polarized when excited with polarized light!!! r = + 2 Microscope: Widefield / Confocal Emission light is depolarized. Advantages: Non-destructive => live cell imaging mages can be taken simultaneously Useful for dimerization studies (e.g. receptor dimerization) Only 1 construct is necessary Disadvantages:???

24 - Microscopy Method: Detects proximity between donor and acceptor fluorophores (up to ~2-8nm) Application: Protein-protein interactions ntramolecular conformational changes Biosensors (e.g. Ca 2+, GTPases, kinases activity) Advantages: ncreases spatial resolution of fluorescence microscopy (~ nm) Limitations: Absence of is not definitive. Due to a long rotational correlation time of GFP (~18ns) no exact distance information can be obtained.

25 Literature Review Truong & kura, Curr Opin Struct Biol (2001), 573. Vogel et al., Sci STKE (2006). Acceptor Photobleaching Roy et al., Methods Mol Biol (2009), 69. Sensitized Emission / Ratio maging Gordon et al., Biophys J (1998), Xia & Liu, Biophys J (2001), Sorkin et al., Curr Biol (2000), Lorenz et al., Curr Biol (2004), 697.

FROM LOCALIZATION TO INTERACTION

FROM 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 information

Co-localization, FRET

Co-localization, FRET Co-localization, FRET Last class FRAP Diffusion This class Co-localization Correlation FRET Co-localization Can you infer function of protein from it s intracellular location How do you measure if two

More information

single-molecule fluorescence resonance energy transfer

single-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 information

Single-Molecule Methods I - in vitro

Single-Molecule Methods I - in vitro Single-Molecule Methods I - in vitro Bo Huang Macromolecules 2014.03.10 F 1 -ATPase: a case study Membrane ADP ATP Rotation of the axle when hydrolyzing ATP Kinosita group, 1997-2005 Single Molecule Methods

More information

Advanced Fluorescence Microscopy I: Fluorescence (Foster) Resonance Energy Transfer

Advanced Fluorescence Microscopy I: Fluorescence (Foster) Resonance Energy Transfer Advanced Fluorescence Microscopy I: Fluorescence (Foster) Resonance Energy Transfer 3.0 Pax 2.5 2.0 1200 800 400 GFP- Pax GFP-Pax + FATmCherry FAT FAT 1.5 Lifetime (ns) 0 1500 2000 2500 3000 Average lifetime

More information

1. Transition dipole moment

1. 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 information

Fluorescence polarisation, anisotropy FRAP

Fluorescence polarisation, anisotropy FRAP Fluorescence polarisation, anisotropy FRAP Reminder: fluorescence spectra Definitions! a. Emission sp. b. Excitation sp. Stokes-shift The difference (measured in nm) between the peak of the excitation

More information

Optical Spectroscopy. Steady State and Time Dependent Fluorescence Measurements. Kai Wen Teng. October 8 th PHYS 403 Fall 2013

Optical Spectroscopy. Steady State and Time Dependent Fluorescence Measurements. Kai Wen Teng. October 8 th PHYS 403 Fall 2013 Optical Spectroscopy Steady State and Time Dependent Fluorescence Measurements Kai Wen Teng October 8 th 2013 PHYS 403 Fall 2013 EM Spectrum of molecules Rotational Energy Infrared Vibrational Energy Near

More information

Rice/TCU REU on Computational Neuroscience. Fundamentals of Molecular Imaging

Rice/TCU REU on Computational Neuroscience. Fundamentals of Molecular Imaging Rice/TCU REU on Computational Neuroscience Fundamentals of Molecular Imaging June 3, 2008 Neal Waxham 713-500-5621 m.n.waxham@uth.tmc.edu Objectives Brief discussion of optical resolution and lasers as

More information

Supporting Information

Supporting 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 information

Fluorescence (Notes 16)

Fluorescence (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 information

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

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 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 information

(i.e. what you should be able to answer at end of lecture)

(i.e. what you should be able to answer at end of lecture) Today s Announcements 1. Test given back next Wednesday 2. HW assigned next Wednesday. 3. Next Monday 1 st discussion about Individual Projects. Today s take-home lessons (i.e. what you should be able

More information

Optics and Spectroscopy

Optics 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 information

Fluorescence 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 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 information

Energy 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 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 information

Lecture 5. Anisotropy decay/data analysis. Enrico Gratton

Lecture 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 information

Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET. David A. Case Rutgers, Spring 2009

Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET. David A. Case Rutgers, Spring 2009 Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET David A. Case Rutgers, Spring 2009 Techniques based on rotational motion What we studied last time probed translational

More information

Fluorescence Spectroscopy

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 information

4 Single molecule FRET

4 Single molecule FRET 4 Single molecule FRET FRET basics Energie Dipole-dipole interaction Teil I SM Fluo, Kap. 4 FRET FRET basics transfer rate (from Fermis Golden Rule) k t = 1 0 1 r 6 apple 2 9 ln(10) n 4 N A 128 5 Z d f

More information

Fluorescence Polarization Anisotropy FPA

Fluorescence 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 information

Fluorescence Spectroscopy

Fluorescence 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 information

Detection of Mercury(II) and Lead(II) with Graphene Oxide- Based Biosensors

Detection of Mercury(II) and Lead(II) with Graphene Oxide- Based Biosensors Detection of Mercury(II) and Lead(II) with Graphene Oxide- Based Biosensors Ming Li, Nianqiang (Nick) Wu* Mechanical & Aerospace Engineering West Virginia University Morgantown, WV 26506 Presentation Outline

More information

Fluorescence 2009 update

Fluorescence 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 information

MITOHEALTH Nordic Centre of Excellence Workshop in: Mitochondrial function and metabolic diseases

MITOHEALTH Nordic Centre of Excellence Workshop in: Mitochondrial function and metabolic diseases MITOHEALTH Nordic Centre of Excellence Workshop in: Mitochondrial function and metabolic diseases Quantitative multi-parameter microscopy of mitochondrial function in living cells Werner J.H. Koopman,

More information

Self-assembled Nanoscale DNA-porphyrin Complex for. Artificial Light-harvesting

Self-assembled Nanoscale DNA-porphyrin Complex for. Artificial Light-harvesting Supporting Information for Self-assembled Nanoscale DNA-porphyrin Complex for Artificial Light-harvesting Jakob G. Woller, Jonas K. Hannestad, and Bo Albinsson Department of Chemical and Biological Engineering/Physical

More information

Supplementary Material

Supplementary Material Supplentary Material Three-Color Alternating-Laser xcitation of Single Molecules: Monitoring Multiple Interactions and Distances Nam Ki Lee, Achillefs N. Kapanidis, Hye an Koh, You Korlann, Sam On Ho,

More information

Interaction mechanism for energy transfer from Ce to Tb ions in silica

Interaction mechanism for energy transfer from Ce to Tb ions in silica Interaction mechanism for energy transfer from Ce to Tb ions in silica HAA Seed Ahmed 1,2, W-S Chae 3, OM Ntwaeaborwa 1 and RE Kroon 1 1 Department of Physics, University of the Free State, South Africa

More information

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Confocal 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 information

Modern Optical Spectroscopy

Modern Optical Spectroscopy Modern Optical Spectroscopy With Exercises and Examples from Biophysics and Biochemistry von William W Parson 1. Auflage Springer-Verlag Berlin Heidelberg 2006 Verlag C.H. Beck im Internet: www.beck.de

More information

Polarised light. Polarised light. Polarised light. Polarizer. Polarisation

Polarised light. Polarised light. Polarised light. Polarizer. Polarisation Polarisation UNIVRSITY OF PÉCS MDICAL SCHOOL Fluorescence anisotrop, FRT In photograph! Miklós Nitrai, Februar 10, 2015 Wh? Polarised light Polarised light Light: lectro-magnetic radiation - a transverse

More information

Fluorescence Spectroscopy

Fluorescence 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 information

Advanced Spectroscopy Laboratory

Advanced Spectroscopy Laboratory Advanced Spectroscopy Laboratory - Raman Spectroscopy - Emission Spectroscopy - Absorption Spectroscopy - Raman Microscopy - Hyperspectral Imaging Spectroscopy FERGIELAB TM Raman Spectroscopy Absorption

More information

Förster Energy Transfer - AKA - Fluorescence Resonance Energy Transfer

Förster Energy Transfer - AKA - Fluorescence Resonance Energy Transfer örster Energy Transfer - K - luorescence esonance Energy Transfer 1. Origins: Theory of Energy Transfer developed by T. örster (örster. 1948. nnalen der Physi. :55-75.). evelopment of ET as a Spectroscopic

More information

1 Fluorescence Resonance Energy Transfer

1 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 information

Homo-FRET detection in wide-field, steady-state microscopy, with mcherry as labeling fluorophore

Homo-FRET detection in wide-field, steady-state microscopy, with mcherry as labeling fluorophore University Utrecht Debey Institute, Biophysics Homo-FRET detection in wide-field, steady-state microscopy, with mcherry as labeling fluorophore Author: Margriet Oomen Supervisors: prof. dr. H.C. Gerritsen

More information

Supporting Information

Supporting Information Supporting Information Energy Transfer-Based Multiplexed Assay of Proteases by Using Gold Nanoparticle and Quantum Dot Conjugates on a Surface Young-Pil Kim, 1, Young-Hee Oh, 1, Eunkyu Oh, 1 Sungho Ko,

More information

CHEM Outline (Part 15) - Luminescence 2013

CHEM 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 information

Luminescence. Photoluminescence (PL) is luminescence that results from optically exciting a sample.

Luminescence. 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 information

Chapter 2 Energy Transfer Review

Chapter 2 Energy Transfer Review Chapter 2 Energy Transfer Review In this chapter, we discuss the basic concepts of excitation energy transfer, making the distinction between radiative and nonradiative, and giving a brief overview on

More information

Laboratory 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 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 information

Fluorescence Resonance Energy Transfer (FRET) in Polymer Films and Polymer Blends

Fluorescence Resonance Energy Transfer (FRET) in Polymer Films and Polymer Blends Fluorescence Resonance Energy Transfer (FRET) in Polymer Films and Polymer Blends Neda Felorzabihi, Jeffrey C. Haley, Pablo Froimowicz, Ghasem R. Bardajee and Mitchell. Winnik epartment of Chemical Engineering

More information

BMB Class 17, November 30, Single Molecule Biophysics (II)

BMB 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 information

High photostability and enhanced fluorescence of gold nanoclusters by silver doping-supporting information

High photostability and enhanced fluorescence of gold nanoclusters by silver doping-supporting information High photostability and enhanced fluorescence of gold nanoclusters by silver doping-supporting information Size measurements Figure S1 P2 FTIR measurements Figure S2 P2 XPS measurements Figure S3 P3 Photo-physical

More information

Fluorescence Spectroscopy

Fluorescence 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 information

Solution set for EXAM IN TFY4265/FY8906 Biophysical microtechniques

Solution 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 information

Luminescence spectroscopy

Luminescence 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 information

Fluorescence and Nuclear Magnetic Resonance (NMR) Spectroscopy

Fluorescence and Nuclear Magnetic Resonance (NMR) Spectroscopy Fluorescence and Nuclear Magnetic Resonance (NMR) Spectroscopy Murphy, B. (2017). Fluorescence and Nuclear Magnetic Resonance Spectroscopy: Lecture 3. Lecture presented at PHAR 423 Lecture in UIC College

More information

The Photon Counting Histogram (PCH)

The Photon Counting Histogram (PCH) The Photon Counting Histogram (PCH) While Fluorescence Correlation Spectroscopy (FCS) can measure the diffusion coefficient and concentration of fluorophores, a complementary method, a photon counting

More information

Manipulating and Probing Enzymatic Conformational Fluctuations and Enzyme-Substrate Interactions by Single-Molecule FRET- Magnetic Tweezers Microscopy

Manipulating and Probing Enzymatic Conformational Fluctuations and Enzyme-Substrate Interactions by Single-Molecule FRET- Magnetic Tweezers Microscopy Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2014 Supporting Information (SI) Manipulating and Probing Enzymatic Conformational Fluctuations

More information

Survival Strategy: Photosynthesis

Survival Strategy: Photosynthesis Energy and Electron Transfer Survival Strategy: Photosynthesis Light Energy Harvested by Plants 6 CO 2 + 6 H 2 O + light energy C 6 H 12 O 6 + 6 O 2 Importance of Photosynthesis Provides energy for plants

More information

Discussion Session prior to the Second Examination: Sunday evening April 13 6 to 8 pm. 161 Noyes Laboratory

Discussion Session prior to the Second Examination: Sunday evening April 13 6 to 8 pm. 161 Noyes Laboratory Discussion Session prior to the Second Examination: Sunday evening April 13 6 to 8 pm 161 Noyes Laboratory Determination of the Stokes Radius by measuring the Rotational Diffusion Coefficient: D rot D

More information

Chapter 15 Molecular Luminescence Spectrometry

Chapter 15 Molecular Luminescence Spectrometry Chapter 15 Molecular Luminescence Spectrometry Two types of Luminescence methods are: 1) Photoluminescence, Light is directed onto a sample, where it is absorbed and imparts excess energy into the material

More information

Singlet. Fluorescence Spectroscopy * LUMO

Singlet. 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 information

Multiphoton Imaging and Spectroscopy in Cell and Tissue Biophysics. J Moger and C P Winlove

Multiphoton Imaging and Spectroscopy in Cell and Tissue Biophysics. J Moger and C P Winlove Multiphoton Imaging and Spectroscopy in Cell and Tissue Biophysics J Moger and C P Winlove Relating Structure to Function Biochemistry Raman microspectrometry Surface enhanced Raman spectrometry (SERS)

More information

Supplementary Materials: Probing the Ion Binding Site in a DNA Holliday Junction Using Förster Resonance Energy Transfer (FRET)

Supplementary Materials: Probing the Ion Binding Site in a DNA Holliday Junction Using Förster Resonance Energy Transfer (FRET) S1 of S5 Supplementary Materials: Probing the Ion Binding Site in a DNA Holliday Junction Using Förster Resonance Energy Transfer (FRET) Jacob L. Litke, Yan Li, Laura M. Nocka and Ishita Mukerji (a) (b)

More information

bio-molecular studies Physical methods in Semmelweis University Osváth Szabolcs

bio-molecular studies Physical methods in Semmelweis University Osváth Szabolcs Physical methods in bio-molecular studies Osváth Szabolcs Semmelweis University szabolcs.osvath@eok.sote.hu Light emission and absorption spectra Stokes shift is the difference (in wavelength or frequency

More information

1 Appendix on the 3 3 -FRET method. Supplemental Data for: Erickson et al., Neuron 31, pp

1 Appendix on the 3 3 -FRET method. Supplemental Data for: Erickson et al., Neuron 31, pp upplemental Data for: Erickson et al., Neuron 31, pp. 973-985 upplemental ppendices on the Three-Cube Method 3 3 - and Extensions of the Method to Characterize Properties of Binding Between Donor and cceptor

More information

Chapter 6 Photoluminescence Spectroscopy

Chapter 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 information

Supplementary Materials

Supplementary 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 information

Measurement Examples. Excitation and Emission Scans. Steady State Fluorescence Anisotropy. Kinetic Measurements

Measurement 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 information

Laboratory 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 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 information

LAB 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 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 information

ECE 240a - Notes on Spontaneous Emission within a Cavity

ECE 240a - Notes on Spontaneous Emission within a Cavity ECE 0a - Notes on Spontaneous Emission within a Cavity Introduction Many treatments of lasers treat the rate of spontaneous emission as specified by the time constant τ sp as a constant that is independent

More information

"Molecular Photochemistry - how to study mechanisms of photochemical reactions?"

Molecular Photochemistry - how to study mechanisms of photochemical reactions? "Molecular Photochemistry - how to study mechanisms of photochemical reactions?" Bronislaw Marciniak Faculty of Chemistry, Adam Mickiewicz University, Poznan, Poland 2014/2015 - lecture 4 Contents 1. Introduction

More information

arxiv: v1 [physics.optics] 8 Jan 2015

arxiv: v1 [physics.optics] 8 Jan 2015 Version 1.0 January 9, 2015 A Theoretical Investigation of Decay and Energy Transfer Rates and Efficiencies Near Gold Nanospheres Cristian A. Marocico, Xia Zhang, and A. Louise Bradley Semiconductor Photonics

More information

Fluorescence Workshop UMN Physics June 8-10, 2006 Basic Spectroscopic Principles Joachim Mueller

Fluorescence Workshop UMN Physics June 8-10, 2006 Basic Spectroscopic Principles Joachim Mueller Fluorescence Workshop UMN Physics June 8-10, 2006 Basic Spectroscopic Principles Joachim Mueller Fluorescence, Light, Absorption, Jablonski Diagram, and Beer-Law First stab at a definition: What is fluorescence?

More information

Introduction to Biomedical Engineering

Introduction to Biomedical Engineering Introduction to Biomedical Engineering Biomedical optics II Kung-Bin Sung 1 Outline Chapter 17: Biomedical optics and lasers Fundamentals of light Light-matter interaction Optical imaging Optical sensing:

More information

SUPPLEMENTARY INFORMATION 1. MATERIALS AND METHODS

SUPPLEMENTARY INFORMATION 1. MATERIALS AND METHODS SUPPLEMENTARY INFORMATION 1. MATERIALS AND METHODS Citrate/phosphate buffer preparation Buffer solutions were prepared with potassium gluconate (10 mm), sodium gluconate (40 mm), sodium phosphate (10 mm),

More information

Characterisation of vibrational modes of adsorbed species

Characterisation of vibrational modes of adsorbed species 17.7.5 Characterisation of vibrational modes of adsorbed species Infrared spectroscopy (IR) See Ch.10. Infrared vibrational spectra originate in transitions between discrete vibrational energy levels of

More information

Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy. Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy

Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy. Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy Topic 2b: X-ray Fluorescence Spectrometry Text: Chapter 12 Rouessac (1 week) 4.0 X-ray Fluorescence Download, read and understand EPA method 6010C ICP-OES Winter 2009 Page 1 Atomic X-ray Spectrometry Fundamental

More information

DETERMINATION OF RELATIVE FLUORESCENCE QUANTUM YIELD USING THE AGILENT CARY ECLIPSE

DETERMINATION OF RELATIVE FLUORESCENCE QUANTUM YIELD USING THE AGILENT CARY ECLIPSE FOOD ANALYSIS DETERMINATION OF RELATIVE FLUORESCENCE QUANTUM YIELD USING THE AGILENT CARY ECLIPSE Solutions for Your Analytical Business Markets and Applications Programs Authors Sangeetha Ramesan Co-Authors

More information

Wavelength 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

Wavelength 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 information

Measuring Colocalization within Fluorescence Microscopy Images

Measuring Colocalization within Fluorescence Microscopy Images from photonics.com: 03/01/2007 http://www.photonics.com/article.aspx?aid=39341 Measuring Colocalization within Fluorescence Microscopy Images Two-color fluorescence-based methods are uncovering molecular

More information

Surface Plasmon Amplification by Stimulated Emission of Radiation. By: Jonathan Massey-Allard Graham Zell Justin Lau

Surface Plasmon Amplification by Stimulated Emission of Radiation. By: Jonathan Massey-Allard Graham Zell Justin Lau Surface Plasmon Amplification by Stimulated Emission of Radiation By: Jonathan Massey-Allard Graham Zell Justin Lau Surface Plasmons (SPs) Quanta of electron oscillations in a plasma. o Electron gas in

More information

Supporting Information

Supporting 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 information

Radiation in the Earth's Atmosphere. Part 1: Absorption and Emission by Atmospheric Gases

Radiation in the Earth's Atmosphere. Part 1: Absorption and Emission by Atmospheric Gases Radiation in the Earth's Atmosphere Part 1: Absorption and Emission by Atmospheric Gases Electromagnetic Waves Electromagnetic waves are transversal. Electric and magnetic fields are perpendicular. In

More information

Quantum Optics and Quantum Information Laboratory

Quantum Optics and Quantum Information Laboratory Quantum Optics and Quantum Information Laboratory OPT 253, Fall 2011 Institute of Optics University of Rochester Instructor: Dr. Lukishova Jonathan Papa Contents Lab 1: Entanglement and Bell s Inequalities

More information

Nanoscopy with Focused Light

Nanoscopy with Focused Light Nanoscopy with Focused Light Stefan W. Hell Max Planck Institute for Biophysical Chemistry Department of NanoBiophotonics Göttingen & German Cancer Research Center (DKFZ) Optical Nanoscopy Division Heidelberg

More information

E L E C T R O P H O S P H O R E S C E N C E

E L E C T R O P H O S P H O R E S C E N C E Organic LEDs part 4 E L E C T R O P H O S P H O R E S C E C E. OLED efficiency 2. Spin 3. Energy transfer 4. Organic phosphors 5. Singlet/triplet ratios 6. Phosphor sensitized fluorescence 7. Endothermic

More information

Chemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES

Chemistry 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 information

Vibrational imaging and microspectroscopies based on coherent anti-stokes Raman scattering (CARS)

Vibrational imaging and microspectroscopies based on coherent anti-stokes Raman scattering (CARS) Vibrational imaging and microspectroscopies based on coherent anti-stokes Raman scattering (CARS) by Andreas Volkmer Universität Stuttgart 3 rd Institute of Physics, University of Stuttgart, Pfaffenwaldring

More information

Triangulating Nucleic Acid Conformations Using Multicolor Surface Energy Transfer

Triangulating Nucleic Acid Conformations Using Multicolor Surface Energy Transfer Triangulating Nucleic cid Conformations Using Multicolor Surface Energy Transfer Supporting Information Ryan. Riskowski 1, Rachel E. rmstrong 2, Nancy L. Greenbaum 3, Geoffrey F. Strouse 1,2 * 1 Molecular

More information

LABORATORY OF ELEMENTARY BIOPHYSICS

LABORATORY 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 information

Single Molecule Spectroscopy and Imaging

Single Molecule Spectroscopy and Imaging Single Molecule Spectroscopy and Imaging Ingo Gregor, Thomas Dertinger, Iris von der Hocht, Jan Sykora, Luru Dai, Jörg Enderlein Institute for Biological Information Processing 1 Forschungszentrum Jülich

More information

Anti-Bunching from a Quantum Dot

Anti-Bunching from a Quantum Dot Anti-Bunching from a Quantum Dot Gerardo I. Viza 1, 1 Department of Physics and Astronomy, University of Rochester, Rochester, NY 14627 We study the nature of non-classical single emitter light experimentally

More information

S1. 1 H NMR spectrum for PTTBD in CDCl 3. Insert shows the expansion of the aromatic region and the sharp proton resonances.

S1. 1 H NMR spectrum for PTTBD in CDCl 3. Insert shows the expansion of the aromatic region and the sharp proton resonances. Supporting Information Tuning the Förster Overlap Integral: Energy Transfer over 20 Angstroms from a Pyrene-based Donor to Borondipyrromethene (Bodipy) Dan Bai, Andrew C. Benniston, Jerry Hagon, Helge

More information

Supplementary information for. Observation of photovoltaic action from photoacid-modified Nafion due to light-driven ion transport

Supplementary information for. Observation of photovoltaic action from photoacid-modified Nafion due to light-driven ion transport Supplementary information for Observation of photovoltaic action from photoacid-modified Nafion due to light-driven ion transport William White, a# Christopher D. Sanborn, a# Ronald S. Reiter, a David

More information

Time 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 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 information

Morphology-dependent resonance induced by two-photon excitation in a micro-sphere trapped by a femtosecond pulsed laser

Morphology-dependent resonance induced by two-photon excitation in a micro-sphere trapped by a femtosecond pulsed laser Morphology-dependent resonance induced by two-photon excitation in a micro-sphere trapped by a femtosecond pulsed laser Dru Morrish, Xiaosong Gan and Min Gu Centre for Micro-Photonics, School of Biophysical

More information

Aula 5 e 6 Transferência de Energia e Transferência de Elétron Caminhos de espécies fotoexcitadas

Aula 5 e 6 Transferência de Energia e Transferência de Elétron Caminhos de espécies fotoexcitadas Fotoquímica Aula 5 e 6 Transferência de Energia e Transferência de Elétron Prof. Amilcar Machulek Junior IQ/USP - CEPEMA Caminhos de espécies fotoexcitadas 1 Diagrama de Jablonski S 2 Relaxation (τ < 1ps)

More information

Lab 11: Must what goes in be the same as what comes out? Spectroscopy & Fluorescence in Chlorophyll.

Lab 11: Must what goes in be the same as what comes out? Spectroscopy & Fluorescence in Chlorophyll. Lab 11: Must what goes in be the same as what comes out? Spectroscopy & Fluorescence in Chlorophyll. Introduction to Fluorescence: Fluorescence is one of the possible mechanisms for emission of light by

More information

Supporting Information. CdS/mesoporous ZnS core/shell particles for efficient and stable photocatalytic hydrogen evolution under visible light

Supporting Information. CdS/mesoporous ZnS core/shell particles for efficient and stable photocatalytic hydrogen evolution under visible light Electronic Supplementary Material (ESI) for Energy & Environmental Science. This journal is The Royal Society of Chemistry 2014 Supporting Information CdS/mesoporous ZnS core/shell particles for efficient

More information

P. Lambrev October 10, 2018

P. 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 information

TIME-RESOLVED OPTICAL SPECTROSCOPY

TIME-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 information

The photoluminescent graphene oxide serves as an acceptor rather. than a donor in the fluorescence resonance energy transfer pair of

The photoluminescent graphene oxide serves as an acceptor rather. than a donor in the fluorescence resonance energy transfer pair of Supplementary Material (ESI) for Chemical Communications This journal is (c) The Royal Society of Chemistry 20XX The photoluminescent graphene oxide serves as an acceptor rather than a donor in the fluorescence

More information

Selected measurements with FluoTime 300

Selected measurements with FluoTime 300 Selected measurements with FluoTime 300 Sebastian Tannert, Peter Kapusta, Felix Koberling, Manoel Veiga, Steffen Rüttinger Uwe Ortmann, Matthias Patting, Marcus Sackrow, Michael Wahl, Rainer Erdmann 12th

More information

Signal and Noise Modeling in Confocal Laser Scanning Fluorescence Microscopy

Signal and Noise Modeling in Confocal Laser Scanning Fluorescence Microscopy Signal and Noise Modeling in Confocal Laser Scanning Fluorescence Microscopy Gerlind Herberich 1, Reinhard Windoffer 2, Rudolf E. Leube 2, and Til Aach 1 1 Institute of Imaging and Computer Vision, RWTH

More information

Ultrafast 2D Spectroscopy of Photosynthetic Light-Harvesting Complexes

Ultrafast 2D Spectroscopy of Photosynthetic Light-Harvesting Complexes Ultrafast 2D Spectroscopy of Photosynthetic Light-Harvesting Complexes PETAR LAMBREV PREAMBLE LASERS IN LIFE SCIENCE LASERS IN MEDICINE AND LIFE SCIENCE, SZEGED 2017 2 Preamble LASERS IN MEDICINE AND LIFE

More information

Chemistry Instrumental Analysis Lecture 17. Chem 4631

Chemistry Instrumental Analysis Lecture 17. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 17 Introduction to Optical Atomic Spectrometry From molecular to elemental analysis there are three major techniques used for elemental analysis: Optical spectrometry

More information