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

Similar documents
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

single-molecule fluorescence resonance energy transfer

Fluorescence Resonance Energy Transfer (FRET) Microscopy

Single-Molecule Methods I - in vitro

Fluorescence Correlation

Optics and Spectroscopy

Petra Schwille and Elke Haustein Fluorescence Correlation Spectroscopy 1 TABLE OF CONTENTS 1 1. INTRODUCTION 2 2. EXPERIMENTAL REALIZATION 4

LABORATORY OF ELEMENTARY BIOPHYSICS

Modular scanning FCS quantifies receptor-ligand interactions in living multicellular organisms

Fluorescence fluctuation microscopy: FRAP and FCS

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

δf / δx = σ F (N 2 -N 1 ) ΔF~N 2 -N 1

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

Singlet. Fluorescence Spectroscopy * LUMO

I. Proteomics by Mass Spectrometry 1. What is an internal standard and what does it accomplish analytically?

Single Molecule Spectroscopy and Imaging

FROM LOCALIZATION TO INTERACTION

Co-localization, FRET

Introduction to FCS. Enrico Gratton. Laboratory for Fluorescence Dynamics Department of Biomedical Engineering University of California, Irvine

Fluorescence Workshop UMN Physics June 8-10, 2006 Quantum Yield and Polarization (1) Joachim Mueller

FLUORESCENCE MICROSCOPY TECHNIQUES PRACTICAL MANUAL FOR

Correlation Spectroscopy in Polymer Physics Methodenseminar im Wahlpflichtfach Basics diffusion and brownian motion correlations functions

Super Resolution Microscopy Structured Illumination

Fluorescence Polarization Anisotropy FPA

What the Einstein Relations Tell Us

Fluorescence (Notes 16)

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

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

Increasing your confidence Proving that data is single molecule. Chem 184 Lecture David Altman 5/27/08

CHEM Outline (Part 15) - Luminescence 2013

Single Emitter Detection with Fluorescence and Extinction Spectroscopy

Nonlinear Optics. Single-Molecule Microscopy Group. Physical Optics Maria Dienerowitz.

Solution set for EXAM IN TFY4265/FY8906 Biophysical microtechniques

Anti-Bunching from a Quantum Dot

Fluorescence polarisation, anisotropy FRAP

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

Lecture 5. Anisotropy decay/data analysis. Enrico Gratton

Laser Dissociation of Protonated PAHs

Laser Detection Techniques

Femtosecond laser applied to biophotonics. Prof. Cleber R. Mendonca

LASERS. Amplifiers: Broad-band communications (avoid down-conversion)

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

Chapter 6 Photoluminescence Spectroscopy

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

Lecture 7 FCS, Autocorrelation, PCH, Cross-correlation

Linear and nonlinear spectroscopy

Multiphoton microscopy

Application of IR Raman Spectroscopy

Chem 681: Student Seminar Series. Two-Photon Induced Fluorescence

Nonlinear Optics. Single-Molecule Microscopy Group. Physical Optics Maria Dienerowitz.

Laserphysik. Prof. Yong Lei & Dr. Yang Xu. Fachgebiet Angewandte Nanophysik, Institut für Physik

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

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful

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

Fluorescence Excitation and Emission Fundamentals

Using Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging

MODERN OPTICS. P47 Optics: Unit 9

Quantum and Nano Optics Laboratory. Jacob Begis Lab partners: Josh Rose, Edward Pei

Fluorescence 2009 update

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching

Chemistry 2. Molecular Photophysics

Fluorescence Spectroscopy

Lab 3 and 4: Single Photon Source

Chapter 15 Molecular Luminescence Spectrometry

Chapter 17: Fundamentals of Spectrophotometry

4. Molecular spectroscopy. Basel, 2008

FLUORESCENCE CORRELATION SPECTROSCOPY

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

Modern Optical Spectroscopy

Fluorescence and Nuclear Magnetic Resonance (NMR) Spectroscopy

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching

Challenges of Single Ion-Channel Biosensors

SUPPLEMENTARY INFORMATION

Generation of light Light sources

Survey on Laser Spectroscopic Techniques for Condensed Matter

Microfabricação em materiais poliméricos usando laser de femtossegundos

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

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

How DLS Works: Interference of Light

Measuring Colocalization within Fluorescence Microscopy Images

Solution structure and dynamics of biopolymers

Homework Due by 5PM September 20 (next class) Does everyone have a topic that has been approved by the faculty?

The Photon Counting Histogram (PCH)

Supplemental Materials and Methods

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy

CHAPTER 3 RESULTS AND DISCUSSION

This document contains the following supporting information: 1. Wide field scanning electron microscope image

Nanoscale confinement of photon and electron

SECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C7: BIOLOGICAL PHYSICS

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

Nano-optics. Topics: How do we image things on the nanoscale? How do we use nanofabrication for new optical devices? COSMOS 2006 Lecture 1

Excited State Processes

Optical Spectroscopy 1 1. Absorption spectroscopy (UV/vis)

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

INTERNATIONAL SCHOOL OF PHYSICS ENRICO FERMI MICROSCOPY APPLIED TO BIOPHOTONICS Varenna (Lake Como) - July 12th to 22nd 2011

The Photon Counting Histogram: Statistical Analysis of Single Molecule Populations

1. Transition dipole moment

Rb, which had been compressed to a density of 1013

Answers to questions on exam in laser-based combustion diagnostics on March 10, 2006

Technology, Techniques and Applications. Ric Allott Business Development Manager

Transcription:

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 excitation sources Multiphoton excitation-advantages/disadvantages Molecules inside cells Applications of MPE to the study of intracellular diffusion and biochemistry Photobleaching Recovery The concept of single molecule analysis Fluorescence Correlation Spectroscopy Fluorescence Cross-Correlation Spectroscopy

Resolution = 0.61λ / NA λ = wavelength of electromagnetic radiation

Spatial and Temporal Scales of Microscopy Temporal scales - picoseconds to months

What Limits Resolution in Microscopy? Numerical Aperture (NA) NA = n sin(θ), where n is the index of refraction and θ the half angle of the illumination cone. Rayleigh criterion: Resolution = 0.61λ / NA R = 1.22λ / (NA obj + NA cond ) n NA = 0.12 θ ~ 7 o Long working distances NA = 0.90 θ ~ 64 o Short working distances Destructive Interference

Characteristics of Light from Lasers Light Amplification by Stimulated Emission of Radiation

Fluorescence Stokes shift Fluorescein Isothiocyanate Following absorption, a number of vibrational levels of the excited state are populated. Molecules in these higher vibrational levels then relax to the lowest vibrational level of the excited state (vibrational relaxation). From the lowest vibrational level, there can be an emission of photon of lower energy (fluorescence)

What is Two Photon Excited Florescence? Two (or more) photons can interact simultaneously with a molecule adding their energies to produce an excitation equal to the sum of their individual energies. i.e. 2 red photons can = 1 blue photon 1 photon excitation Fluorescence 2 photon excitation Increasing Wavelength Increasing Energy

S 1 S 1 Two/(Multi)-Photon-Excitation virtual state ca. 10-15 s Single photon excitation (488 nm) Two photon excitation (900 nm) hν hν/2 Fluorescence hν f S 0 Idea: Simultaneous (10-15 s) absorption of n photons of wavelength Major advantage: Inherent spatial sectioning by I n - dependency of excitation probability. Excitation only in vicinity of focal spot Pulsed excitation = (100 fs, 80 MHz)

MPE is inherently localized to the focus of a high NA objective w 0 λ N. A. 10 0 10 5 1 μm The intensity (squared) declines from z (red arrows) as z -4 Calculated intensity of 740 nm light near focus of 1.2 NA objective

Pulsed laser excitation enhances two-photon absorption 1/f 10-8 s τ I t) I peak = = 10 fτ ( 5 I( t) 10-13 s Average Intensity I(t)

Two Photon Excitation (2PE) S 1 S 0 OPE A F S 1 S 0 A TPE F Advantages For intracellular work: 1. Small focal volume 2. Decreased photobleaching 3. Decreased phototoxicity 4. Increased viability 5. Increased focus depth For cross-correlation work: 6. Single laser line 7. No pinhole necessary 8. Good S/N ratio Disadvantages 1. Greater average Illumination intensities 2. Loss of resolution 3. High cost of pulse laser

Fluorescent Probes Uses of fluorescent molecules: 1. Labels - free dyes that may partition to a specific region of a cell or tissue, or fluorescent molecules that are bound to antibodies, receptor proteins or other biomolecules of interest. 2. Indicators dyes - the probes dynamically bind an ion (Ca ++, H +, Mg ++ ) and then change in either fluorescence intensity, emission or excitation spectrum. 3. Fluorescent proteins such as GFP, that are produced by the organism after the DNA for GFP, or more commonly a GFP fusion protein, is introduced into the cell.

Problems with Fluorescence - Photobleaching and Blinking Molecular fluorophores do not emit fluorescence photons indefinitely - they have a limited lifetime that depends on their chemical structure and the chemical environment they re in. For example, a single rhodamine molecule will emit 10 5-10 6 fluorescence photons before it becomes irreversibly photobleached. Some intrinsically fluorescent biological molecules such as tryptophan (UV excitation) emit, on average 1 photon before the molecule is irreversibly photodamaged. Reversible photobleaching (triplet state, other dark states) can also occur, which limits the photon yield per unit time since the molecule spends a percentage its time in an non-excitable state. (Example - egfp)

Fluorescent Probes molecules EGFP quantum dot silica nanoparticle (rhodamine) N NC CN N 1 nm 3 nm Single fluorophores 6 nm 50 nm Multiple fluorophores

Two Photon Laser Scanning Microscopy Coupled to Spectroscopy Techniques

Optical Methods Applied to Study Protein Dynamics 1. Two-Photon Fluorescence Photobleaching Recovery (TPFPR) 2. Two-Photon Fluorescence Correlation Spectroscopy (TPFCS) 3. Two-Photon Fluorescence Dual-Color Cross-Correlation (TPCCS) crosscorrelation

2 x = ndt n = 2, 4 or 6 for one, two and three dimensional diffusion

Diffusion Mapping of Alexa-488-Labeled Calmodulin in Neurons Using MPFPR Alexa-488-CaM in solution D(t) = 54 µm 2 /sec D(t) of faster diffusing species Species Soma Neurite 10 kd dextran 29.2 29.0 Alexa-488-CaM 28.5 22.3

D = kt 6πηr

Intracellular Diffusion: Far from Simple 500 nm

Applications of Single Molecule Approach to Biochemistry and Cell Biology Fluorescence Correlation Spec./Fluorescence Cross Correlation Spec.

How to detect single molecules? Low concentrations of fluor (<10-9 M) Small volume elements achieved through confocal or multiphoton optics bursts time I em Primary measurement parameter is signal fluctuations induced by: Diffusion of molecules through the open measurement volume Intramolecular dynamics which affect the fluorescence emission

Experimental Apparatus

Analysis of Fluorescence Fluctuations G( τ) = δf(t) δf(t + τ) F(t) 2 Temporal analysis of spontaneous fluorescence fluctuations -δf- Signal fluctuations are induced by: Diffusion of molecules through the open measurement volume Intramolecular dynamics which affect the fluorescence emission

Parameters Provided by Fluorescence Correlation Spectroscopy (FCS)

Examples for fast internal dynamics: flickering Molecules under study: GFP Green Fluorescent Protein) and its mutants: many of them show ph-dependent emission exc. 475nm 1.0 0.8 0.6 0.4 0.2 0.0 pk=5.7. 4 5 6 7 8 9 1011 1213 ph λ[nm] 480 500 520 540 560 580 600

FCS measurements of GFP-a ph sensor GFP blinks on a single molecule scale. Fast dynamics are strongly ph dependent reversible protonation 80 500 dark fraction 60 40 20 0 5 6 7 ph 8 9 10 11 400 300 200 100 0 time constant τ [μs] k f R O + H + R OH k b Protonation Diffusion A λ abs,deprot = 488nm λ abs,prot = 400 nm pk-5.7 AH GFP can be employed as single molecule ph meter!

What to determine by diffusion analysis? D = kt 6πη R h Analysis of molecular structure: diffusion properties depend on hydrodynamic radius 1.0 Correlation G(τ) 0.8 0.6 0.4 0.2 τ 1 τ 2 1.0 0.8 0.6 Y(t) 0.4 0.2 0.0 1E-3 0.01 0.1 1 10 100 1000 Analysis of association/dissociation processes by change in molecular mass 0.0 t [s] 0 1000 2000 3000 4000 k ass =10 4 M -1 s -1 to 10 6 M -1 s -1

Assessing molecular mobility in different cellular compartments 0.8 0.6 buffer cytosol membrane (lipid) membrane (IgE receptor) D=3*10-10 cm 2 /s G(τ) 0.4 Requirement: specific labeling of regions of interest Precision: 0.3 um in XY 1.0 um in Z fast 0.2 D=3*10-6 cm 2 /s 0.0 1E-3 0.01 0.1 1 10 100 1000 10000 τ [ms] slow Determination of molecular speed

Detection of single molecules in membranes + 2 μm + 1 μm ±0 μm -1 μm -2 μm 0.01 0.1 1 10 100 1000 time [ms] 0 2 4 6 8 10 time [s] Only labeled regions contribute to the measured signal

The viscosity of the membrane has been likened to that of olive oil, some 50-100 times that of water D kt = 6πηr

Diffusion in Membranes

Dual-color cross-correlation analysis FCCS Advantage: mobility independent analysis of molecular interactions D = kt 6πη R h RECALL R h ~ (MW) 1/3 Correlation G(τ) 1.0 0.8 0.6 0.4 0.2 0.0 1E-3 0.01 0.1 1 10 100 1000 Principle: only doubly labeled species contributes to cross-correlation signal Red channel: Blue channel: + + cross-c. G ij ( τ ) = δf() t δf ( t+ τ ) i F() t F () t i j j Denominator Numerator

Experimental setup for TPCCS Inherent overlap of excitation volumes Simplified alignment of detection volumes (no pinholes required) G(τ) 0.03 0.02 0.01 Auto Red Auto Green Cross Fit 0.00 1E-3 0.01 0.1 1 10 τ [ms]

Dual-color two-photon cross-correlation (TPCCS) Concept: Excitation of spectrally separable fluorophores with a single IR line Requirement: both dyes show similar emission on a single molecule scale emission η [khz/molecule] 16 14 12 10 8 6 4 2 0 Ideal: 830 nm, < 30mW Rhodamine Green Texas Red 740 760 780 800 820 840 860 880 900 λ [nm] % transmission/emission 100 80 60 40 20 0 (3) (4) (1) (2) (5) Emission bei λ ex =830 nm 450 500 550 600 650 700 λ [nm]

Analysis of DNA-DNA association G RB ( τ ) = RB BR [ V ( C + C )( C + C )] eff R C Diff RB B RB t 1 t 2 t 3 GCCGTCTCTGACTGCTGATGACTACTATCGTATAGTGCGG CGGCAGAGACTGACGACTACTGATGATAGCATATCACGCC Greater specificity for reaction product observation

Intracellular FCCS applications: The toxin system CTX-Cholera ST-Shigella Bacia et al., 2002, Biophy. J. System: Bacterial protein toxins entering the cell in a retrograde fashion Objective: to simultaneously study the endocytic trafficking of Cholera (red label) and Shiga (green label) Toxin

Comparing Endocytic Pathways for CTX and ST G(τ) 0.4 0.2 G(τ) 0.4 0.2 ST CTX Distinct autocorrelations, no cross-correlation: different pathways 0.0 1E-30.01 0.1 1 10 100 0.20 τ[ms] 0.0 1E-30.01 0.1 1 10 100 0.20 τ[ms] CTX-Cholera ST-Shigella G(τ) 0.15 0.10 0.05 G(τ) 0.15 0.10 0.05 CTX CTX Comparable autocorrelations, existing crosscorrelation: same pathway 0.00 1E-30.01 0.1 1 10 100 τ / ms 0.00 1E-30.01 0.1 1 10 100 τ / ms

FCCS reveals where the subunits dissociate (1) Cy-3 G(τ) (1) Cell membrane (2) τ[ms] G(τ) (3) Golgi τ[ms] Cy-5 (3) Dissociation of A and B 5 subunits required to induce toxicity of A (2) Endosomes Cross-correlation finally decays to zero in the Golgi G(τ) τ[ms]

Assessing Binding Ratios of CaM and CaMKII 1/G(0) = N : absolute particle number + EGTA + MgATP egfp-camkii N = 0.73 N = 0.73 cpms = 13.7 cpms = 12.5 Alexa 633CaM N = 130 N = 128 cpms = 3.6 cpms = 4.1 Cross-Correlation (KK) ~0 251.1% (KK/AK 2 ) KK n C20 n 130 = = AK2 C20 + n( n 1) C10 130 + n( n 1)0.73 For n = 1 -> KK = 100 % n = 2 -> KK = 198 % n= 3 -> KK = 296.7 % Therefore, experimental data means an average of 2.5 Alexa 633 CaMs are bound to 1 egfp-camkii.

Protein Signaling Analyzed with Cross-Correlation basal +10 mm Ca 2+ +200 μm EGTA 10 μm 1.0 0.8 +Ca 2+ +MgATP +Ca 2+ +EGTA 0.6 G(τ) 0.4 0.2 0.0 0.01 0.1 1 10 100 1000 τ (ms) Kim, S.A. et al, 2004 PNAS

Other Applications of MPE Uncaging of fluorescent compounds: inherent spatial localization provides excellent spatial selectivity for uncaging In vivo imaging over long time scales (months): e.g., watching the development of amyloid plaques develop over months in the brain of a living animal