Evanescent wave induced Time-resolved Fluorescence

Slides:



Advertisements
Similar presentations
Chapter 26 Geometrical Optics. Units of Chapter 26 The Reflection of Light Forming Images with a Plane Mirror Spherical Mirrors Ray Tracing and the Mirror.
Advertisements

Fluorophores bound to the specimen surface and those in the surrounding medium exist in an equilibrium state. When these molecules are excited and detected.
Announcements Homework for tomorrow… (Ch. 23, Probs. 11, 12, 15, & 48)
Surface Plasmon Spectroscopy Lokanathan Arcot Department of Forest Products Technology School of Chemical Technology Aalto University.
Geometrical Optics and Basic Imaging Light Paths of the Bright Field Microscope E. D. Salmon University of North Carolina at Chapel Hill.
Chemistry on Ultrafast and Ultrasmall Scales Trevor Smith Ken Ghiggino Paul Mulvaney School of Chemistry, University of Melbourne.
Fiber Optics Defining Characteristics: Numerical Aperture Spectral Transmission Diameter.
ENEE4821 Plane Wave in a Good Conductor. ENEE4822 Boundary Conditions at the Surface of a Good Conductor The field amplitude decays exponentially from.
Fiber Optics Defining Characteristics: Numerical Aperture Spectral Transmission Diameter.
C 2001 Wiley, Physics Cutnell & Johnson 5 th Ed. Fig. 27–10 THIN-FILM INTERFERENCE When light shines on a thin film of oil floating on a layer of water,
Methods: Single-Molecule Techniques Biochemistry 4000 Dr. Ute Kothe.
Evanescent fields Professor Viviana Vladutescu. What Everyone Needs to Know About Evanescent Fields Almost four hundred years ago, Newton used a prism.
Reflective losses quickly become significant Eugene Hecht, Optics, Addison-Wesley, Reading, MA, 1998.
P. Moghe, 125:583 1 Microscopy Techniques for Biomaterials and Cell Based Interfaces Professor Prabhas V. Moghe October 26, :583 Fall 2006.
6. Interference by thin films t No phase shift (if n 2 < n 1 ) Phase shift -_____ (if n 2 > n 1 ) If there is a very thin film of material – a few wavelengths.
Microscopy Techniques for Biomaterial Characterization: A Primer Prabhas V. Moghe Lecture 3 September 21, 1999 RU CBE 533 or BME 553; NJIT BME 698.
Physics 1502: Lecture 29 Today’s Agenda Announcements: –Midterm 2: Monday Nov. 16 … –Homework 08: due Friday Optics –Index of Refraction.
The Ray Vector A light ray can be defined by two co-ordinates: x in,  in x out,  out its position, x its slope,  Optical axis optical ray x  These.
Reflection and Refraction of Plane Waves
The Electromagnetic Field. Maxwell Equations Constitutive Equations.
6. Interference by thin films
The Hong Kong Polytechnic University Optics II----by Dr.H.Huang, Department of Applied Physics1 Light Waves Nature of Light: Light can be viewed as both.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 26 Physics, 4 th Edition James S. Walker.
7.6.c Students know light travels in straight lines if the medium it travels through does not change. 7.6.g Students know the angle of reflection of a.
SCPY152 General Physics II Lecture 1 Ray Optics
TIRF Total Internal Reflection Fluorescence Microscopy specialized fluorescence microscopy technique specifically images a very thin optical section (50-250nm)
Total Internal reflection Fluorescence Microscopy: Instrumentation and Applications in Cell biology.
3.18. Defects caused by reflections We have assumed that the paraxial approximation applies in that all rays make small angles with respect to the optical.
C H A P T E R 26 The Refraction of Light: Lenses and Optical Instruments.
Light wave Recall: Light must reflect off of an object before it can be used to see the object. A flat mirror is called a plane mirror. A plane mirror.
Discrete optics v.s. Integrated optics
GEOMETRIC OPTICS Light is a transverse wave made up of oscillating electric and magnetic fields. Click here to view EM wave!EM wave!
PHY138 – Waves, Lecture 7 Today’s overview The Ray Model of Light Reflection Refraction Total Internal Reflection Medical Fibrescopes Apparent Depth.
In describing the propagation of light as a wave we need to understand: wavefronts: a surface passing through points of a wave that have the same phase.
Surface Plasmon Resonance (SPR)
From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005) These PowerPoint color diagrams can only be used by.
In the absence of sources, the Maxwell equations in an infinite medium are.
Functional cellular imaging by light microscopy MICROSCOPIES.
Its now time to see the light…..  A lens is a curved transparent material that is smooth and regularly shaped so that when light strikes it, the light.
M Manser WAVES : Optics (t riple science) By the end of this presentation you should be able to: Identify the differences between converging and diverging.
Prisms, fibers, and reflective lenses
Mirrors.
According to Fresnel formula the angles  1of the incident wave,  2 of the reflected wave and  3 of the refracted wave are given by the equation : 
1 Refraction, the Snell law Light in geometric optics is discussed in rays and represented by a straight line with an arrow indicating the propagation.
Can you list out other applications of lenses?
Designing a Microscopy Experiment Kurt Thorn, PhD Director, Image from Susanne Rafelski, Marshall lab.
Date of download: 6/3/2016 Copyright © 2016 SPIE. All rights reserved. Lens L focuses 488 or 514nm of light from an argon-ion laser at the BFP of a 1.45.
Geometrical Optics.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Index-matching effect. Matching the index of refraction of the bead with the solution.
L3 Refraction Learning Objectives: Describe refraction.
Light. Light is a electromagnetic radiation - a form of energy. Light travels in a straight line. The direction in which light is travelling is known.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Prismless confocal total internal reflection (CTIR) microscope. 532-nm light is.
-Atmospheric Refraction -Total Internal Reflection
Date of download: 7/8/2016 Copyright © 2016 SPIE. All rights reserved. Through-the-objective TIRF creates the evanescent field on the aqueous side of the.
Geometrical Optics.
Refraction and Lenses.
A. WAVE OPTICS B. GEOMETRIC OPTICS Light Rays
6. Interference by thin films
Optics Kathy Geise April 2007
Fresnel's Equations for Reflection and Refraction
Announcements 1/25/12 Prayer
The Refraction of Light
New Turf for CFP/YFP FRET Imaging of Membrane Signaling Molecules
Evanescent Excitation and Emission in Fluorescence Microscopy
Reflection and Refraction
New Turf for CFP/YFP FRET Imaging of Membrane Signaling Molecules
6. Interference by thin films
Actin Dynamics at the Living Cell Submembrane Imaged by Total Internal Reflection Fluorescence Photobleaching  Susan E. Sund, Daniel Axelrod  Biophysical.
Volker Kiessling, Marta K. Domanska, Lukas K. Tamm  Biophysical Journal 
The Refraction of Light
Presentation transcript:

Evanescent wave induced Time-resolved Fluorescence Myoung Hee Lee

Can we see single fluorophores ? far field near field TIRF or TIRFM (Total Internal Reflection Fluorescence Microscopy)

Microspheres in TIR and far-field Fluorescence http://www.nikon.com

Time lapse Sequence of Protein Dynamics http://www.nikon.com

total internal reflection What is TIRF ? total internal reflection evanescent wave (EW) ~ a few hundreds nm this optical section thickness ~ 1/10 for confocal microscopy technique http://www.phys.virginia.edu/education/outreach/8thgradesol/InternalReflectionFrm.htm

What is TIRF ? Key advantage of TIRF Surface selectivity fluorophores Surface selectivity (Shallow penetration depth of EW) Not excited beyond the EW High Signal-to-Noise ratio http://motility.york.ac.uk/poster/tirfm.shtml

Induced Evanescent Wave What happens ? n 1 evanescent wave

Induced Evanescent Wave What happens ? n 1 d for 1D evanescent wave, plane wave

Decay length of Evanescent Wave 1 d for example, air/glass, 400nm excitation, d : about 57 nm

Induced Evanescent Wave http://www.nikon.com

Common Setups of TIRFM Setup with prism or with objective lens http://www.nikon.com

Two types of TIRFM Prism type objective lens type http://www.nikon.com

High numerical Aperture Objective TIRFM http://www.nikon.com

Time-Resolved TIRF study on polarity at a liquid/liquid interface Anal. Chem. 2001, 73, 2421-2428

Schematic diagram of a system for TIRF TCSPC Ti:sapphire laser 100 kHz, 200 fs Glan-laser prism IA : 80O R3809U-50 Anal. Chem. 2001, 73, 2421-2428

Coordinate system of anisotropy experiment X-Y plane is the plane of the interface Anal. Chem. 2001, 73, 2421-2428

Molecular structures of SRB, SR101 and AB1 Anal. Chem. 2001, 73, 2421-2428

Schematic diagram of water / oil interface - + - Oil - cyclohexane carbon tetrachloride tolene Chlorobenzene (CB) o-dichlorobenzene (DCB) 1,2-dichloroethane (DCE) oil Anal. Chem. 2001, 73, 2421-2428

Fluorescence decay curves of SRB nonradiative decay rate const. increases as solvent polarity increases means fast decay At a water/DCE interface (DCE : dichlorobenzene) (b) In water Single exponential function Anal. Chem. 2001, 73, 2421-2428

Photophysical parameters of SRB and Polarities at the water/oil interfaces Anal. Chem. 2001, 73, 2421-2428

Schematic illustrations of flat and rough interfaces At water/oil interface For low polarity of oil (CCl4 and toluene) : thin and flat interface (a) For high polarity of oil (DCB and DCE) : thin but rough interface (b) (for SRB, single exponential decay) Anal. Chem. 2001, 73, 2421-2428

Propagation of a ray in an optical fiber Appendix Propagation of a ray in an optical fiber dcot  z take time  d z : an additional distance for the time , The penetration of a ray undergoing total internal reflection (or Effective lateral shift of the ray) is known as the

What happens ? Appendix Propagation factor for the refracted wave x z Propagation factor for the refracted wave not propagated to the z axis propagated to the surface

D : transverse displacement Appendix Time-averaged normal component of the Poynting vector inside the surface d x z D purely imaginary D : transverse displacement

Appendix evanescent wave light source prism air