1 Correct Sampling. What is SAMPLING? Intensity [a.u.] 2 3456 X [µm] 1.

Slides:



Advertisements
Similar presentations
Bio-optics & Microscopy (MEDS 6450) 11/16/2010 Presented by: Mathilde Bonnemasison Leia Shuhaibar Steve Pirnie Ronghua (Ronnie) Yang Neil MAA, Juskaitis.
Advertisements

Topics Acoustic Optical Modulator Faster scanning methods Laser trapping Fluorescence lifetime imaging.
Digital Radiography.
Nick Beavers Project Manager Deconvolution from Andy Molnar Software Engineer.
Deconvolution of Laser Scanning Confocal Microscope Volumes: Empirical determination of the point spread function Eyal Bar-Kochba ENGN2500: Medical Imaging.
Medical Image Analysis Image Formation Figures come from the textbook: Medical Image Analysis, by Atam P. Dhawan, IEEE Press, 2003.
Dave Piston May 18, 2014 Optical Sectioning 2: Confocal Designs and “Pseudo-confocals” Outline 1.PMT detectors 2.Laser Scanning Design Features 3.Pseudo-confocals.
ABRF meeting 09 Light Microscopy Research Group. Why are there no standards? Imaging was largely an ultrastructure tool Digital imaging only common in.
ABSTRACT Fluorescence Confocal Microscopy (FCM) is nowadays one of the most important tools in biomedicine research. In fact, it makes possible to accurately.
Astronomical Detectors
Image-Pro Premier Basic Training Course
Comparison and Implications of Three Optical Microscopy Data Acquisition Modalities James Butler Ph.D. Nikon Instruments, Inc. Widefield Fluorescence Confocal.
1 Confocal Microscopy David Kelly November 2013 Handbook of Biological Confocal Microscopy. Ed. J. Pawley, Plenum Press Fundamentals of Light Microscopy.
Fluorescence microscopy – Principle and practical consideration Hiro Ohkura.
Preliminary Performance Measurements for Streak Camera with Large-Format Direct-Coupled CCD Readout* 15th Topical Conference on High-Temperature Plasma.
Short pulses in optical microscopy Ivan Scheblykin, Chemical Physics, LU Outline: Introduction to traditional optical microscopy based on single photon.
BMME 560 & BME 590I Medical Imaging: X-ray, CT, and Nuclear Methods X-ray Imaging Part 1.
Sampling, Aliasing, & Mipmaps
Micro PIV  An optical diagnostic technique for microfluidics (e.g. MEMS, biological tissues, inkjet printer head) Requirements: Measure instantaneously.
University of British Columbia CPSC 414 Computer Graphics © Tamara Munzner 1 Sampling Week 7, Fri 17 Oct 2003 p1 demos sampling.
FMRI: Biological Basis and Experiment Design Lecture 7: Gradients and k-space FFT examples –Sampling and aliasing Gradient Gradient echo K-space
Media Cybernetics Deconvolution Approaches and Challenges Jonathan Girroir
CIS 681 Distributed Ray Tracing. CIS 681 Anti-Aliasing Graphics as signal processing –Scene description: continuous signal –Sample –digital representation.
From CCD to EMCCD Scientific imaging for today’s microscopy.
CCD Image Processing: Issues & Solutions. Correction of Raw Image with Bias, Dark, Flat Images Flat Field Image Bias Image Output Image Dark Frame Raw.
Study of Protein Association by Fluorescence-based Methods Kristin Michalski UWM RET Intern In association with Professor Vali Raicu.
Digital Images The nature and acquisition of a digital image.
Content of the lecture Principles of confocal imaging. Different implementations/modes. Primer on multi-photon (MPH) and multi-harmonic (MHG) generation.
lecture 2, linear imaging systems Linear Imaging Systems Example: The Pinhole camera Outline  General goals, definitions  Linear Imaging Systems.
Detectors point count detectors linear position-sensitive detectors area detectors energy dispersive detectors point count detectors linear position-sensitive.
Overview of Scientific Imaging using CCD Arrays Jaal Ghandhi Mechanical Engineering Univ. of Wisconsin-Madison.
Quiz 10/04/14 1. Recently, it has been possible to increase the accuracy of locating a single fluorophore (see diagram). What factors are critical to how.
Detecting Electrons: CCD vs Film Practical CryoEM Course July 26, 2005 Christopher Booth.
Biophotonics lecture 23. November Last week: -Fluorescence microscopy in general, labeling, etc… -How to do optical sectioning and fill the missing.
Sampling theorem In order to accurately reconstruct a signal from a periodically sampled version of it, the sampling frequency must be at least twice the.
Optical Transfer Function
TIRF Total Internal Reflection Fluorescence Microscopy specialized fluorescence microscopy technique specifically images a very thin optical section (50-250nm)
IPC Friedrich-Schiller-Universität Jena 1 Reduction of out of focus light  Excitation light excites fluorescence more or less within the whole sample.
Lecture 4 The Principles of Confocal Microscopy: Components of the microscope. BMS “Introduction to Confocal Microscopy and Image Analysis” 1.
Cell nucleus GFP flow analysis from sequences of LSCFM images Isabel Rodrigues 1,2 and João Sanches 2,3
BMS 524: Lecture 3 Purdue University Cytometry Laboratories Lecture 4 The Principles of Confocal Microscopy: Components of the microscope. BMS “Introduction.
Biophotonics lecture 9. November Last time (Monday 7. November)  Review of Fourier Transforms (will be repeated in part today)  Contrast enhancing.
IPC Friedrich-Schiller-Universität Jena 1 From Wednesday, 9 November 2011 the weekly lectures will be every Wednesday, 8:30 Humboldtstr. 8, Seminar Room.
Tod R. Lauer (NOAO) July 19, 2010 The Formation of Astronomical Images Tod R. Lauer.
Biophotonics lecture 11. January Today: -Correct sampling in microscopy -Deconvolution techniques.
Digital Imaging. Digital image - definition Image = “a two-dimensional function, f(x,y), where x and y are spatial coordinates, and the amplitude of f.
Digital two photon microscopy for multiple fast signals acquisition Laboratory of Advanced Biological Spectroscopy (L.A.B.S.) University of Milan - Bicocca.
Using Multi-Element Detectors to Create Optimal Apertures in Confocal Microscopy This work was supported in part by CenSSIS, the Center for Subsurface.
Image Processing Basics. What are images? An image is a 2-d rectilinear array of pixels.
Arbitrary and Dynamic Patterning in a Programmable Array Microscope
Molecular Cell Biology Light Microscopy in Cell Biology Cooper Modified from a 2010 lecture by Richard McIntosh, University of Colorado.
Gholamreza Anbarjafari, PhD Video Lecturers on Digital Image Processing Digital Image Processing Spatial Aliasing and Image Enhancement.
Fluorescence Microscopy – Avoiding the Pitfalls Perkin-Elmer and McGill Imaging Facility Spinning Disk Confocal Workshop Tuesday May 29 th, 2007.
CCD Image Processing: Issues & Solutions. CCDs: noise sources dark current –signal from unexposed CCD read noise –uncertainty in counting electrons in.
Use Snell’s law to determine the angle of total internal reflection in the coverslip (without oil). Oil immersion objectives More light (no total internal.
Designing a Microscopy Experiment Kurt Thorn, PhD Director, Image from Susanne Rafelski, Marshall lab.
Digital Cameras in Microscopy Kurt Thorn Nikon Imaging QB3/UCSF.
FROM IMAGES TO ANSWERS Deconvolution of Widefield and Confocal images The growing role of deconvolution NE 2007.
Imaging.
Tytus Bernas Biological applications of image processing.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Prismless confocal total internal reflection (CTIR) microscope. 532-nm light is.
Reporter: Chien-Chung Tsai
Date of download: 7/5/2016 Copyright © 2016 SPIE. All rights reserved. Spatial light modulator-two-photon microscope (SLM-2PM) scheme: (1) Ti:Sa laser.
FMRI data acquisition.
Distributed Ray Tracing
Multiphoton Excitation Provides Optical Sections from Deeper within Scattering Specimens than Confocal Imaging  Victoria E. Centonze, John G. White  Biophysical.
Michael Blanchard Imaging Technician
Michael Blanchard Imaging Technician
Distributed Ray Tracing
Transition to the Dark Side
Presentation transcript:

1 Correct Sampling

What is SAMPLING? Intensity [a.u.] X [µm] 1

Aliasing … suppose it is a sine-wave Intensity [a.u.] There are many sine-waves, SAMPLED with the same measurements. Which is the correct one?

Aliasing … suppose it is a sine-wave … maybe we can know! Object: Microscope Image: Intensity Spatial Coordinate Intensity Spatial Coordinate

Aliasing in Fourier-space Fourier-transform of Image Intensity Aliased Frequencies ½ Sampling Frequency ½ Nyquist Frequencies

Pixel sensitivity Intensity [a.u.] X [µm] 1 Convolution of pixel form factor with sampling positions  Multiplication in Fourier-space  Reduced sensitivity at high spatial frequency

Optical Transfer Function |k x,y | [1/m] contrast Cut-off limit 0 1 rectange form-factor specimen sampled

Consequences of high sampling Confocal: high Zoom  more bleaching? No! if laser is dimmed or scan-speed adjusted  bad signal to noise ratio? Yes, but photon positions are only measured more accurately  binning still possible  high SNR. Readout noise is a problem at high spatial sampling (CCD)

9 Optimal Sampling?

Regular sampling Reciprocal  -Sampling Grid Real-space sampling: Multiplied in real space with band-limited information

Widefield Sampling  In-Plane sampling distance  Axial sampling distance

Confocal Sampling  In-Plane sampling distance (very small pinhole) else use widefield equation  Axial sampling distance

Confocal OTFs WF 1 AU 0.3 AU in-plane, in-focus OTF 1.4 NA Objective WF Limit

Hexagonal sampling Advantage: ~17% + less ‚almost empty‘ information collected + less readout-noise approximation in confocal; 3D: ABA, ABC stacking Reciprocal  -Sampling Grid Real-space sampling: Multiplied in real space with band-limited information

63× 1.4 NA Oil Objective (n=1.516), excitation at 488 nm, emission at 520 nm  eff = nm,  = deg widefield in-plane: d xy < 92.8 nm  maximal CCD pixelsize: 63×92.8 = 5.85 µm confocal in-plane:d xy < 54.9 nm widefield axial: d z < nm confocal axial: d z < nm Fluorescence Sampling Example

OTF is not zero but very small (e.g. confocal in-plane frequency) OTF is not zero but very small (e.g. confocal in-plane frequency) Object possesses no higher frequencies You are only interested in certain frequencies (e.g. in counting cells, serious under-sampling is acceptable) Reasons for Undersampling

Detector generates high-frequency noise? Detector generates high-frequency noise?  Measure this noise (e.g. dark exposure and 2D FFT)  Avoid aliasing by sampling above this noise frequency. Traps and Pitfalls

FFT of dark CCD exposure (2 µs)

If you need If you need high resolution or need to detect small samples  sample your image correctly along all dimensions  sample your image correctly along all dimensions Sampling Summary