High Throughput Microscopy

Slides:



Advertisements
Similar presentations
School of Biomedical Engineering, Science & Health Systems V 1.0 SD [040227] NANOSCALE COHERENCE TECHNIQUES FOR X-RAY IMAGING PROGRAM.
Advertisements

Bio-optics & Microscopy (MEDS 6450) 11/16/2010 Presented by: Mathilde Bonnemasison Leia Shuhaibar Steve Pirnie Ronghua (Ronnie) Yang Neil MAA, Juskaitis.
Results of Acceptance Tests of Hyper Suprime-Cam CCDs Yukiko Kamata, Hidehiko Nakaya, Satoshi Miyazaki National Astronomical Observatory of Japan.
Laser Speckle Extensometer ME 53
Lytro The first light field camera for the consumer market
Superconducting rf test facility STF Mechanical grinding development Ken Watanabe ( KEK ) ILWS08 in Chicago 17-Nov-08.
Kawada Industries Inc. has introduced the HRP-2P for Robodex 2002
Light Fields PROPERTIES AND APPLICATIONS. Outline  What are light fields  Acquisition of light fields  from a 3D scene  from a real world scene 
Microscopy with lens arrays
Microlens Array Light Trapping CdTe Solar Cells for use in Concentrator Photovoltaics Student: Patrick Margavio, Mechanical and Aerospace EngineeringFaculty.
© 2010 Adobe Systems Incorporated. All Rights Reserved. T. Georgiev, Adobe Systems A. Lumsdaine, Indiana University The Multi-Focus Plenoptic Camera.
ABRF meeting 09 Light Microscopy Research Group. Why are there no standards? Imaging was largely an ultrastructure tool Digital imaging only common in.
Comparison and Implications of Three Optical Microscopy Data Acquisition Modalities James Butler Ph.D. Nikon Instruments, Inc. Widefield Fluorescence Confocal.
Precision Tilt and Radius of Curvature Sensor Using Double-Pass AOM Kyuman Cho Department of Physics Sogang University.
Optical Diagnostics Hg_jet_meeting, Thomas Tsang tight environment high radiation area non-serviceable area passive components optics only, no.
Micro PIV  An optical diagnostic technique for microfluidics (e.g. MEMS, biological tissues, inkjet printer head) Requirements: Measure instantaneously.
CS485/685 Computer Vision Prof. George Bebis
Linear View Synthesis Using a Dimensionality Gap Light Field Prior
Light field microscopy Marc Levoy, Ren Ng, Andrew Adams Matthew Footer, Mark Horowitz Stanford Computer Graphics Laboratory.
LGS diagnostics Results (so far) Anna Moore, Hal Petrie LGS facility meeting 30 th Jan 2007.
Optical Diagnostics Thomas Tsang tight environment high radiation area non-serviceable area passive components optics only, no active electronics back.
Light field photography and microscopy Marc Levoy Computer Science Department Stanford University.
Evaluate. Review: Light Volume Control: 1. f stops are light transmission standards: f 8 transmits the same amount of light for any lens. 2.Lenses can.
Basic Principles of Imaging and Photometry Lecture #2 Thanks to Shree Nayar, Ravi Ramamoorthi, Pat Hanrahan.
Light Field. Modeling a desktop Image Based Rendering  Fast Realistic Rendering without 3D models.
Image formation & Geometrical Transforms Francisco Gómez J MMS U. Central y UJTL.
Light field photography and videography Marc Levoy Computer Science Department Stanford University.
Eusoballoon optics characterisation Camille Catalano and the Toulouse team Test configuration Calibration of the beam Exploration of the focal plan.
1 CS6825: Image Formation How are images created. How are images created.
TIRF Total Internal Reflection Fluorescence Microscopy specialized fluorescence microscopy technique specifically images a very thin optical section (50-250nm)
SPECTROSCOPIC DIAGNOSTIC COMPLEX FOR STUDYING PULSED TOKAMAK PLASMA Yu. Golubovskii, Yu. Ionikh, A. Mestchanov, V. Milenin, I. Porokhova, N. Timofeev Saint-Petersburg.
Particle Image Velocimetry (PIV) Introduction
Comparing Regular Film to Digital Photography
Dynamically Reparameterized Light Fields Aaron Isaksen, Leonard McMillan (MIT), Steven Gortler (Harvard) Siggraph 2000 Presented by Orion Sky Lawlor cs497yzy.
October 30th, 2007High Average Power Laser Program Workshop 1 Long lifetime optical coatings for 248 nm: development and testing Presented by: Tom Lehecka.
Characterizing Lenslet Arrays for the Keck Adaptive Optics System Laboratory for Adaptive optics (LAO) UC Santa Cruz Name: Abubakarr Bah Home Institution:
1 Palomar Tomograph V. Velur 1, B. Platt 2, M. Britton 1, R. Dekany 1 1 Caltech Optical Observatories, California Institute of Technology 2 Interferometry.
Zone Plate Testing at 1-BM-B Preliminary Results Michael J. Wojcik, Shashidhara Marathe, Naresh Gandhi Kujala,
M. Zamfirescu, M. Ulmeanu, F. Jipa, O. Cretu, A. Moldovan, G. Epurescu, M. Dinescu, R. Dabu National Institute for Laser Plasma and Radiation Physics,
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
Intelligent Vision Systems Image Geometry and Acquisition ENT 496 Ms. HEMA C.R. Lecture 2.
1 2. Focusing Microscopy Object placed close to secondary source: => strong magnification The smaller the focus, the sharper the image! Spectroscopy, tomography.
Digital two photon microscopy for multiple fast signals acquisition Laboratory of Advanced Biological Spectroscopy (L.A.B.S.) University of Milan - Bicocca.
Miysaka Lab. Keisuke Yamada Alexandros Pertsinidis, Yunxiang Zhang & Steven Chu.
Miyasaka Lab. Ikegami Takahiro 100nm Ke Xu, H. P. Babcock, X. Zhuang, Nature Methods, 2012, 9, 185–188. Sub-diffraction limited point spread function achieved.
DIGITAL CAMERAS Prof Oakes. Overview Camera history Digital Cameras/Digital Images Image Capture Image Display Frame Rate Progressive and Interlaced scans.
Arbitrary and Dynamic Patterning in a Programmable Array Microscope
Presented by Darsen Lu (3/19/2007)
Quiz (2/20/08, Chpt 3, ECB) 1. A chemical process where there is a net gain of electrons is called _______________. A chemical process where there is a.
Intelligent Vision Systems Image Geometry and Acquisition ENT 496 Ms. HEMA C.R. Lecture 2.
Camera LENSES, APERTURE AND DEPTH OF FIELD. Camera Lenses Wide angle lenses distort the image so that extreme wide angle can look like its convex such.
Optical Diagnostics Thomas Tsang tight environment high radiation area non-serviceable area passive components optics only, no active electronics transmit.
N A S A G O D D A R D S P A C E F L I G H T C E N T E R I n s t r u m e n t S y n t h e s i s a n d A n a l y s i s L a b o r a t o r y APS Formation Sensor.
1 BROOKHAVEN SCIENCE ASSOCIATES Vibrations effect on 1nm focussing K. Evans-Lutterodt NSLS-II VTG Januaury
Auto-stereoscopic Light-Field Display By: Jesus Caban George Landon.
Date of download: 5/27/2016 Copyright © 2016 SPIE. All rights reserved. (a) Schematic of the light path. The galvo scanners are mounted above periscopes.
Designing a Microscopy Experiment Kurt Thorn, PhD Director, Image from Susanne Rafelski, Marshall lab.
Date of download: 5/30/2016 Copyright © 2016 SPIE. All rights reserved. Working principle of the immersion schemes: (a) focusing in air, (b) focusing through.
Date of download: 5/30/2016 Copyright © 2016 SPIE. All rights reserved. Optical configuration. The function of a BFP imaging lens, added externally to.
Optics SOSI 2016 Matt Chalker
LIGHT BACKSCATTERING ANALYSIS of Textured Silicon SAMPLES
Extended Depth of Field For Long Distance Biometrics
Two-layer ultra-high density x-ray optical memory (X-ROM)
Jason K. King, Brian K. Canfield, Lloyd M. Davis and William H
Light-field Microscopy with a Consumer Light-field Camera Supplementary Material In order to demonstrate the light-field capability of our system as well.
Supported by NIH Grant EB
MFM setup. MFM setup. The excitation lasers are combined in a fiber through an acousto-optic tunable filter, collimated, reflected on a dichroic mirror.
Timed photon counter 5 ΔV 4 ΔV 3 ΔV 30 μm 2 ΔV ΔV Diameter 30 μm Pitch
Volume 110, Issue 4, Pages (February 2016)
Wide-field multiphoton imaging through scattering media without correction by Adrià Escobet-Montalbán, Roman Spesyvtsev, Mingzhou Chen, Wardiya Afshar.
Presentation transcript:

Scanning Microscopy with a Microlens Array 18 October, FiO 2011 Antony Orth and Kenneth Crozier

High Throughput Microscopy High throughput fluorescence imaging by scanning sample under widefield microscope. http://www.olympus.co.uk/microscopy/22_scan_R.htm#

What limits high throughput microscopy? Specs sheet for typical systems advertise ~1s per image. Camera sensor typically ~1Mpx, so throughput is ~1Mpx/s, far below the throughput available with digital cameras. Limiting factors: Motorized stages have small bandwidth. Scanning procedures (focusing, moving FOV) become temporally expensive. Motion blur/lighting. Can we alter optics to alleviate these problems? Break up imaging into small, parallelized fields of view. http://www.olympus.co.uk/microscopy/22_scan_R_Specifications.htm

Talk Outline Use of microlens arrays for fluorescence imaging Experimental setup Array fabrication and characterization Sample fluorescence images Large scale imaging example Image processing Summary and outlook

Experimental Setup Piezo scan Microlens focal length 40 μm Scan area: 20μm x 20μm Step size: 175nm Frame rate: 202 Hz Piezo scan Movie of microlens apertures as sample is scanned

Reflow Mold Microlens Array 1.3mm Lens array molded in optical adhesive (NOA 61, n=1.56) 100 x 100 microlens array Pitch: 55 μm Lens Diameter: 40 μm Lens Height: 15 μm

Focal Spot Characterization 0.8NA Microscope Objective 532 nm Laser FWHM = 790nm Microlens Array

Scanning Fluorescence Images 2μm, 5μm beads 3.6 μm 500nm beads FWHM = 645 nm 3.6 μm Rat femur tissue section

Large-Scale Imaging With Stitching 55 μm x 55 μm 0.8 mm 2μm beads

Large-Scale Imaging With Stitching Highest throughput so far: Frame rate: 202 Hz Sensor area: 256 x 256 pixels (0.065Mpx) Microlenses: 5000 Throughput: 1Mpx/s With optimal camera (IDT NR5-S2): Frame rate: 1000 Hz Sensor area: 2560 x 1920 pixels (4.9Mpx) Microlenses: > 1,000,000 Throughput: 1.2Gpx/s 55 μm x 55 μm 40μm 2μm beads

Light Field Parametrization (s,t) position on CCD maps to initial ray angle (u,v) is position in object space t s Image on CCD M. Levoy et al., J. Microscopy vol. 235 pt.2 2009 p.144

Image Reconstruction Tile red pixels for perspective view Tile sum of green pixels for full aperture view

Perspective Fly-Around Microlens Aperture Microlens Aperture Extracted Pixel 3.6 μm 3.6 μm

Perspective Fly-Around Microlens Aperture Extracted Pixel 3.6 μm

Summary & Outlook Demonstrated parallelized point scanning fluorescence microscopy with a microlens array Demonstrated pixel throughput comparable to commercial systems, but with small sensor size* Demonstrated viewpoint selection of scene *Throughput scales with sensor size: lots of room for speed increase. Next: imaging through coverslips – more involved microlens design

Light Field Capture Microlens apertures Tile aperture images u s v t

Reflow Molding Fabrication Pattern posts of photoresist (AZ-40XT) on silicon Place wafer on hot plate @125oC for 1 min. Resist melts, surface tension provides smooth lens surface PDMS PDMS NOA 61 Microscope slide Inverse mold in PDMS Replicate melted photoresist in optical adhesive (NOA 61) with UV cure Peel off PDMS, microlens array ready for use!

Setup Revisited Image on CCD