Imaging System of a Bose-Einstein Condensation Experiment, and its Automation Fabien Lienhart U.C Berkeley Physics department Stamper-Kurn’s group August,

Slides:



Advertisements
Similar presentations
Observation of beam halo with corona graph
Advertisements

Computer Graphics (Spring 2008) COMS 4160, Lecture 6: Curves 1
QR Code Recognition Based On Image Processing
First Year Seminar: Strontium Project
W. M. Snow Physics Department Indiana University/IUCF EDM collab meeting Monitoring the Cold Neutron Beam (During Experiment) What to measure (fluence.
Chapter 15 Pretest Light and Refraction
Ultrafast XUV Coherent Diffractive Imaging Xunyou GE, CEA Saclay Director : Hamed Merdji.
Ultra-Cold Strontium Atoms in a Pyramidal Magneto-Optical Trap A.J. Barker 1, G. Lochead 2, D. Boddy 2, M. P. A. Jones 2 1 Ponteland High School, Newcastle,
Light and Optics 4.1 Mirrors form images by reflecting light. 4.2
Light = straight path An atom: emits light when an electron moves from a high to a low energy level. absorbs energy as its electrons move from a low.
Laser System for Atom Interferometry Andrew Chew.
Intelligent Systems Lab. Extrinsic Self Calibration of a Camera and a 3D Laser Range Finder from Natural Scenes Davide Scaramuzza, Ahad Harati, and Roland.
Currently: 3 year ( ) NSF-supported UF/IAP collaborative project "Methods and Instruments for High-Precision Characterization of LIGO Optical Components"
Optical Tweezers F scatt F grad 1. Velocity autocorrelation function from the Langevin model kinetic property property of equilibrium fluctuations For.
Imaging x-ray generation and Scattering Tabletop soft x-ray coherent imaging microscopes.
Optical Trapping of Atoms: Characterization and Optimization Charlie Fieseler University of Kentucky UW REU 2011 Subhadeep Gupta.
Optically Pumping Nuclear Magnetic Spin M.R.Ross, D.Morris, P.H. Bucksbaum, T. Chupp Physics Department, University of Michigan J. Taylor, N. Gershenfeld.
BSRT Optics Design BI Days 24 th November 2011 Aurélie Rabiller BE-BI-PM.
Operation of the S4700 FESEM
Lecture II Non dissipative traps Evaporative cooling Bose-Einstein condensation.
A mineral is a naturally occurring, inorganic solid that has a crystal structure and a definite chemical composition.
On the path to Bose-Einstein condensate (BEC) Basic concepts for achieving temperatures below 1 μK Author: Peter Ferjančič Mentors: Denis Arčon and Peter.
Laser System for Atom Interferometry Andrew Chew.
Set-up for Levy Flight of Photons in Resonant Atomic Vapor Danielle Citro (SUNY Oswego), Adailton Feliciano (UFPB), Martine Chevrollier (UFPB), Marcos.
Introducing the LEO 1400 Series
Colleen Downs Stephanie Pietromonaco Sanjay Talluri
Studying dipolar effects in degenerate quantum gases of chromium atoms G. Bismut 1, B. Pasquiou 1, Q. Beaufils 1, R. Chicireanu 2, T. Zanon 3, B. Laburthe-Tolra.
Comparison of Methods to Load a Mirror Magneto-Optical Trap Date: 14 May 2009 Author: C. Erin Savell Advisors: Dr. Shaffer and Arne Schwettmann Acknowledgement:
Image Formation. Input - Digital Images Intensity Images – encoding of light intensity Range Images – encoding of shape and distance They are both a 2-D.
Chapter 3: Image Restoration Geometric Transforms.
Effective lens aperture Deff
Profile Measurement of HSX Plasma Using Thomson Scattering K. Zhai, F.S.B. Anderson, J. Canik, K. Likin, K. J. Willis, D.T. Anderson, HSX Plasma Laboratory,
Light refraction.
Towards a finite ensemble of ultracold fermions Timo Ottenstein Max-Planck-Institute for Nuclear Physics Heidelberg 19th International IUPAP Conference.
BROOKHAVEN SCIENCE ASSOCIATES BIW ’ 06 Lepton Beam Emittance Instrumentation Igor Pinayev National Synchrotron Light Source BNL, Upton, NY.
Degenerate Quantum Gases manipulation on AtomChips Francesco Saverio Cataliotti.
December 4, 2014Computer Vision Lecture 22: Depth 1 Stereo Vision Comparing the similar triangles PMC l and p l LC l, we get: Similarly, for PNC r and.
High-performance Apparatus for Bose-Einstein Condensation of Rubidium Yoshio Torii Erik Streed Micah Boyd Gretchen Campbell Pavel Gorelik Dominik Schneble.
3 He Polarization Tests at UIUC Danielle Chandler David Howell UIUC.
1. How is the index of refraction calculated? How is light refracted as it speeds up? How is light refracted as it slows down? Index of refraction = speed.
Unit 5, Chapter 15 Integrated Science. Unit Five: Light and Optics 15.1 Seeing an Image 15.2 The Human Eye 15.3 Optical Technology Chapter 15 Optics.
Single atom manipulations Benoît Darquié, Silvia Bergamini, Junxiang Zhang, Antoine Browaeys and Philippe Grangier Laboratoire Charles Fabry de l'Institut.
Light scattering and atom amplification in a Bose- Einstein condensate March 25, 2004 Yoshio Torii Institute of Physics, University of Tokyo, Komaba Workshop.
FFAG-Workshop Dec Kumatori Japan Diagnostics for FFAG- accelerator Takahisa ITAHASHI Department of Physics, Osaka Univ. Toyonaka, Osaka, ,Japan.
Ch. 3: Geometric Camera Calibration
Prospects for ultracold metastable helium research: phase separation and BEC of fermionic molecules R. van Rooij, R.A. Rozendaal, I. Barmes & W. Vassen.
Doppler Free LASER Spectroscopy
I.Introduction II. System Design B.E. Unks, N. A. Proite, D. D. Yavuz University of Wisconsin – Madison The above figure shows a block diagram of the apparatus.
Laser Cooling and Trapping Magneto-Optical Traps (MOTs) Far Off Resonant Traps (FORTs) Nicholas Proite.
Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.
Hartmann Sensor for advanced gravitational wave interferometers
Jerzy Zachorowski M. Smoluchowski Institute of Physics, Jagiellonian University Nonlinear Spectroscopy of Cold Atoms, Preparations for the BEC Experiments.
Recent development of the Supersonic Gas-Jet Beam profile monitor
Measurements of Intense Proton Beams using Optical Transition Radiation Vic Scarpine, Fermilab TIPP 2011 Chicago, IL June 10, 2011.
ICONIC Training School, Freiburg, May 25th to 29th, 2010 Image processing for ion/electron imaging Dr. Lionel POISSON Laboratoire Francis PERRIN Saclay,
Status of physics analysis Fabrizio Cei On Behalf of the Physics Analysis Group PSI BVR presentation, February 9, /02/2015Fabrizio Cei1.
Status of RHIC Polarization Studies. Summary of Polarization Studies during Run09 Tune scans: – Nearby 0.7 – Near integer tune Polarization ramp measurement.
Light and Optics Part Three: Optics and Reflection.
Presentation on.  There are many methods for measuring of fiber structure. Such as:  The absorption of infrared radiation  Raman scattering of light.
MSE Radial Resolution with ‘Dirty’ Lens
Design for Embedded Image Processing on FPGAs
Light-Matter Interaction
José Manuel Iñesta José Martínez Sotoca Mateo Buendía
Summary of experience with Tevatron synchrotron light diagnostics
R.A.Melikian,YerPhI, , Zeuthen
Dan Mickelson Supervisor: Brett D. DePaola
Common Classification Tasks
Slab waveguide solution
Cold Atom project 12/02/2019.
Yu.N. Filatov, A.M. Kondratenko, M.A. Kondratenko
Presentation transcript:

Imaging System of a Bose-Einstein Condensation Experiment, and its Automation Fabien Lienhart U.C Berkeley Physics department Stamper-Kurn’s group August, 29th 2003

Plan Recent steps forward in the BEC experiment The Imaging System Automation of the imaging system: Visual Basic in WinView

Improvements and breakthroughs on the BEC experiment Ultrahigh Vacuum fixed MOT laser brighter and monomode Polarization Gradient cooling set First efficient magnetic trappings Next (last?) step…

Back to a Ultra-High Vacuum Problem: water leaking from a coil in the vacuum chamber  Open the chamber, fix the leak, close the chamber and Back to the vacuum Rotary pump Turbomolecular pump 1 week baking-out, monitored by a Rare Gas Analyser Gauge limit Torr

MOT Laser How things work…Problem Ugly beam which could be stronger Solutions Tapered amplifier: up to 300 mW Polarization maintaining optical fiber Results After the fiber: - 70 mW - monomode - good shape Up to 3 billion atoms trapped

Optimizing pg-cooling How things work… Easy case of lin –lin light Improvements Better beam shape Transition between the two pg-cooling steps found: optimization of T and N Results 30  K reached (Time of flight measurement)

First efficient magnetic trappings How Ioffe-Pritchard trap works… Results More than 600 million atoms trapped Lifetimes ranking from 15s (low Bias-Field) to 50s Adiabatic compression achieved

The Imaging System The constraints The experimental device Characterization of the system Results and future work

The Constraints Requirements of the system - Resonant light has to be used: 2-to-3 beam - Top-bottom axis - Keep the polarization of the light - Three very different magnifications: ~ ½, 5 and 16 The difficulties -Top-bottom axis is already crowded! -Only a few gold mirrors can be used at 45 o -Precise magnification needs to be known (quantitative imaging) and no way to place a fine object in the center of the trap!

The Experimental Device

Characterization of the System

Results Mag ½ Magnification:0.510  Resolution:80  m (close to Camera limit) Not to sensitive to the position of the MOT But sensitive to the angle of the last lens (distortion) Mag 5 Magnification:4.60  0.01 Resolution:8.7  m (close to diffraction limit) No distortion Resolution very sensitive to the position of the cloud Mag 16 Magnification:12.0  0.6 Resolution:14  m Position of the camera affects the magnification (.35/cm) without really changing the resolution Very sensitive to the angle of the last lens (distortion)

Automation of the Imaging System How WinView works Adding buttons with WinView Example of routine: rotating the images Future work

How WinView works WinView controls the camera Automating WinView: Using Macros Easy, but limited and buggy Or…

Adding buttons with Visual Basic 1. Write your script in VB Object Oriented Programming Classes which implement WinView 2. Transform it into a DLL 3. Register the DLL 4. A new icon should appear in WinView’s taskbar

The implemented buttons Close All - closes all the windows AutoSave - saves all the windows with the date QuickASCII - saves the image as a text AbsorptionLoop - cycles absorption pictures RotateFrame - rotates the pictures

Example: the rotation Problem Matrix index must be integer numbers Which is not the case after rotation Solutions Implementation of various algorithms 1. Closest neighbor 2. Gaussian interpolation 3. Bicubic interpolation 4.  -Spline method: 2 ideas leading to the best results

Idea 1 - Three-pass rotation

Idea 2 – Efficient 1D interpolation Cubic b-Spline Third orderBasisPiecewise polynomials Advantages - Normalized contributions - Compact support -> local control - Interpolated function is C 2 - Fast implementation: z-transform of the convolution gives an efficient recursive algorithm

Performances of the different methods A.Original B.Clothest neighbor C.Gaussian interpolation D.Bicubic interpolation  -Spline method

Conclusion Work achieved - Imaging system: characterization and limits of the system - WinView: add-ins In the next month -Imaging system: - way to easily calibrate the system - try different lens for mag ½ and 16 - WinView: gaussian fit of the profile of the cloud