CCDs. CCDs—the good (+)  Linear response  photometry is “simple” +High efficiency, compared to other detectors +Sensitive to many wavelengths +2-D arrays.

Slides:



Advertisements
Similar presentations
Institute for Gravitational Research
Advertisements

Charge Couple Devices Charge Couple Devices, or CCDs operate in the charge domain, rather than the current domain, which speeds up their response time.
By Kevin Saunders.  tml tml.
Area Detectors Like film can detect position Like scintillation detector can measure intensity With modern computers can assign hkl from unaligned crystal.
Using a DSLR to Study Variable Stars. Canon 450D - linear over a magnitude using RAW images with a specific setting.
Digital Camera Essential Elements Part 1 Sept
Digital Radiography.
Kamera CCD Astronomi (2) AS3100 Lab. Astronomi Dasar I Prodi Astronomi 2007/2008 B. Dermawan.
Optical Astronomy Imaging Chain: Telescopes & CCDs.
CCDs in Astronomy History of CCDs How do CCDs work ?
Astronomical Detectors
Echelle spectra reduction with IRAF*
Charge Coupled Device (CCD)
High Energy Outreach An Introduction to Photometry for Educators and Beginning Astrophysicists Written and Created by: Tim Graves and the Sonoma State.
06/02/2008CCDs1 Charge Coupled Device M.Umar Javed M.Umar Javed.
Basic Principles of CCD Imaging in Astronomy Based on Slides by Simon Tulloch available from
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.
Methods Eye (visible window) Camera – film Camera – CCD (Digital) Collecting Electromagnetic Information.
14.2 Data Capture Digital Imaging using CCDs. Capacitors  A capacitor is a device that stores charge.  Def’n of Capacitance - The ratio of the charge.
Digital Technology 14.2 Data capture; Digital imaging using charge-coupled devices (CCDs)
Signal vs Noise: Image Calibration First… some terminology:  Light Frame: The individual pictures you take of your target.  Dark Frame: An image taken.
CCD Detectors in High- Resolution Biology Jian Guan
UVP BioImaging Systems Solutions for the Science of Life Digital CCD Cameras 101.
Overview of Scientific Imaging using CCD Arrays Jaal Ghandhi Mechanical Engineering Univ. of Wisconsin-Madison.
Your Observing Challenge: White Dwarfs in Open Star Clusters.
Digital Photography Fundamentals Rule One - all digital cameras capture information at 72 dots per inch (DPI) regardless of their total pixel count and.
Camera Functions Using Your Digital Camera. 1. What happens when you press the shutter button down halfway? What does macro mode allow you to do? Pressing.
In Three Parts. » Know ˃What exposure is ˃What affects exposure » Show ˃Define Exposure ˃Identify an over, under, and perfectly exposed photo ˃Use exposure.
 The CCD sensor was invented in 1969 by Willard Boyle and George E. Smith of AT&T Bell Labs.  Originally intended as a memory device.
Different sources of noise in EM-CCD cameras
Intro to Photography. Types of Cameras Single Lens Reflex A single-lens reflex (SLR) camera typically uses a mirror and prism system that allows the photographer.
Detecting Electrons: CCD vs Film Practical CryoEM Course July 26, 2005 Christopher Booth.
Astronomical Instrumentation Often, astronomers use additional optics between the telescope optics and their detectors. This is called the instrumentation.
FASEP Presents What is the difference between PSD and CCD sensor technology?
Memorandam of the discussion on FMOS observations and data kicked off by Ian Lewis Masayuki Akiyama 14 January 2004 FMOS Science Workshop.
AST3 detector properties
The CCD detector Sami Dib, Max-Planck-Institute for Astronomy, Heidelberg Jean Surdej, Institut d’Astrophysique et de Géophysique, Liège modified by Martin.
Introduction to Optical Detectors: Plates, PMTs and CCDs Matt A. Wood Florida Institute of Technology Dept of Physics and Space Sciences.
CCD Detectors CCD=“charge coupled device” Readout method:
Telescope Guiding with a HyViSI H2RG Used in Guide Mode Lance Simms Detectors for Astronomy /2/09.
10/26/20151 Observational Astrophysics I Astronomical detectors Kitchin pp
Asteroids Image Calibration and Setup Making a Lightcurve What is a Lightcurve? Cole Cook  Physics and Astronomy  University of Wisconsin-Eau Claire.
The Exposure Trio Aperture, Shutter Speed, and ISO.
CDE CDR, September 14, 2004 Your Position, Your Name 1 GATS AIM Science Team Meeting January 23-24, 2007 CIPS Calibration Review, Aimee Merkel, Bill McClintock.
Astronomical Institute University of Bern 31th IADC Meeting, April , 2013, ESOC, Darmstadt, Germany Improved Space Object Observation Techniques.
Observational Astrophysics I
CCD Imaging in amateur & professional astronomy What is a CCD?
TIPS - Oct 13, 2005 M. Sirianni Temperature change for ACS CCDs: initial study on scientific performance M. Sirianni, T. Wheeler, C.Cox, M. Mutchler, A.
Physics 114: Lecture 8 Measuring Noise in Real Data Dale E. Gary NJIT Physics Department.
14 January Observational Astronomy SPECTROSCOPIC data reduction Piskunov & Valenti 2002, A&A 385, 1095.
Charge-Coupled Devices Astrophysics Lesson 5. Learning Objectives Describe and explain the structure and operation of the charge coupled device State.
CCD Image Processing: Issues & Solutions. CCDs: noise sources dark current –signal from unexposed CCD read noise –uncertainty in counting electrons in.
DIGITAL RADIOGRAPHY.
In conclusion the intensity level of the CCD is linear up to the saturation limit, but there is a spilling of charges well before the saturation if.
Comparison of a CCD and the Vanilla CMOS APS for Soft X-ray Diffraction Graeme Stewart a, R. Bates a, A. Blue a, A. Clark c, S. Dhesi b, D. Maneuski a,
1 Topic Report Photodetector and CCD Tuan-Shu Ho.
INSTALLING AUDIO VIDEO CCTV SYSTEM 3. Explain the principles of camera placement monitoring By Sarbini S.Pd, SMK Muh 3 Yogyakarta)
Announcements After a short lecture we will adjourn to the Farm. Tonight is a Dark Sky make-up night. Class will meet Thursday night. If clear: meet at.
Introduction to Camera
“ Who will I blame my mistakes on. ” Dr
Relative Spectral Response and Flat Fields with Internal Calibration Lamps Luisa M. Lara IAA-CSIC Granada (SPAIN)
Charge Transfer Efficiency of Charge Coupled Device
CCD Image Processing …okay, I’ve got a bunch of .fits files, now what?
What I Need To Know About Operating A Camera
Charge Coupled Device Advantages
Detector Basics The purpose of any detector is to record the light collected by the telescope. All detectors transform the incident radiation into a some.
Intro to CCD Imaging Joe Roberts
Module HET606: Tools of Modern Astronomy
Photometric Analysis of Asteroids
Presentation transcript:

CCDs

CCDs—the good (+)  Linear response  photometry is “simple” +High efficiency, compared to other detectors +Sensitive to many wavelengths +2-D arrays possible in large formats +Can be shuttered, or “frame transfer” +High dynamic range (i.e., contrast)

CCDs—the bad (-) -Read noise: electrons not transferred perfectly (but pretty good) -Dark current –Temperature sensitive –Coolant/cooler? –Accumulates condensates (i.e., gook)

CCDs—the ugly Electron wells are finite and imperfect Leakage Saturation blooms Cosmic rays Pixel-to-pixel variation Age-dependent

Linearity (good) Expose to more light, get more electrons—linearly increasing Photometry made easier because signal can be expressed as (data numbers per second), unambiguously Makes comparison of different images easier

Linearity—one more thing Allows straightforward normalization and addition of images

Quantum efficiency Generally, higher than most other detection schemes—that’s good (especially photographic film) Wavelength dependent

Exposure metering Can be shuttered, or Can be “frame transfer”

Dark current Thermal motions of electrons produces a spurious signal that is not due to incident light Temperature-dependent, so most cameras are cooled The level of spurious signal is still linear w.r.t. temperature and exposure duration, so can be subtracted from the “real” images Examples…

Temperature dependence of dark current Q: Why’d we do this? A: The camera is cold, so any residue floating around in the telescope will condense on the CCD. Yuck! Therefore, periodic “bakeouts” to remove gook from the CCD.

Pixel-to-pixel variation Differences in charge transfer efficiency Differences in well depth (less important) Shorted pixels continuously leaking charge Age-dependent (see example) Compensate via flat fielding and subtraction of dark frames

CCD aging

Pixel saturation Potential wells have a finite depth, can hold only a finite number of electrons 100,000 to 200,000 electrons is typical limit When the well is full, where do those electrons go? They spill over into neighboring pixels Example…

Composite Example 1. Raw data

Composite Example 2. Subtract dark frame 3. Correct for stray light (no true flat fields for X-rays) 4. Co-register the cleaned images, normalize for exposure time 5. Replace saturated parts of “long” exposure with pixels from “short” exposure, to yield the final product…

Why composite? Trivial answer: It looks nice. Less trivial answer: Enhanced dynamic range. You get to see the faint parts and the brighter parts, with quantitative accuracy.

Troublesome Aesthetically unpleasant Confuse morphology of imaged object How to remove? One more thing: cosmic rays