Light gathering Power: Magnification with eyepiece:

Similar documents
An Introduction to CCDs. The basic principles of CCD Imaging is explained.

Reflectors vs. Refractors

Charged-Coupled Devices

The Charge-Coupled Device. Many overheads courtesy of Simon Tulloch

Astronomical Cameras

Charge-Coupled Device (CCD) Detectors pixel silicon chip electronics cryogenics

Properties of a Detector

Where detectors are used in science & technology

Introduction to CCD camera

Lecture 15: Fraunhofer diffraction by a circular aperture

Digital Imaging Rochester Institute of Technology

Charge Coupled Devices. C. A. Griffith, Class Notes, PTYS 521, 2016 Not for distribution.

Based on lectures by Bernhard Brandl

Sharpness, Resolution and Interpolation

Photons and solid state detection

Three Ways to Detect Light. We now establish terminology for photon detectors:

Exercise 8: Interference and diffraction

CCDS. Lesson I. Wednesday, August 29, 12

CCD Characteristics Lab

CCD Analogy BUCKETS (PIXELS) HORIZONTAL CONVEYOR BELT (SERIAL REGISTER) VERTICAL CONVEYOR BELTS (CCD COLUMNS) RAIN (PHOTONS)

The New. Astronomy. 2 Practical Focusing

Telescopes and their configurations. Quick review at the GO level

Ultra-high resolution 14,400 pixel trilinear color image sensor

Optical/IR Observational Astronomy Detectors II. David Buckley, SAAO

Three Ways to Detect Light. Following: Lord Rosse image of M33 vs. Hubble image demonstrate how critical detector technology is.

DESIGN NOTE: DIFFRACTION EFFECTS

There is a range of distances over which objects will be in focus; this is called the depth of field of the lens. Objects closer or farther are

Lecture 5. Telescopes (part II) and Detectors

Pocket Pumped Image Analysis Ivan Kotov Brookhaven National Laboratory

Astronomical Detectors. Lecture 3 Astronomy & Astrophysics Fall 2011

TAOS II: Three 88-Megapixel astronomy arrays of large area, backthinned, and low-noise CMOS sensors

PHYSICS. Chapter 35 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

Binocular and Scope Performance 57. Diffraction Effects

Why is There a Black Dot when Defocus = 1λ?

Properties of optical instruments. Projection optical systems

3/5/17. Detector Basics. Quantum Efficiency (QE) and Spectral Response. Quantum Efficiency (QE) and Spectral Response

Observational Astronomy

Telescope Basics by Keith Beadman

Introduction to CCDs. Thanks to Simon Tulloch

Detectors for microscopy - CCDs, APDs and PMTs. Antonia Göhler. Nov 2014

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

Astronomy 341 Fall 2012 Observational Astronomy Haverford College. CCD Terminology

Applications of Optics

Image Formation. Light from distant things. Geometrical optics. Pinhole camera. Chapter 36

Dynamic Range. Can I look at bright and faint things at the same time?

VII. IR Arrays & Readout VIII.CCDs & Readout. This lecture course follows the textbook Detection of

Detectors that cover a dynamic range of more than 1 million in several dimensions

Optical Receivers Theory and Operation

Fundamentals of CMOS Image Sensors

6.014 Recitation 1: Wireless Radio and Optical Links

The Imaging Chain in Optical Astronomy

The Imaging Chain in Optical Astronomy

Adaptive Optics for LIGO

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature:

X-ray Detectors: What are the Needs?

The Design and Construction of an Inexpensive CCD Camera for Astronomical Imaging

IV DETECTORS. Daguerrotype of the Moon, John W. Draper. March 26, 1840 New York

2013 LMIC Imaging Workshop. Sidney L. Shaw Technical Director. - Light and the Image - Detectors - Signal and Noise

Cameras CS / ECE 181B

a simple optical imager

DESIGNING AND IMPLEMENTING AN ADAPTIVE OPTICS SYSTEM FOR THE UH HOKU KE`A OBSERVATORY ABSTRACT

GPI INSTRUMENT PAGES

LE/ESSE Payload Design

Submillimeter Pupil-Plane Wavefront Sensing

How Does One Obtain Spectral/Imaging Information! "

Low Light Level CCD Performance and Issues

Observation Data. Optical Images

IT FR R TDI CCD Image Sensor

Cerro Tololo Inter-American Observatory. CHIRON manual. A. Tokovinin Version 2. May 25, 2011 (manual.pdf)

Charged Coupled Device (CCD) S.Vidhya

Chapter 3 Op,cal Instrumenta,on

Very short introduction to light microscopy and digital imaging

Lecture 20: Optical Tools for MEMS Imaging

,, Last First Initial UNIVERSITY OF CALIFORNIA AT BERKELEY DEPARTMENT OF PHYSICS PHYSICS 7C FALL SEMESTER 2008 LEROY T. KERTH

FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION

Copyright 2000 Society of Photo Instrumentation Engineers.

"Internet Telescope" Performance Requirements

Introduction to Electron Microscopy

Digital camera. Sensor. Memory card. Circuit board

Activity 1: Make a Digital Camera

Introduction. Cambridge University Press Handbook of CCD Astronomy: Second Edition Steve B. Howell Excerpt More information

Fiber Optic Communications

Chromatic X-Ray imaging with a fine pitch CdTe sensor coupled to a large area photon counting pixel ASIC

LECTURE 13 DIFFRACTION. Instructor: Kazumi Tolich

Chapter 25. Optical Instruments

Presented by Jerry Hubbell Lake of the Woods Observatory (MPC I24) President, Rappahannock Astronomy Club

Light Detectors (abbreviated version, sort of) Human Eye Phototubes PMTs CCD etc.

Technical Explanation for Displacement Sensors and Measurement Sensors

What an Observational Astronomer needs to know!

The new CMOS Tracking Camera used at the Zimmerwald Observatory

XMM OM Serendipitous Source Survey Catalogue (XMM-SUSS2.1)

ECEN 4606, UNDERGRADUATE OPTICS LAB

Lecture PowerPoint. Chapter 25 Physics: Principles with Applications, 6 th edition Giancoli

CHARGE-COUPLED DEVICE (CCD)

Components of Optical Instruments 1

You won t be able to measure the incident power precisely. The readout of the power would be lower than the real incident power.

Camera Selection Criteria. Richard Crisp May 25, 2011

Chapter 3 Op+cal Instrumenta+on

Single Sided and Double Sided Silicon MicroStrip Detector R&D

Subject headings: turbulence -- atmospheric effects --techniques: interferometric -- techniques: image processing

Transcription:

Telescopes

Light gathering Power: The amount of light that can be gathered by a telescope in a given amount of time: t 1 /t 2 = (D 2 /D 1 ) 2 The larger the diameter the smaller the amount of time. If you get to use a telescope that is 3 times the diameter, how much less time will it take to gather the same amount of flux? Magnification with eyepiece: Only useful for extended objects: mag = f scope /f eyepiece Typically 25 mm, 12.5 mm, and 6 mm. For a 1m focal length, magnifications are x40, x80, and x170 power.

Field of View: The angular area of the sky imaged on a CCD or viewed through the eyepiece The field of view is a function of the optics of the eyepiece itself and its magnification which is a function of the telescope focal length

F-ratio The ratio of the focal length to the aperture: f/ = f/d Telescopes with small focal lengths (e.g.,f/2) are considered fast while ones with large focal lengths (e.g., f/8) are considered slow. Image Scale: CCDs have individual photoreceptor elements with sizes typically as: 9-30 µ = 0.009-0.030 mm at optical wavelengths image scale (arcsec/pixel) = (206.265 µ)/f µ is the pixel scale in microns and f is the focal length in mm Pixels should be about two times smaller than the resolution delivered by the optics + atmosphere

Campus Telescope The campus telescope is 0.8m in diameter and has a focal ratio of f/6 The CCD on the telescope has 4096x4096 pixels that are 9 µm in size What is the image scale of the CCD? What is the field of view of the CCD?

Nyquist sampling thereom: Optimal sampling requires ~2 pixels per resolution element. Sampling at finer resolution than does not yield more information. Sampling more coarsely means you are losing information

Limit of Resolution Diffraction makes the image of a point source into a central maximum surrounded by circular rings. Resolution: sinθ = 1.22 (λ/d) The position of the first null in the Airy disk

Resolution The angular separation of 2 objects such that the maximum of the first falls on the first minimum of the second. The atmosphere sets a limit on resolution because the waves do not all follow the same path through the atmosphere. This limitation is called seeing Adaptive optics move segments of the telescope mirror independently and in real time to account for these travel differences through the atmosphere and to, therefore, Improve the image beyond the usual seeing

What is a CCD Detector? This is basically the equivalent of a digital camera that we put on the back of a telescope CCDs are the detection device generally used in optical and infrared astronomy We want to count the number of photons that fall in each bin on a grid to get a measurement of the brightness of objects in the sky The image of the sky is recorded as a pattern of electric charge Image area Metal,ceramic or plastic package Serial register Connection pins Gold bond wires Bond pads Silicon chip On-chip amplifier

How do we count photons in each bin? A photon is absorbed by the valence band of a silicon semiconductor moving the electron to the conduction band by the photoelectric effect Photons with wavelengths longer than ~1.2 µm don t have enough energy to push the electron beyond the band gap Impurities in the silicon make the holes migrate away from the positive gate when biased with a positive voltage The full well capacity is the max. number of electrons that can be stored before electrons and holes recombine Increasing energy Conduction Band Valence Band 1.26eV Hole Electron

How do we count photons in each bin? To read the pixels the voltages are varied so that the electrons are shifted by columns and rows into a readout register The number of electrons are then converted to voltages plus a small bias offset (amplification) This voltage is sent to an A/D converter (analog-to-digital) which computes that voltage to a number, the maximum value of which is defined by the number of bits for the device (12, 14, or 16 bits give 4096, 16384, and 65536 respectively)

Photoelectric effect causes electrons to move from one band to the other in the silicon crystal Increasing energy Conduction Band Valence Band 1.26eV Hole Electron

http://spiff.rit.edu/classes/phys445/lectures/ ccd1/ccd_anim.gif

The image area is positioned at the focal plane of the telescope

Every third electrode is connected together making a pixel. Wires running down the edge of the chip make the connection. Channel stops keep charge from moving between columns.

CCD Characteristics http://www-kpno.kpno.noao.edu/ccdchar/ CCDspec/RNvsGain.html