Creative Commons License Copyright © Michael Richmond. This work is licensed under a Creative Commons License.

Astronomical Imaging: Catching up to the 1950s

Michael Richmond
Apr 13, 2013

We live in a world full of electronic gadgets. Smartphones, big-screen television sets, GPS receivers. Every year, they seem to get bigger and better.

Most astronomers today, both professional and amateur, use electronic detectors to take astronomical images. Is there any doubt that our current cameras are bigger and better than any used by scientists decades ago?

YES, there is doubt.

Let me try to convince you that, if we choose one reasonable manner of measuring the quality of a detector, it is only now -- or, perhaps, in the past five years -- that modern electronic detectors have finally caught up to the good old photographic plate.


A brief history of astronomical detectors

For many tens of thousands of years, the only detector used by humans was the good old Mark I eyeball.

Image courtesy of

The eye is more than just a detector -- it includes all the optics you need, too!

Image courtesy of

The eye focuses light rays onto light-sensitive cells in the retina, along the back surface of the eyeball. When enough photons strike a set of these cells, a signal is sent through the optic nerves to the brain.

  quantum efficiency integrate? permanent? linear? ease of use size
Eye 6 % no no no simple 36 sq. mm

In the middle of the nineteenth century, chemists and artists figured out that it was possible to focus light onto a specially prepared film of material which could record the image permanently. The early photographic techniques had very low sensitivity to light -- requiring long exposure times to build up a good picture (that's why the people in early photographs are posed so stiffly). The first photograph of the Moon, a daguerreotype, required Henry Draper to expose the plate for 20 minutes!

Image courtesy of Greenwich Village History

As the decades passed, chemists developed materials which were much more sensitive to light, enabling photographers to take images with exposure times of one second or less. Special emulsions were developed for astrophotography which were especially sensitive to low light levels. Do you recognize any of these names?

Taken from "Kodak Scientific Imaging Products", Kodak Publication L-10, 1987.

Photography offered two big advantages over the human eye:

However, even the best photographic emulsions record only a tiny fraction of all the light that strikes them. Pay attention to the second of these graphs.

As you can see from the films which we are passing out to the audience now, another big advantage film offered to astronomers was its size: one could (with very careful fabrication techniques) spread photographic emulsion over very large areas, over a backing of glass (plates) or plastics (film). Opticians like Bernhard Schmidt designed special telescopes which could project sharp images covering wide areas of the sky onto large photographic plates.

Image courtesy of Wikipedia and Krzysztof ZajÄ…czkowski

You may recognize this particular Schmidt Telescope: it was used to create the Palomar Observatory Sky Survey in the 1950s and the Second Palomar Observatory Sky Survey in the 1980s.

This drawing by Russell Porter is copyright California Institute of Technology's Palomar Observatory.

  quantum efficiency integrate? permanent? linear? ease of use size
Eye 6 % no no no simple 36 sq. mm
Photograph 1 - 5 % yes yes no needs developing 122,000 sq. mm

In 1970, scientists at Bell Labs were thinking about ways to store information in solid-state memory. They came up with the idea of a silicon chip divided into an array of small regions, then moving electric charges into and out of the array. By varying voltages applied to small sections of the chip, the user could couple the charge to specific regions. These chips became known as charge coupled devices, or CCDs.

Image courtesy of yaochen992003's Flickr site

It turns out that silicon has many interesting properties: one is its ability to convert individual photons of light into individual electrons. People soon realized that with a little preparation, CCDs could be used to convert light into an image, and then to transfer that image digitally to a computer. Because the devices were novel and expensive, the first applications were in space: astronomers suggested using CCDs for the cameras aboard the Galileo mission to Jupiter, and on the orbiting telescope we now call the Hubble Space Telescope. As years passed, many companies started to fabricate CCDs for industrial applications and the prices dropped. Even ground-based astronomers -- at first professional, but then amateur -- were able to afford these new imaging devices.

   Q:  When did CCDs really take over in the 
       community of professional astronomers?

         A.   around 1970

         B.   around 1980

         C.   around 1990

Watch as the fraction of papers with the word photographic in the abstract slowly decreases ....

... while the fraction with CCD in the abstract increases.

These silicon-based detectors had two big advantages photographic film

The "sensitivity" part is easy to understand,

but what does the "linear" part mean? It means that if one exposes the detector for twice as many seconds, one OUGHT to record a signal twice as large.

  quantum efficiency integrate? permanent? linear? ease of use size
Eye 6 % no no no simple 36 sq. mm
Photograph 1 - 5 % yes yes no needs developing 122,000 sq. mm
CCD 70% yes mostly yes needs reduction 1,800 sq. mm

It's not the size that counts ...

You may have noticed that size is listed in the tables above. It might seem to be a simple matter -- a bigger detector will be able to measure light over a wider field, so bigger must mean better. Right?

Well, almost. What we really want is the ability to record as much fine detail as possible. If two detectors can distinguish details at the same physical scale, then, sure, the bigger one will capture more information. But what if they differ in the way they respond to light?

Consider the two detectors shown below. Detector A is twice as large as detector B.

     Q:  Which will record more information?

    Detector A                                         Detector B

Let's find out. Below are two pictures of the same region of the Moon, taken with the same optical setup, but two different detectors.

    Detector A                                         Detector B

Want to see the original image?

What really matters is a combination of the size of the detector AND the size of one of its resolution elements. A resolution element (sometimes called a "pixel") is simply the smallest region of the detector which can respond as a single unit to incoming light. We need to compute this combination:

                        physical size of detector (mm)
 number of "pixels"  =  ------------------------------
                        size of resolution element (mm)

Let's look at the CCD: a new camera for the WIYN 0.9-m telescope has a chip made by e2V, model 231-84. It is relatively large by current astronomical standards:

 physical size of detector (mm)        61.44 mm
 ------------------------------   =  ------------  =  4096 
 size of resolution element (mm)       0.015 mm

The chip is square, so the number of resolution elements is 4096 x 4096 = 16 million, if we round off a bit.

Now, photographic emulsion (like CCDs) comes in many varieties, each of which has somewhat different properties. The emulsions used in astronomical applications such as the Palomar Observatory Sky Surveys had relatively coarse grains. The smallest dark spot which forms in response to light consists of a small number of grains and is roughly 5 to 10 microns in diameter. If we adopt the larger size for our calculation, then a plate 14 inches on a side has

 physical size of detector (mm)       355.6   mm
 ------------------------------   =  ------------  =  35,560
 size of resolution element (mm)        0.010 mm

The number of resolution elements is 35,560 x 35,560 = 1.3 billion, if we round off a bit. That is nearly 100 times more information than the big CCD!

What about the human eye? How does it compare using this criterion? Well, there's good news and bad news.

The good news
The good news is that if one examines the retina, the "detector" portion of the human eye, there are many detection elements.
All the following can only be approximate values, since individual human eyes vary widely.

     physical size of detector (mm)        12     mm
     ------------------------------   =  ------------  =  6000
     size of resolution element (mm)        0.002 mm

Using this value, we would estimate the eye to contain roughly 6,000 x 6,000 = 36 million resolution elements, similar to a very large modern CCD.

The bad news
Alas, things aren't so rosy inside the human eye. To begin, the light-sensitive cells, both rods and cones, aren't evenly distributed. Each type is more concentrated near the center of the eye; the very central region, called the fovea, has a very high concentration of cones. When we need to see the fine detail in some area, we move our eyes so that that area falls on the fovea. As a consequence, rods are more sparsely placed in the outer regions of the retina, which make up most of its area.

Moreover, several rod cells will send their signals to a single neuron, especially in the outer regions of the retina. So, even though each rod cell may record the light which strikes it alone, the brain will receive a single signal which represents the mix of responses from a number of cells. This reduces the number of resolution elements considerably.

To get some idea for the change in visual acuity as a function of position on the retina, consider this pretty false-color picture of the Moon (red means "high altitude", blue means "low altitude").

Click on the image to activate eye-o-vision

The total number of axons in the optic nerve is roughly 1 million, which can serve as an estimate of the number of resolution elements in the eye. That's quite a bit smaller than one would expect from the analysis above, and it definitely moves the eye into third place in the "number of resolution elements" contest.

Putting it all together

We've seen that there are a number of factors by which one can compare astronomical detectors. Let's see if we can find a way to combine several of these factors and devise a single metric.

   You have exactly one hour to capture as much
   information about the Orion Nebula region
   as you can.  

The information we collect depends on

If we are interested in a small region of the sky -- say, the area around McNeil's Nebula -- then the CCD is a better choice. Compare these views taken with a LONG exposure on film (on the left) and a SHORT exposure on a CCD (on the right). In order to reach the same depth, we must expose the film for roughly 17 times longer.

Left: 48-inch Palomar Schmidt, 50-minutes on 103aE; Right: 36-inch WIYN, 5 minutes S2KB CCD in R

On the other hand, if we are interested in a wide area on the sky, film is a better choice. The picture above shows nearly the entire the entire CCD image; but it is only a small portion of the entire photographic plate.

A REALLY small portion of the entire photographic plate ...

In order to cover the same area on the sky with a CCD, we would need to take many more exposures, shifting the telescope a bit each time:

So, in the battle between a photographic plate and a single CCD chip, we must compare the longer exposure time for the plate against the multiple exposures required for the CCD. If we use the numbers from our table above , we can compute an overall efficiency for each detector: it's the size (large is better) multiplied by the sensitivity (again, large is better).

             photographic plate        single CCD

size           122,000 sq. mm          1,800 sq. mm

sensitivity      x   3 percent         x  70 percent


"efficiency"     3,600 sq. mm          1,260 sq. mm

Hmmm. By this measure, the photographic plate is the winner. Note that we haven't included the readout time for the CCD, which increases the time required for it to take multiple exposures.

Modern mosaic CCD cameras

Surprisingly enough, when it comes to recording large areas of the sky, the venerable photographic plate can be more efficient than one CCD.

Yes, yes, I've ignored the factors of linearity and dynamic range, which favor the CCD.

But -- what if we put several CCD chips into a single camera to create a mosaic?

One of the first mosaic cameras was created for the Sloan Digital Sky Survey (SDSS for short). The design was a bit unusual: the CCDs were arranged into 6 columns, each of which had a series of 5 chips with different filters. Instead of tracking the stars exactly, the SDSS telescope would move at a slightly non-sidereal rate in a carefully calculated direction; as a result, stars would drift slowly across the camera, along these columns. In less than ten minutes, the camera would collect an image of each object in the five filters, allowing scientists to measure the color of celestial objects.

name # of CCDs # of pixels area first* use
SDSS 30 126 million 72,600 sq. mm 1998

* first regular operation

The Canada-France-Hawaii Telescope (CFHT), built in 1979, has a mirror 3.6 meters in diameter. It sits atop Mauna Kea and is designed to perform well in the infrared as well as the optical. In 2003, astronomers installed a very large camera called MegaCAM in order to carry out large-scale surveys of the sky. You can examine the data collected by this instrument by visiting the CFHT Legacy Survey archive site. You can also browse the CFHT Deep Field #1 with your browser -- there are just too many pixels to show on the screen at once!

name # of CCDs # of pixels area first* use
SDSS 30 126 million 72,600 sq. mm 1998
MegaCAM 36 340 million 62,000 sq. mm 2003

* first regular operation

OmegaCAM is a 32-chip mosaic designed for use on the wide-field VLT Survey Telescope, a 2.6-m telescope in the mountains of Chile. Each of its chips has 2K-by-4K pixels, so the entire instrument contains 16K-by-16K = 268 megapixels. The total area of the camera is 260 x 260 mm, which translates into 1 x 1 degree on the sky.

name # of CCDs # of pixels area first* use
SDSS 30 126 million 72,600 sq. mm 1998
MegaCAM 36 340 million 62,000 sq. mm 2003
OmegaCAM 32 268 million 60,000 sq. mm 2011

* first regular operation

The final stop on our tour of mosaic CCD cameras is one which is still in its testing phase. Hyper-SuprimeCam -- which takes over for regular old SuprimeCam -- will sit at the focus of the Subaru 8.3-meter Telescope on Mauna Kea. By packing over 100 specially designed CCD chips together into an area over 2 feet wide, scientists will be able to cover a field of view roughly 1.5 degrees wide in a single shot.

name # of CCDs # of pixels area first* use
SDSS 30 126 million 72,600 sq. mm 1998
MegaCAM 36 340 million 62,000 sq. mm 2003
OmegaCAM 32 268 million 60,000 sq. mm 2011
Hyper-SuprimeCam 116 973 million 210,000 sq. mm 2013 (?)

* first regular operation

So, we have finally reached a point at which electronic detectors have matched photographic plates in their ability to record large volumes of information in a single exposure. Recall from our earlier calculations that the large photographic plates used in the 1950s for the Palomar Observatory Sky Survey had roughly 1.3 billion resolution elements. The Hyper-SuprimeCam mosaic CCD camera has almost as many -- 0.97 billion -- and records much more of the light which strikes it.

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Creative Commons License Copyright © Michael Richmond. This work is licensed under a Creative Commons License.