Polaroid CCD Camera User Manual

Page 33

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Section 4 - Camera Hardware

Page 29

length is the focal length of the telescope or lens. Also remember that 1° = 3600

arcseconds.

Read Noise - The readout noise of a CCD camera affects the graininess of short exposure

images. For example, a CCD camera with a readout noise of 30 electrons will

give images of objects producing 100 photoelectrons (very dim!) with a Signal to

Noise (S/N) of approximately 3 whereas a perfect camera with no readout noise

would give a Signal to Noise of 10. Again, this is only important for short

exposures or extremely dim objects. As the exposure is increased you rapidly

get into a region where the signal to noise of the final image is due solely to the

exposure interval. In the previous example increasing the exposure to 1000

photoelectrons results in a S/N of roughly 20 on the camera with 30 electrons

readout noise and a S/N of 30 on the noiseless camera. It is also important to

note that with the SBIG CCD cameras the noise due to the sky background will

exceed the readout noise in 15 to 60 seconds on the typical amateur telescopes.

Even the $30,000 priced CCD cameras with 10 electrons of readout noise will not

produce a better image after a minute of exposure!

Full Well Capacity - The full well capacity of the CCD is the number of electrons each pixel can

hold before it starts to loose charge or bleed into adjacent pixels. Larger pixels

hold more electrons. This gives an indication of the dynamic range the camera

is capable of when compared to the readout noise, but for most astronomers this

figure of merit is not all that important. You will rarely takes images that fill the

pixels to the maximum level except for stars in the field of view. Low level

nebulosity will almost always be well below saturation. While integrating

longer would cause more build up of charge, the signal to noise of images like

these is proportional to the square-root of the total number of electrons. To get

twice the signal to noise you would have to increase the exposure 4 times. An
ST-5C with its relatively low full well capacity of 50,000e

-

could produce an

image with a S/N in excess of 200!

Antiblooming - Most SBIG CCD cameras have antiblooming protection. The TI CCDs used in

the ST-5C, ST-237, ST-237A and ST-6 have it built into the CCDs and the Kodak

CCDs used in the ST-7E and ST-8E have Antiblooming versions of the CCDs

available. Blooming is a phenomenon that occurs when pixels fill up. As charge

continues to be generated in a full pixel, it has to go somewhere. In CCDs

without antiblooming protection the charge spills into neighboring pixels,

causing bright streaks in the image. With the CCDs used in the SBIG cameras

the excess charge can be drained off saturated pixels by applying clocking to the

CCD during integration. This protection allows overexposures of 100-fold

without blooming. The trade off is sensitivity. Antiblooming CCDs are less

sensitive than non-antiblooming CCDs. In the case of the ST-7E and ST-8E, for

example, the non-antiblooming versions are very roughly twice as sensitive.

The CCDs used in the ST-9E, ST-10E and ST-1001E detectors do not come

in an antiblooming version.

From the telescope's point of view, the different models offer differing fields of view for a given
focal length, or turned around, to achieve the same field of view the different models require
differing focal lengths. Tables 4.4 and 4.5 below compare the fields of view for the cameras at
several focal lengths, and vice versa.

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