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Composites by Examples

LRGB Composite (IV)

LRGB imaging is nothing else than a conventional combination or stacking of  3 monochrom channels, Red (R), Green (G) and Blue (B) with several high quality grayscale images of the same object, called the (L)uminance, to increase the contrast. Invented by Okano Kunihiko, the LRGB processing is quite simple but requests in this peculiar case either a CCD with a filter wheel (e.g. SBIG CFW-8A or FLI CFW2-7) and many patience or a software able to split the color channels if you use a webcam or a color CCD. Of course, there is always the manual option much cheaper consisting in recording black and white pictures under colored filter (R, G, B filters) completed with a B/W picture in white light for the luminance.

Images of the Serpent Nebula M16 taken from Siding Spring, Australia in June 2019, with a PlanetWave CDK 508mm f/6.8 telescope equipped with a 0.66x focal reducer, FLI filter wheel and FLI PL6303E CCD camera. Total integration time of 95 minutes including 55 minutes in RGB (3x 8x100s under red, green and blue filters) and 40 minutes (8x 300s) in B/W under red filter. The last image is the combination of LRGB channels processed in Photoshop. Here is the RGB image. Documents T.Lombry.

If the use of a color CCD can be very efficient in astrophotography, all the more that new models are very compacts, the LRGB resulting image is nothing else than a colorized black and white picture in which the lightest tones are often vanished. It is especially the case in planetary astrophotography. Indeed, if we take the example the astrophotography of Mars, as the luminance image is usually made in red or IR light, often the lightest blue haze or yellow and white clouds are removed from the RGB picture by the luminance component. Worse, the overall color of the planet is shifted from reddish to the orangeous-pinky color or becomes even grey-pink (see the gallery in French). Hopefully, this issue specific to color CCDs does not occur in picturing deep sky objects (cf. the image galleries of nebulae and galaxies taken with QHY and ZWO color CCDs).

So, to get a true LRGB picture, the luminance must be recorded in visible light, exceptionally in red light using a wide band filter but never in monochromatic light, except if you want to get a special effect. Therefore CCD cameras are more suited to that usage than webcams. A cooled CCD to reduce the electronic noise will satisfy all demanding amateurs, still more if you can add color filter wheel, an optional adaptive optics and a possible derotator if you use a fork mount.

STRETCHING Astrophotography in Photoshop Using Curves and Levels

To read : The True Color of the Pleiades Nebulosity, Roger N. Clark

                                                                                                                           

W61 Green = 6 min

W25 Red = 6 min

W47B Blue = 6 min

Luminance = 2 hours

Above, LRGB individual frames of M45 recorded in 2018 by the author at prime focus of an Altair Optics 70 mm f/7 ED apochromatic refractor equipped with a 1X flattener and a ZWO ASI1600MM Pro CCD (cooled) of 16 Mpixels of 3.8 microns. Integration time of 2h18 min (L=2h, R=G=B=6 min.). Below left, the resulting color picture processed with Pixinsight and Photoshop. At center, a stretched version where curves of each channel have been corrected to bring out the fainter nebulosities but without affecting star colors. At right, M45 recorded in 1998 by Chuck Vaughn from AA6G on TP 2415 film with RGB Shott filters. Total exposure time of 7.5 hours (R=90 min., G=B=180 min.) at prime focus of an Astro-Physics 130 EDT f/8 refractor with Field flattener.

Picturing DSO

In deep-sky astrophotography, the time exposure already long for a single monochrom image (a total integration time of some tens of minutes) must be multiplied by four to get a LRGB image and reached a total of 82 minutes for NGC 253.

If you want for example picturing bright galaxies with a 128 mm apochromat equipped with a monochrom CCD, most amateurs use the next combination : R = G = B = 1x 5 minutes exposure to 6x 30 minutes exposure for each channel plus at least 1 luminance (B/W) image exposed between 20 minutes anda few hours if you can benefit of a very dark sky (close to a desert, in a national park or in high altitude or any location plunged into full darkness). If the focusing, tracking and seeing are perfect, the resulting LRGB image will be stunning of colors and very crisper of details !

To reach that time without the slightest tracking error which is mandatory photographying DSO's, Okano Kunihiko has used a sturdy Takahashi EM200 german mount, one of the few to insure an accurate tracking compatible with the small size of the ST-7 detector (9 microns pixels).

To see : Convert Gray Images Into RGB Color

Two LRGB composite of NGC 253 and M42 created en 1994 by the talented japanese amateur Okano Kunihiko. The key picture is the Luminance component. At left a B/W picture has been added, and at right a near-infrared one. At left, RGB images=20 min each, L=22 min with a Celestron 5" f/10, ST-7 CCD in 2x2 binning mode. At that time, this picture was probably one of the best composite achieved with such a scope. At right, RGB images=60 min each with a 200 mm f/5 telescope on Ektar25 film, L-IR=4 min with a 310 mm scope and CCD HP-1 with IR filter >700 nm.

Of course such a sturdy mount and a high-cost CCD are not mandatory to take LRGB pictures (DSO's or planets), but in the field you will soon discover all advantages of using a robust installation, free of vibration and gambling, even if you work with the lightest webcam.

In this context most high-end Takahashi, Losmandy or Astro-Physics mounts are recommended. Smaller one like Sky-Wachter (Kepler) EQ6 or GT-One are interesting but most lack by default of accurate error corrections capabilities (PEC and Direct Drive are excessive).

The image of M42 is another story and a true performance. This is a mixing of analog and digital technique, the RGB having requested a 180 minutes total exposure due the very low sensitivity of the Kodak Ektar 25 (ISO 25). Once the four images acquired and upload into the computer, the goal was to reduce the "noise" presents in the RGB channels. 

Then a very special technique has been used. The image recorded on an ultra fine grain emulsion has been used as RGB channel, and the image taken with the HPC-1 CCD and infrared filter (passband over 700 nm) has been used for the Luminance. As a result, more "warm" stars appeared. The reddish ones are probably behind or into the bright nebula. As says Okano Kunihiko, "Now, you can see a lot of stars 'through' the Orion Nebula !"

In the LRGB composite of NGC253, only the color information was extracted from the RGB channels, while the "colored" noise was suppressed using a high-pass filter to produce a final composite much clear, which luminance comes from the high-gain grayscale image. The resulting picture displays more saturated colors and a more aesthetic image.

Picturing planets

The LRGB technique can be successfully applied to planetary astrophotography too. The principle is merging from some hundreds to some thousands RGB pictures of a planet with some hundreds of B/W ones to create the Luminance layer. Due to the high contrast of the luminance frame, the overall image will be crisper, more detailled and much more contrasted than an ordinary RGB picture.

Creation of a LRGB picture of Mars using a Luminance image recorded in IR/red light. The resulting image is known as a RRGB but the acrynom LRGB is not false as the first frame is well a B/W luminance image. Image recorded on September 4, 2003 by Sandro Nardella using an Intes Maksutov-Newton of 150 mm f/30 equipped with a Philips Vesta Pro webcam and a UV-IR blocking filter from Baader.

This technique is mainly used by advanced astrophotographers using a webcam or a CCD. This last is the most suited to this method as it can be equipped with a color filters wheel to get the individual LRGB frames that will be postprocessed. The most experimented amateurs using small scopes (100-150 mm) do no hesitate to stack up to thousands individuals frames to get a LRGB composite whereas users of larger scopes (300-450 mm) stack less than 50 images to get a similar result.

All the skill comes in fact from the experience in the field and from the processing on the computer. As for all astronomical subjects, the best snapshots are the ones recorded by a clear and dark night, with very low turbulence under the best seeing. Additionnaly I suggest you to increase your focal ratio using a 2x Barlow or a Tele Vue Powermate 2.5x or higher. If there is the slightest trace of turbulence or a problem of focusing, be sure that the marvellous features you spent many times to record in hundreds exposures will be vanished in a fuzzy blob. Therefore some amateurs do not hesitate to use webcams and to record small animations of about 3 minuts at a rate of 10 frames per second (you get 1800 frames) and to extract the best frames that they stack.

Applying Kunihiko Okano's LRGB techniques, at left Thierry Legault pictured Mars (24.83") on August 20, 2003 using a 12" LX 200 from Meade equipped with a Neptune-100 CCD. This image results of the combination of 125 images of luminance in red light and several RGB. Unsharp masking with QMiPS32. Disadvantage of using a luminance component in red light, blue hazes and yellow clouds present in the atmosphere are no more visible and all the image is too grey. At right Jupiter pictured by Ed Grafton on Nov 7, 2001 using a Celestron C14 at f/68 equipped with a SBIG ST-6 CCD. This is a LRGB made of 4 pictures only.

Some software like Registax from Cor Berrevoets can combine or stack automatically the 4 LRGB frames without splitting them in individual channels. Others amateurs prefer using IRIS from Christian Buil and to do to the work manually or to use more versatile tools like Photoshop or MaxIm DL.

Exposures Composite & Stacked images

This fourth composite technique is an hybrid version of the first. It uses different time exposure to record the full extension of the subject but without enhancing the resulting image with a mask. The second one merged a stack of numerous CCD images post-processed with an unsharp mask to enhance details. Both techniques are stunning by their resolution that exceeds the instrumental resolution.  But scopes are not the only ones to glorify but rather the authors's performances who used all their skills to produce these marvelous pictures.

Image processing software to download : 

ASTROSTACK - IRIS - REGISTAX

At left, AA6G team used a Fuji Velvia film famous for its fine-grain and great color saturation to record a serie of pictures of the Sun corona. Then they merged these images to get this stunning picture, the richest one by its colors and features exhibit in the corona (composite of 6 images at 1/2000, 1/125, 1/32, 1/16, 1/8 and 1/4s on Fuji Velvia film during the total eclipse of the Sun on July 11, 1991 in Baja California. Recorded at prime focus of an Astro-Physics 178 mm f/9 Starfire refractor with 0.6x focal reducer. At center, photomontage of the sun total eclipse of February 26, 1998 photographed from Willemstad in Curaçao, near Aruba by Thierry Lombry with a Pentax MX reflex equipped with a Pentax 300mm f/4 telephoto lens and Kodachrome 64 film. The partial phase was exposed at 1/100s at f/5.6 under a mylar solar filter. The image of the totality is composed of two images exposed 1/100s and 1/2s at f/5.6 then processed under a High Pass filter to accentuate the details in the crown. Two different blending modes were used for the partial phase and for the totality in order to preserve the darkness and the opacity of the lunar disk. At right, using a small scope, all Benjamin Roger's know-how is revealed in this composite of Saturn, crisper and full of details. It is a composite of 10 images of 0.1 s each with an Audine KAF-401E CCD taken on Nov 4, 2000. Each image was processed with an unsharp mask. Celestron Ultima 9.25" Maksutov-Cassegrain with 2x Barlow (f/30).

To combine multiple images most image processing software provide special dedicated tools which use arithmetic functions like adding, subtracting or multiply images. The principle consists to accurately register all images as explain earlier. Only then you can combine these images to create a composite. The resulting picture can be adjusted again using a judicious unsharp mask.

Note that if you are picturing bright DSO's you can post-process your resulting image with a Lucy-Richardson or VanCittert algorithm while Maximum Entropy is useful on faint objects which exhibit a low signal-to-noise ratio.

Isophote mapping

The isophote mapping technique allows you to extract lines of same brightness in images (equidensity) and optionally to attribute false color to the resulting isophotes. For years that was a tedious work in darkroom as explain in another page as we had to create contrasted masks, place them in sandwich with colored filters, repicturing the composite, etc.

But today the computing revolution allow us to perform such tasks in a few mouse clic. Isophote or similar functions are included in some image processing software, from Christian Buil's freeware QMiPS32 or IRIS to expensive IMAGE-32 or MIRA software.

Isophote mapping is a tedious task to perform using the old argentic way but... is much easier and faster using the digital way. At left the result of the Ramp function, at right the Equalization function. This technique reveals areas of equidensity in the image.

In this case, I used IRIS with a FITS image of M51 provided with the software (note that you can read FITS file with FITSview that allows you to save them in BMP). 

In IRIS, the procedure is accessible to a kid : select the appropriate function on the menu, set the dynamic threshold and press the false colors icon. Voilà, you get this marvelous images.

In the same way other software provide a Rotational gradient filter suited to reveal details in radial structure objects such as comets or the sun corona.

When isophotes and gradient filters are well selected, results are always amazing and beautiful, revealing features to the edge of the subject.

Last chapter

H-alpha trichromy and other alterations

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