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Baader Planetarium Methane (889nm) Narrow Bandpass Filter

Baader Trademark (19,559 bytes) Baader 2 inch U filter (107,470 bytes) The methane (CH4) filter developed by the Baader Planetarium of Germany is a specialized filter that allows light to pass through it in the near infrared portion of the spectrum centered at 889nm (8890 angstroms) but only 8nm wide; hence the designation narrow bandpass.

Optical filters take away but they can not add anything to an image that is not there. By diminishing portions of the spectrum that we do not wish to see filters can make what we intend to study appears more prominently. So filters can render obvious that which is otherwise invisible.

Why 889nm?

The infrared channel of the filter passes the reflected light from an object of study at a wavelength where methane strongly absorbs (at 889nm) that light. Where clouds containing methane are present, they scatter the sunlight back away from the planet. Thus, when imaging Jupiter for example then the equatorial belts may in visible light appear white due to high alt ammonia clouds, but when imaged in the methane (CH4) band it will be dark due to methane that is being also there. So the features appear more contrasting and easier to capture changing events.

Right: Baader 1.25 inch diameter Methane Filter as provided since 2010 in heavy duty case (107,470 bytes).
Click on image to see enlarged view (407,179 bytes).

The methane 889nm near infrared filter came to prominence among the amateur astronomy community as this was among those filters incorporated into the NASA Voyager spacecraft, in the NASA Hubble Space Telescope Wide-Field Planetary Camera (WFPC2), in the Space Telescope Imaging Spectrograph (STIS), and in the Cassini CIRS. These instruments have produced amazing details of the cloud structures on Jupiter and details of its Red Spot (see below), Saturn and it's largest moon Titan, and Neptune. Closer to home and more recently, scientists have become alarmed at the increase of 'greenhouse gasses' in the Earth's atmosphere of which methane is among the prominent concerns. So this means space-borne platforms orbiting Earth, including NASA's Giovanni, incorporate one or more methane filters among their other filters to study atmospheric methane too.

Images taken at this wavelength are usually in black and white since there is no color in the traditional sense at 889nm. However, the details imaged at 889 may be given combined with other images taken at other wavelengths to form a false color image. One famous example of this that was widely circulated is the NASA image below:

Methane Filter at Work: False color image of Jupiter's Great Red Spot (GRS)

Jupiter by NASA Galileo Spacecraft (37,777 bytes) At right is the famous false color representation of Jupiter's Great Red Spot taken with Galileo's imaging system. The images are a mosaic of eighteen (18) images, six (6) through each of three different near-infrared (beyond the visible range) filters. The images were taken on 26 June 1996 during the GRS second observing sequence. The images record sunlight that penetrated to different depths in Jupiter's atmosphere before being reflected back by clouds. The image was processed to reveal cloud top heights by the team at Cornell University and has been map-projected to a uniform grid of latitude and longitude. North is at the top.

The Great Red Spot appears pink and the surrounding region blue because of the particular color coding used in this representation. The red color channel shows the reflectance of Jupiter at a wavelength where methane strongly absorbs (889nm). Because of this absorption, only high clouds can reflect sunlight in this wavelength. The green channel in the image represents the reflectance at 732nm wavelength where methane absorbs, but does so less strongly; lower clouds can reflect sunlight in this wavelength. Finally, the blue channel shows the reflectance at the 757nm wavelength where there are essentially no absorbers in the Jovian atmosphere and one sees light reflected from the deepest clouds. Thus, the color of a cloud in this image indicates its height, with red or white being highest and blue or black being lowest. Thus, the color of a cloud in this image indicates its height. Blue or black areas are deep clouds, pink areas are high and thin hazes, white areas are the high thick clouds.

This image shows the Great Red Spot to be relatively high, as are some smaller clouds to the northeast and northwest that are surprisingly like towering thunderstorms found on earth. The deepest clouds are in the collar surrounding the Great Red Spot, and also just to the northwest of the high (bright) cloud in the northwest corner of the image. Preliminary modeling shows these cloud heights to vary over about 30km in altitude.

Launched in October 1989, Galileo entered orbit around Jupiter on 7 December 1995. The spacecraft's mission is to conduct detailed studies of the giant planet, its largest moons and the Jovian magnetic environment. The Jet Propulsion Laboratory, Pasadena, CA managed the mission for NASA's Office of Space Science, Washington, DC. Being a NASA (taxpayer funded) image, this image is in the public domain.

The Baader Methane Filter: What It Can Do For You

This highly specialized filter is designed for use by a a suitable camera and lens or telescope that is provided with an imaging or other sensor systems that are optimized for technical and natural studies in this infrared portion of the spectrum. It also may find some uses in laser applications. The human eye is not sensitive to light beyond about 700nm hence no person can see what is transmitted by this filter, so this filter is not suitable for visual applications.

The Baader Methane filter has such a narrow bandpass (8nm) that the images will be comparatively dim to a sensor than most other imaging filters typically used. Therefore, you are likely to require longer exposures of Jupiter and Saturn in particular with this filter than with other filters in your color filter wheel. The methane band could conceivably be helpful when imaging Uranus on long, guided exposured.

While the Baader Methane filter may be best known for its usefulness for imaging Jupiter and Saturn, this filter is also useful for solar studies too as demonstrated by Piotr Maliński of Poland. Piotr maintains an image gallery with much helpful advice at

Piotr advised Company Seven about imaging with the Baader methane filter:

    "In general it's very dark and requires longer exposures (about 1 sec or more in my case). Standard "old" planetary cameras like DMK21 with ICX098 are quite noisy and have low sensitivity in infrared, thats why I use DSI III Pro - which has bit higher sensitivity and nearly no noise at 1-10 sec exposures. The software (Nebulosity) also helps when focusing this filter with Bahtinow mask (stretch levels of capture frame and focusing on Jupiter moon). DSI III Pro works good but it's not the best thing - it's slow due to the CCD size. I can capture 100 - 150 frames and as it's 16 bit camera the exposures must be longer than 8-bit to get some decent histogram fill and acceptable signal to noise ratio. Some people used cooled SBIG mini cameras (guiders), or add cooling to their Lumeneras. The ultimate solution is the ICX618 CCD which has much higher sensitivity in IR and is/will be available in few planetary cameras: Basler Ace, Point Grey Flea 3 and incoming QHY IMG0H which will have a TEC cooling. So I would recommend methane imaging for people with newer cameras - either ICX618 or EMCCD scientific grade cameras. Big scopes advised. Webcams, NexImage not suitable. Monochrome CCDs.

    Jupiter: it's probably the easiest target for this filter.

    DSI III Pro (ICX285) 16 bit at f/10 requires about 1 sec exposures (can be even pushed to 10 sec without saturation, but seeing will blurr the details). 100 frames will be ok. DMK21 (ICX098) 8 but at f/10 requires also aboyt 1 sec exposures, but due to high noise and low signal to noise ratio - you need IMHO about 1000 frames which would be insane - 16 min of imaging. Smaller ammount of frames gives very noisy image.

    Here is f/10 DSI III Pro bin 2, 1 sec taken 10 Jul 2010:

    Jupiter by Piotr Maliński f/10 DSI III Pro bin 2, 1 sec 7-10-2010 (3,862 bytes)

    and bin1 taken 10 Jul 2010:

    Jupiter by Piotr Maliński f/10 DSI III Pro bin 1, 1 sec 7-10-2010 (12,546 bytes)

    and bin1 at 150% size (drizzle stacking) taken 10 Jul 2010:

    Jupiter by Piotr Maliński f/10 DSI III Pro bin 1, 1 sec 7-10-2010 (10,756 bytes)

    Bigger it gets the more noise show up due to low S/N ratio, but still very good and detailed (all storms visible and some cloud structure). Methane filter will show all moons clearly, on the planets GRS storms will be white, and most of the planet dark due to methane. Impact marks caused by objects that got depper into Jupiter atmosphere tend to leave white spots of material from inner atmospehere that lacks methane.

    Recently some amateurs made a methane image with EMCCD (very very low noise) camera using one meter telescope at Pic Du Midie. The image taken by J-Luc Dauvergn is at

    As for false color images - you can combine 2 or 3 bands into a false color image. You can find UV-G-CH4 images of Jupiter or Saturn. Such combination adds more colors at the poles and can reveal more details in the atmosphere. CH4-RGB where methane band is luminescence also can be made. Combinations are endless but the goal is to get as much details defined by colors as possible. I've made some UV,CH4,RG1000 false color images (where RG1000 pass IR from 1000 nm) taken 24 Sep 2010:

    Jupiter by Piotr Maliński f/10 DSI III Pro false color 9-24-2010 (28,023 bytes)

    or color from two bands Ir8-CH4,CH4,Ir8 (Ir8 - pro planet 804, CH4 - baader methane) taken 21 Aug 2010:

    Jupiter by Piotr Maliński f/10 DSI III Pro color from two bands Ir8-CH4, CH4, Ir8 08-21-2010 (4,804 bytes)

    color from noisy CH4 image was transfered to low noise broad infrared image used as luminescence. Using XXY combination makes X dark places apppear blue, and Y yellow.

    Using WinJUPOS for RGB/LRGB images alows also to equal planet rotation and get a better false color image (and ch4 imaging takes a lot of time).

    It also could be used for solar imaging with Baader Solar foil. It's dark enough for f/10 imaging with DMK21 and using infrared band gives more stable image (although 540 Solar Continuum looks better I think).

    Solar Continuum 540nm images (click to see enlarged view):

    Sun by Piotr Maliński, Solar Continuum 540 nm 10-10-2010 (43,163 bytes) Sun by Piotr Maliński, Solar Continuum 540 nm 10-10-2010 (35,217 bytes)

    Methane 889nm images (click to see enlarged view):

    Sun by Piotr Maliński, Methane 889nm 10-10-2010 (45,347 bytes) Sun by Piotr Maliński, Methane 889nm 10-10-2010 (58,088 bytes)

    Combined images:

    Sun by Piotr Maliński, combined 540nm and 889nm 10-10-2010 (41,449 bytes)

Incidentally, for those of you who wonder if Piotr took these from some immense observatory telescope these images were taken by him with an early 1970's vintage Celestron C-8, a 20cm inch aperture Schmidt-Cassegrain telescope using a Meade DSI III Pro CCD camera from his home deck in an urban location.

As conveyed by another solar observer:

"Sunspots with methane filter looks so dark, almost like through continuum (Baader Solar Continuum Filter). When I use 760nm or even 950nm IR filter,
sunspots has contrast very low (granulation is almost invisible). I can even see some structure in umbra."

WARNING when attempting to image the Sun with these filters note this is not for visual applications. Furthermore, an energy rejection 'pre filter' should be employed to cut the amount of heat that will otherwise accumulate in the telescope. If an energy rejection filter is not used in conjunction with the Methane Filter then the heat can be sufficient to damage the telescope, the Methane Filter, and the imaging system.

How Are These Constructed?

Methane Filter Graph (41,379 bytes) The methane filter developed by Baader Planetarium of Germany is a specialized imaging filter that allows light in the near infrared portion of the spectrum centered at 889nm (8890 angstroms) to pass through but only with a bandwidth that is 8nm wide. This filter was developed in order to measure the state of the methane that is characteristic of Jupiter, Saturn, and the Sun although it is finding uses in other applications too. This filter passes light only in the infrared portion of the spectrum, that is well beyond the visual spectrum where the human eye can see.

"filters take away but can not add anything to an image
by diminishing portions of the spectrum what we intend to study appears more prominently
filters can render obvious that which is otherwise invisible."

Right: Baader Methane Filter transmission curves (41,379 bytes).
Click on image to see enlarged view (61,622 bytes).

The Baader Methane Filter has proved to be useful to amateur and professional astronomers when taking images from Earth of the large gasseous planets and for our Sun. Astronomers involved with imaging from Earth find one of the advantages when working in the red (visible light) up into to the longer wavelengths, including the near-infrared, is that their equipment is less affected by any instability of the atmosphere and so the images taken in these wavelengths can show finer details and more contrast. However, to produce good results generally requires relatively longer exposure times.

Above: Solar spectrum from ~425nm to 925nm illustrating the bandpass of the Baader Methane Filter
as a narrow deep red line above the graph centered at 899nm (107,470 bytes).

In order to achieve the desired bandpass of only a very narrow 8nm bandwidth the filter is made from a disc of high grade Schott RG 830 optical filter glass that has been precisely ground to be plane parallel and then polished until very smooth. This glass undergoes a vacuum deposition coating process with many microns-thin dielectric coating layers of various elements are applied one upon another in a precise order and thicknesses forming a super stack. The coatings are calculated so that the filter ultimately transmits the desired wavelengths while simultaneously rejecting all other wavelengths above or below 889 nm ±3 nm.

The coated glass filter element is housed in a machined aluminum cell, the filter is held there by a machined thread-on retaining ring. The filter name, size, and part number are in silver however this mirror like print when combined with its small size make this information difficult to read under dim red lighting. Company Seven recommends our customers keep these filters in well organized accessory case so that you know which filter is which. It helps to become familiar with how the elements appear too (read descriptions below).

The coatings that are required to attain such a narrow bandpass are difficult and costly to produce, such that for the meantime these filters can only be made consistently in the smaller standard filter size of 1.25 inch (31.7mm) diameter. This size filter housing will thread into most 1.25 inch female fittings and this is suitable for use in many commercial filter wheels however, this filter will not be compatible with larger format CCD systems with detectors whose diagonal dimension exceeds the clear aperture of the filter. While this 1.25 inch (31.7mm) diameter may be inconvenient for our customers who own larger format CCD Color Filter Wheels, there is no great practical disadvantage to imaging the planets through the 1.25 inch (31.7mm) diameter filters because these objects are small enough to be covered by this format, even when employed on the larger Earth-based telescopes. However, the field of view when imaging the Sun may not be as wide as a larger format CCD system could otherwise provide. So one could dedicate one CCD system for imaging these smaller objects, and keep the larger CCD system equipped for imaging the larger, extended deep sky objects.

When viewed parallel to the eye from the female threaded (or field) side, then the filter element appears like a silvered mirror. When looking from the male threaded (instrument) end then the filter element appears like a dim deep red colored mirror.

Please contact us for advice that may be more specific to your requirements.

Common Features Of The Baader Filters:

  • The glass elements used to make the Baader Filters are free of striae, optically finely polished plane parallel to within 30 seconds of arc. This eliminates any double images or ghosting due to wedge errors in the glass. These filters tend to far supersede the quality of common color filter elements which are flame polished. The combination of their fine optical craftsmanship and a comparatively thin profile allows these filters to be inserted anywhere into the optical path without introducing astigmatism or other noticeable defects into the image.

  • The filter will thread into a CCD nosepiece or conventional slip fit accessories with the popular 31.7mm threading.

  • Stackable filters: each filter cell incorporates both a male and a female thread to allow stacking the filters to obtain even narrower passbands or special effects.

  • The filter cell incorporates milled notches which makes handling and threading the filter an easy operation.

  • For protection, each filter is provided with its own transparent plastic case. The case is much more protective than those offered before 2010. This case design is easy to manage, and the cases have dovetail mechanisms so they may be stacked along side each other or one atop another.

    Optional Wood Case
    optional wood case for Questar Color Filter Set. (52,803 bytes).

    The optional wood case is foam lined with cutaway spaces for filters, eyepieces and other small accessories for your telescope. Please refer to our price list for current prices for the filter set and the optional case or contact Company Seven for more information.

    Right: optional wood box for Color Filter Set (52,803 bytes)
    Click on the image to see enlarged view (190,049 bytes).



    1. It is best to protect the filter from sharp edges or any item that could cause a scratch or abrade the glass.

    2. When not in use, store the filter in a its provided rigid container, and it may help you to keep them organized in a fitted carrying case.

    3. Dew may form on the filters, if this happens do not store a wet filter into its airtight container for long periods of time; whenever possible let the filter "dry out" in order to reduce the potential for problems developing associated with Fungus, etc.

    4. Draw any large, loose bits of foreign matter from the surface of the glass with an air bulb or small vacuum. Stubborn particles can be removed with a soft camel's hair brush. Throughout the year, but especially in cold climates when static become more of a problem we particularly recommend the use of a Staticmaster brush.

    5. Place a few drops of an approved lens cleaning solution (by Carl Zeiss or Kodak) or mild soap solution of clear dish washing liquid diluted with distilled water onto a cotton swab. Then gently wipe in a circular motion with little or no pressure. The filter can be damaged if there are tiny abrasive particles on the surface which are pressed in by rubbing hard.


    Contents Copyright 1994-2010 Company Seven with images contributed by Piotr Malińskil; All Rights Reserved