Discover on our page all the essential helper tools specially developed to facilitate your selection for astronomical observations. From specific filter selectors to custom-made dovetail rails, we offer solutions tailored to your needs. Learn more about our products and how they can change your view of the sky.

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Baader Narrowband/Highspeed Filter Selector

To make it easy for you in the future to decide which kind of Highspeed (or Narrowband) filter you need for your telescope, please check the filter selector that provides you the correct individual graph based on your entries.

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Baader Solar Filter Finder

Baader Solar Filter Finder Tool

How do I find the right solar filter for my instrument? Use our Baader Solar Filter Finder and choose your observation device.

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2" ClickLock® clamp for your telescope

Can't find the right ClickLock® clamp for you? Then ask us, we may be able to produce the required clamp for you.

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Request for Baader domes

What information do we need if you are seriously interested in a Baader dome?

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Contact Us

Do you have a general request (for example about deliverability etc.)? Then please contact us via the form below. Fields marked with * must be completed.

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Important note: Please ask specific technical questions about products directly on the page of the corresponding product with the button "Ask question" (see right). This ensures that other customers also benefit from your questions.

What do you look for in an astronomical filter? Everyone has different requirements and goals and with a myriad of filters available today; how do you choose the right filters to unleash the full potential of Astrophotography?

In this blog our customer Ian Aiken gives some high level advice on what to look for when choosing a filter, coupled with reasoning why he choose the Baader's CMOS-Optimized LRGB and Ultra Narrowband f/2 filters, along with example LRGB and SHO images taken with these filters on his Celestron RASA 11 from his Bortle 7 suburban location.

New CMOS-optimized Baader filters

Blog Post by Ian Aiken:

I live in the North East of England in the United Kingdom, which experiences a temperate maritime climate characterized by mild summers and cool winters. Cloudiness can vary throughout the year and it feels like I only get 20 usable clear nights per year at my Bortle 7 location during the 6 months where astronomical darkness actually occurs. I've been an Astrophotographer for over 20 years and I've had all kinds of telescopes, mounts, filters (including Optolong, Astro Hutech, Chroma, Baader) and cameras (Atik, QHYCCD, ZWO, Canon) in this time, for both planetary and deep sky photography. Financially, I've learnt the hard way through fine tuning my current collection to something which supports my sky conditions, budget, time, and imaging goals.

Currently I own a Skywatcher EQ8 mounted in my roll off roof observatory. On this I have a RASA 11 with Baader UFC, QHY268M camera and Baader's CMOS-Optimized LRGB and Ultra-Narrowband f/2 filters.

Here are the factors I've considered when choosing my filters:

  1. Price:
    Assess the price of the product in relation to its features, quality, and performance. Is the price reasonable and competitive compared to similar products in the market? Consider whether the product offers significant advantages or unique features that justify its price.

    In my opinion, Baader filters are absolutely value for money. They've kept the price competitive and performance high. A set of Baader filters costs a little more than a single Chroma. Chroma are good, but did not feel value for money in comparison (Baader 2" LRGB set ~ € 500 vs. Chroma LRGB ~ € 2.238).

  2. Quality:
    Examine the quality of the product. Does it meet your expectations in terms of durability, craftsmanship, and overall build quality? A product that is well-made and built to last will provide better long-term value.

    Baader CMOS-Optimized filters come with Baader Planetarium's Life-Coat technology. Baader warrant the coatings for the life of the filter guaranteeing that the coatings will not peel, flake or physically degrade and they have no issues with you cleaning the filters with fine optical cleaning equipment. You can see the build quality is high, the coatings look durable, and I can understand how Baader can offer such a life time warranty. I don't think anyone else offers this.

  3. Performance:
    Evaluate how well the product performs its intended function. Does it deliver the expected results or fulfil your requirements? Consider its efficiency, accuracy, reliability, and any additional benefits it provides compared to alternative options.

    I'm going to post some images later in this blog, and you can judge the quality for yourself. Yes, there were initial problems with halos and these have been resolved. I haven't had any issues that I am concerned about. Halos can be a real pain, and it's not always the filter that causes this (most cases it is not the filter). Reflections can occur in your imaging system and could be caused by a number of factors: including spacing between optical elements; distance to CMOS camera; the CMOS camera front window itself etc. You have to spend time to understand your entire optical system and its individual nuances.

  4. Features and Specifications:
    Review the features, specifications, and capabilities of the product. Are there any unique or advanced features that differentiate it from competing products? Determine whether these features are essential to your needs and whether they justify the price.

    I opted for high-speed ultra-narrowband to match with my RASA 11. This was based upon my needs (explained a bit further below). In terms of features, what stood out was the features integrated into the filters to help prevent reflections and halos. For instance:
    • Reflex-Blocker - with coatings to reduce halos caused by my imaging system.
    • Parfocal - this helps to not have to refocus so much during a filter change. As a filter change is manual on my RASA 11 with the Baader UFC system, it means less movement with my motorised focuser and I am back to imaging quicker (and the focuser isn't off on some mission to reach focus by going further out of focus, which can happen when using an SCT type design).
    • Blackened edges - again to help reduce reflections in my imaging system, lots of mirrors and glass = high potential for reflection
    • Sealed Coating Edge - each filter is coated individually and not cut from a sheet. This is probably why they will last forever, and Baader are able to offer Life-Coat warranty.
  5. Brand Reputation and Customer Reviews:
    Research the brand's reputation and customer reviews of the product. Look for feedback from other customers who have used the product to gain insights into its performance, reliability, and customer satisfaction. Positive reviews and a strong brand reputation can indicate better value for money.

    Baader Planetarium have been in business since 1966. I've never experienced any poor customer care from dealers or Baader directly (I admit, I've not really had any issues either, with exception of one issues with the early Baader Steeltrack software which was swiftly resolved by Baader themselves). As a family run business, I feel they are passionate with what they do, and want to do the right thing at the right price, making astronomy accessible to all budget types, and truly are Aiders in Astronomy (this is their slogan).
     
  6. Longevity and Future Compatibility:
    Consider the product's longevity and future compatibility. Will it remain relevant and usable for a reasonable period? Assess whether the product is upgradable or compatible with future advancements or technologies to ensure its value over time.

    I have the older Baader 2" CCD filters which are in the same condition that I purchased them in. I have no concerns about the longevity of the Baader CMOS Optimised filters, especially backed by the Life-Coat warranty. 2" filters are going nowhere, and while the sensors on modern CMOS cameras are getting larger, I cannot see the need to upgrade anytime soon. I've been using 2" filters for the past 20 years.
     
  7. Warranty and Customer Support:
    Evaluate the warranty offered by the manufacturer and the availability of customer support. A reliable warranty and responsive customer support can provide additional value by offering peace of mind and assistance in case of any issues or defects.

    Baader offers Life-Coat, a lifetime warranty on their CMOS-Optimized filters (providing used and handled correctly). As a family run business operating for over 50 years, Baader are trustworthy and offer great customer support.
     
  8. Personal Needs and Preferences:
    Finally, consider how well the product aligns with your specific needs, preferences, and intended use. Different products may cater to different requirements, so it's essential to choose one that best suits your circumstances and priorities.

What did I choose?

I decided on the Ultra Narrowband High-Speed filters on my RASA 11. Why? Well, the reasoning may surprise you. While the filters are excellent value for money, my garden backs onto other gardens and my neighbours have lots of LED lights lit, especially on weekends when it's not windy, the moon is not out, and the sky conditions are good. You can picture the challenges already. Also, there are trees which do not belong to me which get in the way. I work full time, and have two small children, time is limited. I'm middle-aged, but not retired, so I cannot stay up all night imaging into the early hours. So, I went for a RASA for high speed imaging, reducing my imaging time significantly. While I may image across multiple nights, I don't need to. It just works for my current situation. The Baader filters are brilliant on the RASA 11, and I'm able to produce some excellent results (see further in the blog) even with all my challenges.

I hope the above helps you make a decision on what filters would be good for your needs. Baader Planetarium has a really nice tool to help you match which filters would be best for your imaging system. At time of writing you can access this tool: Baader Narrowband-/Highspeed Filter Selector

Example of Astrophotography taken with Baader CMOS Optimized Filters

I could talk about how tight the stars are (they are), how the filters have much more contrast than their predecessors (they do), but this can still be very subjective and influenced by sky conditions. My skies aren't great, they really aren't, and I have to battle with all the other issues living in a suburban environment. These images were also shot in reasonably poor conditions with thin haze. I also have to point out that I don't spend a massive amount of time processing my images. I think partly, if you capture good data you can produce a good image. You don't, in my opinion, need to push an imagine in processing so that it looks so bright and colourful. To me this looks over processed, and I prefer the darker looking style images with simple histogram and curves transformations. There's the disclaimers out of the way.

M45 taken with Baader CMOS-Optimized LRGB

My workflow consists of using PixInsight to Calibrate, Stack, Automatic Background Neutralisation, BlurXterminate, NoiseXterminate, and maybe StarXterminate. I may use TGV Denoise post stretching but haven't on these examples. I simply use the ScreenTransferFunction (STF) in PI applied to the Histogram, and a hint of Curves Transformation before exporting off into a PNG/JPG. There's probably so much more I could do, but I don't. Oh, I nearly forgot. I do use PhotometricColorCalobration in PixInsight, which applies a white balance to the image.

NGC 7023 - The Iris Nebula 2 hour integration from Bortle 7 sky

NGC 7023, also known as the Iris Nebula, is a captivating and visually striking celestial object located in the constellation Cepheus. This reflection nebula lies approximately 1,300 light-years away from Earth, and its unique features have made it a favourite target for amateur and professional astronomers alike. The Iris Nebula gets its name from the distinct shape and appearance of its central region, which resembles an iris or an eye. This prominent feature is created by a dense cloud of interstellar dust, which scatters and reflects the light emitted by nearby stars. The dust particles in the nebula also create intricate dark filaments, adding to its overall visual allure. At the heart of NGC 7023 lies a young star cluster, illuminating the surrounding gas and dust with its intense radiation. This interaction gives rise to the vibrant hues of blue and yellow seen in many astro photographs of the nebula.

Imaging System: QHY286M CMOS Camera mounted on RASA 11 with Baader UFC.
Filters: Baader CMOS Optimised LRGB
Mount: Skywatcher EQ8
Exposure Details: 30 x 60 seconds each channel (LRGB).  Total 2 hours integration time from Bortle 7 skies.

NGC 7635 - The Bubble Nebula 17 Hour Integration from Bortle 7 Sky

NGC 7635, famously known as the Bubble Nebula, is a captivating and visually stunning emission nebula located in the constellation Cassiopeia. Its unique structure and distinct appearance have made it a popular target for both amateur and professional astronomers. The Bubble Nebula derives its name from the spherical bubble-like structure at its center, which is created by the powerful stellar wind and radiation emitted by a massive, hot, and young central star. This star, known as BD+60 2522, is estimated to be several times more massive than our Sun and emits intense ultraviolet radiation, which ionizes the surrounding hydrogen gas. The ionized gas then emits light, creating the striking reddish glow seen in images of the nebula.

Imaging System: QHY286M CMOS Camera mounted on RASA 11 with Baader UFC.
Filters: Baader CMOS Optimised 3.5/4nm f/2 Ultra Highspeed (Ultra-Narrowband) filters.
Mount: Skywatcher EQ8
Exposure Details: Ha: 354x60s, SII: 121x60s & 104x120s, OIII: 175x120s. Total ~17 hours integration time from Bortle 7 skies.

Don't ask why the varying exposure! I'd also like to collect more data on SII and OIII in due course given it's about half of what I planned and need. You can tell by the images more is needed. Maybe next time, right? Astrophotography is for life not just for Christmas, or something like that…

I mixed the combination using PixelMath in PixInsight.

And finally to finish off, M45 taken with Baader CMOS-Optimized LRGB on same kits as above.

M45 taken with Baader CMOS-Optimized LRGB

The Universal Filter Changer (UFC) system with its solid mechanics and high flexibility has found a large user base worldwide. Nevertheless, there are always applications that are not covered by the adapters available to date. Therefore, we receive requests for technical drawings from our customers again and again. In the course of further development of our products, we are now pleased to be able to provide the UFC Design Guide.

This design guide contains technical drawings with all the relevant dimensions you need to make your own adapters for both sides of the UFC - be it S70 ring dovetail connection on the telescope- side or the eyepiece/camera-side adaptation:

UFC Design-Guide: Camera-side UFC adapter
Download as PDF

UFC Design-Guide: Telescope-side UFC adapter
Download as PDF

This means that you can now easily design your own adapters for the UFC system and thus implement individual solutions for your special requirements.

We created this small design guide because of the following review by one for our customers. This is a good example of how your feedback and customizations help us continuously improve our products.

He published a very positive review of our UFC system, which highlighted the solidity and flexibility of the UFC system, but also his need for special adaptations, which motivated us to publish these drawings. Our customer has already created his own adapter using our design guide and kindly provided us with pictures as well as his self-created CAD drawings and documentation for it (without warranty), which we are allowed to share here. He himself writes about it:

My new adapter is an off axis guider for the UFC with M68 connection. It is supposed to connect the 2 1/2" corrector of my selfmade Newton (M68 mount) to the UFC and the camera without mechanical compromises. Another design criterion was to realize a clear aperture as large as possible to minimize the vignetting of a full format sensor. Since I had already made very good experiences with a homemade off-axis guider with an M48 connection, I used the Baader information on the UFC to make an M68 off-axis guider with a UFC ring mount that has the required length for my image train. As prism I used a simple 8x8 prism from Chin.

Kai Wickerphotonenfangen.de

We encourage you to share your similar projects and customizations with us and our customers. Your feedback helps us to continuously improve and enhance our products.

Thank you for your support and trust in Baader Planetarium.

Many support requests that reach me via Baader Planetarium are related to the increasing use of USB – no matter whether mounts or cameras are connected, the old connections (RS-232, FireWire...) have largely been replaced by USB. The USB connection has made a triumphal march around the world, and the more devices are connected with it, the number of error messages also grows.

USB 3.0 stands for Universal Serial Bus and is a very fast data interface that is capable of transferring large amounts of data – including large images – to the PC in rapid succession. The raw image files are becoming larger and larger due to the large, high-resolution sensors, and the frame rates for downloading are also increasing more and more – and the interface must be able to cope with this. USB 3.1 came on the market in 2013 and transferred up to 10 Gb per second, shortly afterwards USB 3.2 increased the data rate to 20 Gb per second. In 2019, USB 4.0 with 40 Gb/s was introduced, but this interface version does not yet play a major role until today (Mid 2022). [br]

Schnittstellen

We hear again and again from customers using cameras from QHY or other camera manufacturers such as FLI or SBIG about problems with the USB connection between camera and laptop. We have therefore collected customer enquiries and try to point out a few possible solutions here that may be useful in case of USB problems.

In general, we have to distinguish between two problems:

  • Problem 1: The software, e.g. incompatible drivers after updates of the operating system and
  • Problem 2: The hardware - can large amounts of data be transferred without loss when downloading images?

Now there has to be considered what a user can do when problems occur, and what is caused by the control computer

The software

Windows updates are a big problem. In autumn 2021, for example, there was a Windows update that paralysed almost all USB 3.0 printers worldwide. This automatic operating system update also affected numerous cameras.

Please note: Although both are supplied by QHY, using the native camera driver and the ASCOM-driver can produce different image sizes! That is, the image can be two pixel larger or smaller depending on the driver, so that the images can’t be stacked. So: always use the same driver for your imaging sessions.

[br]The remedy, at least for QHY cameras, was a driver update that QHY provided almost simultaneously with the Windows updates.

In general: Large updates from an existing Windows version to a newer one (perhaps from 8.0 to 10) should always be viewed critically because the USB management is often not updated and there are probably few users who can go so deep into the control panel to fix any problems that may exist there. So: If a stable USB connection to the PC is up and running, it is better to do without an automatic update first.

If an older Windows operating system is to be updated, a new installation - and not an update - is preferable. This is the only way to ensure that the "substructure" is also up to date and that no old code parts can cause problems.

You can read about my experience with the FCCT adapter at the RASA 8. When I took my first pictures with the QHY 163M, I had nothing but trouble on one PC. But the same camera with exactly the same software ran on my second PC from the beginning until today without a problem.

The cause was my sequential update from Win 7 to Win 8.1 and then to Win 10: the USB management in the background had remained at the Win 7 level. As a result, the camera was shown to me in the device manager as ready for use without any problems, but there were often connection problems up to the loss of the downloaded image. By the way: The current All-In-One driver packages on the QHY site are stable and run really well (Win 10)! INDI is also supposed to run, but I haven't checked it.

BUT – There are more potential sources of error!

The hardware

With USB 3.0, the cameras are able to shovel extremely large amounts of data onto the PC in a short time. Even with "fit to screen", i.e. when you only view the whole image in "small" on the monitor, always the whole image is transferred to the PC – and only downsized there. But the full-resolution picture is transferred to the PC in 16 bits!

I often read about drops, half images, patterns or even black images, as well as connection problems. For all those who immediately think that the drivers are badly programmed: No, the camera drivers from QHY are just as good as drivers from other manufacturers and fulfil their function without any problems for many users worldwide! It should not be forgotten here that the PC also plays a role! It is not always the camera manufacturer's fault if things do not work as expected.

Since modern amounts of data are enormous, you should not work with "ancient" computers, even if they already have USB3. The hard disk must also be able to write this data, which usually requires an SSD.

Older computers often have only two USB ports, so that USB hubs have to be used. Passive USB hubs, however, tend to cause problems! If a hub is needed, use an active hub with its own external power supply. ALWAYS connect the camera and guider directly to the PC and not to the hub.

Over and over again, the cables also cause problems. The maximum cable length for USB 3 is three metres; longer USB cables – or even shorter but too cheap cables – also transmit signal, but not at the maximum possible speed. For bridging longer distances, more expensive active cables can be used if necessary. These have integrated signal amplifiers to counteract the technically caused signal loss due to signal attenuation, electrical crosstalk or external interference.

Active cables have their own power supply and can be identified by an external power supply with another cable. For demanding users of our QHY cameras, we offer active extensions in lengths of 5 metres and 10 metres ([product sku="QHYextension" style="imgright"]) . This significantly extends the working radius compared to the 1.8 metre cable included in the scope of delivery.

There are also solutions that convert the USB signal and route it through a network cable for long distances. Finally, signal transmission with optical signals should be mentioned. Here, an electro-optical converter sends the signal through an optical fibre and translates it back for the receiving device.

If the PC is not powerful enough to download and process the data fast enough, the screen in the download sometimes shows only half or completely black images and the data communication breaks down. In this case, it is advisable to treat the new camera to a new control computer as well.

The checklist

If you are having problems with your new astro-camera, please check the following points:

  • If the operating system was (manually or automatically) updated (and it always should for computers with internet access): Install the correct driver package and always keep it up to date. When installing the QHY software, you can choose the appropriate plug-ins.
    Yes, I know the saying: "Never change a running system!" Nevertheless, you should not ignore any security updates of the operating system, and therefore the camera driver must also remain up-to-date.
  • A standard USB3 cable (without amplification!) has a maximum length of 3m - this is the specification for USB 3.0. Longer (or cheap) cables do not deliver the specified speed.
  • To be on the safe side, always use the same USB port on the PC to connect the camera.
  • The QHY SDK can help solve USB communication problems and may be a solution. It is available for download from the QHY site
  • Are there problems with static charging and discharging when you plug the cable into the PC? If this happens, the camera „disappears“ and needs to be re-connected. Be careful in this case: it may even damage the camera under certain circumstances.
  • USB Traffic: Select a value between 1 and 5 in the driver (ASCOM). It does not have to be zero!
  • Camera settings: Deactivate „Live View“ when the camera is not in use!
  • Are the USB contacts still OK? Dirt in the socket or cable or worn-out contacts can also cause problems.
  • Be careful with USB hubs:
    • Because USB 3.0 expects proper communication, some hubs may have problems while others work fine
    • If several applications are using a USB hub at full power, which in turn is plugged into a single USB port on the PC, this is a stress situation for the PC!
  • Power supply via USB: Power supply via the USB port (where the power is thus supplied by the PC) can also affect communication. Power fluctuations can interrupt the connection and the camera has to be reconnected to the PC. (QHY has set up camera + cooling and USB communication separately).
  • The USB ports and their performance is better on newer computers, BUT:
    The cameras always deliver the image in full 1:1 resolution and 16bit to the PC when Live View is active (if no subframe/ROI is selected). In order for the camera to deliver this quickly and stably, it has enough DDR RAM built in.
  • Mini-PCs - small can be too small!
    • Nowadays, small, compact mini-PCs are often used directly at the telescope. If these are overwhelmed with the amount of data from the camera, the camera will deliver half or black images and communication will be interrupted!
    • Therefore, pay close attention to what the (mini) PC can do in the "continuous fire" of the camera, whether it is up to the data transfer from the camera to the PC and how much data it can process.
  • Small can also be too small – I know this from my own experience. I prefer to put my older but proven PCs at the telescope for shooting instead of a new mini PC – which may only create new problems for me!

If you don't know any of these effects - GREAT! Then continue to have fun and take lots of great pictures!

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Wolfgang Paech + Christoph Kaltseis

 


About the authors: [br]

Christoph Kaltseis

Christoph Kaltseis is not only an Adobe Photoshop specialist and as Nikon Professional touring for Nikon, but also an experienced astrophotographer. He is one of the founders of the Central European DeepSky Imaging Conference (www.cedic.at), which is held every two years in Linz since 2009.

In addition to his various projects, Christoph has developed an innovative image sharpening process called APF-R (Absolute Point of Focus)in recent years. The procedure is not always the same, but is adapted to the combination of lens and camera. Therefore, a flexible method was necessary to achieve the desired results.

In his career as an astrophotographer Christoph has also created several APODs (NASA Astronomy Picture of the Day), e.g. the APF-R-processed image of the M33 Galaxy or the Heart of the Orion Nebula (M42).

View all posts from Christoph Kaltseis

 

Wolfgang Paech

Wolfgang Paech has been practicing astronomy for more than 50 years. In addition to his many experiences with observatory domes of all kinds, his core areas are the Sun and the Moon. On the german Website www.chamaeleon-observatory-onjala.de you will find a complete moon atlas, recorded with his standard technique. But even in terms of Deep-Sky and Planetary imaging, as a veteran astrophotographer for many years, nobody can fool him.

The 50+ years of amateur astronomy with many other areas, such as the restoration of historical amateur telescopes, polar light trips and much more are prepared on his private german website at www.astrotech-hannover.de.

View all posts from Dipl.-Ing. Wolfgang Paech

 

 

 

If a sensor diagonal of 22mm is ideal for a sharp image with the RASA 8, but if you have got "only" a camera with a diagonal of 28.5mm is available - is a good image possible at all?

I tried this out and will describe here step by step my way to the finished image with the Baader [product sku="baaderfcct"] an the QHY 268M ([product sku="QHY268"]) on the RASA 8, especially the adjustment of the overall system. I suggest that you read all this before you try it out yourself!

For safety's sake, check every step – and everything at your own risk!

Why Astrophotography with a RASA 8?

I like the RASA 8 very much. It is a very handy OTA and has very good imaging optics. I was able to test the first prototype of the FCCT filter slider and camera filter together with the QHY163M on the RASA 8 some time ago and had a lot of fun. These shots laid the foundation for my enjoyment of the current Ultra Narrowband (UNB) SHO filters.

In the past I could often show that I can "read" the RASAs quite well. What do I mean by "reading a telescope"? Well, that's what I call the "interpretation" of the system's image in focus: am I working with the right settings for the backfocus, and which adjustment are necessary so that the image is perfectly sharp in the center as well as in all corners. The latter is really a challenge with f/2-optics and large camera sensors.

The price/performance ratio of the OTA with 8" aperture is very good with respect to the field and camera, even including the obstruction. The [product sku="baaderfcct"] is a fine addition! According to the technical data of the RASA 8 f2.0, the field can be used up to 30mm chip diagonal, albeit with cutbacks or compromises in the corners – it is optimized for 22mm works up to 32mm. Previously I had "only" shown that the information about the imaging quality of the RASAs is correct if you use them correctly.

Let's go ahead and see what I did with a larger camera than recommended, and what you have to do!

Preparing the RASA 8:

The first thing I did was to remove the "clear glass filter" of the RASA 8, because the backfocus calculation showed that only then I would get exactly the right distance with the FCCT and a spacer ring as well as the filters. This is simply a MUST at f2 - because even 0.5mm is a much too big deviation here and certainly not helpful in my experiment! What plays a minor role with f4 systems or even less light intensity is a world with f2.0.

And always check: Is everything clean and dust-free?

Preparing the QHY 268M:

The  FCCT instructions give a good idea of how to install it on smaller cameras. I took everything off the QHY268M until I had the sensor glass heater in front of me and carefully kept the tiny original M2 screws. Then I was able to mount the camera base part of the FCCT. To do this, the FCCT has to be disassembled into three parts as described in the instructions.

A) Aligning the Baader FCCT to the camera:

It should be said that the sensor of the QHY 268M is installed in portrait format so that "north" is always at the top of the picture. This means that I connected the camera to the FCCT in such a way that the filter is later inserted into the FCCT from above. "Top" can be seen very well on the back of the camera.

There is another consideration behind this orientation: I wanted the power cable to lead away towards the left or right and the USB cable towards the ground. If the cables run nice and straight, a spike can be created; the effect of the spike is then always mirrored.

But at the same time, I would not change the position of the cables during an imaging session. If I pay attention (!) and don't bump into anything, nothing changes during the imaging and I can create and use flats without any problems.

If, on the other hand, I change the position of the cables between the shots, this becomes visible on the stars and leads to artefacts. Changing filters is also easier when there is no cable in the way!

Flats are an absolute must-have: without flats I can't "turn up" the depth of the image as I like to do. If the system is to deliver what I expect, then everything has to be done right during preparation.

And always check: Is everything clean and dust-free?

B) Attaching the FCCT-Tilters to the base of the FCCT with the camera:

Now take the FCCT base and turn the tilter screws until the screw tips are just visible on the inside of the FCCT. The screws must NOT protrude into the FCCT. On the camera side, the FCCT consists of two parts that are separated for assembly, namely the FCCT-QHY flange and the FCCT base with the tilter screws. We do not need the third part, the RASA flange, at the moment.

Important: Make sure that both parts are in alignment so that the filter can be inserted and removed without "pinching & squeezing"!

Next, place the FCCT base on the table in such a way that the pit for the filter faces you. In the next step, take the camera with the mounted FCCT-QHY flange and orient it so that the insertion of the filter also faces you.

Only when both orientations fit can you gently press the camera into the tilter base.[br]

Important: All three pairs of screws should be screwed in and fixed at the same depth, because this way the starting point for the adjustment on the star is not tilted! (And again the check: Is everything clean and dust-free?)

Next, both parts are fixed in place: This is done with the three pairs of screws, which are arranged in pairs with a 120° offset. Please fix the "pull-screw" first until you feel a gentle resistance. Ideally, tighten each tension screw alternately! Then follow the "pressure screws". These must also be fixed! The same applies as for the tension screws: → Tighten until you feel pressure/contact.

Please note: All steps so far, which describe the use of the FCCT, can be done also without a camera in place, so that you can get a feeling for handling it.

Preparing the FCCT at the RASA 8:

Important: I have centred the flange of the FCCT as much as possible!

This means that there is a visible gap between the counter ring of the RASA 8 and the fully assembled FCCT base. My goal now was to make sure that this distance was the same all around. When I tightened the counter ring, I kept checking the centre to the system.

For this purpose, I screwed the FCCT-RASA flange with a spacer and the union nut of the RASA 8

The counter ring is not screwed on too tightly, but firmly - do you know the expression "hand-tight"? Please don't "bang it tight"... Important: Tighten the retaining ring so well / tightly that it doesn't become loose later at night when it cools down.

If I had to fix the camera again during the night, the camera would certainly twist minimally or shift out of the optical axis. I wanted to avoid that at all costs. It needs some practice, but it wasn't my first time with the RASA.

Caution: If you tighten the counter ring too much, you will have to use a lot of force to unscrew it later on, which can lead to the corrector of the RASA 8 moving in the Schmidt plate after several times – then the adjustment is "gone" and the RASA 8 has to be serviced!

(And always check: clean and dust-free!)

By the way: The FCCT-RASA flange can stay on the RASA 8 so that I can still use the dust cover of the RASA 8. This way the optics can be transported. (For this, "only" the camera has to be removed again. Mark the centre of the camera towards the FCCT, this makes it easier to reattach the camera!)

The camera assembly for the FCCT has only to be done once, the FCCT remains on the camera later.

Put the RASA 8 onto the mount and connect all cables

What I do now will accompany me on all the nights I usethis setup - with every image that is downloaded. So it is important!

No "good enough" applies here - no, being really exact is the be-all and end-all here!

A) First I put the RASA 8 on my CGX mount and fixed it with a (slight) overweight to the main mirror, because with the camera attached, the centre of gravity moves forward again. I had already aligned the CGX before - so I didn't have to do that again that night.

I moved the main mirror 8-9 times by half a turn of the focuser counterclockwise - the optics are not in focus! At this moment, I am only concerned with the distribution of the weight, because if I don't do this now, I won't be able to see later whether it is pulling a little more towards the camera or the main mirror.
Shooting with an f2 system not only means that I can gain depth very quickly, no: I can also see every little tracking error - f2 shows that immediately!

AND it is much, much more important that my setup runs well! When I adjust, I need to be able to run the mount for up to 10 seconds or more, without an autoguider - but the stars have to stay round so that I can evaluate the imaging at the edges and in the field well. If the mount would let me down and not run "free and correct", I would adjust for the tracking error and not for the optics!

B) Attaching the QHY 268M at the FCCT-RASA-Flange (Very important, so work with care!)
In the next step, we leave the mount with the RASA 8 fixed in the parking position pointing to the pole star; the optics thus point exactly towards the celestial pole. Now take the camera and place it on the FCCT RASA flange that has been fixed centrally on the RASA 8. Do not let go of the camera during this process!

Turn everything so that the centre of the camera points exactly upwards or to the centre of the lens!

Hold the camera firmly and tighten the screws. I use a star pattern until the screws are tight. To ensure that everything fits, you must finally check the alignment of the camera to the lens!

Check: Are the camera and the FFC centred on each other, and both together again on the RASA? This is necessary so that later the star only moves in one direction or axis when you move one axis of the mount, and not diagonally through the field.

By the way: Perhaps you have already noticed: The screws for adjusting the camera are located on the left (S1) or right (S2) at the top of the FCCT and exactly at the bottom (S3) of the FCCT!

This means that each screw is assigned to an axis in the field! (And always check again: Clean and dust-free! This way you avoid surprises during the recording).

The golden rule: The cables in front of the optics must not move!

Installing the cables and balancing the system

When all steps have been completed (and better checked 2x), now make everything ready for use. To do this, connect the power and USB cables to the camera. In my case, I fix both cables to a heating collar and additionally with Velcro cable ties.

Look at the optics from the front: the cables should - or better: must - run straight and at right angles to each other to the edges of the optics, without bumps, knots, etc.

If the radial course is offset by more than 120° (169°), the cables become "invisible", then there will be no spike on the photo.

Auto-Guiding:

Celestron RASA 8 with StarAid Rev. B & QHY MiniGuide Scope

This time, I have attached the [product sku="1485001B" style="imgright"] with a [product sku="2457000"]. From this point on, the final balancing of the telescope and the completion of the wiring begins.

The balance is checked on both sides of the mount, on the east and the west side. Once the aperture of the RASA 8 points to the north, it is then rotated 180° so that it points to the south. In each case, the optics are aligned parallel to the ground.

In this process I check every position I can reach. The mount must be evenly balanced in all positions. This also serves to check my cable routing - no tension or pressure! Caution: With the cold, cables become "unruly" and affect the tracking!

Done!!! The setup procedure is finished, now follow the first light on the star and the adjustment of the QHY 268M with the FCCT on the RASA 8.[br]

First Light at the stars and collimating QHY 268M with the FCCT to the RASA 8

Collimating the RASA 8 + FCCT + QHY268M with the stars

First, let me give you a few notes on the steps, as well as on the use of the devices in general.

  • I operated the QHY 268M at -10°C with Gain 26 and Offset 60;
  • As a basis I took LRGB data in the eastern and western sky, then H-alpha, OIII and SII; and the whole thing for declination values from -6° up to high in the sky. This gave me an impression of possible deflection or a change in the position of the main mirror as well as the stability of the adjustment and the FCCT to the RASA 8;
  • What I must urge everyone to do is this: Focusing must be on the optical axis, with a very small deviation (less than 150-200 pixels). This is especially true during adjustment! After that it becomes less critical, but a maximum of 1/3 of centre is a golden rule;
  • Correction with bias, darks and flats. Darks and bias I took with the [product sku="2459197" style="imgright"], that worked even when the crescent moon had risen! But of course the telescope was 180° away from the moon and without direct light on the aperture of the RASA.
  • The LRGB and Ultra Narrowband filters must be perfectly clean. So I could test the behaviour with the flats, because the flat only has to correct the course of the brightness, no contamination on chip or filter...
  • Green flats (avg. 31000 ADU) worked well with all Ultra Narrowband filters, although a constant flat saturation seems to me to be an advantage for all channels.

Beginning of the collimation at a star:

The mount was carefully aligned in the normal way - everyone knows best how this works for their own mount. Then I looked for a bright star at an altitude of about 50° degrees to complete the adjustment at my leisure.

Note: The ASCOM driver of the QHY 268M was unchanged since the installation. As a result, every image was upside down.

When the setup is set up as described, the screws S1 / S2 / S3 on the FCCT are assigned as follows; the S1 and S2 are always effective in the diagonal.

  • S1: Upper right to lower left
  • S2: Upper left to lower right
  • S3: Left to right over the field[br]

 

The field of view of the RASA 8 and the QHY 268M at 100% and the edges of the image; there is also shown in which way the adjustment screws act.

The field of view of the RASA 8 and the QHY 268M at 100% and the edges of the image; there is also shown in which way the adjustment screws act.

 

[br]

Test image before the collimation

Test image before the collimation

A) The first step is finding the perfect focus for the RASA 8 (using FWHM-data and brightness!)!

Then, I could take the first shot with these settings:

  • Filter: Lum
  • Exposure time: 10sec
  • Bin: 1x1
  • Save: in a new folder called "collimation“
  • File name: 0001_Start_10sec_Lum
  • Following files: 0002_(corner / Screw etc…)_....

The first thing I noticed in the test shot is a left/right difference, which I will correct later with screw S3. But at first I work with S2, because the deviation was greatest there. This is the rule from now on: the axis / corner of the image where the error is greatest is optimised.

Important: The stars must be perfectly rund in the center of the image! There must be no tracking errors!

Work with great care: Take care of all cables, do not bump the telescope roughly, use a headlamp, hold the hex keys securely,...

B) After the first exposure, I enlarged a subframe of the corner of the image (via the region of interest) where the stars were blurriest/largest.

Then I exposed this image area for 2 - 4 seconds. The exposure time depends on the brightness of the stars in the field.

When adjusting the exposure time, you have to avoid oversaturation of the stars, otherwise no accurate evaluation is possible. I set the shooting mode for these focus subframes to endless loop until the adjustment of the image corner was completed! To evaluate the subframes, turn the monitor so that it is clearly visible if possible and set the zoom to 200 to 400%!

The process: Now it's easy: I say out loud the name of the screw and what I want to do. So "S2 + lower screw (on the FCCT!) + tighten"! As I do this, I always turn the screws about 1/8 of a turn. This helps to get a routine over time: When you say it out loud, it's easier to remember 😊
When I had done this, I waited for two shots, then the mount was steady again and the stars stood still again. Everyone has to find out for themselves what suits their own mount.

As a result and as a goal, the stars must become smaller. Since there is still tilt of the sensor, they do not have to be round yet - but smaller is the goal! Okay!
Now take the whole image field again and look for the next "worst image corner"!
I took the "S1" axis, chose the corner where the stars were again the "biggest", and again the FCCT is turned to make the stars smaller(r).

C) Now that two corners have been "treated", it is time to take a new picture of the whole field.
Now you should see what has happened in the corners of the picture that you have chosen, and what has happened in the opposite corners of the picture! Now you have to decide how happy you are with it!

The goal is (always): The image has become better compared to the previous images, then the direction is good. In my case it got better overall, but the left/right deviation in the image was still there. If there is a noticeable deterioration, you can use the S1 / S2 screws again to correct the image corners with the greatest deviation.

D) Start a new focus routine for the whole lens and focus again in the centre of the image field! (focus very precisely, because the errors become smaller towards the edges!). This is followed by a longer exposed shot of about 10 to 15 seconds. No tracking errors are allowed here!

Now look at all picture corners at min. 100% and compare them with the previous pictures. In my case, I now used the S3 screw, because I had similar stars on the left / right side of the image up to the image corners.
Therefore I took the side in the picture where the stars were the biggest. So again I selected a corner of the image as a focus subframe via region of interest and let it be exposed in an endless loop with 2 to 4 seconds exposure time. Then turn the S3 screw to make the stars smaller. (They may be slightly egg-shaped, but they will become round).

E) Then another shot of the whole field at 10 to 15 seconds exposure time.

Again, check all four corners of the image at 100%. You may have to make another round of adjustments using the screws S1 + S2 or even S3:

  • It always makes sense to refocus after 2-3 corrections in the image corners - the errors are getting smaller!!!
  • These rounds of adjustment are to be made until in the end there are only round stars left in all four corners of the image;
  • The better the air quality (seeing), the better you can see the quality of the adjustment - poor seeing makes it look "good" faster, but there can be a deviation again with better seeing!
  • Since you are adjusting on an f2 system and 3.7mü pixels are small, it can take a while.

I've had time to practice on my RASAs over the last few years - but it's not witchcraft!

Just in case:

You may find that the screws are no longer so easy to tighten. Remember: Too much force is not a good tool!
In this case you have to loosen the S2 + upper screw slightly (1/16 - 1/8 turn). Always do this with an active subframe so that you can see what happens!

Check: Are you turning in the right direction, so is it getting better?

If you are close to perfection, that last little "bit" may have already gone the other way, so that without noticing it you have already gone through the ideal focus! Or it may be the tilt in the field, which can then cause you to have to use the S1 and S2 screw again, because there may be a swing between the corners of the picture and left / right in the field. To eliminate this, more careful adjustment is always necessary!

Conclusion:

One thing has been confirmed over and over again in all the nights I have photographed: You should always focus on the object; drifts in focus worsen the image! Otherwise, I have not noticed any deviation.

On system optimisation: A second 3" rail on top of the RASA 8 would be helpful, so that the StarAid-B can be better balanced above the optics.
I brought the adjustment to the final state in three nights (after a total of about 2.5 hours). It was helpful that I had always recorded data. This allowed me to make a comparison with the previous night in terms of adjustment and stability. This allowed me to determine the consistency of the optics, as well as a stable position of the FCCT. After completing the adjustment, the image was the same on every object.

But don't worry: the time-consuming collimation is only necessary once. From now on, the system remains pleasingly stable, in all tube positions! Both in the eastern and western sky from -6° Dec up to high in the sky... If I had already had optimal seeing conditions on the first night, the collimation would have been done in one evening.

What I had achieves during night 1 was still the on night 2, and what I schieves on night 2 was exactly the same on night 3. Only because of the better seeing in the following nights did I have to optimize the collimation. The time required: 15-20 minutes – if you are not doing it for the first time!

I use a "partially mobile" setup: I usually dismantle the CGX and telescope, but the camera remains on the telescope. With "proper" handling, the alignment remains intact. Only the alignment of the images is a big issue: when the camera is taken down and put back on, the individual sub-frames can easily be twisted against each other.

But since I wanted to have images in narrow band and LRGB for stacking, I had to work so precisely. Pre-stacking showed whether it would work. That's why after a night I always do a run-through with the data and a mix of two nights to see if they will fit together.

The focus must be hit exactly. In case you have gone beyond the focus point, you should focus again from the beginning. The following applies: ALWAYS PRESSURE, i.e. push the mirror upwards by rotating the focuser anti-clockwise!

To achieve perfect focus: Test the FWHM values in a focus pass from intra- to extrafocal and evaluate them!

My RGB filters showed very similar FWHM values. The stars remain round to the edge of the field and show no fringes.

On recording the RGB series:
I took the blue shots when the object was at its highest altitude in the sky, then green and behind, and finally red when the object was already lower. Lum (UV/IR) is the sum of RGB and shows the FWHM averaged.
The focus position of the Ha and SII filters was the same, OIII showed a deviation in focus. After everything is adjusted, it is time to take pictures!

I exposed each subframe for 180 seconds. RASA 8, StarAid, CGX and QHY268M were now working PERFECTLY together. Even a single image gives an idea of what to expect. Here is an original luminance image after 180s - only a mild STF was made and saved in Jpeg.

A "few" shots later, all the images were "in the box", and after image processing, now the result of the effort:[br]

M65 / M66 and only 400mm focal length in LRGB!

LRGB M65 + M66 + NGC3628; Lum: 105min, R/G/B: 30min each channel (=90min); Subs: 180s!; QHY 268M @ -10°C; Celestron RASA 8 + Baader FCCT + Baader LRGB (older version of filters); Celestron CGX + StarAID-B; Size: 66%; Depth: HUGE!; 400mm focal lenght and APF-R; © Christoph Kaltseis

LRGB M65 + M66 + NGC3628; Lum: 105min, R/G/B: 30min each channel (=90min); Subs: 180s!; QHY 268M @ -10°C; Celestron RASA 8 + Baader FCCT + Baader LRGB (older version of filters); Celestron CGX + StarAID-B; Size: 66%; Depth: HUGE!; 400mm focal length and APF-R; © Christoph Kaltseis

 

And to prove that it can be done again and again, here are two more single shots made with the large QHY268M and the RASA8 – the image sequences are stillw aiting for processing:

The spiral galaxy M51, 1x180s with green filter; © Christoph Kaltseis

The spiral galaxy M51, 1x180s with green filter; © Christoph Kaltseis

IC1318, 1x180s with H-alpha 3,5nm Ultra-Narrowband-Filter © Christoph Kaltseis

IC1318, 1x180s with H-alpha 3,5nm Ultra-Narrowband-Filter © Christoph Kaltseis

From time to time customers contact us who have bought a cooled CMOS camera, because they are not satisfied with their image results. They have been working with an uncooled DSLR camera or even a cooled CCD camera and compare the old images with what their new QHY delivers. So we often hear:

My images show way too much noise and hardly any signal from the subject". And many new astrophotographers (or those used to old technology) write to us: "My old images, taken with my DSLR, show much more of the object, even though the new camera is cooled and is supposed to be much more sensitive.

If that were the case, it would be really bad! That's why we want to take a look at CMOS technology here and give you a few hints on how you can dramatically improve your image results, because CMOS sensors in cooled cameras behave differently than CMOS sensors in a DSLR or even CCD cameras.

Everything was better in the past, they say - or let's rather say: everything was different in the past. With the older CCD technology, one had more little work with setting parameters for an exposure.

Was für CCD-Kameras galt, gilt heute nicht mehr!

CCD Kamera (SBIG ST-10XMS, Baujahr 2000) und rechts eine CMOS Kamera (ZWO ASI 071C Pro, Baujahr 2022)
on the left a CCD camera (SBIG ST-10XMS, built in 2000) and on the right a CMOS camera (ZWO ASI 071C Pro, built in 2022)

Back in those days, it was only a matter of connecting the camera to the computer, switching on the cooling (cool as low as possible), selecting the exposure time (expose as long as possible) and then saving the finished raw image. Nothing more was necessary, so everything was relatively easy. For image processing, just subtract a dark and a flat and adjust the tone curve a little in Photoshop. But CCDs do not behave the same as CMOS sensors, the sensors differ considerably in their technology and thus also in the settings for image capture (read our article on this subject, coming soon: CCD versus CMOS).

Das Gain

Gain is equal to amplification; in CMOS technology it means electronic image amplification. The gain is directly comparable to setting the ISO in a DSLR. Here there is the standard choice starting at ISO 100 up to ISO 6400 and with modern cameras far beyond.

The gain setting is one of the most important parameters for CMOS sensors. But beware: the correct choice of GAIN depends on the sensor type and thus on the camera in which the sensor is installed. The manufacturers usually only provide a so-called unity gain value, which is a good starting value for your shots. It is important to note that with the latest CMOS sensors, this should not be confused with the switching point between high and low read noise. With the advancements in CMOS technology, even at the lowest gain settings, the new 16-bit CMOS cameras exceed the requirements for the Unity GAIN setting (less than 1e/ADU).

At the end of this article you will find a table with unity gain settings for common QHY camera models. Later, as your expertise grows, you should optimize the GAIN setting for your needs, your local sky quality, and your standard exposure times. But keep in mind that changes in GAIN settings will also affect changes in other output parameters. The curves of the corresponding camera models show how these look.

The Unity Gain is the setting where Readout Noise changes from a lower to a higher value.

If you raise the ISO of a DSLR or a mirrorless camera from 100 to 800 or 1600 to get a brighter image with otherwise identical parameters (aperture, exposure time), you have to raise the gain on a cooled CMOS camera accordingly.

A GAIN of 1 or 0 is the minimum setting specified by the manufacturers and is comparable to an ISO setting of 6 to 12 on a DSLR. With this setting you could take pictures in bright sunshine.

ISO of a DSLR and GAIN of a CMOS camera have the same effect: when shooting with a very low GAIN, you have to expose for a very long time to get any signal at all from your subject. Tracking, sky quality etc. must be suitable or remain constant during the exposure time.

However, the noise components produced by the CMOS sensor and the sensor electronics (e.g. dark current) are constant! At low GAIN - when there is hardly any signal in the image - your raw images will therefore be very noisy and the signal of the subject will hardly stand out from the noise. When a very low GAIN value is chosen, the so-called full well capacity is also at its highest - and with it the image dynamics. Full well indicates how much charge (light photons) a pixel can collect before it is "full" and thus goes into overexposure with brighter stars. All the brightness that is collected has to be squeezed into the 16bit dynamic range afterwards, where the collected data is stored. (Of course, for this to happen, it must be recorded and stored in 16 bits!) A low GAIN therefore means a high dynamic range, but also longer exposure times and thus greater demands on the constancy of the observation conditions, and a poorer ratio of signal to sensor noise and dark current.

If you set the GAIN value too high for a better signal-to-noise ratio, the image dynamics will be reduced. Stars and bright objects such as the center of the Orion Nebula go into saturation, they will be overexposed and the central area of the nebula "burns out", i.e. there are no more shades of grey or colour, everything is white and overexposed.

Thus, the GAIN can be used to optimally adapt the image acquisition to your observation conditions. The faster your telescope is, the lower the GAIN can be set. Or you can use a shorter exposure time with a higher GAIN. The quality of "your" sky is also important: the darker the longer you can expose. With brighter skies, stack more frames to improve the signal-to-noise ratio.

By the way, the settings of GAIN and OFFSET can be found and adjusted in the ASCOM camera driver.

An example for better understanding:

The faster an optic is, the more the GAIN can be reduced for the same exposure time (compared to a slower telescope or smaller aperture)! In other words: with a faster optic, the exposure time can be shortened for the same GAIN.
If the GAIN value is increased with an average "fast telescope" (which, unlike a telephoto lens, has a fixed aperture or light intensity), the exposure time can be shorter.
-> This always refers to the background ADU and the brightest areas in the image.
There is more than one way to get the maximum of the night. The result is influenced by the number of exposures, the SNR in the stack, better seeing values through shorter exposure times, ...

After the exposure, the background in the image should not be above 10% saturation of 16Bit.
16Bit are 0-65535 tone values and 10% are around 6553 tone values (if you measure the ADU).
Also, the brightest areas of the image should not be overexposed (much)!
The centre of the brightest stars provides a good indication of whether it is not yet overexposed (or only very slightly). With more experience in image processing, this will become clearer, but it can be used as a basis.

The offset

However, there is a second important value to be determined for the optimisation of your CMOS raw images and that is the so-called OFFSET. The OFFSET shifts the histogram (the tone value curve) on the horizontal axis after the analogue-digital conversion.

The histogram shows the brightness distribution of your raw image after the analogue-digital conversion. The horizontal axis shows the distribution of the grey values and the vertical axis shows the number of pixels and thus the corresponding brightness.

Das Histogramm
Histogramm (Explanation in the text)

The offset corresponds to the gamma correction of the image and should be set so that in the end a value of at least 300 ADU remains for the background. This is checked on the exposed image after subtracting the correction images.

What is ADU?

Detailed information about the histogram and ADU (Analogue Digital Unit) can be found here(in German)

http://www.sbig.de/universitaet/glossar-htm/histogramm.htm
http://www.sbig.de/universitaet/glossar-htm/adu.htm

The maximum AD conversion is 16 bits, which corresponds to 65 535 grey levels between black (left in the histogram) and white (right in the histogram). With a 14 bit AD conversion, only 16 384 grey levels are represented; with a 12 bit AD conversion only 4096 grey levels. These grey levels are also called ADUs. With decreasing AD conversion, their histogram is thus compressed, so that the difference in the represented grey levels between black (sky background) and white (brightest stars) becomes significantly smaller.

The picture shows the ADU values of two measured objects for clarification. In the photo, the small planet 1991 RG7 (approx. 18th magnitude) is marked in the small square, and a reference star of the 12th magnitude is marked in the large square.

Es zeigt zur Verdeutlichung die ADU Werte zweier gemessenen Objekte. Im kleinen Quadrat der Kleinplaneten 1991 RG7 (ca. 18. Größenklasse). Im großen Quadrat dazu einen Referenzstern der 12. Größenklasse.

In the evaluation, the minor planet corresponds to number 1, the reference star to number 2. You can clearly see the difference in the two ADU values between 1157 and 39565. It is also logical that in the table the last column with the value for S/N (the signal-to-noise ratio) shows similar ratios. Of course, the small planet has a much worse S/N ratio than the brighter star.

However, let's stay with an AD conversion of 16 bits (0 to 65 535 ADU). After exposure, the background should not exceed 10% of the saturation, which is about 6500 ADU. Also, the brightest areas (bright stars) should not be overexposed yet.

Now, when taking deep sky images, you will always be on the left-hand side of the histogram and your (faint) object of observation will hardly stand out from the sky background. To prevent the signal from disappearing in the negative area of the histogram, the OFFSET shifts the tone curve to the right. The OFFSET should be set so that at the end the sky background remains at a value of about 300 ADU. If the OFFSET is set too low, so-called "dark patches" appear in the sky background, which are very difficult to correct in image processing - apart from the fact that they naturally lose object signal.

Determing the Correct OFFSET in Two Steps

You need to take two images to determine the OFFSET. These are a so-called bias and a dark frame.

To do this, first select an appropriate gain - either from your own experience or according to the output values that QHY CCD specifies for the camera model.

  1. The bias frame detects the electronic noise systematically generated by the AD converter for each pixel. The exposure is recorded with the shortest possible exposure time with the shutter closed (telescope aperture covered) so that no light hits the sensor. The resulting image ideally contains only the noise generated by the readout process itself for each individual pixel - it is referred to as read noise or readout noise.
The Bias as constant noise (but depending on the temperature). Dark current noise is dependent on temperature as well as exposure time and GAIN
The Bias as constant noise (but depending on the temperature). Dark current noise is dependent on temperature as well as exposure time and GAIN.

The bias frame MUST be taken with the same settings for GAIN, sensor temperature, binning and readout mode as the later raw images. Take 30 to 50 bias frames, stack and average them (e.g. DeepSkyStacker). Now you have to measure the signal of the background noise with an image processing software (Fitswork, Pixinsight, Maxim DL). The value should be around 850 ADU. Start with the preset OFFSET value in the camera driver (e.g. 55 for the QHY 268M or 60 for the QHY 600M).

2. Now a dark frame is captured. As with the bias frame, the GAIN, sensor temperature and readout mode must be the same as the images which are later taken of the deep sky objects. The dark frame is also exposed with the camera shutter closed or the telescope aperture covered.For each pixel, tt measures the respective ADU value, which is generated without light incidence only by thermal kinetic energy within the sensor and the camera electronics. This is the dark current noise (Dark Noise).

Now you have to measure the value of the noise again. The value should be about the same as the value of the bias frame, but never lower, otherwise the OFFSET must be increased. This is done either in the ASCOM driver of the camera or in the recording software.

For more accurate results, take several dark images again, which you stack and average.

These two calibrated correction images are essential for later image processing!

From now on, the following happens: If you now take an image of an astronomical object and download it from the camera, the data contains the signals of the camera (the noise) and the sky (the object).

Now, when bias and dark frame are subtracted, the pure signal of your observing object remains, bias and dark current noise are eliminated. By the way, even better than a normal bias is a flat dark.

What should not happen is that the sky background drops below 300 ADU. Otherwise, with 16 bits, the value is too close to zero! Then the OFFSET value must be raised slightly. Around 800 ADU after calibration is OK and corresponds to just under 1 % of the 16 bit tonal range - there is no loss of object signal.

So with the offset you shift the gamma value away from zero, but only so far that the values of darks and bias are about the same.

In addition, pedestal values can be added, often a value around 200 is preset.

By the way, the dark image not only corrects the noise, but also removes all missing pixels of the sensor (hot and cool pixels, see also here for more details). If there are still hot pixels left in the final image after stacking, you should take new darks - and remember that light must not be allowed to enter anywhere, not even at the focuser, the filter drawer or the like. If everything has been subtracted correctly, every hotpixel should have disappeared!

If you notice a pattern in the background, it often has to do with the bias and with a too small or inappropriate offset between the exposures during dithering! A solution is a larger pixel offset between the shots, a flat dark instead of a normal bias (see below) and checking whether the bias was applied correctly in the stack.

Hints:

  • If GAIN, OFFSET or Readout Mode are changed, the calibration images - Bias and Darkframe - MUST be retaken.
  • If you use bias frames, the image processing software MUST "know" that the dark frame also contains the bias value, otherwise it will subtract twice and result in increased noise or negative values

Tabel with Unity Gain values for some QHY cameras

CameraUnity GainSwitch Point High Gain / Low Gain Conversion
QHY 600 M/C25 at Extended Full WellPhotography Mode: 26 / High Gain Mode: 56
QHY 268 M/C30 at Extended Full WellPhotography Mode: 26 / High Gain Mode: 56
QHY 183 M/C10
QHY 163 M/C120
QHY 533 M/C6860
QHY 367C2800
QHY 247 C2200
QHY 128C3300
QHY 168C10
QHY 410C90 (Low Gain)
40 (High Gain)
QHY 294 M/C Pro1600 (11 Mp Mode)
2600 (47 Mp Mode)
11 MP Mode: 1600
QHY 174 GPS17
QHY 550P85

You can find the Unity Gain for further camera models on the QHY Website.

(1)Unity-Gain Value: For example, the latest CMOS sensors clearly show the switching point between "High Gain Conversion" and "Low Gain Conversion." Beyond this GAIN setting, the read noise (e-) drops significantly, and the dynamic range increases due to the lower noise ratio. This switching point between HGC and LGC is not the Unity Gain, where 1 electron per ADU hits the sensor (1e=1ADU).

Wolfgang Paech + Christoph Kaltseis im April 2022


 

About the authors: [br]

Christoph Kaltseis

Christoph Kaltseis is not only an Adobe Photoshop specialist and as Nikon Professional touring for Nikon, but also an experienced astrophotographer. He is one of the founders of the Central European DeepSky Imaging Conference (www.cedic.at), which is held every two years in Linz since 2009.

In addition to his various projects, Christoph has developed an innovative image sharpening process called APF-R (Absolute Point of Focus)in recent years. The procedure is not always the same, but is adapted to the combination of lens and camera. Therefore, a flexible method was necessary to achieve the desired results.

In his career as an astrophotographer Christoph has also created several APODs (NASA Astronomy Picture of the Day), e.g. the APF-R-processed image of the M33 Galaxy or the Heart of the Orion Nebula (M42).

View all posts from Christoph Kaltseis

Wolfgang Paech

Wolfgang Paech has been practicing astronomy for more than 50 years. In addition to his many experiences with observatory domes of all kinds, his core areas are the Sun and the Moon. On the german Website www.chamaeleon-observatory-onjala.de you will find a complete moon atlas, recorded with his standard technique. But even in terms of Deep-Sky and Planetary imaging, as a veteran astrophotographer for many years, nobody can fool him.

The 50+ years of amateur astronomy with many other areas, such as the restoration of historical amateur telescopes, polar light trips and much more are prepared on his private german website at www.astrotech-hannover.de.

View all posts from Dipl.-Ing. Wolfgang Paech

[br]

The QHY533 M/C cooled CMOS Camera is a very good and reasonably priced entry-level camera. It has everything a modern CMOS camera can do. For amateur astronomers interested in all areas of astronomical photography, the QHY 533 C/M can cover a wide range of your images. With its BSI Sony sensor, the camera is extremely sensitive and low-noise in the deep sky range. Thanks to the good cooling performance, long exposure times can be realized with it. The pixel size of 3.76 x 3.76 µm is optimally adapted for shorter focal lengths of 500 to 750 mm.
QHY533

More details can be found on our product page: [product sku="qhy533"]

The exceptionally low noise combined with high sensitivity of the simple and inexpensive QHY-CMOS cameras have made them the choice of many amateur astronomers for solar, lunar, and planetary photography, where stacking and processing a very high number of frames greatly improves the raw sum image ("Lucky Imaging"). With their low noise, the color cameras in particular are also suitable for EAA, i.e. Electronically Aided Astronomy, where the images are combined to a live image directly during the observation via LiveStacking. For this, the software Sharpcap is often used, which naturally supports the QHY cameras, too.

For a beginner, it can be confusing to choose the right camera to start with. We therefore advise you to proceed step by step, starting with the equipment that allows to track (guiding) a telescope mount in such a way that your first attempts will also show pinpoint star images.

Before deciding to buy a new camera, you should give some thought to the following points:

  • Which are the preferred observing objects?
  • Which sensor size do I need for this in combination with the telescope?
  • Which pixel size suits my focal length and "seeing"? There is a helpful calculator site: astronomy.tools
  • Should I work monochrome with filters or with a color camera (OSC - One Shot Color)?
  • Which computer capacity is available?
  • What is the budget?

QHYCCD Deep Sky Cameras for BeginnersQHYCCD Guiding- and Planetary Cameras[br]

Our recommendation for getting started: Guiding and planetary cameras

Guiding cameras for long exposures

For astrophotography with longer exposures, the guiding precision of the telescope mount is crucial. All mounts have some tracking error during the exposure, whether due to mount setup errors or other mechanical causes. This tracking error causes the stars on each shot to become distorted into dashes, which ultimately ruins the image.

The guiding camera, after selecting a suitable guide star - together with appropriate software - ensures that tracking errors of the mount are automatically corrected during exposure and the guide star stays centered on the sensor with sub-pixel accuracy. The guiding module can be connected to an external guiding scope (e.g. [product sku="variofinder"] or the [product sku="MiniGuideScope"] or directly to the imaging telescope via a so-called [product sku="QHYOffAxisGuider"].

QHYCCD has a long history of developing and producing guiding cameras, and was the first to introduce low-cost CMOS technology - including many of the company's own patents - to amateur astronomy. Also, many of the higher-end QHYCCD cameras have a guiding interface that is compatible with the SBIG ST4 standard.

The camera can then be connected directly to the mount via the ST4 interface; the guiding software still runs on the PC connected via USB. This is interesting if the mount is not controlled via the PC anyway. For example, if the mount is also controlled from the laptop via the ASCOM interface, the guiding signals can also be sent via this connection, and the ST4 cable is not needed. The most widely used guiding software is PHD2.

For beginners we would like to introduce two inexpensive modules at this point:

The QHY 5L-II-M is a 1.2 megapixel guiding camera with very high sensitivity (even faint stars can thus be used for tracking) and a USB 2.0 interface. They are ideal for use as lightweight autoguiders or planetary cameras where short exposures are typical.

[product sku="qhy5III678 "]

The second is the QHY 5-III-178M (no longer available) with a faster USB3.0 interface, which in addition to its guiding function can be used even better as a planetary camera for "lucky imaging" (sun, moon and planets) successfully because of the higher data rate. Die QHY 5-III-678 M/C ist die neueste Entwicklung der Version 2 der QHY 5III-Serie von Planeten- und Guidingkameras. Die QHY 5 III 678 M/C kann als verbesserte Version ihres Vorgängers, der QHY 5-III-178M CMOS Kamera betrachtet werden.

[br] The reason for recommending these two products is based on the basic requirements for a good guiding camera. It should have the following features:

  1. Small pixels. Smaller pixels result in higher resolution of the sensor, especially with short guide tube focal lengths and small apertures, which in turn relieve mechanical strain on the mount (size and weight of the guide tube). The QHY-5L-II-M and the QHY-5-III-178M have pixel sizes of 3.75 µm and 2.4 µm, respectively, quite small compared to many competitor cameras on the market.
  2. High sensitivity. Detecting and guiding to faint stars depends on the lens diameter of the guide scope (the larger, the fainter stars can be detected) and on the sensitivity of the sensor's pixels. The sensor of the QHY-5L-II-M has a quantum efficiency of 74%, and the QHY-5-III-178M uses a backside-illuminated sensor with a quantum efficiency of over 80%. With a suitable guide scope, both cameras can detect guide stars in the field of view, regardless of where the guide scope is pointed on the sky. Modern guiding software supports subpixel accuracy, so even a small guiding scope like the VarioFinder or the QHY MiniGuideScope is sufficient for large telescopes, the guiding accuracy is only limited by the air turbulence. An off-axis guider has the advantage that it sees the same image as the imaging camera and mechanical bending of the telescope during the night is not a problem, but it has a smaller field of view.
  3. Small and light weight. Both cameras have a diameter of only 25.4 mm and thus fit directly into any 1¼" eyepiece. The QHY-5L-II-M weighs only 51g, while the QHY-5-III-178M weighs 86 grams. The smaller the size and weight, the less mechanical stress is placed on the guide tube, focuser and mount.
  4. Both cameras are equipped with monochrome sensors, this is sufficient for a pure guiding function. The interface of the QHY-5L-II-M is USB 2.0, fast enough for guiding, while the QHY-5-III-178M has a faster USB 3.0 interface and can also be used as a monochrome solar, lunar and planetary camera due to the high frame rate.
  5. Cameras for "lucky imaging" of bright objects of the solar system. For beginners, photography of planets, the lunar surface and solar structures like sunspots is easier and more promising at the beginning, because the technical effort is much less complicated than in long exposures of deep sky objects. Since exposure times are very short in both guiding and lucky imaging, you can use one can for both applications. However, the module should then preferably have a fast USB 3.0 interface.

 

QHY 5-III Serie USB 3.0 Guiding and Planetary cameras:

The models of the [product sku="QHY5III" style="imgright"] are camera modules for solar, lunar and planetary photography (lucky imaging technique), as well as for guiding applications and partly work as cameras for deep sky photography for beginners with fast USB 3.0 data transfer.[br]

We offer the following products of QHY 5-III series:

Model
QHY-5-III-174M/C 

Mono/
Color

QHY-5-III-178M 

Mono

(no longer available)

QHY-5-III-485C  

Color

QHY-5-III-585C  

Color

QHY-5-III-462 M/C  

Mono/
Color

QHY-5-III-200M 

Mono

QHY-5-III-678 M/C  

Mono/Color

QHY-5-III-715C  

Color

QHY-5-III-290M 

Mono

(no longer available)

Sensor IMX174 IMX178 IMX485 IMX585 IMX462 SC2210 IMX678 IMX715 IMX290
Technology FSI-CMOS BSI-CMOS BSI-CMOS BSI-CMOS BSI-CMOS BSI-CMOS BSI-CMOS BSI-CMOS BSI-CMOS
Format 1/1.2" 1/1.8" 1/1.2" 1/1.2" 1/2.8"
1/1.8"
1/1.8" 1/2.8" 1/2.8"
Sensor Size 11,3 x 7,1 mm 7,4 x 5 mm 11,2 x 6,3 mm 11,1 x 6,3 mm 5,6 x 3,2 mm 7,68 x 4,32 mm 7,7 x 3,2 mm 5,6 x 3,2 mm 5,6 x 3,2 mm
Effective Array 79 mm² 36 mm² 71 mm² 70 mm² 17 mm² 33 mm² 34 mm² 17 mm² 17 mm²
Ratio
16:10 3:2 16:9 16:9 16:9 16:9 16:9 16:9 16:9
Resolution 1920*1200 (2,3 MP) 3072*2048 (6,3 MP) 3840*2160 (8,4 MP) 3.856*2.180 (8,4 MP) 1920*1080 (2,1 MP) 1920*1080 (2 MP) 3856*2180 (2 MP) 3840*2192 (2 MP) 1920*1080 (2,1 MP)
Pixel Size 5,86 µm 2,4 µm 2,9 µm 2,9 µm 2,9 µm 4 µm 2 µm 1,45 µm 2,9 µm
Frame Rate
138 fps 50 fps 44 fps 41 fps 44 fps 96 fps 41 fps 42 fps 44 fps
ADC-Bit depth 12 bit 14 bit 12 bit 12 bit 12 bit 12 bit 12 bit 12 bit 12 bit
Full-Well capacity 32 ke- 15 ke- 12 ke- 32 ke- 12 ke- 8 ke- 9 ke- 5,7 ke- 15,7 ke-
Pixel-Fov (@1000mm) 1,21" 0,5" 0,6" 0,6" 0,6" 0,83" 0,41" 0,3" 0,6"
 

Simulated field of view of the cameras in combination with a focal length of 1000mm

Simulated field of view of the cameras in combination with a focal length of 1000mm

The QHY-5-III series offer a choice of 7 models in total, counting mono and color versions. All offer variants of the Sony STARVIS™ or PREGIUS™ (QHY174) image sensors, designed for surveillance and industrial use.

Primarily, the models differ in sensor size, resulting in the field of view, as can be seen with the moon and an exemplary telescope. The models can be roughly divided into three size classes, whose physical dimensions are defined by their optical format:

  • 1/2.8“, ⌀6,4mm (5,6 x 3,1mm)
  • 1/1.8“, ⌀8,9mm (7,7 x 4,4mm)
  • 1/1.2“, ⌀12,8mm (11,2 x 6,3mm)

The majority of the installed detectors of the planetary cameras are constructed in an aspect ratio of 16:9. Between sensors in the 16:9 video format, the QHY 5-III-178 has a sensor in the classic 3:2 image format, the largest representative QHY 5-III-174 has a rarer 16:10 format. The format, in combination with the resolution, defines the digital output format: for example, the QHY 5-III-462 and QHY 5-III-200 shoots in 1080p HD format. An increasing number of cameras store 4K image & video files, including the QHY 5-III-715/678/485 & 585. You're very flexible in terms of shooting format choice with the QHY 5-III-178 (no longer available) and QHY 5-III-174 with digital crop offer the choice of several ratios, including 1:1, 6:5, 5:4, 4:3, 3:2, 16:10 and 2:1.

Sony STARVIS™ sensors stand for highly sensitive BSI sensors with rear integrated conductive tracks. These allow the area of the photodiode to be maximized in favor of the highest possible conversion rate (quantum efficiency). Sony PREGIUS™ sensors are characterized by a global shutter. Here, the sensor is read out completely, instead of the usual line-by-line readout in rolling shutter cameras. Motion artifacts can thus be excluded.

In the two STARVIS™ generations of Sony sensors, the substrate of the photodiodes is physically deeper than in previous ones, so that photons with longer wavelengths (NIR) can also penetrate deeper into the substrate and release an electron. In addition, the surface of the photodiodes is slightly rough at the microstructure level so that longer wavelength light is refracted and detected. These measures dramatically increase the sensitivity of the sensor to red and near-infrared light. The peak sensitivity (quantum efficiency) of the sensor in the NIR spectral range is almost as high as for light in the visible spectrum. Camera models in the latest generation of STARVIS 2 sensors include the QHY 5-III-678 and QHY 5-III-585, which feature sensitivity enhancement as well as higher dynamic range.

Sony PREGIUS™ sensors are characterized by a global shutter. Here, the sensor is read out completely, instead of the usual line-by-line readout in rolling shutter cameras. Motion artifacts can thus be excluded. The QHY 5-III-174 is the only planetary camera to offer a sensor from this product line.

A special technical feature distinguishes the QHY 5-III-462 and QHY 5-III-485: Their sensors of a new generation feature a "Super High Conversion Gain" mode. The sHCG function allows the generation of a strong output signal at low illuminance and very low readout noise of less than one electron.

The QHY 5-III-178 is the only one of the models to feature 14-bit analog-to-digital conversion on the hardware side and can thus natively discern 16384 brightness steps.

Which planetary cameras are particularly suitable for beginners?

In the color camera segment, we recommend two options:

The [product sku="QHY5III462C" style="imgright"] offers the highest frame rate with full HD resolution as a high-performance planetary camera and, as a special feature, outstanding sensitivity in the infrared spectrum. In addition, it has an excellent price-performance ratio.

It is two CMOS cameras in one. As usual, it can be used to take normal one-shot color images of the planets of the solar system (including the Sun and Moon). In addition, due to the extremely low readout noise, RGB images of brighter DeepSky objects can also be captured at shorter exposure times using the Lucky Imaging technique.

Based on the same Sony sensor technology, but with four times the area, the QHY485 expands the feature set quite significantly, with 4K resolution and the ability to expose a larger area of sky. The high-resolution 8.3MP camera offers 4K resolution and the ability to ecapture a wider field of view - even as an all-sky camera with the included fisheye lens.

The [product sku="1931030"] does not have the sensitivity extended into the infrared part of spectrum, but with the sHCG mode it delivers raw images with exceptionally low readout noise (less than 1e-). The sensor and its electronics deliver frame rates of 18.5 frames (fps) and 16 bit data depth per second via USB 3.0 at full resolution, and even 44 frames per second at 8 bit data depth.

New in the portfolio of the manufacturer is the [product sku="1931031" style="imgright"], which has the technical capabilities of the QHY-5-III-485C but extends it with the extended sensitivity in the infrared spectrum similar to the QHY-5-III-462C and the [product sku="1931038" style="imgleft"], a low cost 2nd generation solar, lunar and planetary camera and at the same time a perfect guiding module for extremely short focal lengths. Similar to the QHY 5-III-462 M/C, the QHY 5-III-715C also features extended sensitivity in the near infrared spectral range.[br]

For those interested in mono cameras or potential filter users, the QHY-5-III-178M is exciting. Its very fine resolution sensor positions itself between those of the QHY 5-III-462 and QHY 5-III-485 in terms of area and resolution, and allows the choice of multiple shooting ratios with only minimal reduction in resolution.

The [product sku="1931024" style="qhy5III678" style="imgleft"] is the latest evolution of version 2 of the QHY 5III series of planetary and guiding cameras. The QHY 5-III-678 M/C can be considered an improved version of the QHY 5-III-178M camera. Like the Sony IMX 178, the new IMX 678 sensor from Sony is a back-illuminated (BSI) sensor in the 1/1.8 inch format. However, compared to the IMX 178, it has a higher resolution (smaller pixels) and a higher QE as well as an increased sensitivity in the near infrared spectral range (NIR).

If you have a need for a fast reading full HD camera, but without the limitations of a Bayer color filter, the [product sku="1931035" style="imgright"] is an exciting mono alternative to the QHY-5-III-462C. [br]

Telecentric System or Barlow Lens?

A Barlow lens is the best-known way to change the focal length and thus the focal ratio of a telescope. A telecentric system is similar to a barlow, but also contains an additional positive lens element. This makes it possible to change the focal length of the telescope and to achieve a parallel beam of light. For most applications, therefore, a barlow lens is fine; but especially in connection with narrow-band interference filters (as for solar observation in H-alpha), the more complex construction of a telecentric system is absolutely necessary. However, both systems have their own advantages

To understand the differences, you must first understand: The position of an image point depends on how far it is away from the centre of the image. With a Barlow lens, the distance increases with the extension factor, so the image is "blown up" after the Barlow.

Schematic presentation of the beams of light with a Barlow lens (dashed: without Barlow element). Light rays farther away from the image center (shown in orange and grey) diverge outwards. See also the animation.

[br]
With a telecentric, all the magnification is done purely within the telecentric system, so the light rays remain parallel and do not diverge outwards. This has some effects in practice.

Schematic presentation of the beams of light with a telecentric (dashed: without telecentric). Light rays farther away from the image plane (shown in orange and grey) remain parallel to those in the image plane (red). See also the animation.

[br]
One of the noticeable properties of a Barlow lens is that it extends the eye relief of an eyepiece, as it widens the optical path of the telescope. Depending on the design (long/short Barlow), the extension factor, the distance to the eyepiece and the focal ratio of the telescope, the eye relief can increase by 20-30%, which can be undesirable, especially with long focal length eyepieces with an already larger eye relief, if the optimal eye position is then high above the eyecup.

At first glance, this effect is unexpected, since the eye relief is a property of the eyepiece. However, due to the Barlow's diverging beams of light, it virtually becomes a part of the eyepiece, as it changes the expected properties of the incident beam of light. The eye relief of an eyepiece is specified for approximately parallel or converging light rays - for diverging light rays, the image plane moves further out.

The widened light beam can also cause light to bypass the lenses of the eyepiece and therefore vignette the image – the vignetting then does not come from the free aperture or the lens diameter of the Barlow lens, but originates in the eyepiece, which is too small for the resulting light bundle!

With telecentric systems, no light is shifted outwards, so the eye relief does not change. However, the light bundle does not widen either - if the lens diameter of the telecentric is smaller than that of the eyepiece or the camera sensor, this leads to vignetting.

Another effect that is often overlooked with Barlow lenses is the dependence of the magnification factor on the distance between the Barlow and the eyepiece/camera. The greater the distance, the higher the magnification – you can find more about this in this PDF: Calculating different Magnifications with the VIP-Barlow. For this reason, many barlow lenses from Baader Planetarium have a modular design and make it possible – similar to a zoom eyepiece - to find the ideal magnification, e.g. in order to adapt the magnification to the resolution of the telescope and camera in planetary photography. Of course, a Barlow only functions optimally in terms of sharpness at the magnification factor for which it was calculated.

Comparison of 2.25x Q-Barow (set to 3x with extension tubes) and [product sku="1363070"]

This is clearly visible in the example of the church spire. Here, for reasons of comparison, the 2.25x Q-Barlow is "abused" with extension tubes to 3x magnification - which causes a clear drop in sharpness. This is a good example that a Barlow lens should be operated in the magnification range for which it was designed.

With a telecentric system, on the other hand, the magnification factor is largely independent of the distance, even though it is also calculated for an optimal working distance. In practice, it is possible to deviate very significantly from this calculated ideal distance without noticeably changing the magnification and image quality. The TZ-3S, for example, has such a benign design that even the huge optical length of a bino-viewer does not cause any loss of contrast or sharpness. You can find test results for the Baader TZ-2 in this PDF:  Baader Telecentric System TZ-2 - How important is the Working Distance?
This means that a Barlow lens is more flexible regarding slight variations of the magnification factor, while a telecentric actually always delivers almost exactly the expected magnification – even if there are other accessories between the telecentric and the eyepiece.

Finally, the shifting of the fokal point must be considered, or more precisely the position of the focuser: with a Barlow lens, the focuser must be retracted one to two centimetres further than without. With a telecentric lens, the focus point shifts less – although this also depends on how well you want to maintain the ideal working distance. You can find more detailed information in this PDF: Baader Telecentric Systems (TZS) for H-α solar filters

This also has advantages and disadvantages. For example, a barlow is often recommended to get into focus even when the focuser cannot be retracted far enough. A special variant of a barlow lens is the glass path corrector, which changes the focus position for a bino-viewer in such a way that you can still come into focus. Please note: A glass path corrector is not a pure barlow lens, but a special variation of it. Since it also corrects the refractive effects of the prisms of a binocular viewer, it is constructed differently from a Barlow lens.

Telecentric Systems and Solar Observation

So both barlow lenses and telecentric systems have their advantages, and with good manufacturing quality they take little away from each other for most applications. For H-alpha solar observation, however, there is no alternative to a telecentric system: with a Barlow lens, the divergence of the rays causes the light rays to pass through the actual H-alpha filter (the etalon) at a slight angle with increasing distance from the centre of the image.

Since an etalon (also known as a filter according to Fabry-Pérot) is based on interference, it is important that the light travels the exact, shortest length between the two λ/100 plane-parallel surfaces of the etalon. It is important to understand that a beam of light in such an etalon - which is only ~2/10 mm thick - is reflected back and forth between the dielectric coatings on both sides up to 1000 times! This is the only way that all unwanted wavelengths can be cancelled out by interference, leaving only the H-alpha light. However, if the beam of light entering the etalon is already divergent because of a Barlow lens – or convergent through a native f/30 objective – then, with a thousandfold reflection, the extinction in the etalon will be different towards the edge than in the centre. As a result, the Half-Band-Width (FWHM) of such an incorrectly used etalon also changes from the centre to the edge ever so slightly, which is absolutely undesirable for high-precision filters with a 0.3-0.7 angstrom (Å) passband. As already mentioned - even telescopes that would by default have the desired focal ratio of f/30 or slower do not have the parallel beam path of a telecentric. In this case, the beam path will still be slightly conical and turn a 0.5Å filter into a 0.7Å filter – or lead to an even wider passband (FWHM).

That's why Baader Planetarium has been offering telecentric systems for many years which are made especially for the high-end Solar Spectrum solar filters and comparable designs, where the etalon is placed far behind the objective. They have been specially designed for the H-alpha line. Since 2022, the series has been supplemented by the achromatic SunDancer II TZ3-S, which is designed for the entire visible spectrum – and thus can even be used for observing the calcium-line when combined with a Calcium-K-line-etalon.

The only disadvantage of telecentrics for H-alpha observation – which is the very long focal length due to the desired focal ratio of f/30 – can be partially compensated for with a reducer (0.4x or 0.7x telecompressor) calculated for the telecentric.

Example of use: [product sku="2459257"]

The Telecentric Systems made by Baader Planetarium

The  [product sku="1363070" style="imgright"] complements the range of Baader telecentrics since 2022; the telecentric is also used in the SunDancer II H-alpha filters - but there additionally with an integrated block filter (which is not available separately). For use with other H-alpha filters that already have a block filter, the TZ3-S is now also available separately without a block filter.

As an achromatic system, it delivers a sharp, high-contrast image across the entire visible spectrum. The image circle at a distance of 96mm is 35mm, making it ideal for planetary photography and for camera sensors up to this diagonal (or generally with a 1.25" mount). On the camera side it offers a T-2 thread, on the telescope side it is equipped with a dual 1.25"/2" nose-piece.

Also since 2022, the [product sku="1363080" style="imgleft"] completes the series of SunDancer telecentrics. Just like the TZ-3S, it is an achromatic system, but with a much larger image circle of 36 mm and a working distance of 97 mm.This makes it suitable for all but the largest SolarSpectrum H-alpha filters, as well as for high-resolution solar and planetary photography in white light. For use with the SunDancer II H-alpha filter, the blocking filter of the H-alpha filter must be installed in the TZ-4S.

The Telecentric System tZ-2 and [product sku="2459256"] have been on the market for some time and were designed especially for the H-alpha line at 656.3nm, where they have their highest Strehl ratio. Both have T-2 connection threads on both sides and a 2" nose-piece on the telescope side. The TZ-2 is no longer in production, because there are no more f/15-telescopes available, too – and as a not achromatic system, it is only suitable for H-alpha-filter at telescopes with such a slow f/ratio. The TZ-4 is still in production and best for telescopes with approximately f/7.5.

Depending on the telescope system used, the [product sku="2459257" style="imgright"] delivers up to 99% Strehl at the H-alpha line of 656.3 nm, even for Calcium-K (396nm) it still delivers diffraction-limited imaging with approx. 80% Strehl. Compared to the twenty years older TZ-4, it offers not only a significantly better optical calculation, but also a larger field of view: With 46mm free aperture, it fits perfectly to the large SolarSpectrum Research Grade filters with 46mm aperture. This means that large camera sensors can also be used on large telescopes with a correspondingly large focal length, in order to survey the entire sun if necessary or to photograph large fields – depending on the resulting focal length. Not least because of the larger image detail, it can make sense to use the Research Grade TZ-3 instead of the TZ-4 and to stop down the telescope to get the required f/30. The loss of lens resolution is usually compensated by the better filter contrast and in combination with a telecompressor the focal length can be reduced.

The 2" Research Grade TZ-3 has 2" SC- T-2 threads on both sides, so that even heavy cameras and filter units can be firmly screwed to the focuser without tilting.

Telecompressors for Telecentric Systems

The free aperture of both the telecentric and the H-alpha filter as well as the focal length of the telescope determine the field of view – i.e. how much of the sun is visible at once.

If a telecompressor (reducer) is used behind a telecentric system, the magnification decreases again, while the image section remains the same. So with a telecompressor, you don't see more of the sun, but the magnification decreases, so that the entire, now smaller image may fit on a camera sensor or observations are possible even in poor seeing, when otherwise the minimum magnification (with high air turbulence) would be too high.

The [product sku="2459260" style="imgright"] reduces the focal length loss-free by a factor of 0.4x. The field of view is then 16 mm at a distance of 74 mm from the camera sensor. Similar to a Barlow lens, the reduction factor depends on the distance, so the working distance should be maintained. Since it significantly compresses the field of view given by the H-alpha filter system, vignetting occurs with large sensors and smaller H-alpha filters, so it is suitable for the large Research Grade filters with 46 or 32 mm aperture.

Due to the smaller lens diameter, the [product sku="2459259" style="imgleft"] can only accommodate the beam of light produced by a filter with an etalon with a maximum diameter of 35 mm. But since it compresses the image less, a 25 mm etalon diameter with the TZ-3, for example, results in a field diameter of approx. 17 mm, so the usable field is comparable to the 0.4x telecompressor. The 0.4x telecompressor would therefore illuminate the same sensor size – but the image section including the sun would be smaller, and a larger part of the image would be vignetted or would only show the back of the filter mount.

Baader M68-Tilter

[product sku="2458170"]

 

Baader M68 Adapter with M68-Tilter + UFC for the QHY600M camera

Baader M68 adapter with M68-Tilter + UFC for the QHY600M camera

The Baader M68 is a system that fulfils many wishes in an elegant way and with high stability. All distances can be set precisely, and with the [product sku="2458170"] an ingenious extension has been added to the system.

But before talking about the tilter, let me tell you how I came to this system. When I was testing the prototype of the [product sku="baaderfcct"] for the RASA 8, I wished that the connection and collimation possibilities for the C14 were just as sophisticated. I have acquired enough experience so that I can "read" the image of the C14 so well that I know whether I am really seeing a tilt or just a problem with the distance. Of course, this led to the desire to use a tilter to adjust the field perfectly to the camera sensor.

I mentioned this idea in passing once during a conversation with the Baader company, and we discussed what functions would have to be incorporated so that imaging with the C14 EdgeHD could be optimised as easily and smoothly as with the RASA 8 and the FCCT. After all, we are talking about a large Schmidt-Cassegrain telescope, and that should be capable of 36.3MP full-frame images – or even more?

The fact that I kept coming close to ma desired image quality, but couldn't reach what I would have liked, may also be due to the fact that I use five different cameras on the C14, and each one is a little bit different, with small subtle differences in sensor position and distance (back focus). It has been clear to me for some time that the backfocus on the EdgeHD has to be met with a tolerance of 0.2mm! And the images get even better when the error is smaller.

Well, and now there is this little "M68 filter wonder", and the handling is very good! But that doesn't change the fact that the optics really have to be very well collimated! Because, of course, it is not possible for a tilter to solve every problem. But if everything fits, then even 61 megapixels can be used on the C14 EHD, with round stars from one corner of the image field to the other.

And how do you get the most out of a 61 megapixels camera attached to the C14EdgeHD? My first tip for proper preparation is to buy a Celestron EdgeHD directly from Baader, because they know a significant tad more about it - I can't write why now, but I know it.

When preparing the optics and adjusting the accessories to match the backfocus, the distance for the M68 system with the tilter unit has to be calculated 0.2 - 0.3mm shorter than the ideal working distance of 146.05mm of C9.25, C11 and C14 EHD telescopes! In the white paper on the EdgeHD series you can see what shape the stars have over the field of a full-frame camera when the distances are correct.

Tip: If you manage to install the M68 tilter in the system so that the screws on the tilter meet the image diagonals and the left / right or top / bottom corners, it is even easier to adjust the system perfectly!

Baader M68 adapter + M68-Tilter + Nikon D810A

Baader M68 adapter + M68-Tilter + Nikon D810A

The camera adapter with the M68 tilter is then attached to the EdgeHD and the star must be focussed with an accuracy of 99.9%. Only then the optics are in "best shape" and photography with up to 61.1MP is feasible.

Then I attach the Nikon D810A and place the tilter into the adaptation in such a way that even if I change the camera, the tilter remains in the system just as it was when I made the adjustment!

When everything is really in place, I collimate the EdgeHD with the help of that star so that the secondary mirror is perfectly orientated to the main mirror. Important: Do not be satisfied with 99% perfection, but gor for 99.9%! This can be done at any moon phase with really GOOD seeing. Then it is the time for the tilter.[br]

What must be done and be taken care of?

Der Baader M68-Tilter on the Celestron C14 EdgeHD. Checking the image in the field with a full frame camera and 36.3MP.

Der Baader M68-Tilter on the Celestron C14 EdgeHD. Checking the image in the field with a full frame camera and 36.3MP.

I use a sturdy dew cap instead of a flexible one that fits exactly on the two 3" rails on the C14. Thus it is not "crooked" - I checked that! To see the field tilt better, I use a Bathinov mask. I put this on the dew cap (flat and not sticking out) and adjust the focus, then I take a picture of about 30 seconds so that I can check the field. (The tracking must be TOP, because otherwise you will try to adjust for this error, too!)

Now I can focus on the worst corner of the image where the Bahtinov mask shows the greatest deviation. I move the star to the corner of the image and change the focus NOT AT ALL! For this, it is ideal if I have previously aligned the M68 Tilter with the axes of the sensor (as far as possible), because then I can find the right adjustment screw with simple trial and error - i.e. by turning a screw and seeing what happens!

If the  image changes in such a way that the middle line of the Bathinov pattern moves towards or away from the centre, then it is the right screw. If nothing happens, then the selected screw is not effective in that corner of the image. Yes, this method requires some time, and I had to work out the practice first.

Tip: As a further aid, the Bathinov mask can be rotated by 90° to see the deviation clearly, if necessary.

Write everything down, note every "turn" of a screw and don't forget: If you can assign a screw to a corner of the picture, make a sketch of it. This sketch shows the position of the M68 tilter in the M68 system. Give each screw a NUMBER and then enter this number in a second sketch, which should represent the sensor. Then you know, screw 1 changes this,... Then you have completed this exercise!

After every second screw that was used for the adjustment, the following applies: Place the star exactly in the centre again and focus! Because the closer you get to perfection, the smaller the deviation of the centre line becomes! Therefore, the focus must be perfect, then you will always recognise the one corner of the picture that still needs to be corrected. This sequence is interrupted by test shots, so expose for 30 seconds and look for the worst picture corner! The whole thing ends at the point where all  corners of the image are at 99% perfection.

If the stars in all the image corners are slightly elongated (egg-shaped towards the outside!) because we used a 0.2-0.3mm shorter backfocus to allow for tilting, then the distance must now be lengthened by 0.2 - 0.3mm. For this purpose, Baader M68 offers M68 Fine-Adjustment rings made of aluminium (0,3 / 0,5 / 1 mm). These are inserted quickly. Then: Focus again and check the field, but this time without the Bathinov mask! In case there is a deviation, simply adjust again, the sketches should make this easier!

Tip: Check the settings of the camera or camera driver if there is an automated flip or a rotation when downloading to the computer – if the images are automatically rotated, the assignment of the screws will not be easier! Depending on this, you can deactivate this automatic image rotation!

Conclusions:

This way, the whole system can be adjusted; if the M68 tilter is removed together with the camera, the adjustment is retained even when the camera is replaced with another one. With the tilter, the M68 system now not only offers the possibility to mount even heavy accessories stable and without vignetting, but is extended by the possibility of simple and stable adjustment.

Iris Nebula NGC 7023 at 3910mm with Nikon D810A

Iris Nebula NGC 7023 at 3910mm with Nikon D810A

The purpose of an Energy Rejection Filter is to prevent as much solar energy as possible from entering the telescope in the first place and thus avoid excessive heating of the etalon of an H-alpha filter.

This is done most effectively by a filter in front of the telescope. At the same time, this prevents the air in the tube from heating up - the telescope remains close to the ambient temperature, and there are no air turbulences inside of the OTA due to temperature differences. If we look at the solar spectrum, it becomes clear that such a filter must primarily block visible light. Ideally, it reflects the solar energy energy instead of absorbing it and and does not heat itself up in the process as well - that's why these filters are called Energy Rejection Filters (ERF for short).

Since it is occasionally asked: A Herschel wedge or a white-light front-filter cannot be used as an ERF because it also darkens the H-alpha line. In H-alpha, the sun is far less bright than in white light, so there would be practically no light left to observe.

The solar spectrum with (red) and without (yellow) the absorption by the Earth's atmosphere. Quelle: https://en.wikipedia.org/wiki/File:Solar_spectrum_en.svg

The solar spectrum with (red) and without (yellow) the absorption by the Earth's atmosphere. Quelle: https://en.wikipedia.org/wiki/File:Solar_spectrum_en.svg

There are usually three types of filters mentioned, when Energy Rejection Filters are discussed.

The most effective ones are Baader D-ERF, which are dielectric Energy Rejection Filters. The dielectric coating allows steep filter edges, so that only the wavelengths around the H-alpha line pass through. (As a special case, D-ERFs can also be made for other spectral lines such as the calcium line at 393nm, or as in the case of the Baader Triband telescopes, they can be designed so that narrow-band deep-sky photography remains possible despite the energy protection filter).

A D-ERF has got a broad transmission window of 80nm centered around the H-alpha-line. All other wavelengths up to those far in the ultra-violet and infrared parts of the spectrum are blocked before they can reach the inside of the telescope. This way, the H-alpha-filter in the telescope's focuser is not stressed by large amounts of energy.

Transmission spectrum of a Baader D-ERF

Transmission spectrum of a Baader D-ERF

An older filter type are simple ERF filters made of red glass. In practice, there were three different types of these ERF filters made, each with its own disadvantages. The cheapest version was made of Aero Glass, which has been used since the 1980s. They let most of the red light (down to 580 nm) pass through and usually did not have very good optical quality. The filters with better optical quality used Schott RG610 or RG630 (or comparable) glass, which block up to 610 or 630nm respectively, but offer no protection from infrared radiation. The energy load for the etalon is therefore higher.

As third option, sometimes yellow ERF-Filters can be found – but they offer almost no protection against energy, as a look at the solar spectrum shows, and should be avoided at all costs. They are only a little bit better than no ERF at all.

As these Energy Rejecting Filters are placed in front of the objective lens, the demands on the optical precision are the same as for the front lenses, so that they are not cheap.

ERF – behind the front lens

Therefore, it becomes attractive to install the Energy Rejection Filter close to the H-alpha-filter, so that a smaller diameter is sufficient. This option is often discussed, especially in the case of self-builds. It has a few disadvantages, among others:

  • The inside of the telescope can heat up, which can cause seeing problems inside of the telescope. Thus, higher magnifications can't be used, and such a solution becomes mostly interesting for smaller telescopes, which can't magnify that high, anyway
  • If the tracking is not perfect and the sun moves out of the field of view, it can shine on and damage the inside of the telescope – just as when projecting the image of sun

Baader SunDancer II H-alpha Filter

[product sku="1363056"]

For smaller telescopes up to 80mm aperture and slower focal ratios (about f/8 or slower), there are complete systems such as the [product sku="1363056"], in which the block filter is paced in front of the telecentric and also corporates as an energy protection filter. The Daystar Quark filters also work without an additional ERF up to 80mm telescope aperture. With these H-alpha filters, the sun can also be observed without an expensive D-ERF; but an additional D-ERF can reduce bad seeing inside of the telescope tube if necessary or lets you use the H-alpha filter on larger telescopes, too.

Sometimes – not only on ATM-websites, but also by some dealers – a yellow ERF-front-filter or even a UV/IR-Cut-filter in front of the star diagonal (and thus in in front of the complete H-alpha-Filter-unit) is recommended as Energy Rejection Filter for these small H-alpha-systems. But a look at the solar spectrum shows the problems of this concept: Only a small fraction of the sun's energy is in the UV/IR part of the spectrum at all; while most energy is in the visible part.

The idea probably originates from visual observation of the sun in white light. There, a UV/IR blocking filter makes sense if you are not sure that the solar filter attenuates the visible light and completely blocks the invisible UV/IR radiation, too. For the eye, unfiltered UV/IR radiation is harmful because we do not notice it; for the filter system of an H-alpha filter, it is not a big problem: if it heats up the filter too much, you can see it in the temperature display and the decreasing image quality long before any damage occurs - unlike in the eye.

A simple UV/IR filter or a yellow filter is thus a bad choice as the only Energy Rejection Filter, as it lets most of the solar energy passes through it.

Our deep sky filters (Halpha, UV/IR and all others) are not suitable for use in a solar telescope near the focal point. They are designed for use in the night sky. The thin filter glass cannot withstand the concentrated solar energy and the mount cannot give the filter glass the necessary room to expand when heated. The filter will inevitably burst if you use it in a solar telescope near the focal point.

For solar observation, our deep sky filters can only be used as an additional safety (e.g. in the eyepiece or in a camera adapter) if an energy camera adapter), if an energy protection filter dampens the solar energy and they are not exposed to it unprotected near the focal point.

With home-made solutions (such as modified PSTs), you must ensure that all filters make sure that all filters fit together. Our Deep Sky filters are NOT intended as a replacement for (D-) ERF pre-filters or even as block filters for solar telescopes and solar filters from other manufacturers such as Coronado or Lunt! Please always use only the recommended accessories from the manufacturer of your solar/H-alpha telescope, and do not do not combine untested filters with your H-alpha filter/telescope. filter/telescope. This can cause damage to your equipment (telescope, solar filter, camera) or even your eyes! We strongly advise against from experimenting on the sun and therefore accept neither responsibility responsibility or liability if damage occurs during your own experiments! damage occurs during your own experiments!

The purpose of an ERF is to protect the expensive etalon from heating up beyond its operating temperature (and in no case beyond the highest storage temperature). If the operating temperature is exceeded, the central wavelength shifts away from the H-alpha line. An electronic temperature control with cooling counteracts this as far as possible. In earlier times, when 4" f/15 telescopes were used for H-alpha observation and no ERF filters could be used, the telescopes were simply stopped down to f/30 - and if the filter became too warm, the objective was covered until the filter had cooled down again. These observation breaks are still a good idea today – if the filter gets too hot, it will be damaged beyond repair.