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Bintel Glebe
Usually ready for pickup in 24 hours
Bintel 84 Wentworth park road, Glebe, 2073, NSW
Phone:(02) 9518 7255
Hours:
Monday9:30 am–5:30 pm
Tuesday9:30 am–5:30 pm
Wednesday9:30 am–5:30 pm
Thursday9:30 am–5:30 pm
Friday9:30 am–5:30 pm
Saturday9:30 am–4 pm
SundayClosed
Newly Added Products
Discover the latest and greatest telescopes, binoculars, and astronomy gear available now on the Bintel website.
2025 products
2025 products
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$4,950.00
Clarity right up to the edge - SWAROVISION Field Flattener
This type of image definition has never been achieved before in any other spotting scope, thanks to the field flattener lenses creating a virtually flat image. Even the finest structures are reproduced with razor-sharp clarity right up to the edge with no need for constant refocusing.
The result: every detail is instantly captured, producing a perfect image without any distortions.
Maximum contrast - Including HD optics
A highly innovative optics design combined with fluoride- containing HD lenses minimise interfering colour fringing. This enables maximum
colour fidelity and leads to a significant improvement in resolution and contrast.
The result: an even more lifelike, contrast-rich image.
A complete view - Large field of view and high zoom range
Nothing escapes you. Thanks to their wide field of view, the ATX/STX spotting scopes provide you with a broader, more exciting platform for your viewing experience.
In spite of their high zoom range, the new generation of spotting scopes offers a large field of view. This allows you to achieve optimum magnification and detail recognition and also makes it extremely easy for you to search for and find objects, especially if they are in motion.
Eye relief plus - Large field of view even for spectacle wearers
SWAROVISION features a long eye relief and the removable twist-in eyecup is individually adjustable.
The result: even spectacle wearers can enjoy a large field of view, not to mention the inimitable edge sharpness. An additional eyecup has been specially developed for spectacle wearers to further increase viewing comfort.
Maximum colour fidelity - Optimised coatings
The enhanced lens and prism coatings (SWARODUR & SWAROTOP) give noticeably better colour reproduction combined with even greater transmission. SWAROCLEAN coatings on the outer lens surfaces create a non-stick effect, making it easier to clean.
The result: even more impressive observing experiences, even in low light.
Ingenious System
The new modular design offers previously unimagined flexibility and you are free to choose the perfect solution as the situation dictates. In collaboration with experts we have developed digiscoping adapters that open up a new realm of ways in which to observe and share the most beautiful moments.
Perfectly designed down to the smallest detail, you will be equipped for any situation.
Just one hand
When every second counts. Imagine a plover flitting over the shore one minute and taking off into the sky the next. The ATX/STX spotting scopes ensure that you are prepared for moments like this. This is because the new position of the zoom ring, which is now directly behind the focusing ring, makes it easier to handle. It means that you can zoom and focus with one hand, while steering the spotting scopes direction with the other.
This completely new ergonomic design offers a crucial benefit for digiscopers in particular. They can now use the camera quickly, easily and accurately with one hand, while the other concentrates on zoom and focus.
Easy to transport
Not a gram too heavy for top optical performance. Size and weight is the name of the game for all those who like to travel or spend long days in the field. The ATX/STX series means that bulky spotting scopes that are difficult to pack and heavy to carry are a thing of the past.
The modular design enables you to store the objective and eyepiece modules separately and the smaller dimensions also mean that you can easily and safely store individual modules in your luggage.
Swarovski ATX 65 Spotting Scope Technical Data
| Magnification | 25 - 60x |
| Objective lens Ø (mm) | 65 |
| Exit pupil Ø (mm) | 2.6 - 1.1 |
| Eye relief (mm) | 20 |
| Field of view at m/1000 m | 41 - 23m |
| Field of view (degrees) | 2.4° - 1.3° |
| Subjective field of view, apparent (degrees) | 57° - 71° |
| Shortest focusing distance (m) | 2.1 |
| Dioptre correction at ∞ (dpt) | 5 |
| Light Transmission (%) | 86 |
| Objective Filter Thread | M 67 x 0.75 |
| Length (mm) | 339 |
| Weight (g) |
1585 |
| Focal Length with TLS APO (mm) |
750 - 1800 |
| Functional temperature | -25°C to +55°C |
| Storage temperature | -30 °C/+70 °C |
| Submersion tightness | 4m / 13ft water depth (filled with nitrogen) |
$8,920.00
The BTX combines the visual power of both eyes with a revolutionary viewing experience. Crucial subtleties can be seen with the crystal clear optics, with every detail now fully on show. A forehead rest and angled view guarantee comfortable viewing for hours on end.
| BTX 65mm | BTX 85mm | BTX 95mm | BTX 115mm | |
| Magnification | 30x | 30x | 35x | 35x |
| Magnification Plus ME1.7x Extender | 50x | 50x | 60x | 60x |
| Effective Objective Lens | 65mm | 85mm | 96mm | 115mm |
| Exit Pupil diameter | 2.2mm | 2.9mm | 2.7mm | 31.mm |
| Ext pupl distance | 21mm | 21mm | 21mm | 21mm |
| Fisld of view | 38 m/1000 m 112 ft/1000 yds |
38 m/1000 m 112 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
| Field of view (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, eyeglass wearers (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, apparent (degrees) | 60° | 60° | 60° | 60° |
| Shortest focusing distance | 2.2 m 7.2 ft |
3.8 m 12.5 ft |
5.0 m 16.4 ft |
5.0 m 16.4 ft |
| Diopter adjustment left/right | ± 4 dpt | ± 4 dpt | ± 4 dpt | ± 4 dpt |
| Diopter correction at ∞ | > 5 dpt | > 5 dpt | > 5 dpt | > 5 dpt |
| Interpupillary distance | 56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
| Objective filter thread | M 67x0.75 | M 87x0.75 | M 97x0.75 | M 118x0.75 |
| Approx. length* | 371 mm 14.6 in |
404 mm 15.9 in |
458 mm 18.0 in |
472 mm 18.6 in |
| Approx. weight | 2195 g 77.3 oz |
2520 g 88.8 oz |
2760 g 97.3 oz |
3520 g 124.2 oz |
| Functional temperature | -25/+55°C -13/+131°F |
|||
| Storage temperature | -30/+70°C -22/+158°F |
|||
| Submersion tightness | 4 m 13 ft |
|||
| Tripod thread | 1/4˝ UNC; 3/8˝ UNC | |||
$7,640.00
The BTX combines the visual power of both eyes with a revolutionary viewing experience. Crucial subtleties can be seen with the crystal clear optics, with every detail now fully on show. A forehead rest and angled view guarantee comfortable viewing for hours on end.
| BTX 65mm | BTX 85mm | BTX 95mm | BTX 115mm | |
| Magnification | 30x | 30x | 35x | 35x |
| Magnification Plus ME1.7x Extender | 50x | 50x | 60x | 60x |
| Effective Objective Lens | 65mm | 85mm | 96mm | 115mm |
| Exit Pupil diameter | 2.2mm | 2.9mm | 2.7mm | 31.mm |
| Ext pupl distance | 21mm | 21mm | 21mm | 21mm |
| Fisld of view | 38 m/1000 m 112 ft/1000 yds |
38 m/1000 m 112 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
| Field of view (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, eyeglass wearers (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, apparent (degrees) | 60° | 60° | 60° | 60° |
| Shortest focusing distance | 2.2 m 7.2 ft |
3.8 m 12.5 ft |
5.0 m 16.4 ft |
5.0 m 16.4 ft |
| Diopter adjustment left/right | ± 4 dpt | ± 4 dpt | ± 4 dpt | ± 4 dpt |
| Diopter correction at ∞ | > 5 dpt | > 5 dpt | > 5 dpt | > 5 dpt |
| Interpupillary distance | 56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
| Objective filter thread | M 67x0.75 | M 87x0.75 | M 97x0.75 | M 118x0.75 |
| Approx. length* | 371 mm 14.6 in |
404 mm 15.9 in |
458 mm 18.0 in |
472 mm 18.6 in |
| Approx. weight | 2195 g 77.3 oz |
2520 g 88.8 oz |
2760 g 97.3 oz |
3520 g 124.2 oz |
| Functional temperature | -25/+55°C -13/+131°F |
|||
| Storage temperature | -30/+70°C -22/+158°F |
|||
| Submersion tightness | 4 m 13 ft |
|||
| Tripod thread | 1/4˝ UNC; 3/8˝ UNC | |||
$6,930.00
The BTX combines the visual power of both eyes with a revolutionary viewing experience. Crucial subtleties can be seen with the crystal clear optics, with every detail now fully on show. A forehead rest and angled view guarantee comfortable viewing for hours on end.
| BTX 65mm | BTX 85mm | BTX 95mm | BTX 115mm | |
| Magnification | 30x | 30x | 35x | 35x |
| Magnification Plus ME1.7x Extender | 50x | 50x | 60x | 60x |
| Effective Objective Lens | 65mm | 85mm | 96mm | 115mm |
| Exit Pupil diameter | 2.2mm | 2.9mm | 2.7mm | 31.mm |
| Ext pupl distance | 21mm | 21mm | 21mm | 21mm |
| Fisld of view | 38 m/1000 m 112 ft/1000 yds |
38 m/1000 m 112 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
| Field of view (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, eyeglass wearers (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, apparent (degrees) | 60° | 60° | 60° | 60° |
| Shortest focusing distance | 2.2 m 7.2 ft |
3.8 m 12.5 ft |
5.0 m 16.4 ft |
5.0 m 16.4 ft |
| Diopter adjustment left/right | ± 4 dpt | ± 4 dpt | ± 4 dpt | ± 4 dpt |
| Diopter correction at ∞ | > 5 dpt | > 5 dpt | > 5 dpt | > 5 dpt |
| Interpupillary distance | 56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
| Objective filter thread | M 67x0.75 | M 87x0.75 | M 97x0.75 | M 118x0.75 |
| Approx. length* | 371 mm 14.6 in |
404 mm 15.9 in |
458 mm 18.0 in |
472 mm 18.6 in |
| Approx. weight | 2195 g 77.3 oz |
2520 g 88.8 oz |
2760 g 97.3 oz |
3520 g 124.2 oz |
| Functional temperature | -25/+55°C -13/+131°F |
|||
| Storage temperature | -30/+70°C -22/+158°F |
|||
| Submersion tightness | 4 m 13 ft |
|||
| Tripod thread | 1/4˝ UNC; 3/8˝ UNC | |||
$5,940.00
The BTX combines the visual power of both eyes with a revolutionary viewing experience. Crucial subtleties can be seen with the crystal clear optics, with every detail now fully on show. A forehead rest and angled view guarantee comfortable viewing for hours on end.
| BTX 65mm | BTX 85mm | BTX 95mm | BTX 115mm | |
| Magnification | 30x | 30x | 35x | 35x |
| Magnification Plus ME1.7x Extender | 50x | 50x | 60x | 60x |
| Effective Objective Lens | 65mm | 85mm | 96mm | 115mm |
| Exit Pupil diameter | 2.2mm | 2.9mm | 2.7mm | 31.mm |
| Ext pupl distance | 21mm | 21mm | 21mm | 21mm |
| Fisld of view | 38 m/1000 m 112 ft/1000 yds |
38 m/1000 m 112 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
32 m/1000 m 96 ft/1000 yds |
| Field of view (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, eyeglass wearers (degrees) | 2.1° | 2.1° | 1.8° | 1.8° |
| Field of view, apparent (degrees) | 60° | 60° | 60° | 60° |
| Shortest focusing distance | 2.2 m 7.2 ft |
3.8 m 12.5 ft |
5.0 m 16.4 ft |
5.0 m 16.4 ft |
| Diopter adjustment left/right | ± 4 dpt | ± 4 dpt | ± 4 dpt | ± 4 dpt |
| Diopter correction at ∞ | > 5 dpt | > 5 dpt | > 5 dpt | > 5 dpt |
| Interpupillary distance | 56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
56-72 mm 2.2-2.9 in |
| Objective filter thread | M 67x0.75 | M 87x0.75 | M 97x0.75 | M 118x0.75 |
| Approx. length* | 371 mm 14.6 in |
404 mm 15.9 in |
458 mm 18.0 in |
472 mm 18.6 in |
| Approx. weight | 2195 g 77.3 oz |
2520 g 88.8 oz |
2760 g 97.3 oz |
3520 g 124.2 oz |
| Functional temperature | -25/+55°C -13/+131°F |
|||
| Storage temperature | -30/+70°C -22/+158°F |
|||
| Submersion tightness | 4 m 13 ft |
|||
| Tripod thread | 1/4˝ UNC; 3/8˝ UNC | |||
From $1,349.00
At just over 4 inches in diameter and a few inches thick (IMX585), the new miniCAM8 is a compact, high-resolution, high-performance, cooled imaging system capable of exceptional, high-quality deep space images as well as high-quality, high-resolution planetary images.
So often, compactness in astro-imaging is achieved at the expense of some other critical feature found in multi-component cooled systems, such as sensor quality or thermoelectric cooling, etc. Such is not the case with the new miniCAM8. Based on Sony’s IMX585 8 MP sensor, the miniCAM8 includes full TE cooling capable of reaching a delta of -45℃ from ambient along with a built-in 8-position filter wheel for complete LRGB and narrowband imaging.
High Near-Infrared Sensitivity
The IMX585 is a Sony Starvis II processor that enables high sensitivity and high dynamic range (HDR). It also improves sensitivity in the near-infrared range by approximately 1.7 times* compared to the IMX485. The new camera miniCAM8 has a maximum quantum efficiency of 60% in the near-infrared band and 92% in the visible wavelength band.
*This data is officially provided by Sony: https://www.sony-semicon.com/cn/news/2021/2021062901.html
BSI
One benefit of the back-illuminated CMOS structure is improved full-well capacity. This is particularly helpful for sensors with small pixels. In a typical front-illuminated sensor, photons from the target entering the photosensitive layer of the sensor must first pass through the metal wiring that is embedded just above the photosensitive layer. The wiring structure reflects some of the photons and reduces the efficiency of the sensor.
In the back-illuminated sensor, the light is allowed to enter the photosensitive surface from the reverse side. In this case, the sensor’s embedded wiring structure is below the photosensitive layer. As a result, more incoming photons strike the photosensitive layer, and more electrons are generated and captured in the pixel well. This ratio of photon to electron production is called quantum efficiency. The higher the quantum efficiency, the more efficient the sensor is at converting photons to electrons, and hence the more sensitive the sensor is to capturing an image of something dim.
Zero Amplify Glow
miniCAM8 is also a zero amplifer glow camera.
Anti-Dew Technology
Based on almost 20-year cooled camera design experience, the QHY cooled camera has implemented the fully dew control solutions. The optic window has a built-in dew heater, and the chamber is protected from internal humidity condensation. An electric heating board for the chamber window can prevent the formation of dew, and the sensor itself is kept dry with our silicon gel tube socket design for control of humidity within the sensor chamber.
Cooling
In addition to dual-stage TE cooling, QHYCCD implements proprietary technology in hardware to control the dark current noise.
Variants
MiniCAM8M Deep Sky Combo -
The astronomical filters included with the miniCAM8 deepsky combo are custom-designed to match the specific characteristics of the cameras. The size is 19 mm * 12 mm * 1.1 mm. The LRGB and SHO narrowband filters for the miniCAM8M deepsky combo are customized by XiMei Filters. The LRGB filters have an optical density (OD) value of 3, while the narrowband filters have an OD value of 5.
MiniCAM8M Planetary Combo -
Includes: miniCAM8M x1; LRGB filter set x1; 20nm Methane filter x1; 40nm UV filter x1; 10nm Na filter x1
MiniCAM8M Photometric Combo -
Includes: miniCAM8M x1; u’, g’, r’, i’, z’ sloan filter set x1
| Model | miniCAM8 |
| CMOS Sensor | Sony IMX585 |
| Mono/Color | Both Available |
| BSI/FSI | BSI |
| Sensor Size | 1/1.2inch |
| Pixel Size | 2.9μm*2.9μm |
| Total Pixel Area | 3856*2180 |
| Effective Pixels | 8 MP |
| Full Well Capacity | 54ke-
Linearity HDR Mode: 46ke- |
| Readout Noise | 0.76 – 7.8 e-
Linearity HDR Mode: 1.0e- |
| Peak QE | M: 92%
C: R: 82%; G: 87%; B: 75% |
| Dynamic Range | Linearity HDR mode: The dynamic range reaches up to 46,300:1, equivalent to 93 dB or 15.5 stops. |
| A/D | Dual 12-bit (output as 16-bit) |
| Full Frame Rates | Full Resolution: 41.5FPS@8bit,23.5FPS @16bit |
| ROI Frame Rates | Full Resolution 1080Lines, 82FPS@8bit, 47FPS@16bit;640Lines, 177FPS@8bit, 105FPS@16bit |
| Exposure Time Range | 11μs-900sec |
| Shutter Type | Electronic Rolling Shutter |
| Built-in Image Buffer | 512MB DDR3 |
| Computer Interface | USB3.0 |
| Telescope Interface | 1.25 inch |
| Optic Window Type | AR+AR |
| Filter Wheel | Built-in 8-Position Carousel |
| Back Focal Length | 17.5mm |
| Cooling System | Dual Stage TEC cooler:
Long exposures (> 1 second) typically -45℃ below ambient |
| Weight | 480g |
$1,249.00
At just over 4 inches in diameter and a few inches thick (IMX585), the new miniCAM8 is a compact, high-resolution, high-performance, cooled imaging system capable of exceptional, high-quality deep space images as well as high-quality, high-resolution planetary images.
So often, compactness in astroimaging is achieved at the expense of some other critical feature found in multi-component cooled systems, such as sensor quality or thermoelectric cooling, etc. Such is not the case with the new miniCAM8. Based on Sony’s IMX585 8 MP sensor, the miniCAM8 includes full TE cooling capable of reaching a delta of -45℃ from ambient along with a built-in 8-position filter wheel for complete LRGB and narrowband imaging.
High Near-Infrared Sensitivity
The IMX585 is a Sony Starvis II processor that enables high sensitivity and high dynamic range (HDR). It also improves sensitivity in the near-infrared range by approximately 1.7 times* compared to the IMX485. The new camera miniCAM8 has a maximum quantum efficiency of 60% in the near-infrared band and 92% in the visible wavelength band.
*This data is officially provided by Sony: https://www.sony-semicon.com/cn/news/2021/2021062901.html
BSI
One benefit of the back-illuminated CMOS structure is improved full-well capacity. This is particularly helpful for sensors with small pixels. In a typical front-illuminated sensor, photons from the target entering the photosensitive layer of the sensor must first pass through the metal wiring that is embedded just above the photosensitive layer. The wiring structure reflects some of the photons and reduces the efficiency of the sensor.
In the back-illuminated sensor, the light is allowed to enter the photosensitive surface from the reverse side. In this case, the sensor’s embedded wiring structure is below the photosensitive layer. As a result, more incoming photons strike the photosensitive layer, and more electrons are generated and captured in the pixel well. This ratio of photon to electron production is called quantum efficiency. The higher the quantum efficiency, the more efficient the sensor is at converting photons to electrons, and hence the more sensitive the sensor is to capturing an image of something dim.
Zero Amplify Glow
miniCAM8 is also a zero amplifier glow camera.
Anti-Dew Technology
Based on almost 20-year cooled camera design experience, the QHY cooled camera has implemented the fully dew control solutions. The optic window has a built-in dew heater, and the chamber is protected from internal humidity condensation. An electric heating board for the chamber window can prevent the formation of dew, and the sensor itself is kept dry with our silicon gel tube socket design for control of humidity within the sensor chamber.
Cooling
In addition to dual-stage TE cooling, QHYCCD implements proprietary technology in hardware to control the dark current noise.
Filters
The astronomical filters included with the miniCAM8 deepsky combos are custom-designed to match the specific characteristics of the cameras. The size is 19 mm * 12 mm * 1.1 mm. The LRGB and SHO narrowband filters for the miniCAM8M deepsky combo are customized by XiMei Filters. The LRGB filters have an optical density (OD) value of 3, while the narrowband filters have an OD value of 5.
| Model | miniCAM8 |
| CMOS Sensor | Sony IMX585 |
| Mono/Color | Both Available |
| BSI/FSI | BSI |
| Sensor Size | 1/1.2inch |
| Pixel Size | 2.9μm*2.9μm |
| Total Pixel Area | 3856*2180 |
| Effective Pixels | 8 MP |
| Full Well Capacity | 54ke-
Linearity HDR Mode: 46ke- |
| Readout Noise | 0.76 – 7.8 e-
Linearity HDR Mode: 1.0e- |
| Peak QE | M: 92%
C: R: 82%; G: 87%; B: 75% |
| Dynamic Range | Linearity HDR mode: The dynamic range reaches up to 46,300:1, equivalent to 93 dB or 15.5 stops. |
| A/D | Dual 12-bit (output as 16-bit) |
| Full Frame Rates | Full Resolution: 41.5FPS@8bit,23.5FPS @16bit |
| ROI Frame Rates | Full Resolution 1080Lines, 82FPS@8bit, 47FPS@16bit;640Lines, 177FPS@8bit, 105FPS@16bit |
| Exposure Time Range | 11μs-900sec |
| Shutter Type | Electronic Rolling Shutter |
| Built-in Image Buffer | 512MB DDR3 |
| Computer Interface | USB3.0 |
| Telescope Interface | 1.25 inch |
| Optic Window Type | AR+AR |
| Filter Wheel | Built-in 8-Position Carousel |
| Back Focal Length | 17.5mm |
| Cooling System | Dual Stage TEC cooler:
Long exposures (> 1 second) typically -45℃ below ambient |
| Weight | 480g |
Solar Maximum is now happening - it's the perfect time to explore the ever changing featured on our nearest star.
The Sky-Watcher Heliostar 76Hα is a specialized prominence telescope designed with advanced safety features to protect the observer’s eyes. It incorporates multiple technologies, including an infrared thermal reflection film to effectively block heat and a dedicated ultraviolet (UV) filter to eliminate harmful rays. These features work in tandem to minimize stray light, ensuring a safe and enhanced viewing experience.
The Sky-Watcher Heliostar 76Hα is a specialized solar telescope designed for enthusiasts eager to explore the Sun’s dynamic features, particularly solar prominences. With a 76mm aperture and a focal length of 630mm (f/8.3), it offers a balanced combination of portability and detailed solar observation.
Key Features:
- Hydrogen-Alpha Observation: The Heliostar 76Hα utilizes a combination of front and rear filters to isolate the hydrogen-alpha wavelength at 656.28 nanometers. This narrowband filtering, with a bandwidth of less than 0.5 angstroms, enables observers to view solar prominences and surface details with exceptional clarity.
- Advanced Optical Design: Incorporating multiple technologies to protect the observer’s eye, the telescope features a thermal infrared reflection film, a special heat-blocking filter, and an ultraviolet light-blocking filter. These components work together to eliminate stray light and ensure safe solar viewing.
- Precision Focusing: Equipped with a 2-inch Crayford focuser, the Heliostar 76Hα allows for smooth and precise focusing adjustments, enhancing the overall observing experience.
The Sky-Watcher Heliostar 76Hα is an excellent choice for both novice and experienced solar observers, offering a safe and detailed view of the Sun’s dynamic phenomena.
Etalon Filter Technology
At the heart of most Hydrogen Alpha solar telescopes lies the etalon filter, a highly precise optical device that isolates the Hα wavelength from the rest of the Sun’s emitted light. An etalon is a type of interferometer, consisting of two parallel mirrors separated by a precise distance. The etalon works by reflecting light multiple times between the mirrors, selectively allowing only wavelengths that satisfy specific resonance conditions to pass through.
In the case of Hα solar telescopes, the etalon is designed to transmit light at the Hα wavelength while blocking all other wavelengths. The key to the etalon’s performance lies in its ability to tune the wavelength it transmits. This is achieved by adjusting the distance between the mirrors or by slightly tilting the etalon, which changes the interference conditions. This tunability is crucial because the Sun's emission at Hα can shift slightly due to Doppler effects as material moves across the Sun’s surface and atmosphere.
There are two primary types of etalon filters used in solar telescopes: single etalon and double etalon systems.
Single Etalon: A single etalon filter typically has a narrower bandwidth, providing high contrast for detailed solar observations but at the cost of limiting the field of view. This makes single etalon systems well-suited for viewing small, high-contrast features like prominences or filaments.
Double Etalon: A double etalon system uses two etalon filters in tandem to improve the wavelength selectivity, reduce the overall bandwidth, and enhance the contrast and image clarity across a wider field of view. Double etalon systems are preferred for more detailed solar studies because they can offer both a sharper image and better tunability, allowing for a more accurate depiction of solar dynamics.
Solis Etalon Technology: Sky-Watcher's Solis technology allows the Heliostar to achieve a 0.5A bandpass without the costly expense and complexity of a second etalon to achieve the same performance. This allows the observer to obtain detailed images of the solar disk right out of the box without any further expense.
Trifid Tuner: Inside the Heliostar is Sky-Watcher's Trifid tuning system. This tuner applies physical pressure to the etalon plates allowing the observer to reach the desired Hydrogen-band. The Trifid tuner uses three support veins to provide a secure tuning for the etalon.
What does Hα mean?
The Sun is mainly composed of hydrogen which it's been busily converting to helium for billions of years and will do for some billions of years to come. Hydrogen gas is energised by the Sun's radiation and emits light on certain wavelength. Hα refers to where one of these wavelengths.
Viewing the Sun through the Heliostar 76Hα lets you discover the Solar chromosphere which is the outer layer of the Sun's atmosphere in great details.
Rather than looking at the Sun in the intense white light we see with our eyes or via a regular solar filter which reduces the overall intensity of the Sun's light so it can be safely viewed with a telescope, a dedicated Solar telescope reveals such details as prominences on the edge of the Sun's disks, filaments, sunspots and more.
As the Sun is such a dynamic environment, what you'll see through this telescope will change from day to day.
Specifications
| Optical Design | Refractor OTA |
| Model Number | SWHELIOSTAR76 |
| Aperture | 76mm |
| Focal Length | 630mm |
| Focal Ratio | f/8.3 |
| Bandwidth | 0.5A |
| Solar Image Size | 6mm |
| Diagonal | 11.5mm 1.25" H-alpha blocking diagonal |
| Blocking Filter Size: | 11.5mm |
| Focuser | Dual-speed Crayford |
| Tube Length | 600mm |
| Weight | 3.8kg |
| Recommended Usage | Advanced Users |
Introducing the ASI676MC, the all-sky camera featuring a unique square
1/1.6-inch image sensor and a super high resolution of 12MP! It is perfectly suited for meteor recording and full sky surveillance. The
square format facilitates easier composition, making mosaic stitch simpler and more efficient, and the high resolution brings you clear details of the Sun and our Moon. With this camera, you may start your marvelous journey
to explore the boundless night sky.
Why Square Format?
One of the biggest benefits of AS1676MC's square format is it makes the whole mosaic construction process much easier by eliminating the need to consider the difference between the long and wide
sides of the format during mosaic stitching. Not only that, the square format also makes the AS1676MC more compatible with various types of lenses such as fisheye lenses and wide-angle lenses. Thus,
ASI676MC is more suitable for tasks such as meteor
recording and full sky surveillance.
Starvis 2 Technology
STARVIS is a sensor technology developed by Sony that surpasses the sensitivity of the human eye. STARVIS 2 is an advancement of STARVIS technology,
supporting an even higher dynamic range. With this technology, ASI676MC exhibits lower readout noise and dark current, along with significantly enhanced
sensitivity in the near-infrared spectrum.
No Amp Glow
AS1676MC does not have any amp glow, no matter
how long the exposure and how high the gain value
you set.
256MB DDR3
The camera is equipped with a USB 3.0 transmission interface and a built-in 256MB DDR3
cache to ensure stable and secure data transmission.
Higher QE Lower Readout Noise
The camera has a built-in HCG mode, which can effectively reduce readout noise at high gain. This allows the camera to maintain the same high dynamic range as it does at low gain. When the gain is 180, the HCG mode is automatically turned on. The readout noise is as low as 0.56e, and the dynamic range can still reach a level close to 11stops.
Quantum Efficiency
The QE curve and readout noise are very important parameters to measure the camera's performance. Higher QE and lower readout noise are necessary to improve the image signal-to-noise ratio. According to our estimation, the QE peak value of ASl676MC is about 83%.
Dark Current Noise
The ASI676MC's lower dark current noise means that the image signal-to-noise ratio is also higher, especially when photographing dark objects, it produces images with better sharpness.
IR-Cut Coated Window
ASI676MC is equipped with an IR-cut coated window in front of the sensor, with a diameter of 21mm and a thickness of 1.1mm. It effectively reduces infrared interference and improves image quality.
$549.00
One of the most anticipated astrophotography products of the the year is on the way!
Rotate your camera with ease and compose your shots with one click -ZWO CAA- ZWO CAA (Camera Angle Adjuster) is ZWO’s new camera rotator, designed to meet the needs of astro imagers looking for that perfect image composition, its outstanding performance, simplified composition process, automated software control , making astrophotography composition easy.
ZWO CAA, making astrophotography easy and fun.
Why ZWO CAA?
1. Compact and Lightweight Design
Despite its lightweight design, the ZWO CAA offers exceptional performance. Measuring 16.5mm thick, it replaces the standard ZWO adapter. Weighs only 465g.
2. High Efficiency
The ZWO CAA is equipped with a high-efficiency stepper motor for smooth and precise operation, which can be positioned precisely to the target angle. Its robust internal structure guarantees zero deformation in the full 360° rotation, ensuring stable and precise operation.
3. High Positioning Accuracy: 0.02°/step
ZWO CAA adjusts the camera angle with an accuracy of 0.02° for each step. The positioning accuracy of the ZWO CAA is better than 0.1 degrees, and the adjusted angular error will not exceed 0.1°.
4. High Rigidity and High Load Capacity: ≤25cN·m*
The ZWO CAA is highly rigid and able to withstand torques less than or equal to 25cNm (centiNm), maintaining operational accuracy and structural stability even under high load conditions.
*Tested by ZWO laboratory, the device can operate stably with ASI461+7x50EFW+1kg additional load (overall ≥4kg).
5. High Speed: 7.5°/s
The ZWO CAA rotates at a speed of up to 7.5° per second, reducing waiting times.
Multi-Compatibility
The ZWO CAA is compatible with a wide range of telescope types and supports multiple imaging software, including ASIAIR, ASIStudio, and ASCOM. It also allows manual control via a compatible hand controller*.
Easy Cable Management
ZWO CAA reduces cable management needs to a single Type-C data cable for power supply and control.
Product Details
- Type-C interface: Power supply and data transmission in one connection.
- HC interface: For connecting the hand controller.
- Locking slot: You can insert a standard hex wrench into the pin hole and lock the rotation to assist in removing jammed adapters or accessories.
Connection
- With the ZWO FF series refractors, with or without the reducer, you can use the standard adapters (M48) supplied with the telescope and your ZWO camera replacing the 16.5mm adapter with the CAA. if you have a Duo or 2600AIR camera and wish to use M54 then an optional adapter is available as an accessory.
- 55mm back focus distance:
Installation Steps
- Step 1. Install the CAA on the threaded drawer tube adapters.
- Step 2. Install the optional M54 (21mm) adapter to maintain the focusing distance.
- Step 3. Install your camera. If you are using a camera with an M48 interface you can change. the ZWO CAA camera threads from M54 to M48 using the supplied accessory plate.
Structural Dimensions
What’s in the Box?
Specifications
From $520.00
The Chroma Technology Z-Sloan SDSS Filter is a precision-designed astronomical filter tailored for photometric accuracy and advanced astrophotography. Conforming to the Sloan Digital Sky Survey (SDSS) photometric system, this filter isolates the z band, a region in the far-red to near-infrared spectrum, ensuring precise data collection and exceptional imaging performance.
With advanced multi-layer dielectric coatings, the Z-Sloan filter offers outstanding transmission in the z band, which typically spans wavelengths from approximately 850 nm to 950 nm, while effectively minimizing light from adjacent bands. It is particularly useful for observing cooler stars, distant galaxies, and objects obscured by interstellar dust, as the z band penetrates these regions more effectively than shorter wavelengths.
Engineered for durability and consistent performance, the Chroma Z-Sloan SDSS Filter maintains its precision under challenging imaging conditions. Whether used for detailed photometric studies or capturing stunning astrophotographic images, this filter provides exceptional clarity and accuracy in the far-red to near-infrared spectrum, making it an indispensable tool for astronomers and astrophotographers seeking superior results.
From $520.00
The Chroma Technology I-Sloan SDSS Filter is a high-precision astronomical filter tailored for photometric accuracy and advanced imaging. Designed in accordance with the Sloan Digital Sky Survey (SDSS) photometric system, this filter isolates the near-infrared (I) band, enabling detailed observations and vivid imaging of celestial objects in this spectrum.
Crafted with advanced multi-layer dielectric coatings, the I-Sloan filter ensures exceptional transmission in the I band while effectively blocking unwanted light from adjacent bands. It is particularly suited for capturing the subtle details of stars, galaxies, and other deep-sky objects in the near-infrared, where unique astrophysical phenomena can be observed.
Built to withstand rigorous use, the Chroma I-Sloan SDSS Filter offers durability and consistent performance across diverse imaging conditions. Whether used for precise photometric studies or astrophotographic projects, this filter provides unparalleled clarity and accuracy in the near-infrared spectrum, making it an essential tool for astronomers and astrophotographers striving for superior results.
From $520.00
The Chroma Technology R-Sloan SDSS Filter is a precision-engineered astronomical filter designed for photometric studies and astrophotography. Conforming to the Sloan Digital Sky Survey (SDSS) photometric system, this filter isolates the red (R) band, ensuring accurate measurements and stunning imaging of celestial objects in the red spectrum.
Featuring advanced multi-layer dielectric coatings, the R-Sloan filter delivers exceptional transmission in the red band while minimizing out-of-band interference. It is ideal for capturing the richness and detail of stars, galaxies, and nebulae, particularly those with significant red emission features, making it an essential tool for both scientific observations and high-quality astrophotography.
Durable and reliable, the Chroma R-Sloan SDSS Filter is designed to withstand challenging imaging environments while maintaining precise performance. Whether you're conducting detailed photometric analyses or creating vivid astrophotographic images, this filter provides outstanding accuracy and clarity in the red band, making it indispensable for astronomers and astrophotographers seeking superior results.
From $520.00
The Chroma Technology U-Sloan SDSS Filter is a high-performance astronomical filter engineered for precise photometric measurements and advanced imaging applications. Designed to align with the Sloan Digital Sky Survey (SDSS) photometric system, this filter isolates the ultraviolet (U) band, ensuring accurate and reliable data for scientific studies and astrophotography.
Constructed with advanced multi-layer dielectric coatings, the U-Sloan filter offers superior transmission in the ultraviolet range while minimizing out-of-band interference. It is ideal for capturing ultraviolet emissions from stars, galaxies, and other celestial phenomena, enabling detailed studies of astrophysical properties and producing visually striking imagery.
Built for durability and consistent performance, the Chroma U-Sloan SDSS Filter resists environmental degradation, maintaining its precision under diverse observing conditions. Whether used for professional research or enhancing your astrophotographic capabilities, this filter delivers exceptional accuracy and clarity in the ultraviolet spectrum, making it an indispensable tool for astronomers and astrophotographers alike.
From $520.00
The Chroma Technology I-Bessell Filter is a premium astronomical filter designed for photometric precision and advanced astrophotography. Aligned with the Bessell photometric system, this filter isolates the infrared (I) band, enabling accurate data collection and enhanced imaging of celestial objects in the near-infrared spectrum.
Utilizing advanced multi-layer dielectric coatings, the I-Bessell filter ensures exceptional transmission in the I band while effectively reducing out-of-band interference. It is ideal for capturing the subtle details and intensities of stars, galaxies, and other deep-sky objects, particularly in the near-infrared region, where many astronomical features become more prominent.
Durable and reliable, the Chroma I-Bessell Filter is designed to withstand challenging imaging environments while delivering consistent performance. Whether you're conducting precise photometric studies or capturing striking astrophotographic images, this filter is an essential tool for professionals and enthusiasts seeking accuracy and excellence in the near-infrared spectrum.
From $520.00
The Chroma Technology 8nm SII filter is a high-performance narrowband filter designed for astrophotography and scientific imaging. It isolates the Sulfur II (SII) emission line at 672.4nm with an 8nm bandwidth, offering excellent contrast and detail for capturing deep-sky objects, especially emission nebulae.
Crafted with precision, this filter incorporates advanced multi-layer dielectric coatings for outstanding light transmission and durability. Its 8nm design balances light collection and selectivity, effectively reducing light pollution and moonlight interference while allowing more signal for fainter objects. Whether you're imaging in urban environments or under pristine dark skies, the Chroma 8nm SII filter delivers sharp, halo-free results with minimal reflections, making it an essential tool for astrophotographers striving for stunning and detailed imagery.
From $840.00
The Chroma Technology 5nm SII filter is a high-performance narrowband filter designed for astrophotography and scientific imaging. It isolates the Sulfur II (SII) emission line at 672.4nm with a narrow 5nm bandwidth, offering excellent contrast and detail for capturing deep-sky objects, especially emission nebulae.
Crafted with precision, this filter incorporates advanced multi-layer dielectric coatings for outstanding light transmission and durability. Its 5nm design effectively minimizes light pollution and moonlight interference, making it suitable for imaging under a variety of conditions. Whether you're capturing images in urban settings or beneath dark skies, the Chroma 5nm SII filter delivers sharp, halo-free results with minimal reflections, making it a must-have for astrophotographers seeking stunning and detailed imagery.
From $1,040.00
The Chroma Technology 3nm SII filter is a high-performance narrowband filter designed for astrophotography and scientific imaging. It isolates the Sulfur II (SII) emission line at 672.4nm with an ultra-narrow 3nm bandwidth, delivering exceptional contrast and detail for capturing deep-sky objects, especially emission nebulae.
Engineered with precision, this filter features advanced multi-layer dielectric coatings for superior light transmission and durability. Its ultra-narrow design significantly reduces light pollution and moonlight interference, making it ideal for imaging under challenging conditions. Whether you're working in urban environments or under pristine dark skies, the Chroma 3nm SII filter ensures sharp, halo-free images with minimal reflections, making it an essential tool for astrophotographers aiming for stunning, detailed results.
From $520.00
The CHROMA TECHNOLOGY OIII (8nm) Filter is a versatile narrowband filter crafted for astrophotography and scientific imaging. Designed to isolate the Oxygen III (OIII) emission line at 500.7nm with an 8nm bandwidth, this filter provides excellent contrast while allowing more light throughput. It’s ideal for capturing stunning deep-sky images, particularly of nebulae, even in light-polluted or moonlit conditions.
Featuring advanced multi-layer dielectric coatings, the CHROMA OIII filter ensures outstanding performance and durability. Its design minimizes halos and reflections while maintaining superior transmission, making it a reliable choice for astrophotographers of all levels, whether working in urban skies or dark-sky locations.
From $840.00
The CHROMA TECHNOLOGY OIII (5nm) Filter is a premium narrowband filter designed for astrophotography and scientific imaging, offering a balanced combination of contrast and light throughput. This filter targets the Oxygen III (OIII) emission line at 500.7nm with a precise 5nm bandwidth, effectively reducing light pollution, moonlight, and other unwanted wavelengths. It provides enhanced contrast and detail, making it ideal for capturing faint nebular structures and intricate deep-sky details.
Built with advanced multi-layer dielectric coatings, the CHROMA OIII filter ensures high transmission and long-lasting performance. Its robust design and rigorous quality control make it an excellent choice for both professional and amateur astrophotographers, delivering stunning high-contrast images with minimal halos or reflections.
From $1,040.00
The CHROMA TECHNOLOGY OIII (3nm) Filter is a high-performance narrowband filter specifically designed for astrophotography and scientific imaging. Engineered with precision, this filter isolates the Oxygen III (OIII) emission line at 500.7nm, providing a tight 3nm bandwidth that significantly reduces light pollution, moonlight, and other unwanted wavelengths. The result is unmatched contrast and clarity, allowing you to capture faint nebular structures and intricate details in deep-sky objects.
Crafted with advanced multi-layer dielectric coatings, the CHROMA OIII filter offers exceptional transmission and durability, ensuring optimal performance for years of use. Its strict quality control standards make it an ideal choice for professional and amateur astrophotographers alike, delivering sharp, high-contrast images with minimal halos or reflections.
From $840.00
The 5nm Chroma H-BETA Filter is a high-performance astrophotography tool crafted to capture stunning details in hydrogen-beta emission nebulae. With its precise 5nm bandwidth, this filter isolates the H-Beta spectral line (486.1nm), boosting contrast and revealing intricate structures in faint nebulae like the Horsehead Nebula and the California Nebula.
Built with premium optical coatings, the Chroma H-BETA filter ensures excellent transmission, maximizing light throughput while effectively blocking unwanted wavelengths such as light pollution and moonlight. Its robust design provides exceptional durability, scratch resistance, and consistent performance across a variety of imaging systems.
Whether you’re using a DSLR, CCD, or CMOS camera, the 5nm Chroma H-BETA filter is an ideal choice for astrophotographers aiming to enhance the depth and detail in their deep-sky images. Discover the cosmos with clarity and precision, as only Chroma can provide.
From $1,040.00
The 3nm Chroma H-BETA Filter is a premium astrophotography tool designed for capturing breathtaking details in hydrogen-beta emission nebulae. With a precise 3nm bandwidth, this filter isolates the H-Beta spectral line (486.1nm), enhancing contrast and revealing subtle features in faint nebulae like the Horsehead Nebula and the California Nebula.
Engineered with superior optical coatings, the Chroma H-BETA filter offers exceptional transmission, ensuring maximum light throughput while effectively blocking unwanted wavelengths such as light pollution and moonlight. Its advanced construction guarantees durability, scratch resistance, and unparalleled performance across a wide range of imaging systems.
Whether you're imaging with a DSLR, CCD, or CMOS camera, the 3nm Chroma H-BETA filter is the perfect choice for astrophotographers seeking to unlock new levels of detail in their deep-sky images. Experience the universe with clarity and precision, as only Chroma can deliver.
The Benro GH2FL Gimbal Head is a collapsible mount designed for spotting scopes, perfect for users who need a portable and space-saving solution. It is ideal for fast-moving wildlife observation and birdwatching.. Its unique folding design allows for easy storage and transport, while the hollow construction reduces weight without compromising durability.
With a load capacity of 10 kg, the GH2FL can support large, heavy spotting scopes. The gimbal head provides smooth and stable movement, enabling you to track fast-moving objects both vertically and horizontally with ease, ensuring sharp, clear views.
The head consists of three components: the base, corner bracket, and quick-release platform, all of which can be used together or separately.
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Low Profile Base: This allows you to mount larger spotting scopes, with a vertical clamp for Arca-Swiss compatible plates. The base has 360-degree rotating mechanisms on both the horizontal and vertical axes for smooth, fluid movement. Separate knobs control pan and tilt adjustments, with a short throw for quick locking of your selected position. The vertical digital scale ensures precise and repeatable height adjustments, while the digital scale on the pan dial allows for accurate angle control. A built-in bubble level helps align the horizon for optimal viewing.
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Corner Bracket: The vertical bracket features an Arca-Swiss plate for secure mounting, while the horizontal section has clamps for additional Arca-Swiss compatible plates on both sides.
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Quick-Release Platform: The PL100N quick-release platform, compatible with the Arca-Swiss system, allows for quick, secure mounting of your scope. The platform’s elongated shape provides additional balancing options depending on the lens used. A double-locking safety feature ensures your scope stays securely in place, and boundary boards on the platform prevent any accidental shifts.
Transportation Options:
- Fold the head directly onto the tripod for compact storage, taking up minimal space.
- Remove the head from the tripod, fold it, and store it in the included bag. The bag features a rigid frame and internal dividers, with a handle and a removable shoulder strap with padding for easy carrying. A metal carabiner is also included for additional convenience.
The Benro GH2FL Gimbal Head is the ideal tool for observing wildlife, tracking birds, or capturing dynamic moments during sports events with precision and stability.
$799.00
The versatile and reliable Benro Gimbal Head GH2N is engineered for dynamic spotting scope use, particularly for observing fast-moving subjects such as wildlife and birds.
Weighing just 1.2 kg, the gimbal head’s hollow structure, reinforced with stiffening ribs, supports an impressive load capacity of 25 kg. With the GH2N, you can achieve extreme angles and perfect balance, allowing your spotting scope to move freely in ways other mounts cannot, making it ideal for tracking the movement of fast-moving objects both vertically and horizontally.
The low center of gravity ensures a stable head position at any tilt. Hydraulic cartridges on both the pan and tilt axes provide smooth and precise movement in all directions. The vertical digital scale allows for accurate, repeatable adjustments to the scope's height, while the panoramic scale helps in precise horizontal positioning and repeated accuracy.
The metal swivel and tilt locks are durable and easy to use, featuring a short stroke for quick locking of your selected position. The Benro PL100N compact, quick-release platform, compatible with the Arca-Swiss system, makes attaching and detaching the scope quick and secure. Markings on the base of the release plate ensure you can precisely return the scope to the same position.
The design of the quick-release plate and its base is optimized to reduce weight without sacrificing strength. A built-in bubble level ensures perfect horizon alignment. The head is supplied with a carrying case for convenient storage and transport.
From $520.00
The 8nm Chroma H-alpha Filter is a high-performance narrowband filter designed for astrophotography enthusiasts and professionals. With a precise 8nm bandwidth, this filter isolates the H-alpha emission line at 656.3nm, allowing you to capture stunning details in nebulae and other deep-sky objects with remarkable contrast and clarity.
Manufactured with exceptional optical quality, the Chroma H-alpha filter minimizes halos and reflections, ensuring sharp and artifact-free images even with fast optical systems. Its durable construction features an anti-reflective coating and resistance to environmental conditions, making it an ideal choice for both remote observatories and portable setups. Whether you're imaging under light-polluted skies or pristine dark skies, the Chroma H-alpha filter elevates your astrophotography to the next level.
$455.00
The Optolong L-Para is a dual narrowband 10nm light pollution filter, specifically designed to filter out unwanted mercury, sodium, and LED light pollution emissions and enhance the detection of nebulae emission lines with a transmittance rate of over 85% and a 10nm FWHM for both OIII (500.7nm) and H-Alpha (656.3nm). It offers superior contrast and anti-halo effects for capturing detailed and vibrant nebulae images.
Key Features:
Broad Compatibility:
A dual narrowband filter suitable for all telescope systems, adaptable to fast optics (focal ratios of F2, F2.8, F3.2, F4) as well as various standard/normal focal ratio telescopes.
Light Pollution Resistance:
Effectively cuts off emission lines from mercury lamps, sodium lamps, LEDs, and other light pollution sources, making it applicable to Bortle Scale1- 7 dark skies.
High Transmission Rate:
In systems with a focal ratio of F2 and above, the transmittance of nebula emission lines OIII and Ha exceed 85%, resulting in higher imaging efficiency.
Excellent Contrast:
The high transmittance of nebula emission lines (OIII & Ha) combined with deep cut-off of light pollution bands significantly improves image contrast and detail richness.
Anti-Halo Characteristics:
The design has undergone several round of optimizations and many times of repeated testing ,resulting in a marked improvement in anti-halo performance, enhancing the capture of bright stars.
Optolong L-Para is a brand new dual narrowband 10nm light pollution filter. The FWHM of L-Para is 10nm for OIII (500.7nm) and H-Alpha (656.3nm) respectively. The transmittance of nebulae emission lines at are both greater than 85% in system with focal ratios of F2 and above. It effectively filters out mercury lamp, sodium lamp, and LED light pollution emission lines. At the same time, it has excellent contrast and anti-halo characteristics, allowing you to capture detailed and vivid nebula images. L-Para is suitable for both normal optical systems and fast optical systems, such as RASA and Hyperstar systems. Even when light is incident at an oblique angle, it can still maintain high transmission rates to provide you with a clear and precise shooting experience.
From $840.00
The 5nm Chroma H-alpha Filter strikes the perfect balance between precision and versatility for astrophotography. With its 5nm bandwidth centered on the H-alpha emission line at 656.3nm, this filter provides exceptional contrast and detail while maintaining a wider passband for increased light throughput, making it ideal for capturing faint nebulosity in less-than-perfect conditions.
Crafted with superior optical coatings and premium materials, the Chroma 5nm filter minimizes reflections and halos, ensuring sharp, high-quality images. It is optimized for fast optical systems and performs brilliantly under both light-polluted and dark skies. Durable and weather-resistant, this filter is built to withstand the rigors of frequent use in any imaging environment.
Whether you're an advanced astrophotographer or just stepping into narrowband imaging, the 5nm Chroma H-alpha Filter offers the perfect combination of clarity, performance, and flexibility to bring your deep-sky images to life.
From $1,040.00
The 3nm Chroma H-alpha Filter is the pinnacle of precision for astrophotography, designed to deliver unmatched contrast and detail for capturing deep-sky objects. Its ultra-narrow 3nm bandwidth isolates the H-alpha emission line at 656.3nm with exceptional precision, effectively eliminating light pollution and other unwanted wavelengths, even in challenging imaging conditions.
Engineered with state-of-the-art coatings and superior optical quality, this filter minimizes halos, reflections, and ghosting, providing crisp, artifact-free images. Ideal for use with fast optical systems, the Chroma 3nm filter excels in revealing the intricate structures of emission nebulae and other faint targets. Its robust, weather-resistant build ensures consistent performance, whether you're imaging in a remote observatory or under urban skies.
For astrophotographers seeking the highest level of detail and contrast, the 3nm Chroma H-alpha filter is the ultimate tool to unlock the beauty of the universe.
From $2,420.00
SBIG AFW Filter Wheels are fast and quiet, and are designed to be compatible with our full line of SBIG cameras. Two size formats are available:
Large Format AFW wheels are ultra-thin, minimizing back focus distance. The standard version, which accommodates filters ranging from 1 mm to 3 mm thick, uses only 0.55″ (14 mm) back focus. The tall version, which accommodates 5 mm thick filters, uses only 0.65″ (16.5 mm) back focus.
Compact Format AFW wheels are a lower-cost option for our compact Aluma CCD and STC-428 cameras. For users needing more filter slots, an adapter is also available to interface our compact format cameras to a Large Format AFW-16-36R.
SBIG AFW Filter Wheels are fast and quiet, and are designed to be compatible with our full line of SBIG cameras. Two size formats are available:
Large Format AFW wheels are ultra-thin, minimizing back focus distance. The standard version, which accommodates filters ranging from 1 mm to 3 mm thick, uses only 0.55″ (14 mm) back focus. The tall version, which accommodates 5 mm thick filters, uses only 0.65″ (16.5 mm) back focus.
Large Format AFW wheels are compatible with all SBIG cameras using our “STX” style adapter plates. This includes our popular Aluma AC Advanced CMOS models as well as our legacy STX and STXL models.
Large Format AFW wheels can also be used on our compact cameras using our AFW to Small Format Camera Adapter. This option provides more filter slots than our Compact Format wheels.
Compact Format AFW wheels are a lower-cost eight filter slot option for our compact Aluma CCD and STC-428 cameras. They also work with most legacy STF and STT models.
Multiple Versions Available
- AFW-16-36R Large Format
- 16 Filter Slots
- 36 mm Round Filters
- Accommodates 1 mm, 2 mm, and 3 mm thick filters
- AFW-16-36RT Tall Large Format
- 16 Filter Slots
- 36 mm Round Filters
- Accommodates 1 mm, 2 mm, 3 mm, and 5 mm thick filters
- AFW-12-50R Large Format
- 12 Filter Slots
- 50 mm Round Filters
- Accommodates 1 mm, 2 mm, and 3 mm thick filters
- AFW-10-50SQ Large Format
- 10 Filter Slots
- 50 mm Square Filters
- Accommodates 1 mm, 2 mm, and 3 mm thick filters
- AFW-10-50ST Tall Large Format
- 10 Filter Slots
- 50 mm Square Filters
- Accommodates 1 mm, 2 mm, 3 mm, and 5 mm thick filters
- AFW-8-36R Compact Format
- 8 Filter Slots
- 36 mm Round Filters
- Accommodates 3 mm thick filters
- Lower cost option for compact cameras
Stackable
Two Lage Format AFW wheels can be stacked to add even more filter slots, using the available Dual AFW Filter Wheel Adapter. “Virtual Slots” can be assigned, which map to different slots on the two wheels. If you leave one slot empty in each wheel you get almost double (less two) available filter slots. If you sometimes need to stack filters then you can have even more virtual slots.
Fast Operation
AFW wheels switch filters quickly, requiring just 1 second to change to an adjacent slot. They can slew in either direction, but when stopping they always approach the filter slot in the same direction to ensure repeatability. If the requested slot is on the far side of the carousel the maximum transition time is approximately 5 seconds.
Improved Filter Compatibility
Large Format AFW supports the most popular filter sizes, convenient spacers are included:
- 3 mm filters – do not use spacer
- 2 mm filters – align notches in spacer with mounting screws
- 1 mm filters – flip over spacer so notches face the filter
- 5 mm filters – AFW-10-50ST only – adds tall spacers and mounting screws
The lower-cost Compact Format AFW supports 3 mm thick filters.
Easy Installation
The AFW series filter wheels are designed to be quickly installed onto the camera without removing the carousel. Removing a single access cover provides access to the filter slots and camera mounting screws. Large Format AFW can be installed without removing filters; the Compact Format will require one filter to be removed.
For the Large Format AFW wheels, two mounting screws are “captive” under the carousel, and can be accessed by turning the carousel by hand to align access holes with the screw heads. The two remaining screws are freely accessible. This makes installation and removal quick and easy.
For the Compact Format AFW wheels, the two mounting screws under the carousel can be accessed through a filter slot by gently moving the carousel off-center.
Once the wheel is attached to the camera, a single cable is connected to the camera’s AUX port. This single cable provides all necessary power and control functions.
Dual Wheel Support
For those users requiring more filters, the AFW Large Format series wheels include the ability to control two filter wheels. The filter wheels can be stacked using our AFW Dual Adapter. A matching three-port low profile cable is included to connect the two wheels to the camera’s control port.
Currently software support is available via an Aluma AC series camera and MaxIm LT or MaxIm DL Pro software. Alternatively, the dual wheel can be controlled via our SBIG USB to Filter Wheel Adapter using its associated ASCOM driver.
The software allows you to configure “virtual” filter slots, that map to specific slots on wheel 1 and wheel 2. Usually one slot is left blank in each wheel, allowing you to select filters from one wheel or the other. It is also possible to arrange for two filters to be used per slot, depending on your requirements.
With one blank slot in each wheel, a pair of AFW-10-50SQ wheels allow you to use 18 filters. Similarly a pair of AFW-12-50R wheels will allow you to use 22 filters, and a pair of AFW-16-36R wheels will allow you to use 30 filters.
StarChaser Autoguider and AO Compatibility
Large Format AFW series wheels are compatible with SBIG StarChaser SC-4, providing self-guiding in front of the filters. They also work with our popular AO-X Adaptive Optics unit, providing the tightest possible star images.
Compact Format AFW wheels are compatible with SBIG StarChaser SC-4C, providing self-guiding in front of the filters. They also work with our popular AO-8A Adaptive Optics unit.
Large Format Camera Model Compatibility
Please note that when smaller filters are used they may vignette larger sensors. Compact models will require the AFW to Small Format Camera Adapter. Some cameras will require an 11066 cable adapter. Some older products are not electrically compatible and need to use the USB-FW adapter.
Small Format Camera Model Compatibility
The lower-cost Small Format AFW-8-36R is compatible with all small format cameras, including Aluma CCD and STC-428. It is also compatible with legacy models including STF-8300, STF-4070, STF-8050, STF-1603, STF-3200, STT-8300, STT-1603, and STT-3200.
Additional compatibility notes:
STC-7 and STC-428-P: The built-in filter wheel prevents the camera from controlling an external wheel. Options are (a) to replace the built-in wheel with an STC-428-M front plate, or (b) stack the AFW on top and control the second wheel via a USB-FW adapter. The two wheels can be operated together using MaxIm DL’s Dual Filter Wheel feature. ACC14 is required.
ST series: Not officially supported. Requires an ACC14. May work directly with camera but this is not guaranteed, as ST cameras have not been tested with AFW. If there is an issue controlling the wheel than a USB-FW adapter will be required.
STL series: Not officially supported. The built-in filter wheel prevents the camera from controlling an external wheel. It is possible to attach an AFW wheel to the STL using the ACC10 STL to StarChaser Adapter and use a USB-FW to control it. Since STL also has an internal filter wheel the combination is best supported using MaxIm DL’s Dual Filter Wheel feature.
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