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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
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21 products
21 products
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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 |
From $65.00
Adjust the brightness level of the Moon, Venus, and other bright objects with the Optolong Variable Polarizer. A standard Moon Filter is similar to a pair of sunglasses. They work fine, but sometimes the scene is too dark or too bright, and there’s not a lot you can do about it. A variable polarizing filter is much more flexible than a Moon filter. It allows you to set the percentage of attenuation by turning the top section of the two-piece filter. Simply attach the 2" threaded filter to a like-sized eyepiece or Astro accessory barrel, and then slowly rotate the top half of the filter—it turns 360°—to achieve the results you desire.
The Optolong Variable Polarizing Filter also works great to cut brightness when you are using your telescope for terrestrial observations or photography. If you have ever done photography through a SLR or DSLR camera, you may have already been introduced to the qualities of a polarizing filter, since it is a very popular accessory for polarizing the light and making the sky appear bluer. You will especially appreciate a polarizing filter when viewing over water or photographing a scene that includes a river or body of water. Simply turn the filter until you achieve the most glare-free results—you will really see the difference.
| 1.25 inch | 2 inch | |
| Brand | Optolong | Optolong |
| Type | Variable Polarizing | Variable Polarizing |
| Substrate Thickness | 2mm | 2mm |
| Clear Aperture | 26mm | 44mm |
| Surface Quality | 60/40 | 60/41 |
| Surface parallelism | 1/4λ | 1/4λ |
| Parallelism | 30" | 30" |
| Thread | M28.5*0.6 | M48*0.75 |
| Single Thread | Yes | Yes |
$329.00
L-四通增强滤镜(L-QEF)是一款用于彩色相机的四通光污染抑制滤镜。它有效地抑制了光污染波长的透射,特别是人工照明(包括汞灯和钠灯)产生的光污染,以及自然天光对拍摄的影响,从而有效地增强了天体的对比度和细节,使物体更加清晰和立体。这款滤镜在提高抗光污染能力的同时,提供了更好的色彩平衡。L-QEF 既可用于广角天文摄影,如夏季和冬季的银河系,也可用于深空物体,如星云、星系、星团等;它可以让您在拍摄过程中节省大量时间,同时获得更好的效果。四通的设计最大限度地提高了星云、星系和其他宽带光谱目标的色彩平衡。
主要特点:
- 消除汞灯和钠灯的光污染,并产生色偏最小的优质宽带图像;
- 信噪比(SNR);
- 近红外截止至 1000nm,降低红外噪声的影响;
- L-QEF对H-Beta/OIII/H-Alpha/SII星云发射线的透过率超过90%,截止深度从OD2到OD4,抗光污染能力大大提高。L-QEF适用于Bortel 1到Bortel 7级的夜空;(不建议使用Bortel 8、Bortel 9环境,请选择Optolong其他窄带滤光片,3nm、7nm类型的滤光片可用。)
- 适用于广泛的深空目标:它覆盖了大多数星云、星系、星团、反射和发射的线信号天文物体,具有更高的对比度和丰富的细节,同时保持了出色的色彩平衡。L-QEF 优于其他同类型的滤镜。
光谱及特性
| 布他林 | 光学玻璃 |
| 厚度 | 1.85 毫米 |
| 半高宽 | 四带通滤波器 |
| 阻断范围 | 300-1000纳米 |
| 阻挡深度 | OD2-OD4 |
| 表面质量 | 60/40 |
| 透射波前 RMS | λ / 4 |
| 并行性 | 30 秒 |
L-Quad Enhance 滤镜根据天体发射线和光污染发射线的特点,有效降低光污染的影响,抑制天体背景光,从而有效增强天体的对比度和细节。使用 L-QEF 滤镜可以帮助您在拍摄过程中节省大量时间,同时获得令人难以置信的效果。
From $260.00
Optolong L-Pro 1.25 inch is multi-bandpass filter which offers better color balance by maximizing the transmission band. The balanced transmission allows astrophotos to be taken with minimal color cast to broadband emission objects such as galaxies, reflection nebulae and globular star clusters.
Warning - Do not use this filter for solar purposes !
Optolong L-Pro (L-Professional) filter is designed to improve the visibility of various deepsky objects. By selectively reducing the transmission of wavelengths of light pollutants, specifically those produced by artificial lightings including mercury vapor lamps, both high & low pressure sodium vapor lights and the unwanted natural light caused by neutral oxygen emission in our atmosphere (i.e. skyglow). Together with the highly transparent in main nebula emission lines at OIII(496nm and 500nm), H-beta (486nm), NII(654nm and 658nm), H-alpha(656nm) as well as SII(672nm), the filter is suitable for enhancing the contrast and details for both visual and photograghic purpose at sub-rural area with heavy light pollution.
Optolong L-Pro is multi-bandpass filter which offers better color balance by maximizing the transmission band. The balanced transmission allows astrophotos to be taken with minimal color cast to broadband emission objects such as galaxies, reflection nebulae and globular star clusters. L-Pro is the best choice for light pollution suppression.
- Optical glass fine material
- Spectrum: 380-750nm
- Surface Quality: 60/40 (Refer to MIL-O-13830)
- Fine-optically polished to ensure accurate 1/4 wavefront and < 30 seconds parallelism over the both surfaces
- High transmission at major nebula emission lines (i.e. H-alpha 656nm, OIII 496nm&500nm, SII 672nm and H-beta 486nm).
- Precision off-band blocking, specifically the major emission lines of artificial light pollution (i.e. Na 589nm, Hg 435nm and 578nm).
From $310.00
L-eNhance filter
The relentless spread of urbanization and its associated light pollution have become a growing problem for all amateur astrophotographers. The current solutions to the problem can be expensive and might include the purchase of a monochrome camera, several types of narrowband filters, and a filter wheel.
Optolong L-eNhance filter provides an economical and practical solution for amateurs. It is a dual-band pass filter that has been designed for DSLR (digital SLR), color CMOS, and monochrome CCD cameras. The convenience and cost-effectiveness of this filter allow amateurs to image a rich selection of astronomical images, even in bright, heavily light-polluted areas. Optolong believes the design of our L-eNhance filter is a technical innovation among filters. It effectively isolates the H-Alpha, H-Beta, and Oxygen III nebula emission lines and achieves a maximum transmission of up to 90%. The performance of this filter delivers images that superbly control the impact of light-polluted skies.
Hydrogen is the largest, the most primitive, the simplest, and the oldest element in the universe. Scientists consider that Hydrogen amounts to more than 90% of visible substances in space. Our sun is 5 billion years old, but so far hydrogen is still the key matter of nuclear fusion. While the sulfur element does not have much scientific significance, keeping H and O is meaningful for the exploration of life.
Therefore, we highlight H-a, H-b, O3, and O2, and reduce the signal of sulfur.
2. Spectrum and Characteristic
Substrate: B270
Thickness: 1.85mm
Tpeak: T>90%
Blocking range: 300-1000nm
Blocking depth: light pollution line blocking >99%
Surface quality: 60/40
Transmitted Wavefront RMS: λ/4
Parallelism: 30s
How to read the chart?
▲The horizontal axis is the Wavelength in Nanometers(nm).
▲The vertical axis is transmission in %.
▲The WHITE line shows the transmission of the filter. The artificial emission lines are shown in Yellow. The emission lines from the constellation are shown in GREEN, BLUE, AND RED.
SKU: 13801
From $520.00
Antlia LRGB-V Pro 系列滤镜专为使用 CCD 和 CMOS 传感器的单色相机而设计。适用的传感器包括 KAF/KAI 传感器、Sony IMX 传感器、GSENSE 和其他传感器制造商。LRGB-V Pro 套件旨在大致均衡来自红色敏感 CCD 探测器通量的 RGB 响应。结果是,您可以实现 1:1:1 均衡的 RGB 曝光,同时具有简化的后期处理和缩短的成像时间的优势。新的 LRGB-V Pro 系列滤镜在绿色和红色通道之间具有精心设计的光谱间隙,以最大限度地减少光污染的影响并提供有用频率的高透射率。滤镜的设计最大限度地捕捉了较暗星系和星云发射的细节。LRGB-V Pro 系列滤镜保证 B 和 G 滤镜中 OIII 波段的高透射率(蓝色和绿色的 OIII 信号 >95%)。B 通道的带宽变窄是为了改善由于 B 通道过度曝光而导致的恒星周围的蓝色通道溢出(光晕)。 Antlia LRGB-V Pro 系列滤光片通过 G 和 R 滤光片之间的宽间隙设计阻挡了 589nm 左右的发射线,从而抑制了高压钠灯和汞路灯的光污染,并实现了更自然的色彩平衡。基板厚度的均匀性使所有 Antlia 滤光片都具有良好的共焦性能。
LRGB-V Pro系列套装的亮点
1. 优质镀膜技术和精细抛光的基片 我们优化了质量选择流程,以确保高度均匀的玻璃基片。我们采用先进的光学镀膜技术和双面精密抛光,使所有滤镜均具有一致的共焦和光学性能。 2. 三个 RGB 通道中的每一个通道都实现了最大化的色彩平衡和对比度以及出色的 S/N 性能 玻璃基板的两侧沉积了数十层涂层,使 LRGB-V Pro 滤镜能够实现高 SNR。防反射涂层和精心设计的光谱间隙可最大限度地减少不必要的光散射,并最大限度地提高每个滤镜通道的有用信号数据。
3. 更紧密的星体轮廓和减少光晕 LRGB-V Pro系列套装的截止率经过高级设计,可最大限度地减少明亮星体周围的光晕并减少星体膨胀。我们精心设计的蓝色通道传输特性针对的是蓝色星体膨胀问题。
用途与性能:
1. 专为单色CCD和CMOS相机设计
2. 天体、星系、星团和星云的出色成像色彩
3. AR增透膜设计,减少二次反射和星晕
4. R-Filter 提供最大程度的 H-alpha 和 S II 发射传输
5. B/G 重叠使 OIII 线的能量加倍
6. 平衡的 RGB 设计为大多数望远镜光学系统提供 1:1:1 的曝光时间
7. 所有 Antlia LRGB-V Pro 滤镜的边缘均经过涂黑处理,以消除杂散光的内部反射
8. 四个 LRGB 滤光片的基板厚度均保持严格的公差
9. 不推荐用于太阳观测和成像
10. 不建议目视观察
重要提示:使用任何共焦滤光片时,用户在长时间成像过程中仍可能会遇到滤光片之间的焦点偏移。重要的是要记住,由于望远镜筒和玻璃光学元件之间的差异收缩,温度变化会改变光路的长度。建议摄影师每 1 到 2 小时手动或自动在软件中检查一次焦点。如果将望远镜从温暖的环境带到室外,则需要更频繁地检查焦点,直到设备稳定在接近环境温度为止。
技术规格:
基础基材:光学基材
滤光片厚度:1.25'' 为 2mm+/-0.05mm
表面质量:S/D(划痕/凹陷)= 60/40(参考 MIL-O-13830)
透射波前:Lambda/4 或更好。
平行度:小于 30 角秒
单面/无胶基材
$649.00
ALP-T 双波段 5nm 滤镜最适合 f 比低于 f/3.6 的光学器件,强烈推荐使用标准 Antlia ALP-T 双波段滤镜。同时,如果您希望使用 f/2.2 以上的任何光学器件获得最佳性能,高速版本是最佳选择。
Antlia ALP-T 双波段 5nm 系列滤光片是一种双线通滤光片,主要用于单次拍摄彩色 (OSC) 相机,例如 DSLR 和天文 OSC 相机。它还可以用作单色相机的窄带滤光片,以节省成像时间。我们的 ALP-T 超双波段滤光片上的高级多层镀膜可有效隔离发射星云的红色 Ha 和蓝绿色 OIII 线光,几乎完全抑制光污染、月光和气辉中不需要的波长的光密度 (OD) 4.5。因此,我们的 ALP-T 双波段 5nm 滤光片可为您的图像提供出色的信噪比和更好的对比度。
Antlia ALP-T 双波段滤镜可同时捕捉两个主要发射星云波段,同时抑制不必要的光污染。它可让您捕捉更清晰的数据,并减少后期处理工作,以将微弱的细节与背景光污染隔离开来。
用途与性能:
专为光学设计,速度低于 f/3.6
专为与 DSLR、CMOS 和 CCD 彩色相机配合使用而设计
抑制不需要的波长的光密度 (OD) 4.5 可增加信噪比
极其陡峭的带通边缘可最大限度地减少内部反射
理想的平顶和中等带通,减少频谱下移
双面抛光基板上的离子枪辅助沉积涂层技术使其成为最一致、最精确的光污染抑制滤光片
设计用于抑制 Bortle 等级 1 至 Bortle 等级 8 的人工照明
近红外 (NIR) 波长最高可达 1050nm
技术规格:
| 氢-α | 氧气 III | |
| 半高宽 | 5纳米 | 5纳米 |
| CWL(中心波长) | 657.8纳米 | 502.2纳米 |
| 峰值传输 | 88% | 82% |
| 阻塞 | ≥OD4.5 @ 300-1050nm | |
| 滤光片厚度 | 2毫米+/-0.05毫米 | |
滤镜环:
2英寸(M48*0.75)
超薄滤光片可最大程度地增大通光孔径,从而最大程度地减少渐晕
黑色阳极氧化处理
激光雕刻不褪色
光谱曲线:
不推荐:
太阳成像
夜间目视观察
不允许:
不要用这个滤镜看太阳
如果不遵守警告,将导致严重的眼睛损伤
From $420.00
L-eXtreme is a two 7nm bandpass filter which can be used with one-shot color cameras like DSLR's (digital SLR), and monochrome CCD cameras, it is also more suited for fast systems. The convenience and cost effectiveness of this filter allows amateurs to image a rich emission nebulas, even in bright, light pollution skies. Optolong believes the design of L-eXtreme filter would be better choice for fast systems in competitive price. It isolates the H-Alpha, and Oxygen III nebula emission lines so that the contrast and signal-to-noise ratio between nebulae were maximized. For people who is living in very light polluted areas, or when the moon is out, the L-eXtreme will be a good filter.
Unlike the Optolong L-eNhance filter which is a tri-band (transmits Hb, Ha, and OIII), the L-eXtreme filter is dual band that passes Ha and OIII emission lines.The advantage of the L-eXtreme filter is that there is no transmission between the H-beta and OIII lines, as there is no nebula emission lines there. In this case, it isn't letting light pollution come through so that maximize nebulas signal and make the sky background darker while imaging. The L-eXtreme filter should better isolate the emission lines only and better protect from light pollution.
Hydrogen is the largest, the most primitive, the simplest, and the oldest element in the universe. Scientists consider that Hydrogen amounts to more than 90% of visible substance in space. Our sun is 5 billion years old, but so far hydrogen is still the key matter of nuclear fusion. While the sulfur element does not have much scientific significance, so keeping H and O is meaning for exploration of life.
Therefore, we highlight H-a, H-b, O3 and O2, and reduce the signal of sulfur.
Spectrum and Characteristics
- Sbustrate: B270
- Thickness: 1.85mm
- Tpeak: T>90%
- Blocking range: 300-1000nm
- Blcoking depth: light pollution line blocking >99%
- Surface quality: 60/40
- Transmitted Wavefront RMS: λ/4
From $1,310.00
Antlia 3nm Pro 超窄带 1.25 英寸滤光片组包括以下物品:
- Antlia 1.25 英寸 H-Alpha 3nm 滤镜
- Antlia 1.25 英寸 OIII 3nm 滤镜
- Antlia 1.25 英寸 SII 3nm 滤镜
Antlia SHO Pro 窄带滤光片将 FWHM(半峰全宽)优化至 3nm 带通。随着带宽变窄,3nm Pro 窄带滤光片通过降低不需要的背景信号来增强发射目标的对比度。Antlia SHO 3nm Pro 滤光片旨在在 671.6nm 线上提供 88% 的透射率,为您提供最大信号和清晰的星云结构。
传统的较宽窄带滤光片由于强烈的(中心波长 (CWL) 偏移)会导致严重的传输损失。我们保证在中心带宽 1nm 范围内 T>88%,这意味着 3nm Pro 窄带滤光片可以保证高透射率,适用于长焦比和快速光学系统。蓝移数据显示,Antlia 3nm Pro 滤光片几乎可以与所有速度高达 f/3 的系统一起使用,发射信号损失最小,并满足 Hyperstar 和 RASA 等快速光学器件的要求。
带外阻断规格为 OD5(0.001%),可提供出色的 SNR(信噪比)和有效截止率,以最大限度地减少来自其他波长的干扰。改进的锐利截止天文摄影 3nm Pro 滤镜旨在最大限度地减少明亮恒星周围的光晕。
用途与性能:
- 高透射率和最小带宽可最大程度地提高对比度
- 陡峭的光谱轮廓最大程度地减少了明亮恒星周围的光晕
- 单一基板可消除内部反射
- 窄带物体:发射星云、行星、沃尔夫-拉叶星云和超新星遗迹
- 在光污染区域和黑暗场所使用
- 月亮升起时延长成像时间
- Antlia 窄带 Pro 滤波器可用于 F/3 系统,信号损失轻微
- 所有 Antlia 窄带滤光片的边缘均经过涂黑处理,以消除杂散光的内部反射
- 卓越的光学可靠性减少了后期图像处理
From $500.00
它是一种 3nm 双波段,旨在大幅减少光污染的影响,3nm 将星云的辐射隔离为 H-Alpha(红色)和 OIII(绿-蓝)。它可以阻挡光污染,最大化星云信号,并使天空背景变暗。它还可以阻挡汞蒸气灯、高压和低压钠蒸气灯的人造光以及由我们大气中的中性氧排放引起的不必要的自然光。最大化星云在 OIII(496nm 和 500nm)和 H-alpha(656nm)中的主要发射线的传输。但是,与 DSLR、彩色/MONO CMOS 和 CCD 一起使用时,此滤镜不适用于快速比率系统。
L-Ultimate的优点在于只通过发射线OIII(500.7nm)和Ha(656.3nm),这样其他光污染发射线全部被排除,成像时只捕捉到星云的发射和反射信号,因此图像的天空背景更暗,最大程度提升了星云的对比度和信噪比。在重光污染区域,该产品还能选择性地过滤通过星云发射线的光污染和杂波信号,最终避免光污染对天文摄影的影响。
与双窄带 L-eNhance 和 L-eXtreme 系列不同的是,L-Ultimate 是一款双 3nm 带宽滤镜,只通过 Ha 和 OIII 发射线。您将获得更暗的天空背景,图像对比度更高,对星星的抑制也更强。L-Ultimate 在光晕性能方面也进行了优化,因此在对亮星物体进行拍摄时不会出现明显的光晕。
特征
| 基材 | 光学玻璃 |
| 半高宽 | OIII 3纳米 Ha 3纳米 |
| 阻断范围 | 300-1000纳米 |
| 阻塞 | >OD4 |
| 表面质量 | 60/40 |
| 透射波前 RMS: | λ / 4 |
| 并行性 | 30秒 |
$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.
$539.00
1. L-eXtreme F/2 简介
Optolong L-eXtreme F/2 是一款双波段(500.7 nm 和 656.28 nm,FWHM=7 nm)窄带通滤光片,满足连续变化角度的透射要求。以天文特征谱线(OIII、Ha)为主要透射波长,OIII 和 H-Alpha 星云发射线在 f2 - f3.3 焦比下准确通过。这是 Optolong 专门为快速光学系统或快速焦比成像系统开发的产品。它在 RASA、HyperStar 和其他快速焦比望远镜上表现良好。
主要特点:
♦与单次彩色天文相机、单色天文相机、数码单反相机配合使用,可以快速获得清晰细致的深空图像;
♦非常适合快速光学系统,如RASA、Hyperstar和其他快速焦比望远镜用户;
♦建议使用焦比为f2至f3.3的快速光学系统;
♦抗光污染、对比度更好、天体细节更多:此滤镜可滤除目标天体以外的背景光和噪音,以获得更佳的图像细节和对比度。L-eXtreme F/2 可有效阻挡光污染,使图像不会受到背景中不必要的灯光和天光的影响。您可以在快速光学系统中快速获得满意的图像。
2. 光谱及特性
L-eXtreme F/2 针对天体的发射线和光污染发射线特点,在遮挡大部分光污染的同时,保留了星云 OIII 和 Ha 的突出色彩。L-eXtreme F2 针对快速光学系统的特点进行了专门设计和优化计算,始终保持 OIII 和 Ha 两个波段的高透过率,帮助用户更准确、更快速地捕捉这些波段的星云发射线,获得更好的天文摄影图像。
如何读图表?
▲横轴为波长,单位为纳米(nm)。
▲纵轴表示透射率,单位为%。
3. 涂层技术
·多层增透膜
·非胶粘型光学基片镀膜
·Optolong滤镜采用基于离子辅助沉积镀膜技术的精密镀膜,经久耐用,耐刮擦,中心波长稳定,不受温度变化的影响。
·行星旋转系统提供涂层的精确性和均匀性,确保通带透射率和带外光密度的高值。
库存单位:14803
From $99.00
The UHC (Ultra High Contrast) broadband filter is designed to improve the visibility of various deepsky objects. By selectively reducing the transmission of wavelengths of light pollutants, specifically those produced by artificial lightings including mercury vapor lamps, both high & low pressure sodium vapor lights and the unwanted natural light caused by neutral oxygen emission in our atmosphere (i.e. skyglow). Together with the highly transparent in main nebula emission lines at OIII(496nm and 500nm), H-beta (486nm), NII(654nm and 658nm), H-alpha(656nm) as well as SII(672nm), the filter is suitable for enhancing the contrast and details for both visual and photograghic purpose at sub-rural area with heavy light pollution.
Main Use and Performance
Suitable for color CCD cameras and unmodified DSLRs.
UHC with narrower passband provides higher contrast than CLS. Thus it is more suitable for urban environment where you suffer from severe light pollution.
UHC has a substantial red passband and offer superb views for objects like the Orion Nebula (M42).
Light pollution filter do not eliminate the effects of light pollution or increase the object’s brightness. In many cases, they increase the contrast between nebula and night sky, not brightening the nebula.
WARNING: The filters of Optolong are not designed for sun observation. DO NOT LOOK AT THE SUN WITH OPTOLONG FILTER. You would be BLIND if you fail to observe the warning.
| Sbustrate | optical glass |
| Tave | >95% |
| Blocking range | 300-700nm |
| Blcoking depth | OD3, light pollution line blocking >99% |
| Surface quality | 60/40 (Refer to MIL-O-13830A, MIL-C-48497A) |
| Transmitted Wavefront RMS | ¼ λ |
| Parallelism | 30s |
$499.00
Optolong L-Synergy Dual Narrowband Filter
The Optolong L-Synergy filter is designed for astrophotographers using DSLR, color CMOS, or CCD cameras who want to achieve stunning narrowband results without switching to a monochrome system. By pairing traditional dual-narrowband (Ha & OIII) concepts with a unique “Ha & OIII + SII & OIII” approach, L-Synergy overcomes the usual limitations of colour cameras and makes Hubble-Palette–style imaging accessible to everyone.
With this filter, you can produce deep, high-contrast SHO-like images of emission nebulae using your existing colour camera—no additional SHO filters or monochrome upgrade required. It’s an affordable way to achieve professional-level results even under bright suburban skies.
Why Choose the L-Synergy Filter?
The L-Synergy is a dual 7 nm narrowband filter engineered for telescopes with an f/ratio of f/3.3 or slower. Years of optical refinement have produced a design that suppresses bright star halos while delivering extremely high transmission in the key emission bands.
-
Selective Narrowband Performance
Transmits only the OIII (500.7 nm) and SII (672.4 nm) nebula emission lines, rejecting unwanted wavelengths and light pollution. -
Exceptional Contrast and Signal-to-Noise
By isolating the oxygen and sulfur signals, the filter produces a darker background sky and dramatically improves contrast—especially valuable in heavily light-polluted environments. -
Light-Pollution Resistant
Filters out the vast majority of urban skyglow, allowing astrophotographers to capture clean, detailed nebula structure from almost any location.
Optical Design
L-Synergy is precision-engineered based on the spectral behaviour of emission nebulae and common light-pollution sources. Its carefully tuned passbands maintain consistently high transmission in both SII and OIII, ensuring accurate colour capture and high-quality data for processing.
The result: a powerful, easy-to-use narrowband solution that unlocks deep-sky imaging performance far beyond what typical colour cameras can achieve, giving more astrophotographers access to true SHO-style imaging.
From $179.00
(Only Compatible with QHY MiniCAM8 Camera)
Deep Sky Filter Set
Includes LRGB and narrowband SHO filters sized at 19 mm × 12 mm × 1.1 mm. The LRGB filters have an optical density (OD) of 3, while the narrowband filters have an OD of 5, providing high contrast and minimal light leakage for deep sky imaging.
Planetary Filter Set
Ideal for planetary observation, this set includes LRGB filters along with a 20nm Methane filter, 40nm UV filter, and 10nm Sodium (Na) filter. Great for capturing fine atmospheric and spectral details.
Photometric Filter Set
A complete Sloan filter set: u’, g’, r’, i’, z’. Suitable for scientific imaging and precise photometric measurements.
Ar III Standalone Filter
The Ar III (Argon III) filter is a narrowband filter centered around 713nm, designed to capture the specific emission line of triply ionized argon. This emission line is commonly observed in planetary nebulae, H II regions, emission-line galaxies, and in the spectroscopy of ionized gases in laboratory plasmas.
$919.00
Optolong L2 Dual-Combo Filter Set
The Optolong L2 Dual-Combo Set includes two premium dual-narrowband filters, L-eXtreme and L-Synergy, designed for colour-camera astrophotography. Compatible with telescopes f/3.3 and slower, this set allows users to capture Hubble Palette deep-sky images without switching to a monochrome camera or buying a full three-filter SHO set. It provides professional-level narrowband imaging with minimal investment.
The L-eXtreme transmits OIII (500.7 nm) and Hα (656.3 nm), blocking unwanted light-pollution wavelengths to deliver bright nebula details with high contrast. Years of refinement optimise performance and reduce bright star halos.
The L-Synergy transmits OIII (500.7 nm) and SII (672.4 nm) with high efficiency while rejecting other wavelengths. It minimises light pollution effects and preserves nebula detail, producing clean data for processing.
The combination of these filters allows colour-camera users to achieve Hubble Palette imaging efficiently. It enhances nebula structure, improves contrast, and enables richer colour separation in light-polluted skies.
The filters are engineered to preserve the distinctive colours of nebulae while filtering out most light pollution. Their tuned transmission profiles ensure strong signal in the target emission lines and high signal-to-noise performance for detailed deep-sky images.
This set is ideal for astrophotographers using colour cameras who want professional-quality narrowband imaging with existing equipment.
$679.00
Antlia SII 3nm Pro 窄带滤光片将 FWHM(半峰全宽)优化至 3nm 带通。随着带宽变窄,3nm Pro 窄带滤光片通过降低不需要的背景信号来增强发射目标的对比度。Antlia SII 3nm Pro 滤光片旨在在 671.6nm 线上提供 88% 的透射率,为您提供最大信号和清晰的星云结构。
传统的较宽窄带滤光片由于强烈的中心波长 (CWL) 偏移而导致传输严重损失。我们保证在中心带宽 1nm 范围内 T>88%,这意味着 3nm Pro 窄带滤光片可以保证高透射率,适用于长焦比和快速光学系统。蓝移数据显示,Antlia SII 3nm Pro 滤光片几乎可以与所有速度高达 f/3 的系统一起使用,发射信号损失最小,并满足 Hyperstar 和 RASA 等快速光学器件的要求。
带外阻断规格为 OD5(0.001%),可提供出色的 SNR(信噪比)和有效截止率,以最大限度地减少来自其他波长的干扰。改进的锐利截止天文摄影 3nm Pro 滤镜旨在最大限度地减少明亮恒星周围的光晕。
用途与性能:
高透射率和最小带宽可最大程度地提高对比度
陡峭的光谱轮廓最大程度地减少了明亮恒星周围的光晕
单一基板可消除内部反射
窄带物体:SII 发射星云、行星、沃尔夫-拉叶星云和超新星遗迹
在光污染区域和黑暗场所使用
月亮升起时延长成像时间
所有 Antlia 窄带 Pro 滤镜均可在 F/3 下使用,但信号会略有损失
所有 Antlia 窄带滤光片的边缘均经过涂黑处理,以消除杂散光的内部反射
卓越的光学可靠性减少了后期图像处理
该滤镜不适用于不包含 SII 发射的深空物体。
技术规格:
基础基板:肖特光学基板
滤光片厚度: 2mm+/-0.05mm(2''安装)
FWHM(半峰全宽): 3nm
CWL(中心波长) :671.6nm
峰值透过率: >88%
阻断: > 5 OD(0.001% 带外阻断)@ 300-1000nm
表面质量: S/D(划痕/凹陷)= 60/40(参考 MIL-O-13830)
透射波前: Lambda/4 或更好。
平行度:小于 30 角秒
单面/无胶基材
保修:3 年防脱层
SKU: ANTLIASii3nm2
$679.00
Antlia OIII 3nm Pro 窄带滤光片将 FWHM(半峰全宽)优化至 3nm 带通。随着带宽变窄,3nm Pro 窄带滤光片通过降低不需要的背景信号来增强发射目标的对比度。Antlia OIII 3nm Pro 滤光片旨在在 500.7nm 线上提供 85% 的透射率,为您提供最大信号和清晰的星云结构。
传统的较宽窄带滤光片由于中心波长 (CWL) 偏移较大,会导致传输损失严重。我们保证在中心带宽 1nm 范围内 T>85%,这意味着 3nm Pro 窄带滤光片可以保证高透射率,适用于长焦比和快速光学系统。Blueshift 数据显示,Antlia 3nm Pro 滤光片可以与几乎所有速度高达 f/3 的系统一起使用,发射信号损失最小,并满足 Hyperstar 和 RASA 等快速光学器件的要求。
带外阻断规格为 OD5(0.001%),可提供出色的 SNR(信噪比)和有效截止率,以最大限度地减少来自其他波长的干扰。改进的锐利截止天文摄影 3nm Pro 滤镜旨在最大限度地减少明亮恒星周围的光晕。
用途与性能:
高透射率和最小带宽可最大程度地提高对比度
陡峭的光谱轮廓最大程度地减少了明亮恒星周围的光晕
单一基板可消除内部反射
窄带物体:OIII 发射星云、行星、沃尔夫-拉叶星云和超新星遗迹
在光污染区域和黑暗场所使用
月亮升起时延长成像时间
Antlia 窄带 Pro 滤波器可用于 F/3 系统,信号损失轻微
所有 Antlia 窄带滤光片的边缘均经过涂黑处理,以消除杂散光的内部反射
卓越的光学可靠性减少了后期图像处理
此滤镜不适用于不含 OIII 发射的深空物体。
技术规格:
基础基材:光学基材
滤光片厚度: 2mm+/-0.05mm(2'' 安装)
FWHM(半峰全宽): 3nm
CWL(中心波长) :500.7nm
峰值透过率: >85%
阻断: > 5 OD(0.001% 带外阻断)@ 300-1000nm
表面质量: S/D(划痕/凹陷)= 60/40(参考 MIL-O-13830)
透射波前: Lambda/4 或更好。
平行度:小于 30 角秒
单面/无胶基材
保修:3 年防脱层保修
请勿使用 ANTLIA 滤镜观察太阳。
当我们为天文成像系统设计滤光片时,我们会考虑它们如何与光学系统协同工作,精心设计阻塞和带通参数以实现最佳效果。带外阻塞率是一项非常重要的性能指标,因为它旨在急剧衰减带外波长。结果是 Antlia OIII 3nm Pro 滤光片在极暗的背景下提供出色的对比度,同时提供 OIII 信号的高传输率。这种滤光片更难以生产出始终如一的高标准。
每片滤镜都经过单独测试和扫描,以确保质量符合高性能参数。最终结果是滤镜实现了出色的对比度,但生产成本较高。我们认为性价比比市场上类似的优质滤镜更具优势。
SKU: ANTLIAOIII3nm2
From $400.00
Optolong LRGB filter set is designed for maximum contrast and with extremely high gradients for clear differentiation of colors. The LRGB filter set divides the spectrum into its components red, green, blue and luminance.
OIII emission overlaps on blue and green filters with maximum transmission to allow high efficiency and natural color imaging. Gap between green and red filters serves to block out the primary Sodium light pollution line at 589nm and improves color balance and separation.
- RGB, parfocal:1:1:1
- Creat images in their true original colors showing a wealth of natural detail;
- Steep bandpass filters to eliminate UV and IR interference;
- Include Luminance (UV/IR Cut), Red, Green, and Blue filters to reproduce the star's color
$689.00
Antlia ALP-T 双波段 5nm 高速滤镜经过优化,可通过略微移动通带和中心波长来配合高速成像系统使用。与标准版本相比,在 f/2.2 和 f/3.6 光学器件之间使用这些高速滤镜,在星云成像中显示出更强大、对比度更高的效果,如果您希望使用任何比 f/2.2 更快的光学器件获得最佳性能,高速版本是最佳选择。
但请记住,计算机模拟的蓝移数据表明,窄带滤光片会将其带宽移至更短的波长,光学速度快于 f/2,发射波长的透射率可能会降低 15%-20%。虽然 Antlia ALP-T 高速滤光片在快速光学器件上使用时,Ha 和 OIII 的透射率也有类似的降低,但根据当前标准版用户的数据,很明显,该滤光片仍然具有增加发射星云对比度和最小化光晕的高性能。
高速版本价格与标准滤光片相同,为高速光学用户带来双重好处。值得一提的是,Antlia 使用 Agilent Cary 的专业分光光度计逐件检查和测量产品,分辨率/狭缝宽度高达 0.2nm,这使我们能够为您提供高度可靠和一致的产品。
Antlia ALP-T 双波段 5nm 系列滤光片是一种双线通滤光片,主要用于单次拍摄彩色 (OSC) 相机,例如 DSLR 和天文 OSC 相机。它还可以用作单色相机的窄带滤光片,以节省成像时间。我们的 ALP-T 超双波段滤光片上的高级多层镀膜可有效隔离发射星云的红色 Ha 和蓝绿色 OIII 线光,几乎完全抑制光污染、月光和气辉中不需要的波长的光密度 (OD)4.5。因此,我们的 ALP-T 双波段 5nm 滤光片可为您的图像提供出色的信噪比和更好的对比度。
该滤光片可以同时捕捉两个主要发射星云带,同时抑制不必要的光污染。它可以让您捕捉到更清晰的数据,并减少后期处理工作量,以便将微弱的细节与背景光污染隔离开来。
用途与性能:
专为快速天文光学设计,特别是 f/2.2 至 f/3.6 比率
专为与 DSLR、CMOS 和 CCD 彩色相机配合使用而设计
抑制不需要的波长的光密度 (OD)4.5 可增加信噪比
极其陡峭的带通边缘可最大限度地减少内部反射
理想的平顶和中等带通,减少频谱下移
双面抛光基板上的离子枪辅助沉积涂层技术使其成为最一致、最精确的光污染抑制滤光片
设计用于抑制 Bortle 等级 1 至 Bortle 等级 8 的人工照明
近红外 (NIR) 波长最高可达 1050nm
技术规格:
| 氢-α | 氧气 III | |
| 半高宽 | 5纳米 | 5纳米 |
| CWL(中心波长) | 657.8纳米 | 502.2纳米 |
| 峰值传输 | 88% | 82% |
| 阻塞 | ≥OD4.5 @ 300-1050nm | |
| 滤光片厚度 | 2毫米+/-0.05毫米 | |
滤镜环:
2英寸(M48*0.75)
超薄滤光片可最大程度地增大通光孔径,从而最大程度地减少渐晕
黑色阳极氧化处理
激光雕刻不褪色
光谱曲线:
不推荐:
太阳成像
夜间目视观察
不允许:
不要用这个滤镜看太阳
如果不遵守警告,将导致严重的眼睛损伤
$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 |
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