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IMPORTANT: Our store is located in Canada. All orders that include products manufactured outside of Canada or USA will be subject to tariffs and duties, regardless of the order value. US customers are responsible for all applicable duties and tariffs, and those will be billed by the carrier, except for the Lacerta upgrade kit, for which we collect them at checkout.

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Baader Planetarium S-II f/3 Ultra-Highspeed-Filter (4nm) – CMOS-optimized

UGC BAA-2961500
Prix d'origine $324.00 - Prix d'origine $660.00
Prix d'origine
$324.00
$324.00 - $660.00
Prix actuel $324.00
Égalisation de prix!
  • 4nm Bandwidth (FWHM)
  • Pre-Shifted for Fast f/3 Optical Systems
  • Available in 1.25" & 2" Mounted, 31mm, 36mm & 50.4mm Unmounted Round, and 50x50mm & 65x65mm Square Sizes
  • CMOS-Optimized with Reflex-Blocker™ Coatings
  • Life-Coat™ Hard Coatings for Durability
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Admissible à la livraison GRATUITE aux USA pour les commandes de plus de 350$.
  • Description
  • FAQ
  • Specifications
  • In the Box
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  • Warranty
  • Baader S-II f/3 Ultra-Highspeed-Filter (4nm) – CMOS-optimized

    The Baader S-II f/3 Ultra-Highspeed Filter isolates the critical 672.4nm sulfur line with an extremely narrow 4nm bandpass, specifically pre-shifted to maintain peak transmission in optical systems as fast as f/3. This CMOS-optimized design uses advanced coatings to deliver maximum signal contrast on faint emission nebulae while completely eliminating the internal reflections and halos that plague modern, highly-reflective sensors. Choose from mounted 1.25" and 2" (M48 x 0.75) cells, unmounted 31mm, 36mm and 50.4mm round filters, or 50x50mm and 65x65mm squares that fully illuminate full-frame and larger sensors.

    Engineered for f/3 Systems: Zero Band-Shift Performance

    Standard narrowband filters suffer from band-shifting when used with very fast optics; the filter's passband moves off the target emission line, crippling transmission. The Baader f/3 Ultra-Highspeed filter solves this by pre-shifting the 4nm passband, ensuring the S-II signal remains centered in the steep light cone of a fast f/3 system. This makes it an essential tool for instruments like RASAs, HyperStars, or fast astrographs where conventional filters fail.

    The 4nm Advantage: Extreme Contrast for S-II Targets

    With a full width at half maximum (FWHM) of just 4nm, every size of this filter provides a significant contrast boost over wider 7nm or 12nm designs. This surgical isolation of the S-II line darkens the sky background, cuts through moonlight or moderate light pollution, and reveals finer, fainter structural details in targets like the Wizard Nebula (NGC 7380) or the core of the Eagle Nebula (M16).

    CMOS-Optimized Coatings for Halo-Free Stars

    Modern CMOS sensors are highly reflective, causing halos and internal reflections with improperly coated filters. This Baader filter series features Reflex-Blocker™ coatings and blackened edges to absorb off-axis light, ensuring crisp, halo-free stars. Additionally, Life-Coat™ hard coatings provide extreme durability, protecting your investment against the rigors of cleaning and use in harsh environments.

    Baader 4nm f/3 S-II vs. 7nm S-II: A Tale of Two Speeds

    Choosing between Baader's S-II filters depends entirely on your telescope's focal ratio. The two are not interchangeable and are designed for different optical systems.

    • Baader 4nm f/3 S-II (This Filter): Its primary advantage is the pre-shifted passband for fast optics. It is the correct choice for fast astrographs such as RASAs and HyperStars. On a slow scope such as an f/10 SCT it is not ideal, as the passband will be off-center.
    • Standard 7nm S-II Filter: Its advantage is its optimization for slower systems. It has a wider 7nm bandpass, which gathers more signal in a shorter time but offers lower contrast. It will suffer severe transmission loss on an f/3 system due to band-shifting.
  • Can I use the Baader 4nm f/3 S-II filter with my f/10 Schmidt-Cassegrain?

    It is not the optimal choice. This filter is pre-shifted for fast systems. On an f/10 telescope, the center of the passband will not be aligned with the S-II emission line, reducing transmission. A filter designed for slower f-ratios, like a standard Baader narrowband S-II filter, would be a more efficient choice for an f/10 SCT.

    How will this Baader 4nm S-II filter perform on the Soul Nebula (IC 1848) with a RASA or HyperStar system?

    It will perform exceptionally well. The RASA's fast optics are exactly what this filter was designed for. The pre-shifted 4nm passband will ensure you capture the maximum S-II signal from the Soul Nebula's structures, while the tight FWHM will deliver extremely high contrast, separating the faint sulfur emissions from the starfield and background sky.

    What does "CMOS-optimized" mean for the Baader 4nm f/3 S-II filter?

    CMOS-optimized refers to the advanced anti-reflection coatings (Reflex-Blocker™) applied to the filter. These coatings are designed to suppress halos and internal reflections caused by the highly reflective surfaces of modern CMOS imaging sensors. This results in cleaner data with tighter, artifact-free stars, especially around bright stars within a nebula.

    Will the Baader 4nm f/3 S-II filter require longer exposure times than a 7nm filter?

    Yes, all else being equal. A narrower 4nm bandpass captures less light overall (both signal and noise) compared to a 7nm filter. To achieve the same signal level, you will need to use longer sub-exposures. The trade-off is that the resulting image will have a significantly darker background and higher contrast.

    Is the Baader 4nm f/3 S-II filter parfocal with other Baader CMOS-optimized filters?

    Yes, Baader engineers their CMOS-optimized filters to be parfocal. When switching between the H-alpha, O-III, and S-II filters in this series using a filter wheel or drawer of the matching size, you should not need to make any significant focus adjustments, saving valuable imaging time.

    What is the benefit of the Life-Coat™ on the Baader 4nm S-II filter?

    Life-Coat™ is a hardened dielectric coating that makes the filter extremely scratch-resistant and durable. It allows the filter to withstand repeated cleanings and harsh environmental conditions (like high humidity) without degrading, ensuring a long operational lifetime.

  • 1.25" Round Mounted

    Filter Type Sulfur-II (S-II) Narrowband
    Size 1.25"
    Bandwidth (FWHM) 4nm
    Optimized Focal Ratio f/3 to f/8
    Sensor Compatibility CMOS-Optimized

    2" Round Mounted

    Filter Type Sulfur-II (S-II) Narrowband
    Central Wavelength 672.4nm
    Bandwidth (FWHM) 4nm
    Size 2"
    Format Mounted (2" filter cell)
    Thread M48 x 0.75
    Optimized Focal Ratio f/3
    Sensor Compatibility CMOS-Optimized (Reflex-Blocker™, Life-Coat™)

    31mm Round Unmounted Filter

    Filter Type S-II (Sulfur-II)
    Bandwidth (FWHM) 4nm
    Size 31mm
    Format Unmounted
    Recommended System Speed f/3 and faster
    Sensor Compatibility CMOS Optimized

    36mm Round Unmounted Filter

    Filter Type Ultra-Narrowband S-II
    Size 36mm Round, Unmounted
    Bandpass 4nm
    Designed Focal Ratio f/3 and faster
    Optimization CMOS-Optimized, Reflex-Blocker™ Coatings

    50.4mm Round Unmounted Filter

    Filter Type Sulfur-II (S-II) Narrowband
    Bandwidth (FWHM) 4nm
    Size 50.4mm
    Format Unmounted, Round
    Optimized Focal Ratio f/3
    Sensor Compatibility CMOS-Optimized
    Sensor Coverage Full-frame (36 x 24mm) without vignetting

    50x50mm Square Filter

    Filter Type Sulfur-II (S-II) Narrowband
    Central Wavelength 672.4nm
    Bandwidth (FWHM) 4nm
    Size 50 x 50mm
    Format Unmounted Square
    Optimized Focal Ratio f/3
    Sensor Compatibility CMOS-Optimized (Reflex-Blocker™)

    65x65mm Square Filter

    Filter Type Ultra-Narrowband S-II (Sulfur-II)
    Bandpass (FWHM) 4nm
    Size 65mm x 65mm
    Format Unmounted Square
    Optimized Focal Ratio f/3 and slower
    Sensor Optimization CMOS
  • Baader Planetarium Warranty