Narrowband Astrophotography From Light-Polluted Skies

Table of Contents

What Is Narrowband Astrophotography and Why It Excels Under Light Pollution?

Narrowband astrophotography isolates the light emitted by specific ionized gases—most commonly hydrogen-alpha (Hα) at 656.3 nm, doubly ionized oxygen (OIII) at 500.7 nm, and singly ionized sulfur (SII) at 672.4 nm. Instead of admitting a broad portion of the spectrum, a narrowband filter passes a very tight band (for example, 3–7 nm full width at half maximum) centered on one of these emission lines. This dramatically rejects urban light pollution and moonlight, revealing nebular detail even from bright, Bortle 7–9 skies.

The Rosette Nebula Caldwell 49 50 Narrowband
Broadband version: [ADD LINK] The Rosette Nebula Caldwell 49 50 Broadband.jpg If you’re following me on social media you’ve already seen this and know that it’s the first real test of my new telescope (An 11″ Celestron F2 RASA)! I captured the nebula firstly in a narrowband test against the full moon. This means only collecting a small sliver of light with filters. The result was pretty cool, but the colours are false. I went back last night and photographed the Rosette again in “broadband” light as the moon had not risen. This allowed me to catch the nebula in it’s beautiful natural colours, but as a consequence you also record a LOT more stars which shine very brightly! This new telescope is super fast. Exposures that used to take me 5-10 minutes are now only 30-90 seconds. In fact, most of the detail here is captured in 30 second exposures – which is INSANE! Experienced imagers will notice a few errors (mostly focus / halos) but I’m pretty happy with this stunning image for a first fully completed shot from this new setup. I’m also using the new Celestron CGX mount and tripod too which is also impressive. New year – new gear! 40 x 30s mono QHY9m CCD 35 x 90s rgb QHY12 CCD 30 x 60s mono/Ha QHY9m CCD
Attribution: Dylan O’Donnell, deography.com

Because many emission nebulae glow strongly in Hα and OIII, narrowband imaging allows city-based astrophotographers to capture high-contrast signal that would otherwise be buried under skyglow when using broadband filters intended for galaxies, reflection nebulae, or natural star color work. Narrowband also lets you image through much of the lunar cycle—critical if you have limited clear nights. As long as your target is reasonably separated from the Moon and not too low in the sky, narrowband can deliver clean, deep data on weeknights and during bright phases.

In practical terms, narrowband astrophotography is especially advantageous when:

  • You live under heavy light pollution and cannot regularly travel to dark sites.
  • You want to image when the Moon is up and bright, without waiting for dark windows.
  • Your targets are primarily emission nebulae: supernova remnants, HII regions, planetary nebulae, or ionized bubbles.

While narrowband is a powerful technique, it is not a universal solution. Targets dominated by continuum emission—galaxies, reflection nebulae, and clusters—are best approached with broadband filters and dark-sky opportunities. Still, a huge subset of the most popular deep-sky objects benefit enormously from narrowband, making it a cornerstone method for urban imagers.

If you are just starting, the remainder of this guide will walk you through the required gear, how to choose appropriate filters, how to determine optimal exposure lengths for your setup, and post-processing workflows like SHO and HOO color mapping.

Essential Gear for Narrowband Imaging: Telescopes, Cameras, and Filters

A solid narrowband setup balances optical quality, tracking performance, and sensor characteristics. You do not need the biggest telescope or the most expensive camera to produce excellent results. Instead, aim for a well-matched system that delivers stable stars, good sampling, and consistent calibration.

Telescopes: Aperture, Focal Ratio, and Field

Short, fast refractors are the most common choice for narrowband. They offer:

  • Simple optical paths with minimal diffraction artifacts.
  • Flat, well-corrected fields when paired with a matched field flattener or reducer/flattener.
  • Wide fields ideal for large emission nebulae like the North America Nebula, Heart and Soul, or the Rosette.
90mm Apochromatic Refractor on NEQ6 Pro German Equatorial mount
This is the 90mm apochromatic refractor actively imaging. The moon and venus is visible as well. 🙂
Attribution: Gustaaf Prins from Haarlem, The Netherlands

Typical refractor apertures range from 60–130 mm, with focal ratios around f/4.8–f/7 (after reducers). Reflectors and astrographs—such as Newtonians or corrected Dall-Kirkhams—can also excel, especially with larger sensors, though they may require more frequent collimation and careful control of tilt and spacing.

Faster systems generally collect signal more quickly, but precise focusing, tilt control, and full-frame illumination become more demanding. The trade-offs are manageable for most hobbyists, and high-quality results are possible across a wide range of focal ratios with good technique.

Mount and Guiding

Accurate tracking is indispensable for the long subexposures common in narrowband. An equatorial mount with reliable periodic error performance and autoguiding is standard. Look for the ability to dither between frames (random sub-pixel shifts) to defeat pattern noise—this becomes crucial for avoiding walking noise during stacking.

AP german equatorial mount with scope
Astro-Physics German Equatorial Mount carrying a Takahashi Fluorite doublet 128mm f/8.1 refractor, aftermarket moonlite focuser; all supported by an ATS portable pier
Attribution: Gn842

Mono vs. One-Shot Color Cameras

You can capture narrowband data with either:

  • Monochrome cameras with individual Hα, OIII, and SII filters in a motorized filter wheel. This offers maximum efficiency because every pixel records the selected line, and you can pick precise bandpasses (e.g., 3 nm). It also enables true SHO and HOO mapping with independent channel control.
  • One-shot color (OSC) cameras paired with dual- or multi-band filters that pass Hα and OIII (and sometimes SII) simultaneously. This is more convenient and faster to set up, and it can produce excellent results on many targets. However, separation between lines is less clean and total integration per line is less flexible.

Modern cooled CMOS sensors dominate astrophotography due to low read noise, high quantum efficiency, and comparatively low cost. An important matching consideration is pixel scale in arcseconds/pixel, determined by pixel size and focal length. Aim to sample seeing-limited resolution near the Nyquist criterion; for typical suburban seeing, around 1–2 arcseconds/pixel often works well. Slightly under-sampling is forgiving and can produce small, sharp-looking stars on wide-field targets.

Filter Wheels and Tilt Adjustment

For mono imaging, an electronic filter wheel (EFW) simplifies acquisition, automates sequencing, and allows autofocus routines per filter. Ensure your backfocus spacing meets your flattener/reducer’s specification. Minute tilt in the imaging train can cause off-axis elongation; consider tilt plates or shims and diagnose with star inspections at the corners.

Before buying filters, understand the trade-offs in bandwidth and halo control, and confirm adequate filter diameter for your sensor and f-ratio to avoid vignetting.

Understanding Narrowband Filters: H-alpha, OIII, SII, and Dual-Band Options

All narrowband filters are not created equal. The passband width, central wavelength tolerance, out-of-band leak suppression, and anti-reflection coatings all influence star halos, contrast, and the consistency of your dataset.

Key Emission Lines and Wavelengths

  • Hα (Hydrogen-alpha, 656.3 nm): The strongest and most forgiving line. Many emission nebulae are rich in Hα. Even under the Moon, Hα remains productive.
  • OIII (Doubly ionized oxygen, 500.7 nm): Sensitive to stellar winds, shock fronts, and oxygen-rich regions. More prone to star halos due to filter coatings and shorter wavelengths. Moonlight and skyglow can encroach more in OIII, benefiting from narrower bandpasses.
  • SII (Singly ionized sulfur, 672.4 nm): Usually the weakest of the three, requiring longer total integration for balanced SHO compositions.

Bandwidth: 3 nm vs. 5–7 nm and Beyond

Narrower filters (e.g., 3 nm) reject more skyglow and moonlight, improving contrast in bright environments. They also better isolate OIII from nearby mercury and sodium emission lines common in urban lighting. The trade-offs:

  • Pros: Higher contrast, improved detail in emission regions, better separation between bands.
  • Cons: More expensive, tighter tolerances on tilt and f-ratio, potential signal attenuation for fast optics where the band shifts relative to the incident cone.

Filters above about 7 nm can be more forgiving, cheaper, and still deliver strong results, particularly in Hα. If your budget allows, a narrower OIII filter often pays the biggest dividends in light-polluted conditions due to improved halo control and skyglow rejection.

Dual- and Multi-Band Filters for OSC

Dual-band filters pass Hα and OIII concurrently to a color sensor. Some tri-band options add SII or broaden OIII/Hβ coverage. They provide:

Rosette nebula tõrva
Telescope: Orion 8″ Astrograph Mount: SkyWatcher EQ6R-PRO Guider: Starlight Xpress Lodestar Corrector: Baader MPCC Mark III Filter: Optolong L-eNhance Camera: Nikon D5600 (unmodified) Software for acquisition and processing: PHD2, APT, DeepSkyStacker, PixInsight, Photoshop Total exposure: about 4.5 hours (+bias and flat frames)
Attribution: Nielander
  • Convenience—no filter wheel or channel sequencing needed.
  • Efficiency—collect multiple lines in one exposure, helpful when nights are short.
  • Constraints—less selective separation of lines and stars; star color tends toward cyan/magenta without additional processing steps to restore more natural hues.

OSC narrowband is an outstanding entry point. As you gain experience, a mono camera with dedicated Hα, OIII, and SII filters grants more control over color mapping and noise balancing.

Filter Size, Tilt, and Halos

Ensure the filter diameter is sufficient for your sensor and f-ratio to avoid vignetting. For APS-C sensors on fast optics, 36 mm unmounted or 2-inch mounted filters are common; full-frame sensors often need 2-inch unmounted or larger. Anti-reflection coatings and good out-of-band blocking help prevent halos, but OIII can still show halos due to sensor microlenses, telescope optics, or reflections in the imaging train. You can mitigate these artifacts by careful spacing, tilt adjustment, and post-processing techniques.

Signal-to-Noise, Exposure Time, and Sub Length Optimization

Narrowband success hinges on collecting sufficient total integration time and choosing subexposure lengths that are long enough to be sky-limited but short enough to avoid dynamic range issues. The core principle is that stacking increases signal-to-noise ratio (SNR) roughly as the square root of the number of subs, assuming noise sources are uncorrelated.

Background-Limited Exposures

For CMOS sensors, aim for a subexposure where sky background noise dominates over read noise—often called being “background-limited.” If your sub is too short, read noise contributes disproportionately. If it’s too long, stars may saturate and you risk losing highlight detail.

As a rule of thumb for narrowband:

  • Typical subexposure lengths range from 180–1200 seconds on CMOS cameras, depending on f-ratio, filter bandwidth, and sky brightness.
  • Hα often permits shorter subs than OIII or SII for similar SNR because Hα emission is typically stronger, but OIII benefits from longer integration to counter skyglow and halo-related issues.

Estimating SNR and Sub Length

While exact calculations require your camera’s read noise, gain, and system throughput, you can approximate background limitation by testing a few subs and checking histogram statistics. A good target: the sky background peak separated from the left edge of the histogram by a noticeable margin. Then ensure brightest stars are not saturating excessively.

Conceptually, SNR relates to the total signal collected and combined noise sources. A simplified model for a single sub can be summarized as:


# Simplified SNR concept per sub (not to scale)
SNR_sub ≈ Signal / sqrt(Signal + Sky + Dark + Read^2)

# Stacking N subs improves SNR by ~sqrt(N)
SNR_total ≈ SNR_sub * sqrt(N)

Illustrative expressions emphasizing the benefit of stacking many subs while ensuring subs are long enough to be sky-limited.

If you find stars clipping at your chosen sub length, you can reduce exposure per sub and compensate by increasing the number of subs. For very bright stars in a field (e.g., around the Veil Nebula), consider a short-exposure star layer captured separately to restore unsaturated star cores in processing.

Gain, Offset, and Full-Well Capacity

Many CMOS cameras offer selectable gain and offset. Higher gain reduces effective read noise but lowers full-well capacity and dynamic range. Narrowband often benefits from moderate gains that balance these factors. The exact values depend on your camera’s characteristics—consult your camera’s documentation for unity gain or recommended astrophotography settings, then verify by testing star saturation and background separation on your setup.

Keep a consistent offset that prevents clipping the black level. Verify with a histogram that no significant portion of the background is crushed against the left edge.

Calibration Frames, Dithering, and Data Quality Control

Good calibration is non-negotiable for clean narrowband images. Narrowband exposures are long, and pattern noise or dust motes can ruin an otherwise excellent dataset if not corrected properly.

Bias, Darks, Flats, and Dark Flats

  • Bias frames: Very short exposures that record the camera’s readout pattern. Some modern CMOS workflows skip classical bias frames in favor of matching dark flats. If you use bias, ensure your software and camera play well with them.
  • Darks: Match the temperature, gain, and exposure length of your lights. Darks remove thermal signal and hot pixels—critical for long narrowband subs.
  • Flats: Correct vignetting and dust shadows. Capture flats for each filter and optical train configuration. A flat field panel or dusk sky with a diffuser can work; aim for mid-histogram illumination and avoid saturation.
  • Dark Flats (or Flat Darks): If you capture flats with finite exposure times on CMOS sensors, use dark flats matching the flat’s exposure to calibrate them correctly.

Maintain a library of darks at your common temperatures and exposure lengths. Flats should be refreshed whenever you change the optical train or notice new dust.

Dithering and Guiding

Dithering moves the pointing slightly between exposures. This breaks up fixed pattern noise and hot pixel trails, enabling stacking algorithms to effectively remove them. If you see diagonal banding in stacks, it’s often a sign of insufficient dithering cadence or magnitude. A dither every 1–3 subs is a good starting point for narrowband. Ensure guiding recovers before starting the next exposure.

Data Screening and Subframe Evaluation

Use subframe diagnostics to reject bad frames—those with trailing, wind shakes, cloud intrusions, or poor FWHM due to seeing. Selectively removing the worst frames can significantly improve your final SNR and detail, especially in OIII and SII channels where total signal is weaker.

During acquisition, monitor star FWHM, eccentricity, and the histogram. If the background level drifts due to high clouds or moonrise, adapt exposure strategy or pivot to a different filter less affected, as discussed in filter selection.

Capture Workflow: Planning, Sequencing, and Nightly Execution

A thoughtful plan maximizes signal and minimizes frustrations. Narrowband imaging spans multiple nights for a single target, often accumulating many hours across channels. A repeatable workflow keeps your data consistent.

Target Selection and Seasonality

Choose targets with strong emission lines and favorable altitude. High altitude reduces atmospheric extinction and improves seeing. Check seasonal visibility: for example, the Cygnus region in summer boasts rich Hα and OIII structures, while winter skies highlight targets like the Rosette and Barnard’s Loop. Use planetarium software to gauge when your target crosses the meridian and spend the bulk of imaging time near culmination.

Moon Phase and Separation

While narrowband tolerates moonlight, OIII is more sensitive to sky brightness. If the Moon is near your target or the phase is very bright, prioritize Hα or SII. If the Moon is low or far from the target, OIII can still be productive. The narrower your OIII filter, the better it will resist moonlight.

Sequencing Filters Across Nights

To balance your dataset:

  • Accumulate more total time in OIII and SII than Hα for SHO: a common starting ratio is Hα:OIII:SII ≈ 1:1.5–2:1.5–2, though the optimal ratio depends on the target.
  • Refocus per filter, especially if your filters are not parfocal or if your optical system is fast. Temperature changes also warrant periodic autofocus routines.
  • Capture Hα when conditions are less ideal (e.g., slight haze or higher moonlight) and reserve your best seeing windows for OIII to maximize subtle shock front detail.

Automation, Plate Solving, and Meridian Flips

Modern acquisition software can automate target centering, guiding, dithering, autofocus, and meridian flips. A robust sequence handles pauses during flips and resumes imaging with the correct filter and focus. Plate solving ensures accurate framing across sessions—important for combining data from different nights or cameras.

Environmental Considerations

Thermal control is vital for consistent calibration. Run your camera at a stable, achievable setpoint (e.g., −10 °C or −20 °C depending on ambient and camera capabilities). Manage dew with heaters on the objective and, if needed, on the filter wheel or adapters. Cable management prevents snags during slews and flips.

Processing Narrowband Data: SHO/HOO Palettes, Stars, and Detail

Processing narrowband data is both science and art. The goal is to combine channels thoughtfully, preserve faint structures, control noise, and render stars attractively. A typical workflow includes calibration, registration, integration (stacking), linear processing, nonlinear stretching, color mapping, and finishing touches.

Calibration, Registration, and Integration

Calibrate each channel with the proper master darks, flats, and bias or dark flats as described in calibration. Register all subs to a common reference frame—often the best Hα sub. Integrate each filter’s data separately to produce master H, O, and S images. Evaluate the masters for gradients, noise, and star profiles.

Linear Processing: Gradient Removal, Deconvolution, and Noise Control

Before stretching, correct gradients with background modeling tools or dynamic background extraction. Use star masks or range masks to protect stars while enhancing nebular contrast. Deconvolution can recover some sharpness; apply conservatively with accurate PSF estimation. Linear noise reduction (e.g., multiscale transforms) can tame chrominance and luminance noise before stretch.

Channel Combination and Color Mapping

Combine channels according to your palette of choice. In SHO, map SII→R, Hα→G, OIII→B. In HOO, map Hα→R and both Hα and OIII to the green and blue channels with appropriate weights. After mapping, perform color calibration steps suited to synthetic palettes—global color balance and tonal adjustments rather than stellar photometric calibration, which is more appropriate for broadband data.


# Example conceptual channel mapping steps
# SHO mapping (SII, Ha, OIII) -> (R, G, B)
R = SII
G = Ha
B = OIII

# HOO mapping (Ha, OIII) -> (R, G, B)
R = Ha
G = 0.2*Ha + 0.8*OIII
B = OIII

Example mappings to establish base color; refine with curves and selective masks.

Star Management

Stars in narrowband can look unnatural due to selective passbands; OIII can produce cyan stars while Hα enriches red hues. Consider strategies such as:

  • Creating a separate star layer (either from narrowband channels or a short broadband exposure) and blending carefully after processing the nebula.
  • Performing star reduction with masks to prevent crowding and emphasize nebulosity.
  • Treating halos locally with masked curves or morphological operations; see troubleshooting for more on halos.

Nonlinear Stretching and Contrast

Stretch the combined image gradually to avoid clipping black or white points. Use masked stretches and local contrast tools to reveal filaments without exploding star sizes. Multiscale sharpening and contrast can selectively enhance structure in shock fronts and stratified gas.

Finishing Touches

After star blending and final color balancing, small-scale noise reduction and color saturation adjustments bring the image together. If you used heavy noise reduction, revisit contrast to prevent softness. Always inspect at multiple zoom levels, confirming that your choices improve the image globally and do not introduce artifacts.

Color Palettes Explained: SHO, HOO, and Dynamic Combinations

One of narrowband’s creative strengths is the ability to assign channels to colors for meaningful or aesthetic results. While there is no single correct palette, some conventions and strategies help you communicate structure effectively.

The Rosette Nebula Caldwell 49 50 Broadband
If you’re following me on social media you’ve already seen this and know that it’s the first real test of my new telescope (An 11″ Celestron F2 RASA)! I captured the nebula firstly in a narrowband test against the full moon. This means only collecting a small sliver of light with filters. The result was pretty cool, but the colours are false. I went back last night and photographed the Rosette again in “broadband” light as the moon had not risen. This allowed me to catch the nebula in it’s beautiful natural colours, but as a consequence you also record a LOT more stars which shine very brightly! This new telescope is super fast. Exposures that used to take me 5-10 minutes are now only 30-90 seconds. In fact, most of the detail here is captured in 30 second exposures – which is INSANE! Experienced imagers will notice a few errors (mostly focus / halos) but I’m pretty happy with this stunning image for a first fully completed shot from this new setup. I’m also using the new Celestron CGX mount and tripod too which is also impressive. New year – new gear! 40 x 30s mono QHY9m CCD 35 x 90s rgb QHY12 CCD 30 x 60s mono/Ha QHY9m CCD Narrowband version (which is also quite nice!) below: [ADD LINK] The Rosette Nebula Caldwell 49 50 Narrowband.jpg
Attribution: Dylan O’Donnell, deography.com

SHO (SII, Hα, OIII)

Often called the “Hubble palette,” SHO maps S, H, and O to red, green, and blue respectively. It tends to highlight sulfur-rich regions in orange/yellow tones and oxygen-rich regions in teal/blue. Hα typically dominates, so balancing the channels by boosting SII and OIII or attenuating Hα is common.

SHO is effective for visualizing stratification and shock fronts and is robust under light pollution. Because SII is often weak, be prepared to invest longer integration time in SII to avoid noisy red channels.

HOO (Hα, OIII, OIII)

HOO maps Hα to red and OIII to green and blue. The resulting images often have natural-looking cyan/teal oxygen regions and red hydrogen regions. HOO can look more “realistic” to many viewers and may be easier to balance. If your OIII is noisy, consider blending a portion of Hα into green to stabilize the palette without overwhelming the oxygen signal.

Dynamic or Hybrid Palettes

Advanced processing might use channel-weighted blends or nonlinear mixing to highlight specific structures:

  • Variable contributions of Hα to the green channel in HOO for controlled teal.
  • Selective mapping where OIII dominates the blue channel in high-ionization zones while Hα contributes to green elsewhere, guided by masks.
  • Star color repair using a dedicated star layer (e.g., a short RGB exposure) to restore more natural stellar hues while preserving narrowband nebulosity.

If you are just starting, begin with straightforward SHO and HOO mappings and evolve to custom blends as you grow comfortable with masks and channel math. Revisit processing techniques to refine these palettes.

Troubleshooting Common Issues: Halos, Gradients, and Walking Noise

Even with careful capture, challenges arise. Recognizing common issues and knowing how to address them saves hours of frustration.

Star Halos in OIII

Blue-green halos around bright stars often originate from internal reflections, filter coatings, or sensor microlenses. Mitigation strategies include:

  • Using narrower OIII filters with strong out-of-band blocking.
  • Ensuring good spacing and orthogonality in the optical train; reduce tilt with adjustment plates if needed.
  • Post-processing with star masks to desaturate or darken halos locally, or blending a star layer acquired with shorter exposures.

Gradients and Uneven Backgrounds

Stray light, nearby streetlights, or moonlight can cause gradients, especially in OIII. Use flat-fielding, good shielding, and gradient extraction tools. A careful flat calibration per filter and session helps prevent residual vignetting from turning into gradients after stretching.

Walking Noise

Walking noise manifests as diagonal streaking after stacking and often results from insufficient dithering combined with hot pixels or fixed pattern noise. Increase your dithering frequency and amplitude, and ensure that guiding fully settles before each sub begins. Thorough dark subtraction further reduces the risk.

Elongated Stars and Tilt

Elongation toward one corner can indicate tilt or backfocus errors. Diagnose by comparing star shapes across the frame and making incremental adjustments to spacing. If the direction of elongation rotates with the camera, inspect the imaging train for non-orthogonality.

Saturated Star Cores

Long narrowband subs can clip bright star cores, especially in rich fields. Capture a set of shorter exposures for stars and blend them into the final image. You can also reduce sub length slightly and increase the number of subs to preserve dynamic range while maintaining total integration time.

Frequently Asked Questions

Can I do narrowband astrophotography with a one-shot color camera?

Yes. Pair an OSC camera with a dual- or multi-band filter that passes Hα and OIII (and sometimes SII). This approach simplifies capture and can produce excellent results, especially on bright nebulae. However, you’ll have less control over per-line integration and separation than with a mono camera. If you plan to explore SHO mapping extensively and want maximum flexibility, a mono camera with individual Hα, OIII, and SII filters is the more capable path.

How much total integration time do I need for narrowband images?

More is almost always better. For a balanced SHO image from bright skies, many astrophotographers aim for 10–20 hours total, with extra weight on OIII and SII. For smaller sensors or very fast optics, you can achieve strong results with less time, but pushing beyond 10 hours typically improves faint structures and smoothness. OIII often benefits from the lion’s share of integration in light-polluted environments.

Final Thoughts on Choosing the Right Narrowband Workflow

Narrowband astrophotography opens the deep sky to those living under city lights. By isolating Hα, OIII, and SII emission lines, you can capture high-contrast nebular detail through much of the lunar cycle and in heavy skyglow. The most important ingredients for success are consistent calibration, careful exposure planning, and a thoughtful processing strategy that balances the channels and controls stars.

Start with a manageable, reliable setup. A modest refractor on a capable equatorial mount, a cooled CMOS camera, and well-chosen narrowband filters can deliver remarkable images. As you refine your approach, revisit the guidance in exposure optimization, tweak your capture sequencing, and experiment with color palettes to tell the story of each nebula. A few extra hours of integration and a bit more care in calibration and dithering often make the difference between a good image and a great one.

Redrosedust wright f2000
A close up view of the Rosette Nebula. The red color comes from Hydrogen.
Attribution: Image based on data obtained as part of the INT Photometric H-Alpha Survey of the Northern Galactic Plane, prepared by Nick Wright, University College London, on behalf of the IPHAS Collaboration

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