In short
- SCD's Mini Blackbird 1280 is a cooled mid-wave infrared (MWIR) detector-dewar-cooler with 1280 × 1024 pixels at 10 µm and a published NETD under 25 mK. Teledyne FLIR's Boson 640 is an uncooled long-wave infrared (LWIR) core with 640 × 512 pixels at 12 µm, and 20–60 mK depending on model and grade.
- At the same field of view, the Blackbird has twice the pixels per degree. Behind a long lens it puts many times more pixels on a small drone than any wide staring camera can.
- The Boson draws about a watt, weighs tens of grams with a lens, has no cryocooler, and comes with a published US export classification and list price. SCD publishes none of those for the Blackbird.
- A 360° staring ring needs 12 cores at 32°. At the narrow fields where the Blackbird's advantage shows, the same ring needs dozens to well over a hundred.
Why compare these two
Two thermal cores sit at opposite ends of the counter-drone design space. Teledyne FLIR's Boson 640 is a small, low-power uncooled long-wave core, widely used in fixed and staring cameras; with its 14 mm lens it covers a 32° horizontal field of view with 640 × 512 pixels at up to 60 Hz. SCD (SemiConductor Devices) makes one of the most compact cooled, high-definition mid-wave cores: the Mini Blackbird 1280, a 1280 × 1024 MWIR detector that weighs under 350 g with its cooler. The question this post asks is what each one actually buys you when the target is a small drone.
Every number on either core comes from the manufacturer's own published material, listed at the end. Where arithmetic is involved, the assumptions are stated next to each table.
The two cores on paper
SCD publishes two Mini Blackbird 1280 variants. The product page and its linked datasheet describe a HOT XBn version. A separate 2024 datasheet describes an HFM ("Hot Full Mid-wave") version with a wider band and a higher frame rate. Both are shown below.
| SCD Mini Blackbird 1280 (XBn) | SCD Mini Blackbird 1280 HFM | Teledyne FLIR Boson 640 | |
|---|---|---|---|
| Band | MWIR, 3.6–4.2 µm (1–4.2 µm on request) | MWIR, 3.6–4.9 µm | LWIR, 8–14 µm |
| Detector | Cooled HOT XBn, FPA at 150 K | Cooled HOT HFM, 120 K operating temp. | Uncooled VOx microbolometer |
| Format / pitch | 1280 × 1024 / 10 µm | 1280 × 1024 / 10 µm | 640 × 512 / 12 µm |
| NETD (published) | < 25 mK at 70% well fill (2 Me⁻ capacitor) | 25 mK at 70% well fill | Boson: ≤40 / ≤50 / ≤60 mK (Industrial / Professional / Consumer). Boson+: ≤20 / ≤30 mK (Industrial / Professional) |
| Max frame rate | 90 Hz raw full window; 60 Hz fully processed | 100 Hz raw (Medium Camera Link) | 60 Hz (30 Hz selectable); export "slow" variants below 9 Hz |
| Optics | F/3.4 or F/4 cold stop; lens from integrator | F/4; lens from integrator | Catalogue lenses, e.g. 14 mm f/1.00 (32°) and 55 mm f/1.01 (8°) |
| Power | Cooler < 2.5 W + proximity electronics < 2.5 W (23 °C, 60 Hz); "about 5W" total | 10 W (25 °C steady state) | 500–1,550 mW depending on configuration and temperature |
| Size / weight | 80 mm along the optical axis; < 350 g | 80 mm; < 350 g | 21 × 21 × 11 mm without lens; 39 g and 35 mm long with the 14 mm lens |
| Cooler | Stirling micro-cooler; options K580, SX-020, RM1S | Split linear | None |
| Output | Camera Link, 13-bit | Digital LVDS / Camera Link | CMOS, BT656-like or USB3 video |
| Export classification | Not stated by SCD | Not stated by SCD | NDAA compliant, ITAR free, EAR 6A003.b.4.a (FLIR) |
| Published price | None found | None found | $4,334–$6,450 at a US distributor for the 14 mm radiometric core, by sensitivity grade |
Two cautions about this table. First, a Mini Blackbird is not a camera. SCD supplies the detector, dewar and cooler with optional proximity electronics. An integrator still has to add the lens, the enclosure and the video pipeline. A Boson ships as a complete core with a lens. Second, the NETD figures are measured at different f-numbers: F/4 for the Blackbird and f/1.0 for the Boson. Each figure is fair to its own sensor, but they are not one test.
What each band actually sees
A small quadcopter is not a jet. Its heat comes from motors, speed controllers and the battery, and most of the airframe sits near ambient temperature. Wien's law puts the emission peak of a 300 K (27 °C) object at about 9.7 µm. Even at 340 K (67 °C), a hot motor housing, the peak is about 8.5 µm. Both fall inside the Boson's 8–14 µm band and well outside the Blackbird's 3.6–4.2 µm band.
Blackbody arithmetic makes the gap concrete. A 300 K surface emits about 147 times more radiance in 8–14 µm than in 3.6–4.2 µm, and about 405 times more photons. Against the HFM variant's 3.6–4.9 µm band, the ratios are about 36 and 89. The mid-wave band compensates in two ways. Its radiance changes faster with temperature: about 4% per kelvin at 300 K, against about 1.5% for 8–14 µm. And a cooled photon detector is far more sensitive per photon than a microbolometer. This is why cooled MWIR cores still reach lower NETDs than uncooled LWIR, despite seeing fewer photons from room-temperature objects. Teledyne FLIR's own guidance places uncooled cameras in the long-wave band because that is where ambient-temperature targets emit most of their energy.
The atmosphere also matters. In Teledyne FLIR's fog-modelling article, LWIR penetrated fog better than MWIR in every case they studied: about four times the range in Category II fog. MWIR did best in the hot conditions of summer or tropical climates, and was more affected by pollutants. In rain the two bands performed similarly. The article's own conclusion is that sensitivity and target signature still have to be weighed for each application. Field signature work on small rotorcraft has compared the two bands directly. Fudala et al. (2019) measured a DJI Phantom 4 and a DJI Inspire in both bands, against clear sky, cloud and land, at three aspect angles. Results like these depend on the scene, so neither band can be declared the winner from them.
Some things are clear. Against a clear sky, a drone in LWIR is a warm object on a cold background. Teledyne FLIR notes that, against the cold sky, an infrared camera can often detect a moving drone as a cluster as small as 2 × 2 pixels. Neither band removes the hard cases, such as warm cloud edges, birds and sun glints. Those are an algorithm problem whichever band you pick.
Pixels on target: the Blackbird's real advantage
Here is the geometry. Assumptions: a 0.35 m quadcopter, a square target, and pixels across the target = size ÷ (range × IFOV), where IFOV = pixel pitch ÷ focal length. The Boson lenses are FLIR catalogue lenses. SCD publishes no lens, so every Blackbird focal length below is an assumption, chosen either to match the Boson's field of view or to represent a typical long cooled zoom.
| Configuration | Focal length | HFOV | Px/degree | Px @ 250 m | Px @ 500 m | Px @ 1 km | Px @ 2 km | Cores for 360° |
|---|---|---|---|---|---|---|---|---|
| Boson 640, 14 mm | 14 mm | 30.7°* | 20.9 | 1.63 | 0.82 | 0.41 | 0.20 | 12 |
| Mini Blackbird 1280, matched FOV (assumed lens) | 23.3 mm | 30.7° | 41.7 | 3.27 | 1.63 | 0.82 | 0.41 | 12 |
| Boson 640, 55 mm | 55 mm | 8.0° | 80.1 | 6.42 | 3.21 | 1.60 | 0.80 | 46 |
| Mini Blackbird 1280, matched FOV (assumed lens) | 91.7 mm | 8.0° | 160.2 | 12.83 | 6.42 | 3.21 | 1.60 | 46 |
| Mini Blackbird 1280, 300 mm (assumed lens) | 300 mm | 2.4° | 523.7 | 42.0 | 21.0 | 10.5 | 5.25 | 148 |
*Computed from pitch, array width and focal length. FLIR publishes 32.0° for this lens, about 20 pixels per degree, which changes these counts by about 4%.
Read the table in three ways.
At the same field of view, the Blackbird has twice the linear resolution. That means twice the pixels across the target at every range, and in pure geometry a sub-pixel drone fills four times as much of each pixel. Add a published NETD of 25 mK, against 20–60 mK across the Boson family, and the Blackbird has the lower noise floor. Sensitivity is its first clear win.
There is a catch at wide fields. Diffraction blurs a point into a spot with an angular diameter of about 2.44 × wavelength × f-number ÷ focal length. For the Boson's 14 mm f/1.0 lens at 10 µm, that spot is about 1.7 mrad. For a Blackbird at F/4 with a matched 23 mm lens at 3.9 µm, it is about 1.6 mrad, nearly the same. At matched wide fields, the Blackbird's extra pixels sample almost the same blur more finely. They do not separate detail twice as well, and the four-fold geometric fill gain shrinks, because the blur spreads the drone's signal over several of the smaller pixels. This simple model leaves out aberrations and turbulence.
The cooled core earns its keep at long focal lengths. This is the second clear win, and the bigger one. A cooled detector is sensitive enough to work behind slow optics. Teledyne FLIR notes that cooled MWIR can use lenses as slow as f/5.5, allowing focal lengths beyond 1,000 mm at a manageable lens size and cost. It also puts the cost crossover from uncooled LWIR to cooled MWIR at focal lengths above about 250 mm. An uncooled core needs f/1-class optics, so its aperture grows with focal length. Behind a 300 mm lens, the Blackbird resolves a 0.35 m drone at 2 km with about five pixels, while the 14 mm Boson sees a fifth of a pixel. If you need to identify a small drone at long range, this is the right tool.
- SCD USA, "Mini Blackbird 1280" product page — https://scdusa-ir.com/products/mini-blackbird-1280/
- SCD USA, Mini Blackbird SXGA datasheet (HOT XBn), linked from the product page — https://scdusa-ir.com/wp-content/uploads/2023/04/Mini_Blackbird-1280_14-2-18_updated-V2a.pdf
- SCD USA, Mini Blackbird 1280 HFM datasheet V1d — https://scdusa-ir.com/wp-content/uploads/2024/10/Mini_Blackbird-1280_HFM_V1d.pdf
- Teledyne FLIR OEM, "Boson — Uncooled, LWIR OEM Thermal Camera Module" product page (specs, sensitivity grades, Boson+ comparison, model list incl. 20640A032, export statement) — https://oem.flir.com/products/boson/
- FLIR, Boson Thermal Imaging Core Product Datasheet, Doc. 102-2013-40 Rel. 330, Oct 2019 (distributor-hosted copy; Table 1, Tables 10–11) — https://www.elimec.co.il/_Uploads/dbsAttachedFiles/Boson.pdf
- OEM Cameras, Teledyne FLIR Boson 640 × 512 14 mm 32° HFoV radiometric core listing (variant prices) — https://www.oemcameras.com/products/20640a032-htm
- Teledyne FLIR OEM, "Thermal Infrared Sensor Design Considerations for Counter-UAS Defense" — https://oem.flir.com/learn/discover/thermal-infrared-sensor-design-considerations-for-counter-uas-defense/
- Teledyne FLIR, "Can Thermal Imaging See Through Fog and Rain?" — https://www.flir.com/discover/rd-science/can-thermal-imaging-see-through-fog-and-rain/
- N. Fudala et al., "Comparison of midwave versus longwave intensity signatures for infrared search and track of small rotorcraft unmanned aerial vehicles," Optical Engineering 58(4) 043107, 2019 — https://doi.org/10.1117/1.OE.58.4.043107
- NIST CODATA, Wien wavelength displacement law constant — https://physics.nist.gov/cgi-bin/cuu/Value?bwien
Independent commentary by GOTEAM. Not affiliated with or endorsed by SCD or Teledyne FLIR. Specifications are quoted from each manufacturer's published material and have not been independently tested by us. Pixel counts, diffraction spots, blackbody ratios and ring sizes are our own arithmetic, and every Blackbird focal length in them is an assumption, not an SCD product.
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