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Ariel spectrometer difference

Ariel was designed as a measurement-critical spectrometer for MProbe systems, with low-aberration optics, astigmatism correction and firmware data correction built into the instrument.

Ariel astigmatism-corrected fiber-optic spectrometer front view
Ariel astigmatism-corrected fiber-optic spectrometer.

What is Ariel?

Ariel is an astigmatism-corrected fiber-optic spectrometer using an unfolded, fixed and rugged Czerny-Turner optical bench with 80 mm focal length. It uses a 2048-pixel CMOS detector, USB 2.0 and 1 Gb LAN communication, and performs data correction and conditioning in firmware.

Why Ariel?

Many compact fiber-optic spectrometers are optimized for low cost and small size. In an MProbe system, the spectrometer is not a commodity part; it determines signal quality, measurement speed, repeatability and the ability to resolve weak interference fringes. Ariel uses different engineering trade-offs in optical configuration and calibration.

Comparison table of optical design choices for fiber-optic spectrometers
Optical-design trade-offs for compact fiber-optic spectrometers.

Optical design choices

An unfolded Czerny-Turner design keeps the optical paths separated, reducing scattered light compared with crossed-path compact designs. A fixed optical bench improves mechanical and thermal stability, which matters in industrial environments where vibration and drift can make annual recalibration difficult.

Ariel's 80 mm optical bench avoids the high grating dispersion typically needed in a smaller 40 mm bench. That helps reduce astigmatism and coma while preserving clean peak shape across the spectrum.

Unfolded Czerny-Turner spectrometer layout
Unfolded Czerny-Turner layout.
Crossed Czerny-Turner spectrometer layout
Crossed Czerny-Turner layout.

Astigmatism correction

Off-axis light reflected from a spherical mirror focuses at different positions in the sagittal and meridional planes. A point at the entrance slit becomes a line at the sensor, reducing light collection and degrading spectral shape. Ariel uses a toroidal mirror to correct astigmatism without adding a separate cylindrical-lens element.

Ariel spectrometer astigmatism correction comparison at the sensor plane
Sensor-plane comparison: Ariel corrected image, same design without correction, and higher-dispersion uncorrected design.

Data calibration and correction

Wavelength calibration is essential, but active CMOS detector arrays need more than wavelength correction. Each pixel has its own charge-to-voltage conversion and source follower, so dark signal, non-linearity and fixed-pattern noise vary by pixel. Ariel corrects these effects in firmware using factory calibration data.

CMOS detector pixel signal conversion path
CMOS detector signal conversion path for each pixel.
Ariel spectrometer signal correction diagram
Signal correction path: dark signal, non-linearity and optional fixed-pattern-noise correction.

Dark signal correction

Dark signal depends on integration time and temperature. In CMOS detectors, each pixel can have a different dark-current level and a different rate of change. Ariel stores calibrated correction coefficients and applies them based on detector temperature and integration time.

Dark signal dependence on integration time
Dark-signal dependence on integration time.

Non-linearity and fixed-pattern noise

The S11639 CMOS detector is close to linear at lower signals, but non-linearity increases near the top of the range and differs slightly pixel to pixel. Ariel corrects non-linearity through factory calibration. Fixed-pattern noise is also present in CMOS arrays; baseline calibration corrects much of it, and optional FPN calibration can further improve spectrum smoothness.

Typical detector pixel non-linearity before and after correction
Typical detector-pixel non-linearity before and after correction.
Fixed-pattern noise in CMOS detector pixels
Fixed-pattern noise in CMOS detector pixels.

Related system: Ariel spectrometer.

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