Performance of an uncooled imaging interferometric spectrometer with intrinsic background radiation

Abstract. A signal-to-noise performance of an imaging Michelson interferometer based on corner cubes is modeled and experimental results are presented. The influence from the background radiation of the uncooled sensor is explained. The noise equivalent spectral radiance is determined in the 700 to 1300  cm  −  1 range at two spectral resolutions using blackbody sources. The performance of the sensor system is tested on a scene at an average temperature of 19°C. From these results, the performance is given in terms of number of samples and spectral resolution. The performance model is used to predict the sensor performance at different scene temperatures.


Introduction
The properties of the corner-cube interferometer were analyzed at an early stage. 1 An imaging corner-cube Michelson spectrometer has been designed and presented. 2,3 This design is more compact than the Sagnac configuration, less sensitive to beamsplitter imbalance, and easy to align. However, the corner cubes must have good wavefront quality and proper alignment to maintain high modulation efficiency. It is important that the fore-optics design limits the potential vignetting effects by positioning the entrance pupil of the imaging lens inside the interferometer. 4 The technology has subsequently been applied in field detection experiments. 5 The signal-to-noise and imaging characteristics of interferometric instruments compared to dispersive spectrometers are important issues. In remote sensing applications, it is a challenge to find a common figure of merit. 6 Fellgett and Jacquinot advantages are often cited for interferometric instruments although these advantages come with various caveats. In the thermal spectral region, dispersive instruments are sensitive to internal radiation from the slit mount, grating losses, etc. Interferometric instruments without a slit can be designed to be more flux efficient. For room temperature sensors, internal back-radiation from the sensor into the interferometer and back to the sensor is sometimes a dominating factor. It can be shown that with object temperatures below the intrinsic sensor temperature, interferograms with reversed sign are obtained. At equal temperature, the signal may almost disappear depending on potential difference in emissivity between the intrinsic source and the object being studied. The spectral signal obtained from the measurement must be corrected for the internal source to obtain the spectrum of the object. An interesting class of sensors are the microbolometer cameras. Even for these high temperature sensors, the sensitivity can be <30 mK at F∕1 optics and at a frame rate of 30 Hz. 7 Establishing the signal-to-noise ratio (SNR) for the uncooled interferometric systems is of considerable interest. Although such systems have been studied over several decades, the SNR related to remote sensing applications is not fully understood. This paper is an effort to support the future application-oriented development of such systems. The importance of background radiation is shown and modeled. The effect of the choice of scanning mode (static scene or scanned scene) and the resulting difference in SNR is described. The results should be useful in selecting proper applications for this technology.
In the next section, the theoretical model of the sensor system is presented. Experimental results and model agreements are presented in Sec. 3. Results are discussed and conclusions given in Sec. 4.

Sensor System Model
The imaging spectrometer presented here can be designed for remote sensing in two different modes. In the staring mode, the interferogram is obtained by moving the corner cube along the x axis as shown in Fig. 1. In the static Fourier transform spectrometer, the interferogram is obtained by scanning the scene over the field of view (FOV). 8 For a double-sided interferogram, the zero-path-difference (ZPD) fringe is positioned close to the center of the image. Every position in the scene is tracked over the FOV and in this way the interferograms of all scene positions are obtained. The noise characteristics is in this case not only dependent of the temporal noise characteristics of the individual pixels but also on the quality of the nonuniformity correction and the stability over time of this correction. The scene scanning direction is described by the y axis in the models as follows.
Considering an incident plane monochromatic wave with irradiance E 0 , the irradiance at the detector for an optical path difference (OPD) equal to x, where x is the OPD from the ZPD point, is given by 9 E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 0 1 ; 1 1 6 ; 4 6 5 where τ 1 and τ 2 are the total transmissions in the two respectively arms. If wavenumbers (wherẽ σ ¼ 1∕λ) are used, this equation becomes E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 0 2 ; 1 1 6 ; 4 0 0 where τ b ¼ τ 1 þτ 2 2 and m ¼ 2 ffiffiffiffiffiffi τ 1 τ 2 p τ 1 þτ 2 are coefficients corresponding to the overall bias component and the modulation depth, respectively. If τ 1 ¼ τ 2 , the modulation m becomes unity. Ideally  4)]. By moving the left corner cube along the optical axis (to the left, þΔX , or to the right, −ΔX ), the position of the ZPD fringe will be moved over the array [Eq. (5)]. In the figure, the ZPD fringe has been moved downward by moving the left corner cube to the right (the corner cube marked blue). A scanning of a scene is performed using a stepper motor, enabling a uniform movement of the left corner cube along the optical axis.
Phase errors due to corner cube imperfections can lower the modulation depth. 10 The polarization properties of the corner cubes might also influence the modulation depth. 11 Allowing for an unknown phase-distortion function, Eq. (2) now becomes Assuming a low temperature blackbody target in the first measurement, i.e., S 1 , and a high temperature blackbody in the second measurement, i.e. S 2 , the following relation is obtained E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 2 ; 1 1 6 ; 7 1 1 E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 3 ; 1 1 6 ; 6 5 5 where L 1 and L 2 are the blackbody radiances at temperatures T 1 and T 2 , respectively, where T 1 < T sensor and T 2 > T sensor . The blackbody radiance is given as E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 4 ; 1 1 6 ; 6 0 7 where h is the Planck constant, c is the speed of light, and k is the Boltzmann constant. The wavenumberσ is here given in SI units. The scale must be changed to obtain the unit of cm −1 common among spectroscopists. The interferogram is obtained by sampling over the OPD from −l to l relative to the ZPD at equidistant positions. If the stepping size is δx and N samples are obtained on each side of the ZPD, the total number of samples is 2N þ 1. The maximum OPD is l ¼ Nδx. The maximum wavenumber,σ max , is obtained fromσ max ¼ 1∕δx. The Nyquist wavenumber is half this value orσ Nyquist ¼ 1∕ð2δxÞ. The wavenumber step is δσ ¼σ max ∕ð2NÞ ¼ 1∕ð2lÞ. This is also the common definition of spectral resolution. In practice, there are many ways that this resolution might be compromised, primarily from deficiencies in the optics.
The Fourier transform of the sampled interferogram is given as E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 5 ; 1 1 6 ; 4 2 1 where the zero-wavenumber term appears at position 1. This transformation preserves the signal power. This means, e.g., that for a random signal, the transformed signal preserves the same power. This is useful when discussing SNRs. Taking the absolute value of a complex number however changes the statistical properties. If the initial random noise is a normal probability distribution with variance σ 2 n , the transformed noise will have a Rayleigh distribution. The Rayleigh probability density function is given by E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 6 ; 1 1 6 ; 2 9 8 where the variance is given by σ 2 R ¼ ð2 − π∕2Þ σ 2 n and σ 2 n is the initial sensor-signal noise variance. The spectral signal bias of the Rayleigh distribution is bias ¼ ffiffiffiffiffiffiffiffi π∕2 p σ n . These results can be used in calculating the expected spectral SNR at given number of samples and spectral resolution.
The spectral SNR (denoted with subscript ofσ) at a specific object radiance is given by E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 7 ; 1 1 6 ; 1 8 9 SNR˜σ and E Q -T A R G E T ; t e m p : i n t r a l i n k -; e 0 1 8 ; 1 1 6 ; 1 3 3 NESRσ where NESR is the noise equivalent spectral radiance required in the object plane and S 0 ðσÞ ¼ RðσÞL 0 ðσÞ. The noise equivalent temperature difference (NETD) can be obtained from where NETD is commonly determined at a blackbody temperature of 20°C. The optimal number of channels depends on the spectral structure of the target. If the only difference between samples is a wavenumber-independent emissivity, only separation in terms of a graybody emissivity is needed. This is still a quite challenging task since atmospheric absorption and emission and reflected radiation have to be taken into account. Often the object surface is assumed to be diffuse making reflected radiation independent of surface orientation. This obviously does not apply to specular surfaces, for which the cloud cover variation can be of importance. Often, however, the downwelling radiation is neglected. It is also assumed that the range variation in the scene is small. It is important to include spectral regions with low atmospheric absorption, i.e., bands close to 10 μm. To obtain emissivity for each channel, a supplementary assumption has to be added. Often the observation that many solid objects show a smooth emissivity behavior is used to make the problem solvable.
If scenes are obtained at short ranges, the atmospheric absorption can be ignored. With the limited SNR that can be obtained with an uncooled system, the practical application is on separating objects in the scene due to their combined temperature and emissivity variation.
The sensor framerate is often set to a fixed value, usually the maximum framerate allowed by the thermal time constant. An important factor is the total time for obtaining a spectral image. With a fixed recording time and fixed framerate, the number of frames is determined. Given a fixed number of frames, how is the system optimized for a particular purpose? This will depend on the spectral range and the required Nyquist wavenumber. Aliasing is avoided by the filtering effect of the detector spectral responsivity. This also means that only the spectral region where the sensor spectral responsivity is high (resulting in reasonable SNR) is of interest. The minimum wavenumber limitσ max ¼ 2σ Nyquist where the Nyquist wavenumber is at the onset of aliasing effects. With a spectral resolution of δσ, the number of one-sided samples are N ¼σ max ∕ð2δσÞ. Table 1-3 give experimental settings for the sensor system as presented here.
With a framerate of 25 Hz, the following recording times as given in Table 2 are obtained. The SNR varies for the four cases, as expected. The normalized SNR varies as given in Table 3. Table 1 Number of samples at maximum wavenumber. From these settings, it seems beneficial to not set the Nyquist wavenumber any higher than necessary. This could conflict with the bandwidth requirements with respect to resolving spectral features to obtain adequate spectral discrimination. The SNR result can therefore not be taken as the only criterion for optimizing the acquisition of the scene's spectral information. This will be discussed further below.

Experimental Methods
The interferometric imaging sensor using an uncooled detector array is shown in Fig. 2. The spectrum can be obtained by either scanning one of the corner cubes along its axis or by scanning the image along a panoramic scene. In the latter case, the responsivity of each pixel must be the same to a high accuracy. This is difficult to achieve by a nonuniformity correction (NUC) process, and therefore some SNR degradation is expected. The noise properties are slightly different for the two cases but should be qualitatively similar. Most of the analysis below is done using the scanning of one of the corner cubes.
The setup is a slightly modified standard Michelson configuration. As described in Ref. 2, the two plane mirrors were substituted with two front-surface (Au coated) corner-cube reflectors, of 63.5-mm diameter, purchased from Edmund Scientific. Specified retroreflection parallelism was 1 second of arc. The beamsplitter and a nominally identical compensator plate, purchased from II-VI Infrared, were made from ZnSe, in rectangular format 70 mm × 100 mm × 7 mm. One surface of the beamsplitter was a nominal 50/50 LWIR beamsplitter coating, while the other surface (and those of the compensator) was coated with a broadband antireflector, with <1% reflection across the 8 to 14 μm band. The two ZnSe plates were mounted together, separated by metallic shims of about 0.25-mm thickness, with the beamsplitter coating on an interior surface.
The uncooled LWIR camera, A655SC (FLIR Systems), has a microbolometer focal-plane array. It has 640 × 480 pixels, a pixel pitch of 17 μm and a spectral response between 7 and 14 μm. The NETD is <30 mK and the digital output range is 14 bits. The focal length of the F∕1.0 lens is 41.3 mm, providing an FOV of ∼11 deg ×15 deg. The maximum full frame rate is 50 Hz.
The frame rate during scanning was typically set to 25 or 50 Hz. The translation speed of the left corner cube along the optical axis during scanning was 0.01 mm∕s, provided by the stepper motor, TDC001 (Thorlabs). A schematic sketch of the scanning mechanism of the interferometric imaging sensor was shown in Fig. 1. Fig. 2 The hyperspectral camera (with a protective cover removed). The basic parts are two corner-cube mirrors: a beamsplitter and an LWIR uncooled camera. A lateral shift d is introduced in the left corner-cube mirror, which can be moved along its (optical) axis by a stepper motor (Thorlabs TDC001) where AEΔx denotes differences from the ZPD position.
There are two ways of obtaining an interferogram. When one of the corner cubes is scanned along its optical axis, a temporal interferogram is obtained at each imaging pixel. Noise is dominated by the temporal noise and not affected by sensor nonuniformities since the spectrum is obtained at each individual pixel. The (Gaussian-distributed) noise of the temporal interferogram is measured to be σ x ¼ 4.3 DN where x denotes scanning the corner cube along the x-coordinate. The temporal NETD is 30 mK corresponding to 3.4 DN. Keeping the corner cubes at fixed positions, the interferogram is obtained by scanning the scene and monitoring the signal from the same object position during this scan. With this approach, there are several errors that can degrade the SNR. The most important one is the ability to obtain NUC of the sensor. Even for a well-behaved system, the noise is expected to increase substantially. In the example shown here in Fig. 3, the noise level is increasing to σ y ¼ 10.0 DN, where y denotes scanning the scene in the y-coordinate direction. The noise is more than doubled. The radiometric correction of the sensor is of outmost importance and in particular in scanning of the scene, which have practical advantages. The spectral signal standard deviation based on Rayleigh statistics is σ x;R ¼ 2.8 DN and σ y;R ¼ 6.6 DN, respectively. There is also a small bias, bias x;R ¼ 5.4 DN and bias y;R ¼ 12.5 DN. The test of the experimental system will hereafter be based on scanning the corner cube.
A blackbody source model SR-800R from CI Systems was used for radiance calibration. The signal was first studied for a blackbody target at 60°C at a constant nominal spectral resolution of δσ ¼ 27 cm −1 and varying the number of samples N samples ¼ 2N þ 1, where N was equal to N ¼ f80; 120; 240g. The Nyquist wavenumber will under these conditions be proportional to N andσ Nyquist ¼ f2155;3232.5;6465g cm −1 . With the Fourier transform as defined above, the signal is proportional to ffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi 2N þ 1 p . The SNR can be increased by increasing the number of samples. With a constant framerate, this will require increased recording time. With a framerate of 25 Hz, the signals shown in Fig. 4 are obtained after t rec ¼ f3.2; 4.8; 9.6g s at optimal sampling.
A higher SNR can be obtained by sampling at a lower spectral resolution. This comes at a cost of poorer ability to resolve narrower bands. Whether this potential loss of information is acceptable depends on the specific application, i.e., the spectral properties of the object under study.
The spectral resolution was set to δσ ¼ 54 cm −1 and the number of samples set to N samples ¼ 2N þ 1, where N was equal to N ¼ f40; 60; 120g. The Nyquist wavenumbers are Fig. 3 The same spectrum obtained in two different ways when imaging a blackbody at 60°C. The blue curve is obtained when translating the corner-cube along the optical axis, i.e., changing the x -coordinate while keeping the y -coordinate at zero in Eq. (5). The red curve is obtained when scanning in the image plane, i.e., changing the y -coordinate while keeping the x -coordinate at zero. the same as already mentioned, i.e.,σ Nyquist ¼ f2155; 3232.5; 6465g cm −1 . Again, the signal is proportional to ffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi 2N þ 1 p . With a framerate of 25 Hz, the signals shown in Fig. 5 are obtained after t rec ¼ f1.6; 2.4; 4.8g s at optimal sampling. Similar data to those obtained for the 60°C blackbody target were also obtained for a 10°C target. The sensor temperature is in between these two temperatures, and the sensor radiance can be determined as described already. The resulting sensor spectral radiance is shown in Fig. 6. These data were compared to blackbody radiation, and the corresponding sensor temperature was determined to 32°C. This radiation is back injected into the interferometric system and will always be present since the sensor is stabilized at this temperature. This must be considered when deriving the final spectral signal from any object of interest.
Simultaneously when determining the sensor radiation, the spectral response of the sensor can be obtained by Eq. (12). The result is shown in Fig. 7. The relative responsivity is in good agreement with published typical response for this type of sensors.
Correcting the signal with respect to the back-injected radiance from the sensor, the target spectrum can be obtained. This is illustrated for the target at 10°C in Fig. 8. The agreement is reasonable considering the type of sensor involved.
The correction due to the back-radiation from the uncooled sensor is important to obtain reliable radiometric measurements. There is a concern that radiation emanating from the inside of the sensor system could result in interferences with a phase variation of S 1 that deviates from S 2 in Eq. (12). A common procedure in practice is to use the absolute value of each parameter. If both S 1 and S 2 have the same phase dependence, this works well. Phase error due to asymmetric sampling relative to the ZPD is here disregarded. However, there is a possibility that radiation emanating from the internal parts of the interferometer, i.e., S 2 , can result in phase variations that deviate from those experienced by S 1 . 14 This is especially the case when the emitter is placed between the sensor and the interferometer. 15 The interferogram resulting from the radiation from the sensor is expected to have a phase difference of π radians relative to the radiation from the target. If this is exactly true, the simple procedure using absolute values as described above still works. If there are deviations from this ideal case, the complex-valued processing in Ref. 14 could improve results. It is therefore of interest to quantify the magnitude of possible errors for each interferometer design. The responsivity was calculated using Eq. (10) in Ref. 14. . The Nyquist wavenumber is 2155, 3232.5, and 6465 cm −1 , respectively. The signal is constituted by two counteracting contributions: the external blackbody radiation and the intrinsic radiation emanating from the sensor. Fig. 6 The sensor radiance is here shown in the blue curve. By combining signals from the 10°C and the 60°C blackbodies, the internal sensor radiance can be determined as described above. The sensor temperature is determined to 32°C and represented by the red curve. Since the sensor is temperature stabilized at this temperature, this internal radiation will always be present in the measurements. The difference between the result above using absolute values and the complex-valued treatment is <0.5 per cent. Also, the phase variation in S 2 was measured using Eq. (7) of Ref. 14. The phase varied between −0.15 and 0.07 rad. Also differences in spectral results are negligible.
The noise statistics will be slightly different. The variance is almost equal for both cases while the bias obtained when using absolute values is absent when using the complex-valued method.
The temporal NESR measurement shown in Fig. 9 was obtained at two different measurements with spectral resolutions, 27 cm −1 at 240 samples and 54 cm −1 at 120 samples and Fig. 8 Taking the internal radiation into account, the corresponding object radiance can be calculated. The measured radiance from the blackbody with the nominal temperature 10°C is shown. The theoretical radiance curve is shown in red for the temperature 8.3°C. Fig. 7 The detector responsivity can be determined in the same way as the internal radiation. The relative response is shown as a function of wavelength to make comparison with published sensor data easier. measured sensor noise properties. The result scales well with the assumption that responsivity can be modelled as RðσÞ δσ. Under these conditions, the responsivity at the larger bandwidth is a factor ffiffi ffi 2 p larger than the smaller bandwidth. This does, however, not mean that the larger bandwidth contains more information. The advantage in using a larger spectral bandwidth applies only for targets with spectral features broad enough to be resolved. The expected spectral features of the object must be considered when selecting appropriate spectral resolution to achieve an optimal number of uncorrelated spectral bands.
According to Eq. (17), the SNR can be obtained from the NESR results with respect to the temperature of the scene. An example is given in Fig. 10 for a scene under consideration. This example is for the case of scanning the corner cube.
Since the sensor is far from BLIP, it is assumed that the back-injected internal radiation does not contribute to the observed noise in any considerable way.
These kinds of sensors are most frequently used as scene scanning instrument where the spatial part of the interferogram is interrogated. As seen in Fig. 11, the noise level is then increased by more than a factor of 2 due to limited capability in NUC. This limitation is difficult to compensate for by oversampling since the nonuniformities require frequent renewing of the NUC calibration that interrupts the recording of the scene data. In any event, accurate NUC procedures are needed to obtain satisfactory results.
Although the larger bandwidth has a higher SNR that does not necessarily mean that it contains more information. This depends on the spectral variation in the scene. An indication of these conditions is given in the example below. The scene temperature is estimated to 19°C. Figure 12 is obtained at a bandwidth of 54 cm −1 and Fig. 13 is obtained at a bandwidth of 27 cm −1 . It can be observed that the performance is remarkably similar in the two cases although the SNR is higher in Fig. 12 compared to Fig. 13. The three-color components are obtained by selecting specific components from a PCA. The components are for both Figs. 12 and 13 as follows: blue channel:PC1; green channel: PC3; and red channel: PC6. The results depend on the type of signal processing selected; a more detailed analysis of those issues is beyond the scope of this paper.
An average scene spectral signal is adopted and all objects in the scene are treated as a deviation from this spectral signal. This simplifies the detection algorithm when only relative changes are being considered. In Fig. 14, a comparison is shown between the average scene spectral signal and a set of spectral values of the target shown in yellow in Figs. 12 and 13. The broader spectral band signal (green in Fig. 14) has been scaled by a ffiffi ffi 2 p to obtain the same signal levels as for the narrower spectral band (red in Fig. 14). As can be observed, there are some spectral variations that distinguish the target from average scene signal although the noise level is substantial at this SNR. The SNR obtained in these measurements are therefore considered to be a minimum for useful results.
The scene in Fig. 15 was obtained in the summer at sunset with the targets in shadow. The distance to the targets is about 20 m and the camera is placed 12 m above ground. The small round disc to the left consists of crumpled aluminum foil (high reflectivity material), the red plate is made of granite (silicate rich material), and the green plate is made of limestone (carbonate rich   ) are signal distribution of the yellow target in Fig. 12 and red datapoints are signal distribution of the same target in Fig. 13.  material). The blue background is a grass field with low reflectivity. As in the previous example, an average spectral signal of the scene is calculated and all objects in the scene are treated as a deviation from this spectral signal. The principal components shown in Fig. 15 are: blue channel: PC1; green channel: PC7; and red channel: PC5.
In Fig. 16, the emissivity is derived by comparing the target radiance with a blackbody radiance at the estimated scene temperature 20°C. The green targets show a dip in emissivity at 11.2 μm, typical for limestone while the red target shows an increase in emissivity with wavelength, typical for silicate-rich material.

Discussion and Conclusion
A theoretical model and experimental results are reported for the imaging spectrometer described. The interferometric system design was presented in Ref. 2 and is here modified using an uncooled imaging sensor with low NETD. The camera uses a standard lens, which is why vignetting is not avoided but is compensated for using blackbody sources in flat-field correction.  Vignetting can be avoided using lenses with the pupil positioned at the entrance of the corner cubes. 16 The effect of NUC instability is different for the data obtained by scanning the scene compared to data obtained by scanning one of the corner cubes. Scanning the corner cube results in a higher SNR, provided the scene and the sensor platform are static. If the sensor is placed on an airborne vehicle, limitations in pointing accuracy will likely degrade the performance. For a scene scanning system, internal radiometric calibration and frequent NUC might be required. Fig. 17 Boundary for the number of samples at a given bandwidth as defined above. Scene temperature is 19°C. The blue curve is for scanning the corner cube and the red curve is for a scene scan. The importance of accurate nonuniformity corrections is obvious. Fig. 18 Number of samples as a function of bandwidth at different scene temperatures. Blue curve is at 10°C, green curve at 20°C, and red curve at 30°C. The curves are representative for the corner cube scanning system. Besides FPA nonuniformities, limitations can be introduced by registration errors from processing the interferometric image sequence in a scene scanning recording. Registration can be supported by supplementary measurements with an inertial measurement unit (IMU), external cameras monitoring the scene or the interferometric images themselves. The impact of registration errors depends on the local variation in spectral radiance.
The required spectral resolution depends on the application. For sensing of pollutant clouds, the spectral resolution must be higher than demonstrated in the present experiments 17 except for gases with broad band signatures such as Freon.
The signal noise is assumed to be dominated by the sensor noise. Besides the sensor noise, the SNR will be determined by the bandwidth and the number of samples. The bandwidth is governed by the scanning range. When scanning the corner cube, the present sensor performance is shown in the blue curve of Fig. 17 where ffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi 2N þ 1 p δσ ¼ 600. For scene scanning, the corresponding limit is ffiffiffiffiffiffiffiffiffiffiffiffiffiffi ffi 2N þ 1 p δσ ¼ 1400. This applies to a scene at 19°C. The number of samples is equal to 2N þ 1. In Fig. 17, it can be observed that for high spectral resolution, many samples are required. When separating different types of materials with rather narrow spectral features, the scene must be static and stable over a longer time to allow for these sampling requirements. The relation to the scene temperature is shown in Fig. 18.
From these results, it can be concluded that the technology considered here is useful for static scenes at reasonably high temperatures when a modest spectral resolution is sufficient. The frame rate of the sensor is often fixed, so the number of samples translates into a recording time. This will often be the practical limitation of an application under consideration.