Flood Mode Tests:
In flood-mode tests the RTB 3000 illuminates the detector with unfocused blackbody energy from either the extended area source or the high temperature cavity source. Flood-mode tests include responsivity, noise, uniformity, detectivity, and linearity. Source location is precisely established using the RTB 3000’s graduated optical rail and quick-change kinematic mounts, for accurate control of irradiance.

Responsivity
Responsivity is the change in electrical output per unit of radiometric input. To measure responsivity, an extended area blackbody is placed immediately in front of the detector array, or a high temperature cavity blackbody with the required aperture size is placed at a required distance from the detector. Responsivity is a critical measured value, as it is used to calculate D*, NEDT, NEI, and quantum efficiency. The flexible design of the RTB 3000 allows the test engineer to select the responsivity test configuration that best fits the preferred test philosophy.

Noise
The noise measurement test is another flood-mode test. The extended area blackbody source, set at or near ambient temperature, floods the detector. With a fixed input, the noise is the root-mean-square deviation of the electrical output over time. Noise is another critical measured value used to calculate D*, NEDT, and NEI. The state-of-the-art SBIR blackbody sources incorporated into the RTB 3000 allow stable and accurate noise measurements to be performed.

flood mode 1

Uniformity
Uniformity is a measure of pixel-to-pixel variation in output of a focal plane array while it is flooded with constant, uniform irradiance. The extended area blackbody is positioned to fill the detector field of view, providing uniform infrared stimulus to the array. Data for each element of the array is collected, and standard deviation or other statistics are calculated.

Detectivity
Detectivity (D*) is a useful calculated figure of merit for comparing one detector to another. D* is the responsivity times the square root of the detector area divided by the noise spectral density. D* calculation is a standard feature of the RTB’s optional software packages. The D* figure is commonly reported with reference to a specific blackbody temperature. The RTB 3000’s blackbody sources supply all standard temperatures typically used for D* measurements.

flood mode 2

Uniformity
Uniformity is a measure of pixel-to-pixel variation in output of a focal plane array while it is flooded with constant, uniform irradiance. The extended area blackbody is positioned to fill the detector field of view, providing uniform infrared stimulus to the array. Data for each element of the array is collected, and standard deviation or other statistics are calculated.

Detectivity
Detectivity (D*) is a useful calculated figure of merit for comparing one detector to another. D* is the responsivity times the square root of the detector area divided by the noise spectral density. D* calculation is a standard feature of the RTB’s optional software packages. The D* figure is commonly reported with reference to a specific blackbody temperature. The RTB 3000’s blackbody sources supply all standard temperatures typically used for D* measurements.

flood mode 3

The RTB 3000 provides a new approach to testing linearity that avoids the limitations of the traditional approach. Rather than measuring the absolute value of the output voltage of the detector throughout its range, the slope of the V(Q) curve is measured at selected points. To do this, the detector is illuminated simultaneously by both the extended area source and by the modulated high temperature source. Varying the temperature of the extended area source allows the nominal irradiance to be set. The modulated high temperature source provides a precisely repeatable variation around this nominal value. The a.c. component of the detector output will be proportional to the detector responsivity. The slope of V(Q) is proportional to the resulting a.c. component of the detector output. Using this method, deviation from linearity can be determined with extremely high accuracy.

Collimated Mode Tests:

The tests describe previously are done on detectors or systems that do not form an image. The capability of the RTB 3000 is easily extended to allow testing of imaging systems: a collimating mirror is added, illuminating the imaging system with collimated energy from the differential blackbody source and target wheel or the cavity source and aperture wheel. This allows routine measurement of MTF, SiTF, NETD, and MRTD at the system level, and eliminates the need for a separate IR target projector system.

AUTO MRTD (Minimum Resolvable Temperature Difference)

AutoMRTD is calculated from the NETD and MTF multiplied by a response function, K(f):

    AutoMRTD = K(f) x [NETD/MTF]

    Where K(F) = ManMRTD/[NETD/MTF]

The K(f) values are determined from a statistical sample of ManMRTD measurements. The range of ManMRTD measurements taken depends on the specifics of the system under test. Ideally, several different trained operators take measurements several times a day for several days. The average of these measurements are used to calculate the K(f)’s. Since these values are derived from previous tests, no additional targets are needed.

SiTF (Signal Transfer Function)

SiTF is the slope of the output voltage vs. differential temperature curve. To measure SiTF, the UUT views the Half-Moon Target. The mean values are calculated from the ambient area and from the signal area. The voltage difference corresponding to the temperature difference is obtained. The differential temperature is then changed to obtain another data point. When a set of points (typically six) is obtained, the slope of a line tangent to the curve is computed. This slope is the SiTF. The SiTF is used in the NETD calculation.

MTF (Modulation Transfer Function)

MTF is calculated from an edge input, using the Half-Moon Target. The edge trace is differentiated to obtain the line-spread function, and a Fast Fourier Transform (FFT) is performed to obtain the frequency values.

This frequency output is normalized to get the 0 to 100% modulation values. The software will display a graph of modulation versus spatial frequency. MTF data is also used in the Auto MRT Module.

NETD (Noise Equivalent Temperature Difference)

NETD is found by measuring the zero-signal noise from a Square Target or an open aperture, and dividing by the SiTF. The NETD is used in the Auto MRTD calculation.

Standard System – The base system of the RTB 3000 IR Detector Test Bench is capable of performing all of the common focused and flood-mode tests necessary to characterize IR detectors, linear arrays, and focal plane arrays.

COMPONENT FEATURES
Optical Bench Assembly 30″ x 60″, Quick-change kinematic mounts, fold mirrors, graduated optical rails.
High Temperature Blackbody 50 – 1000ºC, 1″ aperture; microprocessor control; IEEE-488 Interface.
Chopper / Modulator 1 – 1000 Hz standard; stop-open, stop-closed; IEEE-488 Interface.
Shutter 2 position, IEEE-488 Interface.
Filter Wheel 5 position, 1″ aperture; IEEE-488 Interface. Aperture sizes of .050″, .100″, .200″,
.400″, and .600″ are standard. Other sizes are available.
Extended Area Blackbody 4″ square aperture, 0ºC to 100ºC (-25ºC to +75ºC ΔT) standard;
microprocessor control; IEEE-488 Interface.
Sliver Mirror Flat micro mirror on movable stage assembly.
X-Y-Z Lens Stage 1 inch travel, 3 axis; microprocessor control; IEEE-488 Interface;
lens mount for standard focusing lens.
Focusing Lens 100mm efl, f/3, 3-5 micron. And /or 100mm efl, f/2, 8-12 micron lens.
Optional Components –
By incorporating optional components, the RTB can be expanded to support system level testing.
Target Wheel 2″ aperture, 12 position; IEEE-488 Interface. Standard FLIR test targets available.
Collimator 6″ diameter, 30″ efl off-axis parabolic primary mirror; plano fold mirror.
6″ Extended Area Blackbody The standard 4″ extended area blackbody can be replaced with a
6″ square aperture blackbody to support large aperture flood-mode testing.