High Resolution
|
Detectors (litres) | Crystals | |
---|---|---|
Helicopter | up to 33.6 downward | 4 - 8 |
up to 8.4 upward | 1 or 2 | |
Fixed wing | up to 50.4 downward | 8 - 12 |
up to 8.4 of upward | 1 or 2 |
High resolution aeromagnetic data can be gathered simultaneously with either system. In the fixed wing aircraft, the cesium magnetometer sensor is mounted in a stinger on the tail of the aircraft with the capability to include sensors in a horizontal and/or vertical gradiometer configuration. The helicopter has either a stinger or a towed bird with cesium magnetometer sensors, singly or in a gradiometer configuration.
SGL has implemented a spectral component analysis noise reduction processing technique, based on the method of Hovgaard and Grasty (of Radiation Solutions and Gamma-Bob respectively). The noise reduction technique, called Noise Adjusted Singular Value Decomposition (NASVD), uses the full spectrum data to enhance the resolution of radiometric data. The reduction in statistical noise is equivalent to increasing the detector volume by a factor of between three and four. SGL also uses a combination of spectrum fitting and NASVD to produce maps of cesium, and other man-made nuclides, from the 256 channel radiometric data.
SGL uses SGSpec and Radiation Solutions Inc. (RSI) spectrometers, which are recognized as the most advanced airborne spectrometer systems available. They include an onboard computer which allows real-time signal processing analysis previously available only in laboratory instruments. The combination of automatic gain control for individual crystals, multi-channel analysis, and full spectrum recording removes many of the limitations inherent in the older airborne systems.
SGSpec and RS-500 use spectrum analysis techniques to control the gain of the system. The system constantly monitors the natural thorium or potassium peak of each crystal detector, and using a Gaussian least squares algorithm, adjusts the gain of each crystal individually. In addition, each crystal resolution is calculated in real-time and the operator is informed if the crystal is out of specification.
SGSpec and RS-500 are designedto provide high quality signal processing with a minimum of operator intervention. This enables the spectrometer to be operated in a variety of conditions and minimizes operator error.
Crystal Detector Controller | ||||
---|---|---|---|---|
Real-time spectrum analysis for each
individual crystal ensures optimum stabilization and
resolution. This is achieved by the use of a
sophisticated Gaussian curve fitting algorithm for
centroid analysis of the natural thorium or
potassium peak.
Each crystal has individual pole-zero cancellation, semi-Gaussian shaping and an advanced baseline restorer. Real-time graphical display for system and spectrum monitoring. Accurate pile-up rejection for simultaneous pulses allows quantitative gamma-ray spectrum analysis almost independent of system count rate. Special circuitry analyses for pulse pile-up and permits only detector signals from single events to be analyzed. Residual pulse pile-up: pulses separated by more than the fast channel resolving time, and less than 1.05 x peak times are rejected. |
||||
Analog to Digital Converter - ADC | ||||
Individual A/D converters |
One per detector | |||
Number of channels |
1024 per detector | |||
ADC clock rate | RSI: 50 MHz SGSpec: 80 MHz |
|||
Linearity | Integral: less than 0.2% Differential: less than 1% |
|||
Average system dead-time |
No conversion time | |||
Live time channel | Actual system live time output with digital data allowing post correction of system dead-time to an accuracy of 0.1% | |||
Maximum number of counts/channel | 1,048,576 [20 bit] | |||
Thresholds | Lower: software selectable from
channel 2-50 in 1 channel steps Upper: 3 MeV, A/D offset is software selectable |
|||
Cosmic channel | All pulses above 3 MeV are summed and recorded in the cosmic channel as a direct measure of cosmic ray activity | |||
Maximum input count rate |
100,000 cps | |||
Digital Data Recorded | ||||
System resolution and detector resolution are automatically computed for each crystal and are recorded to provide accurate in-flight and post-flight quality assurance.) | ||||
Window mode | Eight user selectable windows typically corresponding to the total counts, potassium, uranium and thorium. The eight windows allow these 4 parameters to be recorded in both upward and downward detectors, plus one cosmic channel for pulses >3 MeV. | |||
Full spectrum mode |
Full 1024-channel spectrum with user selected end points. Individual detector and system resolution are recorded for both upward and downward crystals providing accurate post-flight data quality control. |