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The XR-100T-CZT represents a breakthrough in x-ray detector technology by providing "off-the-shelf" performance previously available only from expensive cryogenically cooled systems.


Features

  • CZT Detector
  • Peltier Cooler
  • Cooled FET
  • Amptek A250 Preamp
  • Temperature Monitor
  • Beryllium Window
  • Hermetic Package (TO-8)

Applications

CZT Application Notes

[detector diagram]
Model XR-100T-CZT is a new high performance x-ray and gamma ray detector, preamplifier, and cooler system using a 3 x 3 x 2 mm Cadmium Zinc Telluride (CZT) detector mounted on a thermoelectric cooler. Also on the cooler are the input FET feedback components to the Amptek A250 charge sensitive preamp. The internal components are kept at approximately -30 ºC and can be monitored by a temperature sensitive integrated circuit. The hermetic TO-8 package of the detector has a light tight, vacuum tight 10 mil (250 µm) Beryllium window.

All the critical connections between the detector and the preamplifier have been made internally to the XR-100T-CZT to ensure quick, first time operation by the user. The XR-100T-CZT is provided complete with BNC connectors and power cable.

In order to facilitate the use of the detector, Model PX2T-CZT Power Supply and Shaping Amplifier was developed. The PX2T-CZT is AC powered and provides all four voltages needed to operate the XR-100T-CZT plus a shaping amplifier. The output from the PX2T-CZT can be connected directly to a Multichannel Analyzer (MCA)

The XR-100T-CZT is capable of detecting energies from a few keV to several hundreds of keV!

[Co57 Spectrum]

Theory of Operation

X-rays & gamma rays interact with CZT atoms to create an average of one electron/hole pair for every 5.0 eV of energy lost in the CZT. Depending on the energy of the incoming radiation, this energy loss is dominated by either the photoelectric effect or Compton scattering. The probability or efficiency of the detector to "stop" the incoming radiation and create electron/hole pairs increases with thethickness of CZT.

In order to facilitate the electron/hole collection process in the CZT detector, a 400 volt potential is applied. This voltage is too high for operation at room temperature, as it will cause excessive leakage, and eventually a breakdown. Since the detector in the XR-100T-CZT is cooled, the leakage current is reduced considerably, thus permitting the high bias voltage.

Electron/hole pairs created by radiation, which interact with the CZT near the back contact of the detector, result in fluctuations of charge collection times. These fluctuations are observed as rise time variations of the voltage step at the output of the charge sensitive preamplifier. As a result, the acquired spectra suffer from increased background counts and degrade energy resolution. To reduce these effects, a Rise Time Discrimination (RTD) circuit has been developed for the PX2T-CZT amplifier. When the RTD is active, the shaped pulses are internally gated and only pulses corresponding to "full charge collection" events are allowed to be sent to the Multichannel Analyzer (MCA) for analysis.

The thermoelectric cooler cools both the CZT detector and the input FET transistor to the A250 charge sensitive preamplifier. Cooling the FET reduces its leakage current and increases the transconductance, which in turn reduce the electronic noise of the system.

In order to further reduce electronic noise, the feedback capacitor and part of the current feedback network to the A250 preamp are also placed on the same substrate as the detector and FET. This minimizes parasitic capacitance at the input.

A temperature monitoring integrated circuit is placed on the cooled substrate to provide a direct reading of the temperature of the internal components, which will vary with room temperature. Once the internal temperature gets below minus 10 ºC the performance of the XR-100T-CZT will not change with a temperature variation of a few degrees. Hence, accurate temperature control is not necessary when using the XR-100T-CZT inside the laboratory.


[system block diagram]
Figure 1. XR-100T-CZT Connection Diagram

[amplifier output]
Figure 2. PX2T-CZT Amplifier Output


XR-100T-CZT Specifications

General
Detector typeCadmium Zinc Telluride; Cd0.9Zn0.1Te (CZT)
Detector size3 x 3 mm (9 mm2)
Detector thickness2 mm
Energy resolution @ 122 keV,  57Co1.5 keV FWHM, typical
Dark counts<5 x 10-3 counts/sec @ 10 keV < E < 1 MeV
Detector windowBe, 10 mil thick (250 m)
PreamplifierAmptek Model A250, with Current Divider Feedback
Case Size3.75 x 1.75 x 1.13 in (9.5 x 4.4 x 2.9 cm)
Case weight4.4 ounces (125 g)
Total powerLess than 1 watt

Inputs
Test input20 mV test pulse ~30 keV
Preamp power? volts @ 25 mA
Detector power+400 volts @ 1 A
Cooler power
 
Current = 0.7 A maximum
Voltage = 2.1 volts maximum

Outputs
Preamplifier:
Sensitivity
Polarity

0.73 mV/keV
Negative signal out (1 kohm max. load)
Temperature monitor:
Sensitivity

1 A corresponds to 1 K

The output pulse produced by the PX2T-CZT Shaping Amplifier is optimum for most applications using cooled CZT detectors, and can be connected directly to the input of a Multichannel Analyzer (MCA). If different shaping time constants or gains are needed, an external NIM type shaping amplifier with base line restoration can be used.

XR-100-CZT Connections
Preamp outputBNC coaxial connector
Test inputBNC coaxial connector
Power6-Pin, LEMO connector with 5 ft cable
Pin 1: +8 volt temperature monitor power
Pin 2: +H.V. detector bias, +400 volt max.
Pin 3: -8 volt preamp power
Pin 4: +8 volt preamp power
Pin 5: Cooler power return
Pin 6: Cooler power (0 to +2.1 volt @ 0.7 A max.)
Case: Ground and shield

PX2T-CZT Specifications

General
Size6 x 6 x 3.5 inches (15.3 x 15.3 x 8.9 cm)
Weight2.5 lbs (1.15 kg)

Shaping amplifer
PolarityPositive unipolar
Shaping Time3 s
Pulse width7.2 s FWHM, see Figure 2
Shaping type7 pole "Triangular" with Base Line Restoration, Pileup Rejection, and Rise Time Discrimination (RTD)
Sensitivity with XR-100T-CZT6 to 60 mV/keV
Output range+6.0 volts into 500 ohm load
Output impedance50 ohms

PX2T-CZT Connections
Input from XR-100T-CZTFront panel BNC
Output to MCAFront panel BNC
Pileup Rejection (PU)Rear panel BNC, Positive TTL
For the duration of this output gate, any detected pulse must be rejected by the MCA.
Input Count Rate (ICR)Rear panel BNC, Positive TTL < 2s
When connected to a counter, the ICR countrate corresponds to the total number of x ray events that strike the detector.
Probe power9-pin D-connector (cable provided)
Pin 1: +8 volt preamp power
Pin 2: -8 volt preamp power
Pin 3: 0 to +3 volt cooler power @ 0.7 A max.
Pin 4: +8 volt temperature monitor power
Pin 5: +H.V. detector bias, +400 volt max.
Pin 6: Ground and case
Pin 7: Cooler power return
Pin 8: Ground and case
Pin 9: Ground and case
AC powerStandard IEC 320 receptacle, 110-250 VAC, 50/60 Hz (cable provided)


Options


CZT Detection Efficiency

For 2mm thick CZT and 10 mil (250 µm) Be window (window dominates low energy response).
[czt efficiency log]
Log-log plot of interaction probability between 1 keV and 1 MeV.

[czt efficiency linear]
Linear plot of interaction probability over the lower energy range.

For a more detailed explanation of the efficiency of CZT and the effects of Rise Time Discrimination see the Efficiency of XR-100T-CZT Detectors Application Note (ANCZT-1 Rev. 1)


Sample Spectra and Applications
Medical Applications
Uranium and Plutonium Detection
Art and Archaeology
X-Ray Fluorescence - A Description
XR-100T-CZT Photographs
XR-100T-CZT, PX2T-CZT, and MCA8000A Connection Diagram
Mechanical Dimensions
Vacuum Applications
Collimator Kit

CZT Application Notes

See also the XR-100CR at 186 eV resolution, and the new ROVER---a completely portable detector system.

XR-100T-CZT Specifications in PDF format


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Revised February 6, 2001