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672 spectrum amplifier

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672 spectrum amplifier

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Brief description:High-performance energy spectroscopy for all types of radiation detectors (Ge, Si, scintillation

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Detailed introduction

ORTEC 672 Spectroscopy Amplifier
  • High-performance energy spectroscopy for all types of radiation detectors (Ge, Si, scintillation; proportional counters)
  • Automatic pole-zero adjustment* easily sets up for any radiation detector
  • Optional triangle and Gaussian filters double the time constant of resolution
  • Automatic noise discriminators on the stack rejector and baseline restorer eliminate all screwdriver adjustments
  • Automatic baseline recovery rate for performance at low and high count rates
  • Differential inputs reduce ground loop noise
  • Preamplifier automatic compensation reset recovery via transistor reset

The ORTEC Model 672 high-performance energy spectrum amplifier is ideally suited for use with germanium, Si (Li) and silicon charged particle radiation detectors. It can also be used with scintillation radiation detectors and proportional counters.
  • information +

    • Download link 672 Brochure
    • Download link 672 Brochure (A4)
    • Download link 672 Manual
  • More information +


    The Type 672 input accepts a positive or negative signal from the radiation detector preamplifier and provides a positive 0 to 10 V output signal suitable for single or multi-channel pulse height analyzers. Its gain varies continuously between 2.5 and 1500.

    Automation of all key adjustments makes the Model 672 easy to set up for any radiation detector, enabling optimal performance even if the operator has no expertise.

    An automatic pole-zero adjustment feature significantly simplifies amplifier tuning, compensating for the decay time of the preamplifier pulses. This minimizes operator skill requirements and effort to achieve good energy resolution and peak position stability at moderate to high count rates. After changing the time constant or replacing detectors, simply press the AUTO PZ button and wait a few seconds for the AUTO PZ BUSY LED to turn off for precise pole zero (PZ) adjustment. This procedure does not require an oscilloscope. AUTO PZ memory is protected against power failure.

    In cases where, for example, the preamplifier pulse shape starts to deform from the normal exponential decay, then PZ cancellation is not possible. In this case, using manual PZ adjustment mode can sometimes slightly improve high count rate performance, resulting in a compromise solution.

    A front panel switch on the Model 672 selects triangular or Gaussian pulse shape for the UNIPOLAR (unipolar) output connector. The noise performance of the triangular pulse shape is equivalent to the Gaussian pulse shape with a 17% longer shaping time constant. In applications where the series noise component is dominant (short shaping time constant) and a stacking rejector is used, the triangular shape usually has the same dead time and slightly lower noise than the Gaussian pulse shape. Front panel switch selectable shaping time constant for each detector and application. Six time constants range from 0.5 to 10 μs, and the TRIANGULAR/GAUSSIAN switch combination provides 12 different shaping times. Bipolar outputs are also provided for measurements requiring zero-crossing timing.

    To minimize spectral distortion at medium and high count rates, the unipolar output uses a high-performance, gated, baseline restorer with multiple automation levels. An automatic positive and negative noise discriminator ensures that the baseline restorer operates only on the true baseline between pulses and is not affected by noise level changes. It does not require the operator to adjust the baseline restorer when gain, shaping time constant, or detector characteristics change. Negative overload recovery from reset pulses generated by transistor reset preamplifiers and pulsed optical feedback preamplifiers is also handled automatically. The monitoring circuit will shut down the baseline restorer and provide a reject signal to the multi-channel analyzer until the baseline has safely recovered from the overload.

    Several operating modes can be selected for the baseline restorer. To make PZ adjustment manually or automatically, select the PZ position. This location may also be used in applications requiring the slowest baseline recovery rate. For situations where low-frequency noise interference is a problem, high rates can be selected. On detectors where PZ cancellation is not possible, the automatic baseline restorer rate provides performance at low and high count rates.

    An efficient stacking rejector is integrated into the Type 672 Spectral Amplifier. It provides output logic pulses to associated multi-channel analyzers to suppress spectral distortion caused by pulses stacking on top of each other at high count rates (Figure 3). The fast amplifier in the stack rejector includes a gated baseline restorer with automatic noise discriminator. A multi-colored stack-up indicator LED on the front panel indicates the amplifier's processing efficiency. At low count rates, the LED flashes green. The LED will turn yellow at moderate count rates and red when pulse stacking loss >70%.

    If long connecting cables are used between the detector preamplifier output and the amplifier input, cable noise caused by the environment may have an impact. The Type 672 offers two solutions. For low to moderate interference frequencies, the differential input mode can be used with paired cables from the preamplifier to suppress noise. At high frequencies, a common-mode suppression transformer built into the Type 672 input reduces noise pickup. Transformers effectively eliminate interference from display raster generators in personal computers.

    All toggle switches on the front panel can be locked to prevent accidental changes to desired settings.

  • Specifications +


    Performance

    NOTE: Unless otherwise stated, performance specifications are for use on unipolar outputs2 μsGaussian shaping, manualPZmode andAUTO BLRmode for measurement.

    gain range

    from2.5Arrive1500Continuously adjustable. The gain isCOARSE(coarse) andFINE GAIN(trimming gain).

    Unipolar pulse
    shape

    The available switches areUNIPOLARThe (unipolar) output selects an approximately triangular pulse shape or an approximately Gaussian pulse shape.

    bipolar output
    pulse shape

    Bipolar output pulses from0.1% rise time to amplitude is of selected shaping time1.65times. The zero-crossing time of the bipolar output pulse is delayed by the selected shaping time from the amplitude of the Gaussian unipolar output.0.33times.

    integral nonlinearity
    (unipolar output)

    from0Arrive+10 V <±0.025%。

    noise

    for gain> 100, the equivalent input noise<5.0 μV rms, in manualPZmode, gain> 1000time<4.5 μV rms, or inAUTO Pzmode, gain>100time<6.0 μV。

    temperature
    coefficient
    (0to50°C)

    • Unipolar output gain<±0.005%/°C, DC level<±7.5 μV/°C。
    • Bipolar output gain <±0.007%/°C, DC level<±30 μV/°C。

    swim

    in50:1Dynamic range, bipolar zero-crossing swim<±3 ns。

    Overload recovery

    Unipolar and bipolar outputs use gain in2.5within a non-overload pulse width fromX1000Overload returns to rated output2Within %.

    spectrum broadening†

    At count rates up to100,000count/seconds,FWHMwidening usually<8% while the count rate is up to200,000count/seconds, expand<15%. Under the following conditions, for60Coradioactive1.33-MeVGamma rays are measured: the efficiency is10% ofORTEC GAMMA-X PLUSDetector, unipolar output1.33-MeVThe amplitude of gamma rays is8.5V。

    spectral shift†

    At count rates up to100,000count/seconds, the peak displacement is usually<±0.018% while the count rate is up to200,000count/seconds<±0.05%. Under the conditions specified by the spectrum broadening, for1.33-MeVrays for measurement.

    Differential input

    Differential nonlinearity follows from-9 VArrive+9 V <±0.012%. Enter ±10 V(DC plus signal). common mode rejection ratio> 1000。

    Pulse accumulation rejector

    threshold Automatically set above the noise level on the fast amplifier signal. independent of slow amplifierBLRthreshold.
    • minimum detectable signal Limited by detector and preamplifier noise characteristics.
    • Pulse pair resolution Usually500 ns. Use under the following conditions60Co 1.33-MeVGamma ray measurement: Efficiency is10% germanium detector, unipolar output1.33-MeVThe amplitude of gamma rays is4V,50,000count/seconds.

    †If measurements are made with a detector that generates a large number of slow rise time pulses or with a detector of lower quality than specified, the results may not be reproducible.


    Controls and lights

    Fine-tune gain

    Front panel with locking dial,10Coil precision potentiometers are available0.5Arrive1.5Continuously variable direct gain coefficient.

    Coarse gain adjustment

    Front panel, eight-position switch optional5、10、20、100、200、500and1000gain coefficient.

    shaping time

    Six-position switch on front panel selects pulse shaping filter circuit0.5、1、2、3、6and10 μsplastic surgery time.

    UNIplastic surgery

    The two-position locking toggle switch on the front panel can beUNIPOLAR(Unipolar) output selection of Gaussian or triangular pulse shaping.

    Input

    Front panel, four-position switch optional+or-input polarity, and differential (DIFF) or standard (NORM) input mode. inNORMmode, only useNORMInput connector. inDIFFmode, the preamplifier signal cable is connected toNORMinput, while another cable whose center conductor is connected to the preamplifier ground via an impedance matching resistor is connected toDIFF REFinput terminal. The impedance matching resistor must match the output impedance of the preamplifier.

    BAL(Difference
    input gain balance)

    installed inside the modulePCon the board20Ring potentiometer can matchNORMandDIFF REFinput gain to achieveDIFFCommon mode noise rejection in mode.

    PZ Auto/Man
    switch

    Locking toggle switch optionalAUTO(auto) orMAN(Manual) pole-zero cancellation adjustment mode. Both modes allow the40 μsto ∞ with a preamplifier exponential decay time constantPZCancel.

    automaticPZbutton

    WhenPZThe switch is inAUTO PZposition, momentarily pressAUTO PZbutton to openBUSY LEDand startPZAutomatic adjustment of cancellation circuits. After the adjustment is completed,BUSY LEDwill go out. Once completed, this will remain until the button is pressed againPZAdjust. timesPZThe memory of adjustments is protected against unexpected power outages.

    ManualPZadjust

    on the front panel20The loop potentiometer can be adjusted with a screwdriverPZCancel. As long asPZThe switch is inMAN(Manual) position, the value adjusted by the screwdriver is effective. For transistor reset preamps or pulsed optical feedback preamps, manually adjust counterclockwisePZ。

    Limit button

    Plug in and front panelUNIPOLAR(Unipolar) diode limiter in series with output connector and test point. Observe within a more sensitive oscilloscope rangePZAdjusting the accuracy prevents overload distortion in the oscilloscope.

    BLRrate

    Front panel, three-position locking, toggle switch can be used to select the baseline recovery rate.PZThe fixed rate provided by the position, used to adjustPZCancel. Automatic position at low count rates withPZThe position's rate matches, but as the count rate increases, the recovery rate will also increase. The high-rate position is used to suppress low-frequency interference.

    PURaccept/rejectLED

    multicolorLEDIndicates the percentage of pulses that were rejected due to pulse pile-up. greenLEDexpress0-40%, yellow indicates40-70%, shown in red> 70%。


    Input

    Norm

    front panelBNCThe connector accepts preamplifier signals of either polarity with a rise time less than the selected shaping time and an exponential decay time constant of40 μsto ∞. For input switch settings, the coarse gain is5When the input impedance is1000Ω, coarse gain setting ≥10When the input impedance is465Ω. for+Enter the switch setting and the coarse gain is5When the input impedance is2000Ω, coarse gain ≥10When the input impedance is1460Ω. The inputs are DC coupled and protected to ±25 V。

    Linear

    Rear panel connector. withNORMThe input is the same.

    Diff Ref

    When operating in differential input mode, the front panelBNCConnector for the ground reference interface of the preamplifier. only inDIFFUsed in modeINPUTswitch to operate. for+ DIFFEnter the switch setting and the coarse gain is5When the input impedance is1000Ω, coarse gain setting ≥10When the input impedance is465Ω. For – DIFFEnter the switch setting and the coarse gain is5When the input impedance is2000Ω, coarse gain ≥10When the input impedance is1460Ω. Inputs are DC coupled; protected to ±25 V。

    prohibited

    rear panelBNCThe input connector accepts a reset signal from a transistor reset preamplifier or a pulsed optical feedback preamplifier. You can use the correctNIMStandard logic pulse orTTLlevel. Logic is selectable as active high or active low via PC board jumpers. Disabling the input will activate protection against distortion caused by preamplifier reset. This includes turning off the baseline restorer, monitoring the unipolar output for negative overload recovery, and generatingPUR(rejection) andBUSY(Busy) signal.PURandBUSY(Busy) logic pulse is used in the relevantADCOr prevent analysis and correction reset dead time in multi-channel analyzers.


    Output

    unipolar,
    UNI

    Front and rear panelsBNCThe connector provides positive, unipolar pulses with a linear output range of0to+10 V. Front panel output impedance<1Ω. Using PCB jumpers, optional<1Ω or93Rear panel output impedance in Ω. The output DC returns to0±5 mVAnd has short circuit protection function.

    bipolar,BI

    Front and rear panelsBNCThe connector provides bipolar pulses with predominantly positive lobes. The linear output range is0to±10 V. Front panel output impedance<1Ω. Using PCB jumpers, optional<1Ω or93Rear panel output impedance in Ω. The baseline between pulses has0±10 mVDC level. Short circuit protection.

    CRM

    The rate meter output has a rear panelBNCConnector is provided for each linear input pulse that exceeds the stackup detector threshold250 nswide+5 Vlogic signal. The output impedance is50Ω。

    busy

    rear panelBNCThe connector remains active for the duration that the linear signal exceeds the positive or negative baseline restorer threshold or stacking detector threshold or duringINHIBITThe input signal is provided for the duration of the+5 Vlogic pulse. This applies to relatedADCor dead time correction for multi-channel analyzers. RightNIMStandard logic pulses are selectable as active high or active low via printed circuit board jumpers. The output impedance is50Ω。

    PUR

    The stack rejection output is a rear panelBNCconnector. When pulse build-up is detected, it will provide+5 V NIMStandard logic pulse. A pulse reset preamplifier's output exists during reset and resets overload recovery. The output pulses are selectable as active high or active low via printed circuit board jumpers. The output impedance is50Ω. related toADCor used in conjunction with a multi-channel analyzer to prevent analysis of distorted pulses.

    preamplifier

    rear panel standardORTECconnector(Amphenol 17-10090) to power the associated preamplifier. with all standardsORTECPower cord compatible on preamplifier.


    electrical and mechanical

    required
    power supply

    672Model consists of ±24 Vand±12 VofNIMpower box (e.g.ORTEC 4001A/4002Atype power box/power supply). The required power supply is+24 V,90 mA;-24 V,170 mA;+12 V,330 mAand-12 V,

    190 mA。

    weight

    Net weight 2.3Kilogram (5.0pounds). Shipping weight 3.6Kilogram (8.0pounds).

    Size

    NIMStandard double wide module,6.90 x 22.13cm (2.70 x 8.714inches) front panel, conforming toDOE/ER-0457Trequirements.










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    Model

    Description

    672

    spectrum amplifier

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