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Document type: 

Title: 

Revision date: 

Revision: 

User's Manual (MUT) 

Mod. N968 Spectroscopy Amplifier 

14/06/2004 

 
 
 

NPO: 

Filename: 

Number of pages: 

Page: 

00100/03:N968x.MUTx/04 

N968_REV4.DOC 

14 

12 

 

3. Functional description 

3.1  Shaping determination 

 
The proper shaping time constant must be seen as the better compromise in order to 
match high count rates requirements (which lead to small time constant) and good signal-
to-noise ratios (which lead to big values). For scintillation counters the energy resolution 
depends largely on the detector (scintillator and photomultiplier), therefore a shaping time 
constant of about four times the decay time constant of the scintillator is a reasonable 
value. 
Gas proportional counters usually have a collection time in the 0.5 ÷ 5 µs range, so a ~2 µs 
time constant could provide a good resolution.  
Instead, for surface barrier semiconductors, a time constant in the 0.5 ÷ 2 µs range is 
recommended.  

3.2  Equipment facilities 

 
In order to provide the User with an equipment suitable for almost any spectroscopy 
application, the Mod. N968 includes: 
 

− 

a Pile-up Rejector/Live Time Corrector (PUR/LTC) circuitry which allows operation with 
minimal dependence on system count rate. The PUR circuit interrogates incoming 
pulses for pile up and generates a signal that prevents the ADC from converting the 
piled up events. The LTC circuit then generates a system dead time that extends the 
collection time to compensate for the events lost due to pileup rejection. The result is 
lower background, better resolution and accurate live time information for the best 
possible analysis results. 

 

− 

a gated Baseline Restorer (BLR), which includes a discriminator that operates the 
sensing circuits that normally establish the baseline reference of the Multichannel 
Analyzer (MCA). Performance of the spectrometer depends on the precision of the 
setting of the BLR threshold. Such automatic threshold control typically gives as good 
or better results than those the most experienced operator could achieve manually. 

 

 

− 

a Pole Zero (PZ) Visual Indicator: a LED adviser which leads to high precision 
adjustment of the pole-zero cancellation, for exact compensation of the decay time of 
the preamplifier signal. Two LEDs indicate either over-compensation or under-
compensation. 

 

− 

a Bipolar Output, which provides a zero-crossing pulse, suitable for precisely detecting 
the radiation arrival time. In fact, the zero-crossing of the pulse occurs with a constant 
delay with respect to the onset of the pulse, independently from the amplitude, thus 
allowing to reduce time-walk effects. 

 

− 

an Inhibit Output, which provides a pulse when pile-up occurs. This pulse shall be 
applied to the MCA’s anticoincidence input in order to prevent it from measuring and 
storing a non-valid amplitude. 

Содержание 968

Страница 1: ...Technical Information Manual MOD N968 14 June 2004 Revision n 4 SPECTROSCOPY AMPLIFIER MANUAL REV 4 NPO 00100 03 N968x MUTx 04...

Страница 2: ...he User accident or any abnormal conditions or operations CAEN declines all responsibility for damages or injuries caused by an improper use of the Modules due to negligence on behalf of the User It i...

Страница 3: ...PANEL DISPLAYS 9 2 7 INPUT OUTPUT CONNECTIONS 9 2 8 TECHNICAL SPECIFICATION TABLE 10 3 FUNCTIONAL DESCRIPTION 12 3 1 SHAPING DETERMINATION 12 3 2 EQUIPMENT FACILITIES 12 3 3 CIRCUIT DESCRIPTION 13 LIS...

Страница 4: ...t panel switch allows to select between positive and negative input signals Gain setting can be performed continuously in the 10 1500 range product of Coarse Fine and Superfine Gain Two internal jumpe...

Страница 5: ...mplifier 14 06 2004 4 NPO Filename Number of pages Page 00100 03 N968x MUTx 04 N968_REV4 DOC 14 5 2 Technical specifications 2 1 Packaging The Model N968 is housed in a single width NIM module 2 2 Pow...

Страница 6: ...OC 14 6 2 3 Front and back panel Fig 2 1 Mod N968 Front and back panel Mod N968 FINE GAIN 0 5 1 5 COARSE GAIN SFG SHAPING TIME POS NEG INPUT DELAY ON OFF DC UNI BI PREAMP OUT INPUT UNI BI CRM BUSY INH...

Страница 7: ...switch selects time constants for active pulse shaping filter network from 0 5 1 2 3 6 and 10 s PZ ADJ1 Screwdriver adjustable potentiometer to set the pole zero cancellation to compensate input decay...

Страница 8: ...or x0 1 PRS Polarity sw3 allows to configure the module in order to accept on the PRS input either positive or negative pulses If the preamplifier connected to the N968 does not feature the PRS set t...

Страница 9: ...0 V Front panel INPUT is provided with a test point RTP Rise Time Protection Rear panel BNC connector TTL signal 50 impedance it is provided by the Multichannel Analyzer MCA to communicate to the ampl...

Страница 10: ...Gaussian peaking time 2 4 Ts pulse width at 0 1 level equal to 2 9 times the peaking time Bipolar shape approximate derivative time to crossover 3 Ts Integral non linearity 0 025 2 s shaping time Tem...

Страница 11: ...N968x MUTx 04 N968_REV4 DOC 14 11 Fig 2 3 UNIpolar Output Equivalent RMS Noise Vs Shaping Time Ts Fig 2 4 BIpolar Output Equivalent RMS Noise Vs Shaping Time Ts UNIPOLAR OUT 0 1 2 3 4 5 6 7 8 9 0 2 4...

Страница 12: ...ents the ADC from converting the piled up events The LTC circuit then generates a system dead time that extends the collection time to compensate for the events lost due to pileup rejection The result...

Страница 13: ...ch forms the pulse semi gaussian profile The chain composed by both the amplifying and the shaping stages is configured as gated amplifier in order to compensate the amplifiers thermical drift and off...

Страница 14: ...sy output and to provide another CRM pulse In the meantime at the arrival of the second pulse a bistable set by the first pulse produces the Inhibit output The LTC function is also shown in Fig 3 2 af...

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