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Gain stability and the LYSO beam radiation monitor measurements

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Presentation on theme: "Gain stability and the LYSO beam radiation monitor measurements"— Presentation transcript:

1 Gain stability and the LYSO beam radiation monitor measurements
UiB G. Eigen, E. van der Kraaij, A. Marinov, J. Zalieckas, Z. Zhou A.Marinov

2 Gain Stability Sudies Analyzing the data taken by E. van der Kraaij in the period of Feb. 2014 Gain stability of KETEK SiPMs as function of Temperature. The noise effect at High temperatures. Gain is defined as Distance between 1 pe and 2 pe peaks A.Marinov

3 Problems with the Data Quality at high Temperatures
A.Marinov

4 Gain vs Temp 30… 35 40 35 45 Analyses made by Jiri Kvasnicka 45
A.Marinov

5 Gain Stability Studies
Runs taken with the Adaptive power supply Runs taken with keithley power supply Analyses where made with tools done by Eric van der Kraaij A.Marinov

6 Conclusions At high temperatures the data set are affected by the noise Possible reason can be, an oscillation of the amplifier observed by Ivo Polak. A.Marinov

7 Beam Radiation Monitor
Our task is to build a beam radiation monitor for KLOE at the DaFne experiment in Frascati Detector consists of an array of 8 LYSO crystals arranged in a ring around the beam pipe to record beam radiation photons in 100 keV energy range Each crystal (dimension: 0.5 x 0.5 x 4 cm3) is wrapped in ESR film and is read out with a KETEK SiPM having an active area of 3 x 3 mm2 with x 20 mm2 pixels (SiPM is not on the market) We have tested all 8 crystals and 8 novel KETEK SiPMS using 133Ba, 57Co, 22Na, 137Cs and 60Co sources Attach crystals to SiPMs with optical grease (use glue later) Amplify signal with charge-sensitive preamp AD8000 (gain: 8.5) Record Signal with 14-bit Caen ADC read out with Labview Design of the mechanical support structure requires a visit to Frascati to inspect beam area, as many cables are tied to the beam pipe 30th of June A.Marinov

8 LYSO crystal wrapping Mirror wrapped in 3 layers of ESR film
Optimal energy resolution is achieved when we use 3 layers of ESR film as reflector across the surface of the crystal. Results are shown on next slides Reflector frame A.Marinov

9 Test Setup at Bergen University
LYSO crystal Alu Enclosure Picture of the setup source LYSO crystal 5x5x40 mm fADC KETEK SiPM V1729A A.Marinov

10 Improving the Noise/Signal ratio
The output signal from the AD8000 using a Ketek MP204va W8 SiPM. Pulse amplitude is 256mV, Pulse length ~ 200ns, Noise level practically is 0 Pedestal Important step before the data taking Noise reduced when we use double shielding of the AD8000 amplifier and SiPM. Using a start point grounding avoid ground loops A.Marinov

11 Spectrum Na22 511keV 1275keV A.Marinov

12 Spectrum Na22 511keV sE/E=7.3% A.Marinov

13 Spectrum Ba133 81keV 356keV A.Marinov

14 Spectrum Cs137 661keV A.Marinov

15 Energy scale is linear at least up to 1.33 MeV
Co60 – 1332keV Na keV Co60 – 1173keV Measured energies of the follow sources Co57 Co60 Ba133 Na22 Cs137 Cs137 – 661keV Na22 – 511keV Ba133 – 356keV Co keV Ba133 – 80keV A.Marinov

16 The present Readout electronics
Vb 2x AD800 - Ouput + Low noise Good Dynamic Stable work 450ns Integration time A.Marinov

17 Summary All 8 crystals are performing very well and they are ready for the DaFne application Faster amplifier is under development by Ivo Polak Mechanical boxing and support are still under discussions A.Marinov

18 Beam Radiation Monitor Time Line
We have optimized the light collection and tested all SiPMs and 8 crystals  all perform well Apply final wrapping to 8 LYSO crystals and glue them to a SiPM  test performance including time resolution Design mechanical support structure after visit to Frascati. After completion of mechanical support structure at UiB, we install detector at DaFne and test it with beam- fall 2014 Write report and publication – End of 2014 A.Marinov

19 Thank you A.Marinov


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