Presentation is loading. Please wait.

Presentation is loading. Please wait.

Performances of a pixel ionization chamber to monitor a voxel scan hadron beam A.Boriano 3, F.Bourhaleb 2,3, R. Cirio 3, M. Donetti 2,3, F. Marchetto 3,

Similar presentations


Presentation on theme: "Performances of a pixel ionization chamber to monitor a voxel scan hadron beam A.Boriano 3, F.Bourhaleb 2,3, R. Cirio 3, M. Donetti 2,3, F. Marchetto 3,"— Presentation transcript:

1 Performances of a pixel ionization chamber to monitor a voxel scan hadron beam A.Boriano 3, F.Bourhaleb 2,3, R. Cirio 3, M. Donetti 2,3, F. Marchetto 3, C. Peroni 3, C.J. Sanz Freire 1,3 1 Ion Beam Applications, Louvain la-Neuve, Belgium 2 TERA Foundation, Novara, Italy 3 University and INFN, Torino, Italy

2 PTCOG 2002 - Cataniasanz@to.infn.it outline outline Mechanical structure of the pixel ionisation chamber Mechanical structure of the pixel ionisation chamber Read-out: electronics and performances Read-out: electronics and performances Data Acquisition System Data Acquisition System Results from test with protons at PSI Results from test with protons at PSI Results from test with C +6 at GSI (2000) Results from test with C +6 at GSI (2000) Preliminary results from test with C +6 at GSI (2002) Preliminary results from test with C +6 at GSI (2002)

3 PTCOG 2002 - Cataniasanz@to.infn.it The pixel chamber parallel plate ionization chamber anode segmented in 1024 square pixels pixel dimension = 7.5 X 7.5 mm 2 sensitive area = 24 X 24 cm 2 1 mm water equivalent thickness front-end electronics, located around the chamber, to perform analog to digital conversion

4 PTCOG 2002 - Cataniasanz@to.infn.it Detector design The detector has to be thin to minimize the effects on the beam energy and shape Anode and cathode are glued to frames in order to assure the mechanical rigidity and the gap thickness Water equivalent thickness < 1 mm

5 PTCOG 2002 - Cataniasanz@to.infn.it Front-end electronics located around the chamber we have developed a full custom chip ( TERA05 ) every chip has 64 channels that convert the collected charge into counts

6 PTCOG 2002 - Cataniasanz@to.infn.it Linearity at 100 fC charge quantum 20 pA < I < 0.6  A Linearity better than 0.7 %

7 PTCOG 2002 - Cataniasanz@to.infn.it Linearity at 600 fC charge quantum 10 pA < I < 2  A Linearity better than 0.3 %

8 PTCOG 2002 - Cataniasanz@to.infn.it Reproducibility of charge quantum I = 49.96 nA Qc = 600 fC 24 ºC < T < 27 ºC 1 month 6 measures

9 PTCOG 2002 - Cataniasanz@to.infn.it Data acquisition Signals (RS422 standard) are delivered via twisted pair flat cables (100 m maximum length) max transfer rate = 10 MHz = 40 Mbyte/s read out transfer time = 50  s read out cycle total time = 100  s real time operating system <100 m

10 PTCOG 2002 - Cataniasanz@to.infn.it Beam test at PSI PSI test with a 138 MeV proton beam PSI test with a 138 MeV proton beam 7 mm FWHM beam 7 mm FWHM beam Spot-scanning Spot-scanning Uniformity of the response ~0.9% Uniformity of the response ~0.9% Profiles measurement ok Profiles measurement ok

11 PTCOG 2002 - Cataniasanz@to.infn.it Beam test at GSI Beam characteristics raster-scan delivery system C +6, beam dimension = 8.8 mm (FWHM) data acquisition synchronized with raster-scan Aims spatial resolution homogeneity of response

12 PTCOG 2002 - Cataniasanz@to.infn.it Spatial resolution Spatial resolution  < 0.2 mm

13 PTCOG 2002 - Cataniasanz@to.infn.it Homogeneity of the response 18 × 18 cm 2 uniform field  = 1.1 %  = 2.0 %

14 PTCOG 2002 - Cataniasanz@to.infn.it PMC FIFOFIFO CPU Pixel chamber PC OUT 16 bit Operative Systen VxWorks with Tornado II environment 1024 pixel 4 chip 4 chip 4 chip DAQ- test gsi 2002

15 PTCOG 2002 - Cataniasanz@to.infn.it 49 pixels map The map follows the beam... Daq with 49 pixels map

16 PTCOG 2002 - Cataniasanz@to.infn.it Beam intensity dependence 1 single voxel treated with several beam intensities Deviation from linearity is within 1%

17 PTCOG 2002 - Cataniasanz@to.infn.it Spatial resolution 14x14 cm 2 field ~2100 voxels DAQ: 7x7 map that follows the beam Spatial resolution  < 0.2 mm

18 PTCOG 2002 - Cataniasanz@to.infn.it

19 PTCOG 2002 - Cataniasanz@to.infn.it

20 PTCOG 2002 - Cataniasanz@to.infn.it Detector design Thick version When used in plastic phantom the detector can be thick. With photon or electron beam air gap has to be minimized. Anode and cathode are glued to a plastic slab, which is a grid of 1024 holes. Each hole can be considered as an independent sensitive volume.

21 PTCOG 2002 - Cataniasanz@to.infn.it TERA0 5 Very Large Scale Integration (VLSI) i  f conversion output  Q int 100 fC<charge quantum<800 fC I max = 4  A 64 channels 16 bit wide counters multiplexed digital output dead-time free readout max read out rate = 10 MHz channel # 1 channel # 64

22 PTCOG 2002 - Cataniasanz@to.infn.it Read out electronics Recycling Integrator architecture.

23 PTCOG 2002 - Cataniasanz@to.infn.it Spread of charge quanta RMS  1 % I = 49.96 nA 26 chips

24 PTCOG 2002 - Cataniasanz@to.infn.it Data acquisition connection by twisted pair flat cables (100 m max) max rate transfer = 1 MHz = 2 Mbyte/s read out transfer time = 1 ms PCI DAQ card LabVIEW software cheap solution easy to handle Slow data acquisition


Download ppt "Performances of a pixel ionization chamber to monitor a voxel scan hadron beam A.Boriano 3, F.Bourhaleb 2,3, R. Cirio 3, M. Donetti 2,3, F. Marchetto 3,"

Similar presentations


Ads by Google