Paul Scherrer Institut Proton Irradiation Facility (PIF) at Laboratory For Astrophysics    

Paul Scherrer Institut
CH-5232 Villigen PSI
Phone +41 56 310 21 11
Fax +41 56 310 21 99


 

    
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  Experimental Site


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Updated:
23.03.2005
E-Mail: wojtek.hajdas@psi.ch


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High Energy Site

Experimental Site

The initial proton beam for PIF is delivered from the PROSCAN accelerator with 
the help of the primary energy degrader, which allows to set the initial beam energy
from 250 MeV down to 70 MeV. The beam is subsequently guided to the Experimental
Area where PIF facility is located. 
Having energy of the beam degraded directly after accelerator exit causes also
its intensity reduction on target. 
Additional safety reasons put the maximum beam intensity in the PIF area up to
2 nA for energies above 200 MeV, 5 nA for energies from 100 MeV to 200 MeV and
10 nA for energies below 100 MeV.   As PROSCAN accelerator serves also two GANTRY stations
and OPTIS2 facility for cancer treatment, most of PIF exposures are conducted
during weekends and nighshifts.

The PIF experimental set-up consists of the local PIF energy degrader, beam collimating 
and monitoring devices (Photo 1).

 

Photo 1. PIF-PROSCAN downstream view with ionization chamber, energy degrader and wire chamber.

Movable XY table with the sample holder (see Photo 2) enables easy mounting of the
user's device under test (DUT) on the beam. 

Photo 2. PIF-NA3 rear view of the XY-table with movable arm and sample holder.

The laser mounted downstream from the XY table allows to center the DUT and control 
its position (see Photo 3).


Photo 3. PIF-NA3 Side view with the laser for sample centering and beam dump. 
The door of the beam dump are closed during the test setup to protect people against 
radioactivity coming from the beam dump.

Irradiations are usually carried out in air. The maximum allowed energy is 254 MeV and the 
maximum current is limited to about 1 nA due to air activation in the experimental area.

According to experience and user requirements, the monitor detectors are selected for each
experiment individually: ionization chambers, Si-detectors, plastic scintillators. Schematic view
of the experimental set-up is shown in Figure below:

(Full size 72 kB)

Figure 1. PIF-NA3 Experimental site (not in scale). 

The irradiation is controlled through a set of scalers and a PC-based data acquisition system. 
The system monitors proton flux and dose rate, calculates the total deposited dose and 
controls the position of the sample as well as beam focus parameters. It also allows for 
setting the beam energy with the help of the PIF local energy degrader. This makes it
possible  to perform fully automated irradiations with arbitrary proton spectra.

 

Main Features

  • Initial proton energies: 254, 102 and 60 MeV

  • Energies available using the PIF degrader:
    quasi continuously from 35 (6) MeV up to 254 (60) MeV

  • Energy straggling for the 300 MeV initial beam beam:
    e.g. FWHM=7.2 MeV at 200.0 MeV, FWHM=15.4 MeV at 50.0 MeV.

  • The maximum beam intensity at 254 MeV: 1 nA

  • The maximum flux at 254 MeV with 10 mA split beam (focused beam):
    2.5*108 protons/sec/cm2

  • Beam profiles are either flat or Gaussian-form with minimum FWHM=6 cm

  • Irradiations take place in air

  • The maximum diameter of the irradiated area: f 9 cm

  • The accuracy of the flux/dose determination: 5%

  • Neutron background: less than 10-4 neutrons/proton/cm2

  • Irradiations, devices and sample positioning are supervised by the computer

  • Sample mounting frame 25 x 25 cm2 (SEU and HIF facilities compatible)
    is attached to the XY table

  • Data acquisition system allows automatic runs with user pre-defined
    irradiation criteria