5c881ddec2b0678d9bf4f97fc19108a0.ppt
- Количество слайдов: 32
BTF @ LNF DAFNE Beam Test Facility (BTF). From single up to 1010 e-/e+, g and neutrons B. Buonomo, G. Mazzitelli, L. Quintieri, P. Valente, with the support of the DAFNE operators and accelerator division staff and all the users who help us developing diagnostic and improving the facility G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
The DAFNE BTF high current Linac: § 1 - 500 m. A e- 100 m. A e+, § 1 - 10 ns pulses, at least 107 particles The BTF is a e-/e+ test-beam facility in the Frascati DAFNE collider complex Need to attenuate the primary beam: § Single particle regime is ideal for detector testing purposes § Allows to tune the beam intensity § Allows to tune the beam energy G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
BTF layout control room 5. 5 m 4 m Hall LINAC tunnel momentum analyzer main ring G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009 BTF Hall
LINAC beam attenuation 0 1 e- 103 102 2 e- 3 e- detector 10 1 LINAC Beam 1 -500 m. A 0 100 300 500 tunable Cu target: 1. 7, 2. 0, 2. 3 X 0 450 magnet N. of particles W slits Selected energy (Me. V) G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
BTF beam characteristic Beam (e- or e+) intensity can be adjusted by means of the energy dispersion and collimators, down to single particle per pulses Number (particles/pulse) 1 105 1 1010 Energy (Me. V) 25 -500 25 750 Repetition rate (Hz) 20 -50 50 Pulse Duration (ns) 10 1 or 10 p resolution 1% Spot size (mm) Divergence (mmrad) sx, y ≈ 2 (single particle) up to 10*10 (high multiplicity) s’x, y ≈ 2 (single particle) up to 10 (high multiplicity) Multi-purpose facility: • H. E. detector calibration and setup • Low energy calorimetry & resolution • Low energy electromagnetic interaction studies • High multiplicity efficiency • Detectors aging and efficiency • Beam diagnostics G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
BTF Operation … The BTF was commissioned in 2002 and start operation with users since the beginning of 2003. Beam is delivered 24 h/day with an efficiency of 96% but when in parasitic mode together with DAFNE main operation the duty cycle is degraded ~ 45% due to continuous injection into the main ring. In 2004 a dedicated transfer line was build and in 2006 a fast pulsed power supply has been installed increasing the duty cycle up ~ 90%. 2006 -2007 DAFNE run users requests beam request in last 4 years (multi users are counted twice) 2007 - 224 days 2006 - 244 days 2005 - 364 days 2004 - 282 days G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009 DAFNE-L
Present RUN 193 days in 2008. A typical real access 80 -90% of allocated time G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Equipment: infrastructure • one meeting room (Wi. Fi) • one guest office (LAN-Wi. Fi) Control room: Pc’s, Controls console, printer cabling, crate and racks, etc 5. 5 m 4 m main entrance: radioprotection wall can be removed on demand Linac tunnel G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Equipment: infrastructure § permanent DAQ TDC/QDC/ADC/scaler/disc. available § NIM, VME, CAMAC Branch, VME controllers § ‘Devil’/VMIC VME and CAMAC controller, NIM modules § Remotely controlled trolley § Gas system § HV system… § crates, rack, etc. C 2 H 6 C 4 H 10 CO 2 Noble Gas § HV SY 2527 (3/4 KV neg, 3/4 KV pos, 15 KV pos) § 40 ch. CAEN SY 127 pos. § Cabling BTF HALL-BTF CR § Network: Wi-Fi, dedicated-LAN, WAN, printer http: //www. lnf. infn. it/acceleratori/btf/ G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Equipment: Diagnostics low multiplicity diagnostic (1 -100): • • (back detector) lead glass, 5× 5× 35 - 10× 35 cm Pb. WO 4 crystal 3*3*11 cm lead/scintillator fibers (KLOE type), 25× 50× 30 cm 2× 2 mm spot size in Na. I high resolution 30× 30 cm fiber hodoscope (front/trigger detector/not destructive/tracking) multipurpose plastic scintillators 10 x 0. 5 cm, 10 x 30 x 0. 5 cm, 1 x 15 x 0, 5 cm hodoscope; two bundle of 1 mm fiber for a total active area of 48 x 48 mm 2 Silicon tracker (high gain) 2× 2 mm spot size in Silicon XY chamber 3 GEM (Gas Electron Multiplier) detector G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Examples of experimental setup (P 326 Prototype inefficiency 200 Me. V) energy spectrum inefficiency VS threshold - no tagging - tagging loose G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009 - FC max - N/Ntot - FC min
Example of experimental setup (MEG) beam exit sci-fi profile detector (MEG test for sci time resolution) back detector (Na. I calorimeter) on line monitor e- spectra XY beam sci-profile G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
BTF photon tagged source AGILE GRID photon calibration The AGILE Gamma Ray Imaging Detector calibration at BTF is aimed at obtaining detailed data on all possible geometries and conditions. BTF can provide data in the most significant spectrometer energy region (20 -700 Me. V) silicon detector silicon tagging target Be window G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009 AGILE GRID
Equipment: Diagnostics (con’t) • medium multiplicity diagnostic (100 -108): (front detector/not destructive) • Cerenkov light emission • Silicon Beam Chamber (low and tunable gain) • Triple GEM TPC (under development) • high multiplicity diagnostic (107 -1010): (front detector) • low noise (3× 106 particles) BCM • high sensitivity fluorescence flags – cromox, Be, yag: ce G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Compact-Triple Projection GEM It’s essentially a small TPC with a 3 -4 cm drift Also high current beam can be monitored in position (TDC) and d. E/d. X (ADC) BTF beam box cross section ASDQ or Carioca GEM 16 samples for each readout The detector will be realized with standard 10 x 10 cm 2 GEMs inside a G 10 box; the readout will be realized with F. Murtas et all - ASDQ (first phase) at CERN for test beam - then Carioca Cards (second phase) at BTF Possible DE/Dx measurements (LVDS width proportional to signal charge) G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
RAP experiment @ BTF G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Background attenuation BOX: W=40 cm; H=50 cm, L=50 cm 2. 5 cm of DENSIMET-180: (95% W + 0. 5 % Fe-Ni) 2. 5 cm of 5% BORON Polyethylene tunable Cu target High current LINAC beam n attenuation g attenuation A tungsten box is going to be installed in order to shield the high divergent beam coming from the Cu degrader target – an attenuation of ~ 100 is expected by simulation (FLUKA) G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Idea for a neutron facility @ BTF • General interest of BTF scientific community for the neutron production at BTF • Possibility to test detector diagnostic at low neutron flux and low energy • Generation of the knowhow needed for next generation of high energy source (see FEL) • Possibility to have a new European facility in ISO standard G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Study of optimized target: lead TGT sphere R=12 X 0 Up to 100 Me. V the spectrum is described as a Maxwellian distribution with average around 1 Me. V Monte Carlo simulation ( by Fluka code) Approaching the higher energies the Quasi-Deuteron Effects adds a tail of highenergy neutrons to the Giant resonance spectrum. The slope becomes stepper as the incident electron energy is approached Fluka result: 1. 6826 10 -1 neutron/primary G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Experimental Set-up BTF Experimental Hall Target with multiple beam extraction lines (MC model) e- beam neutron exit at different angle Transfer Line study supported and founded by CNS 5 in Sep. 2008 to realize the target, beam dumper and trolley G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Application form to access BTF Pasquale Di Nezza - INFN, LNF Flavio Gatti - INFN, Genova Clara Matteuzzi (Chairperson) - INFN, Milano Giovanni Mazzitelli (Responsible) - INFN, LNF Antonio Passeri - INFN, Roma III Paolo Valente - INFN, Roma I Beam Test Facility Secretariat: Annette Donkerlo G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Access BTF @ LNF • btf@lnf. infn. it for scientific and technical question. • btfsupport@lnf. infn. it for administration support. Mailing list INFN scientific CN coordinators INFN group responsible BTF users G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
General information ht tp : //w ww . ln f. in fn. i t/a c ce ler ato ri/ bt f/ technical documentation for users and operators is available on the web as well as beam request, shift archive, schedule, documentation, virtual logbook, etc The BTF was widely used as a TARI facility in the EU 6 th Framework Program …and will be involved in the EU 7 th Framework Program G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Job 50% done by temporary employ at risk… Thanks for your attention, http: //www. lnf. infn. it/acceleratori/btf G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Spare G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Calorimetric counting number of produced electrons counted by total energy deposited in lead/scintillating fiber calorimeter (KLOE type): 50 Me. V limited to few tens of Me. V, due to energy resolution limited to few tens of particles, due to saturation effects calorimetric is OK at low intensity, not for high multiplicity beams: e. g. the AIRFLY experiment, designed to measure absolute fluorescence yield in air and its energy dependence, needs: § full energy range § maximum beam intensity G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Beam profile (AGILE Si tracker) 2 layers (x, y) 384 strips, analog readout 410 mm thick, single-side, AC coupled strips, 121 mm pitch, 242 mm readout pitch Optimal focusing at 493 Me. V, measured spot size: s 2 2 mm 2 Defocused Beam spot measured with all transfer line quadrupoles off: 55 35 mm 2, limited by vacuum pipe section G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Sci-fi profile detector § A permanent beam position and size monitor needed, both for beam steering and optimization purposes, and for providing useful information for detector testing, complementing the beam intensity monitors § Such a position sensitive detector should have: § negligible mass, not to spoil beam characteristics (energy, divergence, spot size) § good resolution, as compared to beam typical size (1 mm required) § sensitivity both for single particle (even at low energy) and at high beam intensity § 4 layers of fibers glued together cladded scintillating fibers, Pol. Hi. Tech type 0046, 1 mm diameter § staggered by ½ fiber to minimize dead zones G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Sci-fi profile detector energy dependence of the beam spot size H size (mm) § Charge weighted profiles for x and y fiber bundles y (mm) E (Me. V) x (mm) Consistent with beam image from Silicon tracker G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Cerenkov beam monitor detector, designed and built, in collaboration with the AIRFLY group, based on Cerenkov light emission § Cross-calibrated with calorimetric measurement at low particle multiplicity § Used to monitor beam intensity at higher intensity up 104 105 particles, in the full energy range filter dynamical range can be further extended: § calibrated optical filter in front of the PMT § use air as Cerenkov radiator detector tested up to 1010 particles with a cross calibration with BCM 45 o mirror Plexiglas radiator G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009 PMT
Calorimeter No optical filter Calorimeter Cerenkov/Calorimeter ratio : 10 optical filter (measured attenuation = 0. 096) Calorimeter/Cerenkov calibration Cerenkov beam monitor Calorimeter Cerenkov/Calorimeter ratio G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
Beam profile (FLAG fluorescence target) Very low current beam image on 1 Inc yag: ce Flag = metallic high fluorescence plate viewed by a camera Different fluorescence targets(Be, cromox, yag: ce) for very low current beam SIDHHARTA diagnostics G. Mazzitelli – CSN 1 La Sapienza -28 Jan. 2009
5c881ddec2b0678d9bf4f97fc19108a0.ppt