1 / 13

Stato del calorimetro elettromagnetico

Stato del calorimetro elettromagnetico. Nuove misure a TERAS (maggio) TEST beam al PSI (ottobre – novembre-dicembre) Lxe facility Criostato. TERAS g Beam Line. Compton Spectrum (E g -Ec/2) 2 +(Ec/2) 2. Electron beam Energy: 764MeV Energy spread: 0.48%(sigma)

Download Presentation

Stato del calorimetro elettromagnetico

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Stato del calorimetro elettromagnetico • Nuove misure a TERAS (maggio) • TEST beam al PSI (ottobre – novembre-dicembre) • Lxe facility • Criostato

  2. TERAS g Beam Line • Compton Spectrum • (Eg-Ec/2)2+(Ec/2)2 • Electron beam • Energy: 764MeV • Energy spread: 0.48%(sigma) • Divergence: <0.1mrad(sigma) • Beam size: 1.6mm(sigma) • Laser photon • Energy: 1.17e-6x4 eV (for 40MeV) • Energy spread: 2x10-5 (FWHM) • Divergence: unknown • Beam size: unknown Collimator size

  3. LP operato con Xenon purificato g Data MC simulation D D Short labs Previous Test D= • D: depth parameter D: 20~100  0~25cm D Long labs This Test D D

  4. Energy Spectrum Fitting • For understanding simply… • Suppose Response function is an asymmetric Gaussian • Principle… Compton Spectrum Response function Eg Npe s left Convolution of Compton Spectrum Response Function s right

  5. Energy Spectrum Fitting cont’d • Require D(depth parameter)>45 • ~34% of events in the range of 40MeV+/-4MeV are discarded by this requirement • Suppose Compton Spectrum around the edge (E-Ec/2)2+Ec2/4 • Detector Response Function • Gaussian with Exponential tail f(x) = Nexp{t/s2(t/2-(x-x0)}, x<x0+t Nexp{-1/2((x-x0)/s)2}, x>x0+t • Convolution • Integration +/- 5s • Fitting is done in two steps • Determine the edge position • Fix the edge in the 2nd fitting for determining the other prams Detection efficiency (estimated by MC) : 74% within +/- 4% energy cut at 52.8 MeV (cf. Progress Report Jul 02) (16% of events are lost due to interaction with material in front of the active volume) 26%

  6. Energy Resolution vs. Depth Parameter • For g incident at the detector center • D > 35, 45, 55….85 • Resolution: < 2% in sigma except shallow events (D<45). D Number of Photoelectrons

  7. LP al PSI (meta’ agosto): test in ottobre/novembre con fotoni monocromatici

  8. The elementary process  - (essentially) at rest captured on protons:  - p  0 n  - p  n  0   Photon spectrum 129 MeV 54.9 82.9

  9. -- beam C T A Mod Experimental configuration TARGET? • Rate • Background • Thin/small (angle/X0) • Handling NaI Previous use • GH2 (Panofsky….) • LH2 (PIBETA) • CH2 (MEGA, prec.misure) • LiH (e  at SIN) Coincidence: C & !A & NaI (Offline: & LXe) LXe

  10. Misure del 1999 8%FWHM • D=100 cm • 10 x 10 window • 9.5 hours • 60 cm (NaI) 75 cm (CsI) • 11 x 13 window

  11. Lxe facility

  12. Criostato • Necessita’ di rivedere il disegno (appoggio esterno ) • Selezione materiale finestra di ingresso • Simulazioni nuovo progetto • Contatto con Ditte produttrici il prima possibile

  13. Photon Detector schedule 2002 2003 2004 2005 Large Prototype Beam Test Beam Test Engineering runs Vessel Design Manufactoring Assembly & Test PMT Delivery + Testing Assembly Test Refrigerator Manufactoring Assembly Liq. Purification Design Manufactoring Assembly Test Milestone

More Related