18/05/06p. nedelec - 4th air fluorescence workshop measurements of fly with macfly
TRANSCRIPT
18/05/06 P. Nedelec - 4th Air Fluorescence Workshop
Measurements of FLY with MACFLY
2
Measurement of Air Cerenkov and Fluorescence Light Yield
http://wwwlapp.in2p3.fr/MACFLY/
LAPP (France): Pierre COLIN, Patrick NEDELEC;LIP (Portugal): Antonio ONOFRE;JINR (Russia): Leonid TKATCHEV, Artem CHUKANOV, Basar SABIROV, Yuri NEFEDOV, Sergei POROKHOVOI, Dmitry NAUMOV.
Collaboration:
3
Original Goals
To Measure Air FLY variations as a function of atmospheric conditions:
Reproduce and study in laboratory the light emitted
by an “extensive air shower” (EAS)
15 km
2 km
EAS
Temperature Pressure Humidity
- 60°C
10°C
100 hPa
800 hPa
0 %
1 %
Alt
itu
de
(km
)
4MACFLY project = 2 devices
Vacuum pump
N2 Air
Ar
O3
Beam:- β Source- CERN- JINR
PMT
Preshower
Gauge : P,T,H2O
H2O
shower
Gas system
MACFLY 1(for beam)
MACFLY 2(for shower)
5
MF1: a reference device
• Single track events device– Light, compact, movable (plane?),…
• Used both– @ Lab (quiet) – on Test Beam (noisy)
• Measure:– Air/N2FLY– Cherenkov contribution
• Used for comparison with– Other experiments– MF2
6Macfly 1 @ LaboratoryPompe à
vide
90Sr β Source
PMT1
PMT2Electrons
beam
Scintillator
PM Trigger
Radioactive source
Sr90
Optic fibres
Pressure sensor
Main tankTemperature
sensor
Input/ouput of gas
PMT
Vacuum pump
Trigger PMT
7
MF1 cut view
EMI
9820
QA
EMI9820QA
PMT EMI 9820QAQuartz Window
Filters Quartz Lens
Mirror : ~98%(multi-layers)
Light Guide
Electron beam
15 cm
Macfly 1 optical system
EMI9820QA
5 cm
Filter
Filters Transmittance (Schott BG3 and GG385)
8
MF2: looking for real showers
• A “From single track to showers” device– Heavy, Big, Fix ,…
• Used:– Only on Test Beam Line
• Measure:
– Air/N2 FLY induced by a e- shower (10-50 GeV)
– From 0 to Xmax radiation length
• Used to:– Perform original measurements– for comparison with Monte Carlo prg (G4,…)
9
Macfly 2 (MF2)Ø
96 cm
146 cm
Volume : ~1m3Input/Output of gas system
CERN Beam
PMT
Sensors (P,T)
Cooper target(Preshower)
10
MF2 working process
EM
I
EMI
Black surface
Ø10 cm
Light guide
Filters
Preshower
Electromagnetic Shower
Preshower system:
PMT EMI 9820QAQuartz Window
Electron beam
Stack of copper disks (Thickness :1cm)
Lead shield
11
Measurement campaigns
> At JINR ? : (MF1)– Microtron(12 MeV) and Phasotron (170 MeV) – Pressure and temperature dependencies
> In Lab : (MF1)– Radioactive source (1.5 MeV electron)– Pressure dependence
> At CERN : (MF1+MF2)– SPS test Beam (5-100 GeV e-, μ-, π-)– Pressure dependence: ; Temp., H2O: – Shower age dependence (MF2)
Too noisy! Then a Fire !!!
12
MACFLY set up overview at CERN
Macfly 2
Delay chamber
MF2
Trigger TriggerMF1
Thermal Box
Small Trigger
MF1 in its thermal box
Pumping system
Large Trigger
Delay chamber
13
Macfly Data
Event by event acquisition
PMT signal read by a QADC (Gate=100ns)
Very Low signal: mean=0.01photoelectron
Expected FLY ~ 4 ph/m
~106 triggers/run (1/2 data+1/2 Bgd)
14
Delay chamber
MF2
Trigger TriggerMF1
Thermal Box
Macfly Data selection
Centered events
15
MacFly: Fluo. Signal extraction
DL = FLY x εMF + CDL + Bgd
PMT Detected Light (fit method)
Cherenkov Detected Light
(Geant4 simulation)
Background (Vacuum
measurement)
Fluorescence Light Yield (in photons)
Detector efficiency
(Calibration)
FLY/E = FLY / EdepDeposed Energy(Geant4 Simulation)
16
Macfly Data
Detected Light: PMT spectrum fit Method
Pedestal : (~99% of events)
Single photoelectron(~1% of event)
2 photoelectrons
DL = FLY x εMF + CDL + Bgd
17
MacFly: Geant4 Simulation
Geometrical Acceptance(Optical Properties of surfaces were previously measured)
εMF = Accgeo x QEPMT
DL = FLY x εMF + CDL + Bgd
18
MacFly: Geant4 Simulation
DL = FLY x εMF + CDL + Bgd
Cherenkov Light: compare simulation with data
LensesCerenkovcatcher
e-
Cherenkov light in MF1
19
MacFly: data
Background:
DL = FLY x εMF + CDL + Bgd
• Well measured events– Random triggers (@lab)– Off-spill triggers (@beam)– Vacuum On-spill triggers (@beam)
20
MacFly: Geant4 Simulation
Radiation length (#X0) 0 disc
1 disc
3 disc
5 disc
7 disc10 disc
Pre-Shower
Deposed Energy in MF2
Deposed Energy:
FLY/E = FLY / Edep
21
Detected Light Composition
DL(Macfly data)
CDL(Simulation)
Bgd(Measurement)
FDLFluorescence detected light
MF1 : 50 GeV e- in airMF1 : 50 GeV e- in air MF1 : 50 GeV e- in N2MF1 : 50 GeV e- in N2
MF1 : 1.5 MeV e- in airMF1 : 1.5 MeV e- in air MF2 : 50GeV Shower in airMF2 : 50GeV Shower in air
22Systematic errors of MF1
Error Sources
MF1 (Dry Air)
CERN Lab.
QE of PMT 10% 10%
Geo. Acc. 8.2% 7.5%
DL Recon. 3.5% 4%
CDL Simu. 2% 0%
Bgd Meas. 2% 1%
FLY : 13.7% 13.2%Edep 1% 1%
FLY/E : 13.7% 13.2%
23
MF1 result: Pressure dependence
We create a model of air FLY proportional to deposed energy which fit all Macfly data.
(Dry air and pure Nitrogen)
24
MF1 result: Energy dependence
Reference point : Dry air at 1atm. & 23ºC: FLY/E = 18 ph/MeVReference point : Dry air at 1atm. & 23ºC: FLY/E = 18 ph/MeV
dEdX: Berger-Seltzer formula All experiments are coherent
25
Absolute measurement
Reference point : Dry air at 1atm. & 23ºC : FLY/E = 18 ph/MeVReference point : Dry air at 1atm. & 23ºC : FLY/E = 18 ph/MeV
dEdX: Berger-Seltzer formula All experiments are coherent
Error< 10% ?
26
MF2 result: Shower age dependence
500 hPa data
100 hPa data
PDG model of shower development
Air FLY follows the shower development !Air FLY follows the shower development !
27
MF2: Air FLY deposed Energy
FLY/Edep and pressure variations independent of the excitation source
FLY/Edep and pressure variations independent of the excitation source
28
Conclusion
Measurements done: P. Colin thesis Dry air and pure Nitrogen fluorescence 1.5 MeV, 20 GeV and 50 GeV incident electron Lab. measurement of air Shower FLY Pressure and Shower age dependencies
Fluorescence model: Air FLY Edep Fitted on Macfly data Compatible with previous exp. (<10%)
Back to the future: PMT calibration Temperature dependence Papers in preparation
Systematic down to: ~10%