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The Electromagnetic Calorimeter (EC) at SciBooNE C. Mariani (Columbia University) for the SciBooNE collaboration

The Electromagnetic Calorimeter (EC) at SciBooNEhome.fnal.gov/~mariani/calor08.pdf · HV system SMACS server (SciBooNE enclosure): • Perform cyclic read out of the all system (

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Page 1: The Electromagnetic Calorimeter (EC) at SciBooNEhome.fnal.gov/~mariani/calor08.pdf · HV system SMACS server (SciBooNE enclosure): • Perform cyclic read out of the all system (

C.Mariani@Calor08 1

The Electromagnetic Calorimeter (EC) at SciBooNE

C. Mariani (Columbia University) for the SciBooNE collaboration

Page 2: The Electromagnetic Calorimeter (EC) at SciBooNEhome.fnal.gov/~mariani/calor08.pdf · HV system SMACS server (SciBooNE enclosure): • Perform cyclic read out of the all system (

C.Mariani@Calor08 2

Page 3: The Electromagnetic Calorimeter (EC) at SciBooNEhome.fnal.gov/~mariani/calor08.pdf · HV system SMACS server (SciBooNE enclosure): • Perform cyclic read out of the all system (

C.Mariani@Calor08 3

• SciBooNE:• Motivation;• Configuration;• EC @ SciBooNE;

• EC description: • support structure; • module configuration;• DAQ and HV system;• Online monitoring;• Calibration

Outline

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C.Mariani@Calor08 4

MINOS, NuMIK2K, NOvA

MiniBooNE, T2K

Super-K atmospheric ν

QE

DIS

• imperative for future osc exps to preciselypredict signal & bkgd rates- will be more sensitive

to sources of systematic error

• increased interest inmore precise σν meas

• interesting nuclear effectsexpected in this E region(shadowing in the nucleus, low Q2)

• new data from MiniBooNE & K2K shedding light on this

• More data at 1GeV with finegrained resolution will complete the picture

σν in this E range interesting:

Physics motivation

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C.Mariani@Calor08 5

Decay region

25 m50 m 450 m

MiniBooNE Detector

SciBarSciBarMiniBooNE beamlineMiniBooNE beamline

4m

3.5m

1m

MRDMRD

SciBarSciBar (4 X(4 X00))(Fiducial:10t)(Fiducial:10t)

EcalEcal(11X(11X00))

1.7m

3m

3mνν

100m from the targetOn-axis position(1~2)x1019 POT/month

SciBooNE configuration

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C.Mariani@Calor08 6

EC motivationsPhysics capabilities

Longitudinal containment (85% at 3GeV);Energy reconstruction for electrons and gammas;Electron vs (muon or pion) IDπo reconstruction;

Physics outputνe energy spectrumπo cross-section and spectrumEnhance PID and event classification

Physics goalLongitudinal energy flow containmentElectrons and photons final states

Page 7: The Electromagnetic Calorimeter (EC) at SciBooNEhome.fnal.gov/~mariani/calor08.pdf · HV system SMACS server (SciBooNE enclosure): • Perform cyclic read out of the all system (

C.Mariani@Calor08 7

.)%(..)(.. sysstatCCCCe 203061 ±±=

μνν

EC results@K2K

Phys. Rev. D74:072003, 2006

νe flux

Phys. Rev. D in preparation

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C.Mariani@Calor08 8

EC – Electromagnetic calorimeter(University of Rome “La Sapienza” and INFN Roma)

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C.Mariani@Calor08 9

Module configurationSpaghetti calorimeter:

• 1 mm scintillating fibers in grooves of lead foils 1 mm thick;• Scintillating fibers (Kuraray SCS-F81), 500 cm attenuation length;• Ratio fiber/lead 1:4 (in volume);

• Module dimension (4x8cm2x265cm):

• 4x4 cm2 readout cells, read from both ends;

4 cm

265 c

m

8 cm

4 cm

The modules were originally build by INFN for CHORUS(1992) and then re-used by the HARP experiment at CERN, K2K at KEK (Japan)

and now SciBooNE at Fermilab.

Readout cells

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C.Mariani@Calor08 10

INFN

HARP (2001) CERN

K2K (2003) KEK

SciBooNE (2007) FERMILAB

CHORUS (1993)

CALORIMETER MODULE'S TRAVELS...

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C.Mariani@Calor08 11

2 readout cell from both ends:

• Hexagonal light guides;• Yellow filters (Kodak Wratten 6);• Hamamatsu R1355/SM (green extended);• Signal readout through differential pairs cable 100m long;Fiber bundle

Light guide

PMT & HV divider

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C.Mariani@Calor08 12

Support Structure

64 “spaghetti” calorimeter modules (4x8cm2x265cm):

• 32 horizontal and 32 vertical modules;

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C.Mariani@Calor08 13

NIM VME

SciBarTrigger and Trig. ID

Busy signalPCADC Gate Read Out

Busy clearBusy clear

EC logic (conceptual)

Trig. ID

Event number

DAQ system

logic ADC Readout

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C.Mariani@Calor08 14

• Three trigger signals:• Cosmic;• Pedestal;• Beam data;

• DAQ:

• Acquisition time < 1ms;

• Acquisition rate up to 1.5 kHz;

• 8 QDCs (Caen V792):• 12 bit resolution;• 5.7 ms/ch conversion time;• 600 ns fast clear time;

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C.Mariani@Calor08 15

PC

2 mainframesCAEN SY527

+16 HV cardsCAEN A734N

Control room Alarm and warning

EC HV system

monitor

HV system

Load setting

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C.Mariani@Calor08 16

HV systemSMACS server (SciBooNE enclosure):

• Perform cyclic read out of the all system (< 1s) to get status of each channel, readout voltages and current;

• All “HV events” are logged in a local DB;• A tree browser allow navigation of the HV channels, a led represent the

status of each channel;• Selecting a channel from the browser, the status voltage, current and their

time plots are accessible through tabs;• Individual channel setting can be changed interactively;

SMACS client (control room):• Client-server communication (ASCII strings through winsock);

• Multiple clients can run simultaneously;• Map display of pmt online status (green/yellow/red: ok/warning/alarm);• Double left-click on a pmt shows set/monitored voltage and current and

online condition;• Cannot modify HV setting;

SMACS = Slow Monitor And Control System. Visual basic software interface originally developed by INFN Roma for the CDF-TOF system

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C.Mariani@Calor08 17

Server:

• Map display of pmt status like the client side;• Double click on client windows on a channel to get status and set/monitored

voltage, current, change setting and turn on/off channel;• Monitor the number of clients connected to the server.

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C.Mariani@Calor08 18

Monitoring Client (SciBooNE CR):

• Map display of pmt status;• Double click on a channel to get status;

• Alarm window automatic pop-up;• Send email and call pager;

• Window logging past allarm;

Double click:status

• Green Channels are ok;

• Yellow channel: warning;

• Red channel: alarm

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C.Mariani@Calor08 19

Online monitoring

Monitor in real time (for cosmic trigger and beam trigger):• ADC hitmap;

• Average deposited energy for each channel;

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C.Mariani@Calor08 20

Before installing

The detector was fully installed in an assembly area before transportation to the detector enclosure. Commissioning with cosmic ray data provided:

• HV adjustment of the 256 channels;• Equalization of the response of all the 64 modules; • Measurement of the number of PE;• Measuring the attenuation length of fibers in each of the 64 modules;

After the installation in the SciBooNE enclosure we monitor constantly:• Pedestal absolute value and pedestal width (every 10 minutes);• Energy deposited by cosmic muons → Gain of each channel ;• Voltage and current of each PMT channel;

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C.Mariani@Calor08 21

Muon typical response

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C.Mariani@Calor08 22

Pulse height distributionBefore HV adjustment After HV adjustment

Spread = 22%

Spread = 10%

After equalization, spread < 1% Number of PE = 10.4 on average

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C.Mariani@Calor08 23

Distribution of the attenuation length

In 1992 the measured attenuation length in CHORUS was around 500 cm, after 15 years result to be around 400 cm

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C.Mariani@Calor08 24

Reconstructed muons energy loss (data)

MIP energy loss in both the EC planes (Horizontal + Vertical) using cosmic rays SciBooNE data

E = sqrt(ADC1ADC2) x InterCalib x Abs.Calib x C_Att.Length.

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C.Mariani@Calor08 25

MC simulation

In order to simulate the response of the EC detectors, the GEANT4 package is used to simulate the detector geometry and the interactions and tracking of particles.

The energy loss of a particle in each individual EC sensitive fiber is simulated.

The energy deposition is converted in the detector response taking into account effects like:• the light attenuation along the fibers;• the Poisson fluctuation of the number of photo electrons;• the PMT resolution;• the electronic noise.

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C.Mariani@Calor08 26

DATA-MC agreement for the ADC distribution

Claudio Giganti, Tesi di Laurea (2007), Universita' di Roma "La Sapienza"

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C.Mariani@Calor08 27

Muon dE/dx energy resolution

We studied the energy resolution (σ(E)/Etrue) for the dE/dx of cosmic muons as a function of Etrue.

To obtain σ(E)/Etrue we computed, for each bin, the width of the distribution [(Erec * Cabs) – Etrue] and we divided this value for the mean value of Etrue.

][%)1.06.6()(

GeVEEE ±

<dE/dx>MIP= 106 MeV

σ(E) = 21.5 MeV

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C.Mariani@Calor08 28

Ce/μ and Energy resolution for electrons in the MC

To study the response of the EC we sum up the energy in all the EC modules and we compare the reconstructed and true energy. For the reconstructed energy we use the absolute calibration measured for cosmic ray muons Cμ

Ce/μ = 1.19 ± 0.07

][%)1.08.12()(

GeVEEE ±

The resolution for electron was measured 13%/sqrt(E) in a test beam at CERN for the Chorus experiment

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C.Mariani@Calor08 29

Candidate SciBooNE NC neutrino interaction with a π0 production in the final state