Coincidence analysis in ANTARES: Potassium-40 and muons Brief overview of ANTARES experiment ...
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Transcript of Coincidence analysis in ANTARES: Potassium-40 and muons Brief overview of ANTARES experiment ...
Coincidence analysis in ANTARES:Potassium-40 and muons
Brief overview of ANTARES experiment Potassium-40 calibration technique Adjacent floor coincidences as very basic atmospheric muon signal
ITEP winter schoolFeb 12, 2008
Dmitry Zaborov(ITEP, Moscow, Russia)
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 2
Detection principle
č
43°Sea floor
p
104
atm
p, 107
at
m
Reconstruction of trajectory (~ ) from timing and position of PMT hits
interaction
Cherenkov light from
3D PMTarray
1-100 cosm
effective area ~ 0.1 km2 in TeV rangeangular resolution ~ 0.3º at 10 TeVHadronic showers
from CC/NC interactions can be detected as well
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 3
Detector layout
~70 m
12 lines (900 PMTs) 25 storeys / line 3 PMTs/storey
350 m
100 m
14.5 m
Junctionbox
Readout cables
40 km toshoreHorizontal layout
Sea bed ~ -2500 m
a storey
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 4
Current status
L11
L9
L12
L7
L8
L6
L4
L2
L3
L5
L1
IL07
seismometer
100 m
N
Junction box
Submarinecable
to shore
42°50’ N
6°10’E
10 detector lines +
instrumentation line
operational (since December 07)
(Feb. 2008)
2 more lines coming soon
~ 2 muons/sec
~ 5 neutrino/day (atmospheric) L10
* Cable path is shown only indicatively
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 5
Basic detection and calibration elements
Hydrophone:acoustic positioning
Optical Module:10” PMT in 17” glass sphere
photon detection
Local Control Module(in Ti container):Front-end ASIC, Clock, DAQ/SC,
compass/roll/pitch
Optical Beaconwith blue LEDs:timing calibration
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 6
In situ calibration with Potassium-40
40K
40Ca
e- ( decay)
Cherenkov
Gaussian peak on coincidence plot
Peak offset
Rate of correlated coincidences
High precision (~5%) monitoring of OM
efficiencies
time calibration confirmed
15 Hz
MC prediction 13+/-4 Hz
(“NIM” angular acceptance)Mean ≈ 0
RMS 0.7 nsNo dependence on bioluminescent activity has been observed - this confirms the single photon character of bioluminescent emission
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 7
Example: calibration of Line 8Three OM sensitivity factors si can be extracted using 3 equations
rateij = k * si * sj
factor k gives absolute scale;k can be determined from Monte-Carlo (or, in opposite, used to constrain parameters of Monte-Carlo)
OM-OM time offsets determined using K-40 (basically single photoelectrons)w.r.t Dark room calibration (high amplitude laser pulse)
* No charge calibration used* No walk correction included
Unofficial technical plot
Unofficial technical plot
I,j=1,2,3
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 8
Time evolution (example)
Time delays seem stable (within our accuracy)
Gradual decrease is probably due to PMT gain drift
Steep changes are threshold tunings
Unofficial technical plot
Unofficial technical plot
K40 runs are taken once a week
K40 trigger can run in parallel with other triggers (e.g. GRB trigger or
directional triggers) and can be even used for physics analysis as is
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 9
Time evolution of average K-40 coincidence rate
start at 12 Hz “degradation”
tuning 2
One year of “degradation” could be fully compensated by the tuning
tuning 2-> 15.5 Hz
* Other Lines show similar behavior
tuning 1
Unofficial technical plot
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 10
Delay between adjacent floors (theory)
Δt = L / c ≈ 50 ns Δt ~ L n / c ~ 70 ns
L
Δt ~ 0
But light hits back of the OM
≈ fixed number for exactly vertical muons a wide distribution in general
from
to
The most basic signal of physics events in ANTARES
Delay between storeys No systematic
errors from trigger or
reconstruction algorithms
No background
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 11
Adjacent floor coincidences: measurementIntegral under the peak ~ muon flux
Shape is sensitive to angular acceptance of optical modules and angular distribution of muon flux
The effect of muon flux reduction with depth is directly (!) measured
Low energy threshold(compared to full reconstruction)
The analysis can be repeated for every detector storey separately
This plot is preliminaryActual comparison of peak amplitude with Monte Carlo will be made after OM angular acceptance issues are fixed, OM efficiency is well known and all dead time corrections applied
Feb 12, 2008 D. Zaborov. Coincidence analysis in ANTARES 12
Summary
• A calibration technique using Cherenkov light from Potassium-40 decays in sea water has been developed– Sensitivity of optical modules is now controlled using K-40– K-40 is also a useful tool for time calibration
• A simple but powerful technique for atmospheric muon measurement is developed based on the idea of adjacent floor coincidences– First results allowed to reject one of the models of OM angular
acceptance– Depth dependence and absolute normalization of atmospheric
muon flux can be extracted using this new approach– Possibility to reject certain hadronic interaction models or (less
likely) primary flux models is being investigated– Promising prospects to use adjacent floor coincidences in the
trigger