Why radiodetection of UHECR still matters ? Karlsruhe Institute of Technology Germany 20/02/2014
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Why radiodetection of UHECR still matters ?Lessons learned from the CODALEMA II & III experiments
+ Measurement of the primary particle energy+ Localization of the radio emitting sources
+ Towards the identification of the primary particle
Dr. Ahmed REBAIThursday, February 20, 2014
Das Karlsruher Institut für Technologie
Laboratoire de physique subatomique et des technologies associées Nantes
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This work has been made a part under a grant from Region Pays de la Loire France and
CNRS/IN2P3 (Centre national de la recherche scientifique).
I would also like to thank Dr. Andreas Haungs and Dr. Tim Huege for the invitation
and Dr. Sabine Bucher for her administrative collaboration
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Introduction
Recent Results in Ultra High Energy Cosmic Rays physics and their interpretation
Radiodetection of UHECR
The CODALEMA Experiment
●The measurement of the energy of the primary particle
Localization of the radio-emission source
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Ultra High Energy Cosmic Rays puzzles
Many regions :- Low energies- Knees- ankle Many origins :- solar- galactic-extragalactic and ?Many techniques : Direct: satellites, balloons Indirect: ground base arrays (fluorescence,
particle detectors and antennas)
Open questions:Origin ? Nature ? Limit ?
Power law: Flux ~ E-2.7
Gaisser T. K. et al. Front. Phys. China. 8 (2013)
Transition ???
Knee
GZ
K o
r S
OM
ET
HIN
G E
LS
E?
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Current results on the Ultra High Energy Cosmic Rays Physics
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UHECR Origins
Question: How to reach 100 EeV (1020 eV)?
Cosmological origin (top-down mechanism) Massive particles decay (M.c2 ~ 1024
eV) Signature: photons/neutrinos Excluded by the Pierre Auger
Experiment (The Astrophysical Journal Letters, 755:L4 (7pp), 2012 August 10)
Astrophysic origin (bottom-up mechanism) Accélération de Fermi des particules chargées (Fermi: Phys. Rev. 75, 1169,
1949) => Limite ~ 1018 eV Proximité d'objets astrophysiques
=> Now, need to find sources
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Sky maps @ Ep>55 EeV
UHECR sources
South hemisphere : Auger North hemisphere : TA/Hires
TA/Hires : directional correlation 44% (Astrophys.J. 757 (2012) 26)
Auger :increase of statistics and decrease of statistical correlation (61% to 33%)(Science 318 (2007) no. 5852, 938–943)
Propagation: effect of the Intergalactic magnetic fields?
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UHECR propagation : GZK effect
During the 90s => disagreement between AGASA (Japan)-Hires1 (USA) experiments
2008: GZK cut confirmedby TA/Hires (Phys, Rev. Lett. 101 (2008) 061101) by Auger in 2010 (Phys. Lett. B 685 (2010) 239–246)
Interaction of UHECR with the Cosmic Microwave Background CMB
Auger
=>limit the observable universe at 100 Mpc=> depends on the primary nature=> @3.119 eV : Max energy of acceleration or propagation ?
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UHECR Nature
Auger : Heavy composition favoured (Phys.Rev.Lett.104:091101,2010)
TA/Hires : lightening of the composition in function of the energy (Phys.Rev.Lett.104:161101,2010)
Xmax
: depth of the shower
maximum development => related to the nature of the primary
Difficulties on measurements and interpretations and strongly increasing cross-section
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Proton interaction cross section @57TeV
(Phys.Rev.Lett. 109 (2012) 062002)
Constrained the hadronic models (QGSJET, Sibyll, Epos) used in particle physics
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UHECR detection methodsParticle detection on the ground : Cerenkov detectors Scintillators
Detection of the fluorescence light
Advantages Disadvantages
Ground based detectors
Duty cycle near to 100% Dependence on hadronic modelsDeployed large surfaces > 1000 km2
Fluorescence telescopes
Low dependence on hadronic models Large volume detection
Low duty cycle near to 10%
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Spectrum remains understood @UHEIll-defined chemical composition @UHEUnknown astrophysical origin @UHELow statistics at extreme energies
Radio-detection of Extensive Air Shower:A complementary detection method in evaluation11
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γγ
ee e e
γ γee
Electromagnetic cascadePions cascadeNucleons cascade
γe γe γe
nπ°2n(Κ±π± ...hadrons)
Near shower axis Hadrons
π± desintegration
µ µ µµ
~90% of γ (>50 keV) ~9% electrons (>250 keV)~1% µ (>1 GeV) small hadron fraction
Sol
z First interaction
Xmax Nmax
Extensive Air Shower 12
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Radio-detection of EAS
9% electrons/positrons
Radio emission mechanisms
Geomagnetic effect => deviation of electrons/positrons under the geomagnetic field effect => bipolar emission, transverse current, synchrotron emission => linear polarisation
Askaryan Negative charge-excess radiation => temporal variation of the negative charge excess => monopolar emission => radial field + Cherenkov-like coherence effect? (2010)
Forme du signal radio
Distanceshower-antenna
Radio signal shape
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Unipolar pulse models :
● REAS1, REAS2, ReAIRES
Bipolar pulse models:
● MGMR, REAS3, SELFAS2
Radio emission theoretical modelsComprehension of the radio signal => Intense theoretical efforts => several models available :
● Microscopic : use of CORSIKA and AIRES codes● Macroscopic : simplistic assumptions on the EAS phenomenology
+The total electric field
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MHz radio-detection experiments
EASIER
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AUGER
TREND
AERALOFAR
LOPES
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CODALEMA experiment @Nançay• Radio-astronomy environment
• Electromagnetic quiet environment
• Far from big cities => Non-existence of strong transmitter
• But no possibility for end-to-end calibration.
~1 Km
~2 Km
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CODALEMA Actual SetupArray of 24 short antennas 21 polar. E-W
Array of 17 scintillatorExperiment TriggerEnergy Estimator Shower core locationArrival direction
Decametric array18 groups of 8 log-periodic phased antennas
30 self-triggered Antennas2 polar. (E-W + N-S) Objective : 60 on 1.5 km2
4 detector arrays
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CODALEMA II : method of detection
Slave trigger mode
recording of the radio sky state
recording of the radio sky state
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Radio transient selection
Recording radio waveforms in 0-200 MHz:Sampling frequency 1Gs / s on 2520 Points
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Filtered radio transients
Event = 2 physical quantities/antenna (transient maximum amplitude and time of maximum transient )
Corrections :+Cables delays+Attenuation+Antennas gain
Digital filtering in the [20-83] MHz band
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Reconstruction of physical observables
Hypothesis : a plane wave front with equation :u.x+v.y+w.z+cte = 0(u,v,w) normal vector coordinates
Electric field profile
Arrivals direction : θ zenith angle ϕ azimuth angle
Allan model: exponential function with 4 parameters Ε = ε
0 exp(-d/d
0(x
c,y
c))
=> ε0 electric field on the shower axis
=> d0 radio shower lateral distance
=> (xc,y
c) shower core on the ground
Event = 2 physical quantities- Maximum amplitude of the transient- Time of maximum transient
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CODALEMA Results
CODALEMA model |vXB|EW
=>Est-West Polarisation of the electric field
=> Signal amplitude ~ |vXB|EW
D. Ardouin et al. Astro.ph 31 2009
Deficit of events near the magnetic axis
Evidence of a geomagnetic effect in the electric field generation mechanisms
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B
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The primary particle energy measurement with ε0 radio observable
+ A. Rebai et al. ArXiv:1210.1739, Oct. 2012 (submitted to Astro.Ph)+ ARENA2012, AIP Conf. Proc. 1535, 99-104 (2013)
ε0
Primary particle energy E
p
Correction factors:+ Geomagnetic emission?+ Askaryan charge-excess radiation?+ Cherenkov-like coherence effect?
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Study of correlation between Ep and ε
0
E0 ~ Ep^alpha avec alpha ~ 1.0=> dépendance linéaire
Corrélation dépend :Erreurs sur EpErreurs sur e0
Fit function :
3 assumptions :* Linear-linear fit* Gaussian error * Independence relation between ε
0 and E
p
Goodness of fit study => Standard deviation of the distribution of E
p and E
0 residual
Existence of outlier events
σ(Ep)/E
p ~ 30%
σ(ε0)/ε
0 ~ 22% (Monte-Carlo)
(Only statistical errors No systematics for this study)
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1st correction factor : geomagnetic emissionGeomagnetic effect :
ε0 ~
E
p.|(vXB)
EW|
ε '0 ~
E
p.|(v'XB)
EW|
=> ε0 → ε
0 /|(vXB)
EW|
Overestimation of the energy of the events near to the geomagnetic axisBut no effect in E
p
=> The existence of a second contribution
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Additional mechanismAn simple assumption :Contribution proportional to the energy (i.e. total charge produced in the shower)
ε0 ~
E
p.|(vXB)
EW| + E
p.c
=> ε0 → ε
0 / ( |(vXB)
EW| + c )
0 < |(vXB)EW
| < 1
c > 0
Best resolution for |(vXB)EW
| close to 1 and c=0
=> Geomagnetic effect dominance
For small |(vXB)EW
| => improvement in
resolution when c increase => Ep.c dominates
70 events per window
Qu
alit
y cr
iter
ia
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Additional mechanism
Can we combine this new contribution to an existing electric field emission mechanism ?
Shower axis perpendicular component Shower axis parallel component
ε0 ~
E
p.|(vXB)
EW|+E
p.c.|sin(θ).sin(ϕ)|
Resolution degradation=> we reject the hypothesis
Interpretations with the current data set of 315 events:ε
0 ~
E
p.|(vXB)
EW|+E
p.c
1st term depends on the geomagnetic effect2nd term depends on the shower total charge => Askaryan charge-excess mechanism ?
ε0 ~
E
p.|(vXB)
EW|(1+c/|(vXB)
EW|+d/|(vXB)
EW|2+ ….)
Analogy with a magnetic field deflection created by a dipole => deflection of charged particles increases with |(vXB)
EW| => distance
between the particles increases => s there a limit imposed by the coherence of the emission??
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Summary of the analysisOur interpretation with only 315 events :
ε0 ~
E
p.|(vXB)
EW| + E
p.c
1st term depends in the geomagnetic emission2nd term depends in the shower charge => Askaryan negative charge-excess mechanism ?
ε0 ~
E
p.|(vXB)
EW|.(1+c/|(vXB)
EW|)
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Energy resolution
Monte Carlo: Construction (E0, E
P)
distributions for fixed (∆E0, ∆E
P)
=> Construction of the abacus σ(EP-
E0)/E
P
=> σ(E
0) ~ 20%
=> Adopting a better parametrization RLDF (Gaussian)=> Improving the analysis chain + including systematic errors
Radio energy spectrum after calibrationRadio energy “Particle” energy
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Localization of radio emission sources➢ Motivations
➢ Experimental observations➢ Mathematical framework
➢ Ill-posedness formulation➢ Convex hull concept
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A. Rebai et al. arXiv:1208.3539+ ARENA2012, AIP Conf. Proc. 1535, 99-104 (2013)
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Towards a self-radio trigger
In 3 years : 2030 eventsIn 4 days : 107 eventsAntenna trigger Antennas triggered by scintillators
Noise sources appearance
Objective : avoid to trigger the antenna array by another array
Transition from prototype experiments triggered by a particle detector arrays to self-triggered antenna arrays deployed on large surfaces
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Study of the radio interference (RFI)
Need to accurately locate interference sources to remove it => spherical emission assumption
Anthropogenic sources:Aircraft, power lines, transformers,electric motors ...Natural sources: Atmospheric storm discharges...
This is the crucial problem to be fixed in order to make radiodetection auto-triggering mode (radio trigger)!
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● The near field and far field are regions of the radio emission around the source
● Near field => spherical wavefront (airplanes, electric transformers …)
● Far field => planar wavefront (the sun during solar flare periods cf. J. Lamblin for the CODALEMA collab.. Radiodetection of astronomical phenomena in the cosmic ray dedicated CODALEMA experiment. In Proceeding of the 30th ICRC 2008)
Why a spherical wavefront hypothesis ?
source
Near field Far field
2*D2/λ
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Near to Lofar array
EDF electric transformer
Electric gate of a farm
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RFI localization
►Correct localization expected for a spherical reconstruction:● immobile sources● Large number of detected events
+ Source/array position effect
►► localization problem ?
►►numerical simulation
CODALEMA III
TREND
AERA
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Model and simulation of the spherical waveTest array Spherical Propagation
1-Source at distance Rs
2- Arrival times distribution Computing
3-Introduction of errors
4-Generation of 1000 events
5-Reconstruction of the emission centre by minimizing an objective function with Simplex and Levenberg Marquardt (LVM) algorithms
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Time resolution effect
Simplex algorithm: direct search (no gradient calculation)
Effect of temporal error :● σ
t=0 ns : good localization with a
statistical estimator● σ
t=3, 10 ns : Degradation of
reconstruction: spread of the Rs
distribution
σt=0 ns
σt=3 ns
σt=10 ns
Elongated distribution points : but θ, ϕ => good estimation !!!
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LVM algorithm
Sensibility in initial conditions : Rini >> R
s => False results
Small modification in Rini => unpredictable results
=> Need to refine the analysis: apply other selection criteria
Initial conditions effect37
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Simulation conclusions
When the temporal resolution increases: :
Reconstruction degradation=> distribution points spread
Bias appearance
==> Need for a detailed study of this spherical minimization
But the temporal resolution is not the only factor
● Source position relative to the array :✔ Source outside the array => bad reconstruction✗ Source inside the array => good reconstruction
Localization sensitive to the minimization algorithms (simplex and Levenberg-marquardt, linear search)
Initial conditions dependence
Multiple solutions (degeneration)
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The followed approachThe minimization algorithms based on f descent direction search to reach the minimum (local or global) ● Solution = function minimum found● Global minimum => convex function => unicity of the
solution● Local minimum => non-convexe function=>
degeneration of the solution● Need to watch the first differential (minima)
and second (convexity)
Study the convexity of f:Jacobian and Hessian
● Coercivity of the objective function
● Sylvester criterion
● Ill-posed problem in the sense of Hadamard
● Ill-conditioned problem
Classification of the localization problem
in a more general framework
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Convexity of the objective function
Reasoning on the principal Hessian minor of order 4:
Sylvester Criterion : f is convex ⇔ All Hessian minors are positive
=> a negative minor => f is not convex => existence of several minimum
We choose
symbolic calculus:
With M is the Minkowski matrix
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Distribution of f minima
Search of minima:
=> Importance of the barycentre of the spatio-temporal variations of tagged antennas
Existence of a privileged direction of barycentre-source
● Importance of the closest antennas to the source
Analogy with the barycentre formula:
Difficulties in resolution => use of an empirical method
symbolic calculus:
=>
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1D array case3 hypothesis :● Source inside the array● Source outside the array● Source outside the array but off-line
Source interne
Particular role for the segment => convex hullRole of the nearest antenna to the source
Source externe
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1D array case (external source)
Source outside the segment and off-line
Constraints => light cones
Unconstrained Minimization results => Solutions lie on a half-line
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2D array case (internal source)
Convex hull role
Real case : source inside the antenna array
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2D array case (external source)
Presence of local minima Distribution on a line
Role of the convex hull
Existence of privileged half-line
Real case : source on the ground and outside the array convex hull (RFI sources)
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2D array case : source in the sky
Good estimation of the arrivals direction
source
Antenna array on the ground
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Ill-conditioned problem47Condition number : measure how sensitive a function is to changes or errors in the input
κ(H)=||H-1||*||H|| ~ λmax
(H)/λmin
(H) (eignevalues of H)
(F. Delprat-Jannaud and P. Lailly, Ill-Posed and Well-Posed Formulation of the Reflection Travel Time Tomography Problem, J. of Geophysical Research, vol. 98, No. B4, p. 6589, April 10, 1993.)
Low condition number (~1) => well-conditioned problem
High condition number (>>1) => ill-conditioned problem
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Classification of the localization problem
(1902) A physics problem is ill-posed if:1 – no solution
or2 – has many solutions
or3 – the solution has a strong dependence
In the different parameters of the problem (initial conditions, boundary conditions, data errors)
(2) et (3) => localization problem is ill-posed in the case of a source external to the tagged antenna convex hull
localization problem is well posed in the case of an internal source to the convex hull of antenna
Jacque Hadamard
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Best method to circumvent the problem is not yet found
R(estimated)=4000 m R(estimated)=9700 m
Direct search attempt
1 - Quantification of the phase space in a cubic grid: step ~ 50 m in space, time step ~ 10 ns
2 - Using the planar fit to determine the search directions in the phase space
3 - Calculate the value of f on a grid
4 - Search absolute minimum
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Best method to circumvent the problem is not yet found
Direct search attempt
But in the case of a source in the sky => Bias
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Source on the ground
PhD of Diego Torres
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And now EAS ?
Observation of a time shift relative to the plane wavefront assumption
But only one realization per event ► Problem for a statistical estimation of the source position
Hypothesis : the signal maximum amplitude linkedTo the development region of the shower (X
max ?)
51Dimensions of the charged particles pancake:+ Longitudinal spreading ~ few meters (J. Linsley, "Thickness of the particle swarm in cosmic-ray air showers," Journal Phys G vol. 12, No. 1., P. 51, 1986)+ Lateral spreading: limited by the effect of coherence => band [23-83] MHz => ~ 3 - ~ 13 m
Apparent point source localized in space => spherical emission
Data
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3D detectors in the water and in the iceVolume detector array (not a new idea) : Askaryan during the 70s and DUMAND array during 90s.
Slide from ARENA 2010 presentation “H. Ralf”
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3D detectors in the water and the ice53
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Exposure of high altitude antennas (mountains, ballons, satellite) P. Motloch, N. Hollon, P. Privitera, On the prospects of ultra-high energy cosmic rays detection by high altitude antennas (arXiv:1309.0561) accepted in Astro. Part.
3D convex hull: Towards 3D antenna array
Our idea
A. Rebai and Ramzi Boussaid Formulation of the emission sources localization problem in the case
of a selftriggered radio-detection experiment: Between Ill-posedness and Regularization (to be submitted)
Anita
Forte satellite
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Conclusions
+ Energy analysis was improved
indication of the presence of several radio emission mechanisms
Estimation of the energy resolution of ~ 20%
+ Prespective: More accurate LDF (Gaussian) => resolution enhancement
+ RFI observations and simulations => difficulties in interpretations
Study the objective function
Role of the convex hull
Role of the half-line that binds the antennas barycentre and the source
We need to work with mathematicians (multidisciplinary approach)
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