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CODALEMA Geomagnetic effect observed by the Codalema experiment Lilian Martin SUBATECH CNRS/Universit de Nantes/ cole des Mines de Nantes Lilian Martin, RICAP'09, Rome, Italy 1 Outline The CODALEMA experiment Some examples of radio


  1. CODALEMA Geomagnetic effect observed by the Codalema experiment Lilian Martin SUBATECH CNRS/Université de Nantes/ École des Mines de Nantes Lilian Martin, RICAP'09, Rome, Italy 1

  2. Outline • The CODALEMA experiment • Some examples of radio signals • Radio detection efficiency and angular asymmetry • Interpretation in terms of a geomagnetic effect • Hardware developments • Upgrades Lilian Martin, RICAP'09, Rome, Italy 2

  3. CODALEMA goals • To measure the radio signal associated to the atmospheric shower produced by highly energetic cosmic rays reaching the Earth • To revisit a technique unsuccessfully explored 40 years ago by : – understanding the radio production mechanisms – Identifying key observables correlated to the air shower and the primary cosmic particle features • To develop a detection technique competitive with conventional surface detectors in terms of : – Quality of data (sensitivity, resolution) – Efficiency and duty cycle – Simplicity, robustness and COST Lilian Martin, RICAP'09, Rome, Italy 3

  4. The CODALEMA collaboration Observatory Paris-Meudon LAL Orsay 2002 : first tests with LPCE logarithmic antennas ESEO Orléans Observatory Angers Nançay Subatech LAOB Nantes Besançon LPSC Grenoble 2009 : large arrays routinely taking data Lilian Martin, RICAP'09, Rome, Italy 4

  5. Experimental setup : 3 instruments The Decametric array (DAM) : 144 log-periodic antennas (80x80 m ² ) 24 dipole antennas (two arms of 600m) 17 Surface Detectors (340x340 m ² ) Lilian Martin, RICAP'09, Rome, Italy 5

  6. Some pictures Lilian Martin, RICAP'09, Rome, Italy 6

  7. The CODALEMA short active dipole Simple and cheap Frequency response at Nançay Smoth radiation patterns Low noise Wide bandwidth High dynamic Good linearity FM AM 1 MHz 150 MHz Lilian Martin, RICAP'09, Rome, Italy 7

  8. Trigger and data acquisition • Trigger logic : Custom board allowing to remotely change : – threshold values – coincidence conditions ADC ADC ADC • MATACQ ADC : 300 MHz, 12bits, 1GS/s, 2500 samples, 4 channels, VME or GPIB Trigger • Slow trigger rate : logic – GPIB reading DAQ – LabVIEW for DAQ and monitoring Storage Coincidence of the 5 central SD : Trigger rate of ~200 events/day Lilian Martin, RICAP'09, Rome, Italy 8

  9. Data processing Filtering 23-83+110-130 MHz Filtering Corrected signals Tagging Times, amplitudes Positioning* Arrival directions Tagging and positioning Shower core position North Amplitudes Lateral distribution CIC UHECR energy Coincidences Selection of well Tag reconstructed UHECR Prediction from SD * positioning by computing the time difference of arrival ( TDOA ) of the South signal received by three or more SD/antennas. Lilian Martin, RICAP'09, Rome, Italy 9

  10. Measured data : some examples Time signals Pulses restricted to some antennas Variations in the lateral distribution of amplitudes Low energy event : • Clear transient signal in filtered time series Frequency spectrum • No clear contribution in the Not that much besides the AM and FM bands frequency domain Lilian Martin, RICAP'09, Rome, Italy 10

  11. Measured data : some examples Unfiltered ! Very large event : • Transient signal in raw data • Large contribution in the spectrum Lilian Martin, RICAP'09, Rome, Italy 11

  12. Event selection Shower core positions Information on the shower : • arrival direction • shower core position • Energy estimate (CIC method) 2 classes of SD events for the analysis Internal events : Station with the maximum signal not on one edge of the array. Correct estimate of Internal events shower energy and core position. External events : Unreliable estimate of shower energy Correlation SD-Antennas and core position. Correct arrival direction. Coincidences (SD and Antennas): angular difference < 20° time offset < 100 ns Good coincidences Lilian Martin, RICAP'09, Rome, Italy 12

  13. Radio detection efficiency Effective data taking time 355 days Scint. Detectors Trigger (SD events) 61500 Reconstructed antenna events 750 (2.1/day) Coincidences (SD and antennas) 620 (1.7/day) Coincidences (Internal) 157 (0.4/day) Extend the SD array ! Radio 5. 10 16 eV CODALEMA is performing radio measurements at the detection threshold → E th ~5. 10 16 eV Full efficiency is not observed Lilian Martin, RICAP'09, Rome, Italy 13

  14. Observed azimuthal asymmetry N The deficit is clearly in the southern region : θ θ ϕ ϕ N south /N total = 0.17 The SD azimuthal W distribution is flat : not a E trigger effect Independent subsets of events give similar results S Larger effects on smaller energy events Geomagnetic field direction Lilian Martin, RICAP'09, Rome, Italy 14

  15. A toy model to understand the asymmetry B α shower S N E SD zenithal distribution Total Lorentz force (E α sin( α ) ) Trigger acceptance X ( zenithal angle distribution ) Antenna lobe X (EZNEC simulation) Projection on East-West axis X (CODALEMA antenna polarization) Lilian Martin, RICAP'09, Rome, Italy 15

  16. Azimuthal asymmetry : comparisons The model reproduces quite well the observed distributions : • The maximums and local maximum • The minimums Model Azimuth Zenith data model Data Lilian Martin, RICAP'09, Rome, Italy 16

  17. Asymmetry : understanding the efficiency At 10 17 eV and Nançay, the efficiency scales linearly with |vxB| EW : Assumption of detection proportional the field amplitude is OK E’ = E . |(vxB) EW | Energy weighted by the cross product. Efficiency tends to reach 100% This linearity is probably only valid at threshold. Must be different at other energies. Lilian Martin, RICAP'09, Rome, Italy 17

  18. Measuring the NS polarization Is this picture valid for the NS polarization ? 3 NS antenna in the array Data Model Zenith Azimuth The statistic is lower but at the first look : YES Most of the events are coming from East and West directions Lilian Martin, RICAP'09, Rome, Italy 18

  19. Signal polarity The model assumes the electric field magnitude to Model Positive be proportional to |(vxB) EW |. Is the signal polarity given by (vxB) EW ? + Event Signal : antenna tag are signed Negative Event sign : given by the majority of signed tags - Data Model Data In the NS polarization Lilian Martin, RICAP'09, Rome, Italy 19

  20. CODALEMA upgrade : improving the antenna New prototype more suited for : robustness, easy production, 2 polar. measurements Test prototype Measurement with a prototype Simplified half antenna (one polar.) Improved sensitivity (galactic noise dominated) and stronger radio-diffusion suppression - 3 0 - 4 0 - 5 0 - 6 0 - 7 0 - 8 0 Galactic noise - 9 0 - 1 0 0 - 1 1 0 System noise - 1 2 0 S t a r t 1 M H z 1 1 . 9 M H z / S t o p 1 2 0 M H z Lilian Martin, RICAP'09, Rome, Italy 20

  21. CODALEMA upgrade : autonomous station French efforts to develop an autonomous system : - first prototypes were built with commercial material and existing Auger electronics : in used at Radio Auger (first cosmic events self triggered on radio signal) - development of a custom made new system is under test at CODALEMA and soon at Radio Auger Autonomous in terms of power, trigger, DAQ, coms. Support for the antenna (top) Batteries (back) Metallic box for protection and electric shielding Electronics crate (front) Lilian Martin, RICAP'09, Rome, Italy 21

  22. New electronic crate Ethernet Trigger Timing Power ADC Onboard PC (fits in the rack) Lilian Martin, RICAP'09, Rome, Italy 22

  23. Foreseen upgrades of the antenna array Replacement of the existing dipole antennas by butterfly antennas. Installation of (semi)-autonomous station in the current array for testing and debugging Extension of the current array – Higher antenna density at the center – Extension at larger scales Installation for testing in Argentina Tentative implementation of new stations at Nançay Lilian Martin, RICAP'09, Rome, Italy 23

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