1. FDWAVE : USING THE FD TELESCOPES TO DETECT THE MICRO WAVE RADIATION PRODUCED BY ATMOSPHERIC SHOWERS Simulation C. Di Giulio, for FDWAVE Chicago, October 2010

2. Spherical mirror with radius of curvature of 3.4 m Camera of pmt placed on a spherical focal surface with a FOV ~ 30 o x30 o FD Telescope

3. FD camera 440 PMTs on a spherical surface (Photonis XP 3062) Pixel 1.5 o Spot ≈ 1/3 pixel Mercedes 90 cm light collectors to recover border inefficiencies  Auger FD: 10560 PMTs “mercedes star” with aluminized mylar reflecting walls

4. Spherical mirror with radius of curvature of 3.4 m Camera of pmt placed on a spherical focal surface with a FOV ~ 30 o x30 o Diaphragm with diameter of 2.2 m FD Telescope

5. Schmidt optics C F Circle of minimum Confusion Diameter 1.5 cm Spherical aberration C F ● Coma suppressed Diaphragm C F ● Coma aberration Spherical focal surface

6. Spherical mirror with radius of curvature of 3.4 m Camera of pmt placed on a spherical focal surface with a FOV ~ 30 o x30 o Diaphragm with diameter of 2.2 m Corrector ring to increase the aperture + UV optical filter FD Telescope

7. Use LL1 & LL6 to detect microwave radiation equipping the empty pixels with microwave radio receivers Pixels without photomultipliers (removed to be installed in HEAT - - Photonis stopped the production) 220 pixels available (not considering the columns adjacent to pmts) FDWAVE

8. 14 3 First 32 horn positions

9. LL6 No pmts Use the profile reconstructed with pmts to estimate the energy deposit seen by radio receivers Use the standard FD trigger and readout the radio receivers every FD shower candidate ? FDWAVE

10. LL mirrors are produced with aluminium --> good reflectivity Reflector Spherical FD Parabolic microwave telescope spherical aberration in the focus all rays have the same phase! BUT: the parabolic dish is not suitable for track imaging purposes because of the strong aberrations for inclined rays  the best reflector is spherical !!! Optics

11. Parabolic vs Spherical Image good only near the center of the field. Only the star in the center of the field is on the optical axis. Spherical--> Schmidt camera Good image over large field Only part of the mirror it’s used to produce the image. Every image it’s produce by similar part of the mirror Every stars lies on the optical axis of such part correcting plates? Unnecessary for radiofrequency

12. Bibliography on Spherical Reflector in  wave

13. FD optics simulation Diaphragm 2.2 m Camera shadow ≈ 1 m GRASP www.ticra.com waves in only in one plane Radio receivers in the camera center at 1.657 m from the mirror ~ 7 GHz -  HP =60 0 Auger mirror R = 3.4 m

14. GRASP FEED Specifications: FEED: Fondamental Mode circula waveguide. Pattern:Gaussian Beam Pattern Definition Taper angle = 55.8 deg Taper = -12 Polarsation = linear x Far forced = off Factor db=0 deg=0

15. Spherical aberration Spherical Parabolic Gain (G) with respect to isotropy emission Simulation without Diaphragm and Camera shadow viewing angle Parabolic it’s better than spherical ~ 35 dBi ~ 15 dBi

16. Simulation with Diaphragm Aperture Parabolic Spherical Gain (G) with respect to isotropy emission viewing angle

17. Simulation with Diaphragm and Camera shadow Parabolic Spherical secondary lobes due mainly to camera shadow ~ 10 dBi Gain (G) with respect to isotropy emission viewing angle ~ 10 dBi

18. Optimal Wavelenght pixel field of view Half Power Beam Width optimal camera body 4.56 cm inserting antenna in camera holes  lower limit on 1.5 0 : 5 GHz > 6.6 GHz  6 cm antenna

19. Telescope Aperture constant within 1% aperture from Gain efficiency factor

20. FEED Conical Horn in the frequency range [9-11] GHz support (can be removed) connector for output signal (can be put in another position) waveguide  24.5 mm (<b) circular aperture  42 mm (<a) camera holes b=38 mm maximum aperture a=45.6 mm Contacts with SATIMO experts to lower the frequency (0.7 0 -0.8 0 )

21. Horn positions

22. Tempered Glass 3dB Transfert loss. Filter attenuation: as tempered glass??

23. Expected flux density P.W.Gorham et al., Phys.Rew. D78, 032007 (2008) Background ≈ 100 K + penalty factor (100 K?) 1÷2 Signal / Background staying within FD building (diaphragm, …) bandwidth

24. quadratic scaling linear scaling 15 km 10 km Possibility to increase I/  t > 100 ns averaging over more showers and FADC traces Rate in LL6 above 10 18.5 eV: 50 events/year Signal / Background

25. Elettronics & DAQ amplifier ANTENNA power detector FADC Log-power detector AD8317 up to 10 GHz 55 dB dyn. range typical signals very low I A eff  f ≈ -90 dBm (1 pW)  we need 50 dB amplification with low noise to match the power detector dynamic range AMF-5F-07100840-08-13P 7.1-8.4 GHzGain 53 dBT noise = 58.7 K use the FD FADCs  a trigger signal is needed  radio signals will be available in a friendly style

26. CONCLUSIONS The possibility to detect the microwave emission from air shower using the FD telescope optic it’s under investigation. To detect different part of the same shower with different techinque (Fluor. and Microwave) it will be nice. We need a background measurement in the FD building to estimate the system noise temperature.