1. Hagar Landsman, University of Wisconsin, Madison

2. The plan for the next 10 minutes (and the next 5 years) IceCube RF extension Review of current hardware Status Stay tuned for the next 2 talks ARA – Askaryan Radio Array New collaborative effort The grand scheme Results from last season Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 2

3. 3 IceCube’s radio extension  In ice digitization. Combination of ANITA/IceCube/RICE technologies: 2 clusters in 2006-2007 3 clusters in 2008-2009 Depth of 1450 m or 300 m AKA “AURA”  Envelope detection. 6 units deployed at -35, -5 meters (2009-2010) 6 units in other depth/location (On top of a building, terminated, -250m) AKA “SATRA”  Calibration Set of transmitters and passive antennas for calibration (including cable symmetrical antennas) Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 3

4. 4 IceCube-radio hardware Fully digitized WFs surface junction box Counting house Use IceCube’s resources: holes, comm. and power Each Cluster contains:  Digital Radio Module (DRM) – Electronics  4 Antennas – With front end electronics  1 Array Calibration Unit (ACU) - Transmitter Deployed above the IceCube array:  “Free” Deep holes  “Free” Power distribution and communication Signal conditioning and amplification happen at the front end  RICE Broad band fat dipole antennas centered at 400 MHz  450 MHz Notch filter  200 MHz High pass filter (2 units with 100Mhz)  ~50dB amplifiers (+~20 dB in front end) Signal is digitized and triggers formed in DRM (a’la’ANITA)  512 samples per 256 ns (2 GSPS).  Wide frequency range and multiple antennas are required for triggering Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 4

5. 5 Transient style detection DAQ box sjb 30 m 5 m satra IceCube cable Nick name: SATRA - (Sensor Array for Transient Radio Astrophysics ) Transient detector (“SATRA”) – 6 in ice units on 3 strings in holes #8, #9 and #16 – 1 antenna each: 2 antennas per hole. – 35m and 5 m deep – Each pair of antennas has a local-coincidence triggering – Dry holes – Log amp envelope detection Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 5

6. Some results Ice index of refraction n(z) Ice Attenuation Length (point to point) Environmental noise Reconstruction algorithms See Mike Richman’s and Chris Weaver’s talk 6 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 6

7. The ARA Vision 80 km 2 area 37 stations equally spaced on a triangular grid Large separation between stations (1.3km) 3 stations forms a “super cluster” Sharing power, comms, and calibration source ~30m Station: 4 closely spaced strings 200m deep Digitization and Triggering on surface DAQ Housing Vpol Antenna Hpol Antenna String: 4 antennas, V-pol and H-pol Designed to fit in 15cm holes 150-800 MHz sensitivity Cable pass through antenna Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 7

8. Optimized for neutrino counting: A single station can provide and form a trigger  Decreases trig time window, lower background and therefore thresholds.  Lowers the energy threshold. allowing single string hits. Detecting down-going events: (4.4sr) Between +45 above, -5 below horizon Deep ice contributes in higher energies Hagar LandsmanARA Spring 2011, Madison ~30m 200m 2.5 km 1300m ARA Concept γ Interaction vertex RF radiation The goal is to count events, not reconstruct the angles as would be needed for observatory class instrument

9. ARA - A New collaboration was born NSF Grant “Collaborative Research: MRI-R2 Instrument Development of the Askaryan Radio Array, a Large-scale Radio Cherenkov Detector at the South Pole“ phase 1 funded More than 10 institutions from US, Europe, Taiwan, Japan Including IceCube & ANITA & RICE leading institutes. Hagar LandsmanARA Spring 2011, Madison 9 2010-2011  Install testbed  EMI survey away from the station  Test ice properties  Testing station prototypes (antennas and electronics)  Calibration activities  Install 3 deep RF Pulsers  Conduct Drilling tests  Install 3 Wind turbines for testing

10. This season’s on ice achievements ARA Test Bed Successfully installed ~3.2 km away from the Pole. 16 antennas at different depths, down to ~20m. Signal digitization and triggering happens on a central box on the surface. Power and comms through cables. Current status: Detector is up and running. Very high efficiency and live time. No unexpected EMI source. Up to now, no evidence for wind generated EMI Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 10

11. This season’s on ice achievements ARA Test Bed – Trigger rates 9:00 am weather balloon launch 9:00 pm weather balloon launch Test Bed is taking data continuously Trigger rates are low and stable – below 4 Hz Clear winter/summer rate difference Weather balloon launches CW clearly seen Austral winter sssshhhhh Austral summer A lot of on-ice activity Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 11

12. This season’s on ice achievements ARA Test Bed – Galactic center Noise measured on the surface antennas preliminary Data used from January 18 to April 14 Using two surface antennas Galactic noise clearly seen over thermal (~ -130 dbW) Expected galactic Thermal Total Ch 1 Ch 2 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 12

13. 3 high voltage calibration Tx installed on IceCube strings at ~1.5 and 2.5km Deep (2450m) pulser seen by all antennas in the ARA testbed! Testbed is a horizontal distance of ~1.6 km away- total distance 3.2 km. Points to an attenuation length of >700m (analysis ongoing). Time delays between different antennas used to estimate T resolution. This season’s on ice achievements Deep pulsers on IceCube strings σ time =97 ps mV ns Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 13

14. Challenges in constructing and operating a large array Tested two different drills: - Drilling speed - Depth - Hole diameter, smoothness - Logistics Installed several models of wind turbines - Measuring and comparing wind speed, power yield. -Weather effects to be evaluated next summer This season’s on ice achievements Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 14

15. On going analyses with IceCube radio extensions, A collaboration has been formed to build an englacial array large enough to detect cosmogenic neutrinos An array concept has been proposed. The first phase funded. Fine tuning of instrumentation and detector spacing to be optimized during the development phase Successful first South-Pole season Facing several challenges in building and operating a large scale detector such as power distributions and fast drilling. Work has commenced in preparation for the next season Eventual large scale array will determine cosmogenic neutrino flux and tackle associated long standing questions of cosmic rays.SummarySummary Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 15

16. Backup slides Hagar LandsmanARA Spring 2011, Madison 16

17. This season’s on ice achievements Deep pulsers on IceCube strings Blind spots due to ray tracing. The deeper we get the larger the horizon is. This was the last access to deep holes. 3 high voltage calibration Tx installed on IceCube strings at ~1.5 and 2.5km Azimuthally symmetric bicone antenna -eliminates systematics from cable shadowing effects Goals: radio glaciology and calibration Hagar LandsmanARA Spring 2011, Madison Depth [km] 3 1 2 0 Distance [km] 43210 Ray traces 200m Depth [km] Distance [km] 3 1 2 0 43210 Ray traces 1500m Depth [km] Horizon [km] Horizon for 3 different receiver depths 0 1.8 0.6 1.2 00.511.52.52 20 m 200m 1000m Receiver Transmitter 17

18. Ray Propagation Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 18

19. ARA expected performance Effective volume Ongoing simulation studies to optimize detector geometry, and make the best use of the 2.5km ice target. 17181920 Neutrino Energy [eV] Effective volume [km 3 sr] 10 100 1000 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 19

20. Solution: Use Cherenkov photons in RF Longer attenuation length in ice  larger spacing  less hardware Less scattering for RF In ice. Cherenkov radiation pattern is preserved Don’t need many hits to resolve direction No need to drill wide holes Better ice at the top. No need to drill deep. Antennas are more robust than PMTs. The isolated South Pole is RF quite and Any EMI activity is regulated Deep ice (2.5km) contributes to effective volume It is easy to detect RF Pavel Alekseyevich Cherenkov (1904-1990) Gurgen Askaryan (1928-1997) Remember: Less photons are emitted in longer wave length. Smaller signal in the radio frequencies…. But for high energy cascades this RF radiation becomes coherence and enhanced “Askaryan effect” Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 20

21. Askaryan Effect Heritage RICE Radio Ice Cerenkov Experiment Array of single dipole antennas deployed between 100 and 300m near the South Pole, covered an area of 200m x 200m. (mostly in AMANDA holes) Used digital oscilloscope on surface for data acquisition ANITA ANtarctic Impulsive Transient Antenna : surveys the ice cap from high altitude for RF refracted out of the ice (~40 km height of fly, ~1.1M km 2 field of view) IceCube Radio Co deployed with IceCube at 30m, 350m and 1400 m. Full in ice digitization. The Askaryan effect Was measured in a special SLAC experiment. Extensive simulation of the radiation cone exist, and predictions are in agreement with the measurement. Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 21

22. Highest energy neutrinos….Why ? There is a high energy universe out there we know very little about! HE Neutrinos are expected to be produced together with photons and protons through pions decay. Neutrinos add complimentary information to gamma astronomy With neutrinos we can look further away p p +      n +  p+      n +   v e  e veve veve Cosmic rays with energies of more than 10 20 eV were observed. Their source, or acceleration mechanism are unknown. Sufficiently energetic Cosmic rays interact on photon background and loose energy No energetic CR from large distances (>50MPc) Flux of neutrino : “Guaranteed source” Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 22

23. Current IceCube configuration: Effective area: Yields less than 1 cosmogenic event/year Making IceCube bigger is an option: Some geometry optimization is possible, though: Still need dense array scattering Still need deep holes for better ice Any additional string will cost ~1M $ * (See Christopher Wiebusch talk this session) A larger detector requires a more efficient and less costly technology. * Rough estimation, Real cost will likely be higher Why not Build a Larger IceCube? IceCube can detect cosmogenic neutrinos, but not enough of them … More than 60% of DOMs triggered Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 23

24. The Game Plan Establish cosmogenic neutrino fluxes Resolve Energy Spectrum Neutrino direction Reconstruction Flavor analysis Particle physics ~10 ~1000 Small set of well established events. Coarse energy reco Energy reconstruction by denser sampling of each event Angular resolution of less than 0.1 rad Events/year Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 24

25. GZK ARA expected performance detector sensitivities RICE 2006 ARA (3 years) ANITA (3 flights) Pure Iron UHECR IceCube (3 years) Auger Tau (3 years) How strong should a source be, for it to be detected by a detector Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 25

26. ARA expected performance Reconstruction Vertex reconstruction : Where in the ice did the Neutrino interact? Using timing information from different antennas. Distance to vertex (for calorimetry) Location of Vertex (Background rejection Neutrino Direction and Energy: Where in space did the Neutrino come from? Combining amplitude and polarization information with Cherenkov cone models. ARA is not optimized for this. Simulated Angular resolution: ~6° Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 26

27. Phase 1: 3 years plan 2010-2011  Install testbed  EMI survey away from the station  Test ice properties  Begin testing station prototypes  Calibration activities  Install 3 deep RF Pulsers  Conduct Drilling tests  Install 3 Wind turbines for testing 2011-2012  Install ARA in ice station  Install Power/comm hub 2012-2013  Install ARA in ice station  Install autonomous Power/comm hub Large array challenges: Power source Power and communication distribution Drilling (size, depth, drilling time) EMI Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 27

28. Finding the right drill Why it is a big deal for us Finding the right drill Why it is a big deal for us Detector design: Hole diameter impacts antennas design Wet/dry hole Depth possibilities: Shadowing effect  Deeper is better Ice Temperature  Shallower is better Logistics: Drill will have to be moved several times a season Short setup and drilling time Simple operation Cost & schedule: Use existing technologies. Keep it fast, save and simple Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 28

29. Cutter head drill hole-shavings extracted using compressed air Extra compressors required at SP altitude Lots of cargo to get it to the Pole Dry, 4 inch hole Deepest holes achieved: ~60 m in less than 1 hour. Limited by air pressure leakage through the firn Cutter head drill hole-shavings extracted using compressed air Extra compressors required at SP altitude Lots of cargo to get it to the Pole Dry, 4 inch hole Deepest holes achieved: ~60 m in less than 1 hour. Limited by air pressure leakage through the firn This season’s on ice achievements Drill Test 1 : Rapid Air Movement Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 29

30. Carried on three sleds pulled by tractor 0.5 – 1m per minute ( 200m in ~1/2 day ) 6” hole Wet hole- must be pumped out or electronic made watertight Deepest hole drilled ~160 m Carried on three sleds pulled by tractor 0.5 – 1m per minute ( 200m in ~1/2 day ) 6” hole Wet hole- must be pumped out or electronic made watertight Deepest hole drilled ~160 m ARA hot water drill sleds Drill in Operation This season’s on ice achievements Drill Test 2 : Hot water drill Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 30

31. Three different turbines were installed. Measuring and comparing wind speed, power yield. Weather effects to be evaluated next summer. This season’s on ice achievements Wind Turbines Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 31

32. Antennas design: 150-850 MHz Designed to fit in 15cm holes Azimuthal symmetric Cables pass through antenna. No shadowing. 32 ARA’s prototype antennas

33. This is the perfect time South Pole Ice Studies N(z), Atten Askaryan and Simulation Ice Drilling Askaryan effect characteristics Polar operation South Pole EMI/RF environment In ice electronics and hardware design In ice electronics and hardware design 33

34. Ice Properties: Attenuation length Depends on ice temperature. Colder ice at the top. Reflection Studies (2004) (Down to bedrock, 200-700MHz): “normalize” average attenuation according to temperature profile. Besson et al. J.Glaciology, 51,173,231,2005 2 on going “point to point” analyses using NARC/RICE and the new deep pulse. (34 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 34

35. Neutrino interact in ice  showers Charge asymmetry: 20%-30% more electrons than positrons. Moliere Radius in Ice ~ 10 cm: This is a characteristic transverse dimension of EM showers. <<R Moliere (optical), random phases  P  N >>R Moliere (RF), coherent  P  N 2 Hadronic EM Askaryan effect Vast majority of shower particles are in the low E regime dominates by EM interaction with matter Less Positrons: Positron in shower annihilate with electrons in matter e + +e -   Positron in shower Bhabha scattered on electrons in matter e + e -  e + e - More electrons: Gammas in shower Compton scattered on electron in matter e - +   e - +   Many e -,e +,   Interact with matter  Excess of electrons  Cherenkov radiation  Coherent for wavelength larger than shower dimensions 35 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 35

36. Measurements of the Askaryan effect Typical pulse profile Strong <1ns pulse 200 V/m Simulated curve normalized to experimental results Expected shower profiled verified Expected polarization verified (100% linear) Coherence verified. New Results, for ANITA calibration – in Ice Salt Ice D.Salzberg, P. Gorham et al. Were preformed at SLAC (Saltzberg, Gorham et al. 2000-2006) on variety of mediums (sand, salt, ice) 3 Gev electrons are dumped into target and produce EM showers. Array of antennas surrounding the target Measures the RF output Results: RF pulses were correlated with presence of shower 36 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 36

37. 37 Ice Properties: Index Of Refraction RICE Measurements (2004, Down to 150 m, 200MHz-1GHz) Ice Core Measurements (…-1983, down to 237 meters) Kravchenko et al. J.Glaciology, 50,171,2004 1.77 Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 37

38. 38 Ray tracing from pulser to SATRA Source at -250m Bottom antenna -35m Top antenna -5m Depth [m] XY separation [m] surface Direct rays Reflected rays Measured time differences: Time differences between direct rays And between direct and reflected rays can be calculated Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 38

39. 39 SATRA Average envelope WFs For In Ice Pulser events Hole 16, Bottom Hole 16, Top Hole 9, Top Hole 8, Top Hole 9, Bottom Hole 8, Bottom ~44 bins = ~139 ns Simulated results=137 ns Simulated results=14 ns Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 39

40. 40 Based on set of hit time differences between antennas and between primary and secondary hits on the same antenna, a limit on the index of refraction model can be obtained. Systematics taken into account: n_deep, Geometry, timing resolution, WF features n_c n_shallow Hagar LandsmanIceCube RF extension and ARA APS 2011, Anaheim,CA 40