Multi-PMT Optical Module Designs for IceCube-Gen2

Similar documents
Muon track reconstruction and veto performance with D-Egg sensor for IceCube-Gen2

Muon track reconstruction and veto performance with D-Egg sensor for IceCube-Gen2

PoS(ICRC2017)1052. Overview and Performance of the Wavelength-shifting Optical Module (WOM) The IceCube-Gen2 collaboration

PoS(PD07)031. General performance of the IceCube detector and the calibration results

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2)

PoS(ICRC2015)1106. GEANT4 simulation of optical modules in neutrino telescopes. Christophe M.F. Hugon

Aspects of the optical system relevant for the KM3NeT timing calibration

Search for a diffuse cosmic neutrino flux with ANTARES using track and cascade events

From DeepCore to PINGU

Particle Physics Beyond Laboratory Energies

Determination of parameters of cascade showers in the water calorimeter using 3D-distribution of Cherenkov light

PoS(EPS-HEP2017)008. Status of the KM3NeT/ARCA telescope

KM3NeT-ARCA project status and plan

PoS(ICRC2015)568. An Estimate of the Live Time of Optical Measurements of Air Showers at the South Pole

Status and Perspectives for KM3NeT/ORCA

PoS(ICRC2017)945. In-ice self-veto techniques for IceCube-Gen2. The IceCube-Gen2 Collaboration

arxiv: v1 [hep-ex] 20 Jan 2016

PoS(NEUTEL2015)056. Neutrino mass hierarchy with PINGU

IceCube. francis halzen. why would you want to build a a kilometer scale neutrino detector? IceCube: a cubic kilometer detector

Detecting Stopping Track Muons with the IceCube Neutrino Observatory

Muon Reconstruction in IceCube

High Energy Neutrino Astronomy

Results from the ANTARES neutrino telescope

PoS(NOW2016)041. IceCube and High Energy Neutrinos. J. Kiryluk (for the IceCube Collaboration)

Status of the KM3NeT Project. Oleg Kalekin Astroparticle Physics Workshop Baikal, Ulan-Ude Maksimiha

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory

Oscillations on Ice Tyce DeYoung Department of Physics Pennsylvania State University Exotic Physics with Neutrino Telescopes Marseilles April 5, 2013

A method of observing Cherenkov light at the Yakutsk EAS array

IceCube Results & PINGU Perspectives

PoS(ICRC2015)1155. Design study of an air-cherenkov telescope for harsh environments with efficient air-shower detection at 100 TeV.

An autonomous underwater telescope for measuring the scattering of light in the deep sea

IceAct Air Cherenkov telescopes for the South Pole

THE KM3NET NEUTRINO TELESCOPE IN THE MEDITERRANEAN SEA

Dept. of Physics and Astronomy, Michigan State University, 567 Wilson Rd., East Lansing, MI 48824, USA

IceCube: Dawn of Multi-Messenger Astronomy

Correlation between the UHECRs measured by the Pierre Auger Observatory and Telescope Array and neutrino candidate events from IceCube

neutrino astronomy francis halzen University of Wisconsin

Neutrino Astronomy. Ph 135 Scott Wilbur

Wavelength Shifters as (new) light sensors

Neutrino Radiography of the Earth with the IceCube Neutrino Observatory

PoS(TIPP2014)033. Upgrade of MEG Liquid Xenon Calorimeter. Ryu SAWADA. ICEPP, the University of Tokyo

Results of the search for magnetic

Status of the BAIKAL-GVD Project

THE EHE EVENT AND PROSPECTS FROM THE ICECUBE NEUTRINO OBSERVATORY. Lu Lu 千葉大

neutrino astronomy francis halzen university of wisconsin

Neutrino Mass Hierarchy and other physics in H 2 0 (ORCA & PINGU) Aart Heijboer Nikhef, Amsterdam, KM3NeT collaboration

arxiv: v1 [physics.ins-det] 3 Feb 2011

KM3NeT. P. Piattelli, INFN SciNeGHE 2010, Trieste, september

Measurement of High Energy Neutrino Nucleon Cross Section and Astrophysical Neutrino Flux Anisotropy Study of Cascade Channel with IceCube

Gustav Wikström. for the IceCube collaboration

arxiv: v1 [astro-ph.he] 28 Jan 2013

Radioactivity measurements for the ERMES project at the STELLA facility

PoS(ICRC2015)641. Cloud Monitoring using Nitrogen Laser for LHAASO Experiment. Z.D. Sun 1,Y. Zhang 2,F.R. Zhu 1 for the LHAASO Collaboration

Neutrino Oscillation Tomography

NEUTRINO ASTRONOMY AT THE SOUTH POLE

PoS(Texas 2010)235. KM3NeT: A km 3 -scale neutrino telescope in the Mediterranean Sea. Véronique Van Elewyck, for the KM3NeT Consortium

The Cosmic Ray Air Fluorescence Fresnel lens Telescope (CRAFFT) for the next generation UHECR observatory

Frederick Reines and Clyde Cowan report the first direct evidence for neutrinos.

Long-term stability plastic scintillation for LHAASO-KM2A

Design studies for a neutrino telescope based on optical fiber hydrophones

Radiation (Particle) Detection and Measurement

Hands on Project: Large Photocathode PMT Characterization

Astroparticle Physics

Neutrino Astronomy fast-forward

Progress and latest results from Baikal, Nestor, NEMO and KM3NeT

Thin Calorimetry for Cosmic-Ray Studies Outside the Earth s Atmosphere. 1 Introduction

XMASS 1.5, the next step of the XMASS experiment

PoS(EPS-HEP2015)068. The PINGU detector

Origin of Cosmic Rays

High energy neutrino astronomy with the ANTARES Cherenkov telescope

(Towards) a km 3 detector in the Mediterranean Sea

KM3NeT and Baikal-GVD New Northern Neutrino Telescopes

Simulations for H.E.S.S.

STATUS OF ATLAS TILE CALORIMETER AND STUDY OF MUON INTERACTIONS. 1 Brief Description of the ATLAS Tile Calorimeter

PoS(ICHEP2016)474. SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor

KM3NeT. Astro-particle and Oscillations Research with Cosmics in the Abyss (ARCA & ORCA)

Particle Physics with Neutrino Telescope Aart Heijboer, Nikhef

IceCube & DeepCore Overview and Dark Matter Searches. Matthias Danninger for the IceCube collaboration

Measurements of Liquid Scintillator Light Yield for Future Neutrino Experiments

Symmetries and in-medium effects

X- & γ-ray Instrumentation

Indirect detection of Dark Matter with the ANTARES Neutrino Telescope

Shoei NAKAYAMA Kamioka Observatory, Institute for Cosmic Ray Research, The University of Tokyo

PoS(TIPP2014)073. Development of a High Detection Efficiency and Low-Cost Imaging Gamma-Ray Camera γi. M. Kagaya

The Pierre Auger Observatory Status - First Results - Plans

Search for diffuse cosmic neutrino fluxes with the ANTARES detector

Search for the Sources of High Energy Astrophysical Neutrinos with VERITAS

The new Siderius Nuncius: Astronomy without light

The KM3NeT Multi-PMT Digital Optical Module

PoS(PhotoDet 2012)010

High Energy Neutrino Astrophysics Latest results and future prospects

Timing calibration of the LHAASO-KM2A electromagnetic particle detectors

XMASS: a large single-phase liquid-xenon detector

Mediterranean Neutrino Telescopes

Multi-messenger studies of point sources using AMANDA/IceCube data and strategies

arxiv: v1 [astro-ph.im] 14 Aug 2015

Seminar. Large Area Single Photon Detectors

Compton Camera. Compton Camera

Chapter 4 Scintillation Detectors

Search for GeV neutrinos associated with solar flares with IceCube

Transcription:

EPJ Web of Conferences 116, 01001 (2016) DOI: 10.1051/epjconf/201611601001 C Owned by the authors, published by EDP Sciences, 2016 Multi-PMT Optical Module Designs for IceCube-Gen2 Alexander Kappes a Erlangen Centre for Astroparticle Physics, Friedrich-Alexander-Universität Erlangen-Nürnberg, 91058 Erlangen, Germany Abstract. IceCube-Gen2 is the planned next generation neutrino telescope at the South Pole incorporating a high-energy array for neutrino astronomy and a dense array (PINGU) aimed at the determination of the neutrino mass hierarchy. Here, we present alternative designs to IceCube-Gen2 s single-pmt baseline optical module which are currently being developed. These designs feature up to 24 smaller photomultipliers and use glass and gel with enhanced UV transparency to increase the number of detected photons and provide additional information. Thereby, they have the potential to significantly enhance the performance of IceCube-Gen2. 1. Introduction The design of the Digital Optical Module (DOM) used in the IceCube detector [1] has proven to be highly reliable and, thereby, has played a key role in providing the high-quality data that enabled the recent discovery of high-energy cosmic neutrinos [2]. For the next-generation neutrino telescope in the deep ice at the South Pole, IceCube-Gen2, about 10,000 additional optical sensors will be deployed. These are required to operate reliably without maintenance over the full livetime of the detector of 10+ years at depths down to 2,700 m with pressures up to 550 bar 1 and temperatures down to 45 C.In view of these harsh environmental conditions, the baseline design for IceCube-Gen2 is an advancement of the successful IceCube-DOM design. While all parts exposed to the high pressure are retained, developments in recent years allow to significantly simplify the readout electronics, thereby reducing complexity and power consumption [3]. Like the original DOM, this new design features a single large 10" photomultiplier (PMT) pointing downwards, resulting in a very asymmetric angular acceptance. In particular, in view of the recent success in observing cosmic neutrinos from the Southern hemisphere [2], i.e. detecting events entering the detector from above, this strongly downward peaked sensitivity is an undesirable feature 2.In addition, the single-pmt design doesn t provide any information on the arrival directions of the detected photons, and the absorption of photons by the current DOM glass increases rapidly as the wavelength of a e-mail: kappes@icecube.wisc.edu 1 This pressure is reached during freeze-in. 2 In fact, the IceCube DOM also has some sensitivity to photons produced above the optical module due to backscattering in the ice. However, scattered photons lose directional information on their origin. This is an Open Access article distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

EPJ Web of Conferences Figure 1. Renderings of the D-Egg (left, taken from [4]) and mdom (right) concepts for IceCube-Gen2. In case of the latter, the top part of the black PMT holding structure visible in the lower half has been removed. photons decreases below 400 nm, thereby losing the UV photons from the Cherenkov spectrum which rises with 1/λ 2. Therefore, in parallel to the development of this baseline design, new detector concepts are being explored that aim at improving on these and other features. Two of them are the so-called D-Egg [4] and mdom [5] concepts which use multiple PMTs and glass with improved UV transparency. Another concept, discussed in [6], uses large surfaces of wavelength shifters to significantly enhance the number of detected photons at low costs. 2. The D-Egg and mdom concepts The idea of optical sensors with multiple PMTs was first proposed in 1979 in the framework of the DUMAND project [7]. The D-Egg concept, depicted in Fig. 1 left, incorporates two oppositely oriented 8" PMTs (R5912-100 HQE) housed in an ellipsoidal pressure vessel. At its widest part, the pressure vessel measures 300 mm ( 12") and, hence, is about 1" narrower than the standard IceCube DOM. This allows for drilling narrower holes into the ice, thereby saving fuel costs and drilling time. First pressure tests up to 700 bar including penetrator, a dummy PMT and optical gel were successful. The observed bubble formation in the gel is under investigation. The glass of the pressure vessel as well as the optical gel for coupling the PMTs to the glass have been developed to provide increased UV transparency. For readout of each PMT, the analog waveforms will be continuously sampled with a fast ADC. The mdom concept (Fig. 1 right), which is based on the KM3NeT optical module [8], pushes the multi-pmt concept even further and incorporates 24 3" PMTS (HamamatsuR12199-02) into a pressure vessel of 358 mm (14") diameter. The large number of PMTs allows to gain information on the direction of a light source already on the single module level and coincidences between PMTs can, e.g, be used for suppression of background. Each PMT has a base attached to it that, in addition to containing electronics that generates the high voltage via a Cockcroft Walton circuit 3, performs advanced signal processing. For readout of the 24 PMTs, a multi-level comparator design with up to 63 thresholds is envisioned which samples the signal of each PMT already on the PMT base. Each comparator will provide the leading-edge time and the time over threshold. 3 Developed by Nikhef for the KM3NeT optical module. 01001-p.2

Very Large Volume Neutrino Telescope (VLVnT-2015) Figure 2. Transmissivity of different pressure vessel glasses as function of wavelength. The measurement for the D-Egg and mdom glasses were performed in air and losses due to reflection deducted. For illustrative purposes, the 1/λ 2 Cherenkov spectrum is also shown with an arbitrary scale. 2.1 UV sensitivity Due to the Cherenkov spectrum increasing with 1/λ 2, already minor extensions of the sensitivity to shorter wavelengths increases the number of detected photons significantly. The achievable gain is weakened by the fact that both scattering and absorption length rise below 400 nm. However, a sizable gain remains even for larger distances between photon source and optical module. For the IceCube DOM, the limiting factor here is the transmissivity of the pressure vessel which starts to significantly absorb photons already at 400 nm (see Fig. 2) and reaches 50% transmissivity around 345 nm. The glass of the D-Egg, specifically developed to provide better UV transparency by reducing its Fe 2 O 3 concentration, features a significantly lower cutoff wavelength and reaches 50% around 320 nm. In particular, it also maintains its maximum transmissivity to much lower wavelengths. The mdom glass, which is the standard glass used by the manufacturer (NAUTILUS Marine Service GmbH) for their deep-see pressure vessels, reaches 50% transmissivity around 330 nm, thereby being only slightly worse than the special UV-transparent glass. Both glasses therefore represent attractive alternatives to the one used in the current optical modules. Their contamination with radioactive elements still needs to be determined carefully though, as this has a large impact on the dark count rate of the PMTs in the otherwise very radioactive pure environment in the deep ice. 2.2 Effective areas In addition to an increased UV transparency, both new concepts also feature increased photocathode area (D-Egg: 2 320 cm 2 = 640 cm 2 ; mdom: 24 50 cm 2 = 1200 cm 2 ) compared to the current IceCube DOM with 500 cm 2. Also, both the Gen2 baseline design and the D-Egg concept foresee the usage of super-bialkali photocathode material which provides up to 20% higher photon detection efficiency. Whether this also poses a cost-effective option for the 3" PMTs used in the mdom has to be evaluated. Figure 3 shows the effective areas for the D-Egg and mdom concepts including quantum efficiency. Compared to the single-pmt baseline design (not shown), the D-Egg shows a significantly reduced angular dependence with a maximum reduction of about 20%. Owing to its large number of PMTs, the mdom features an even more uniform angular acceptance with a maximum variation of 01001-p.3

EPJ Web of Conferences cosθ 1.0 ] 2 Effective area [cm 100 80 60 40 20 0 300 350400450 wavelength [nm] 500 550600650 0 20 40 60 80100120140160180 zenith angle θ [ ] 0.8 0.6 0.4 0.2 0.0 0.2 0.4 0.6 0.8 1.0 310 nm 470 nm 320 nm 380 nm PRELIMINARY Figure 3. Left: Effective area of the D-Egg including PMT quantum efficiency as a function of wavelength for different photon zenith angles (module orientation as in Fig. 1 left). Taken from [4]. Right: Hammer projection of the mdom photon acceptance including PMT quantum efficiency represented as effective area as a function of direction of the incident photons in zenith and azimuth angle (module orientation as in Fig. 1 right). Values are shown for different photon wavelengths. Due to the symmetry in the orientation of the PMTs, each shown quadrants is representative of the total solid angle for the respective wavelength. 12%. Both new concepts therefore improve significantly on the amount of effective area per optical module and its uniformity in solid angle. Detailed measurements and simulations currently underway will allow to quantify the impact of these improvements on the detector performance. 3. Conclusions Parallel to the advancement of the proven IceCube DOM design, several alternative designs for the next generation neutrino telescope at the South Pole, IceCube-Gen2, are being investigated. These designs improve on several aspects of the Gen-2 baseline design, in particular the uniformity of the angular acceptance and the overall photon acceptance. The aim is to develop prototypes within the next two years which can be tested under real conditions in the deep ice at the South Pole in advance of the installation of the actual IceCube-Gen2 detector. A first mechanical design for both sensor types has been completed and the development of specific read-out electronics has commenced. Conceptual prototypes are planned for 2016. Simulations currently undertaken address the impact of the utilization of the new module concepts on the performance of IceCube-Gen2 which is expected to benefit from the increased effective area and superior information on the recorded photons. In the end, a combination of different module types may turn out to be most effective. References [1] F. Halzen, S.R. Klein, Rev. Sci. Instrum. 81, 081101 (2010), arxiv:1007.1247 [2] M. Aartsen et al. (IceCube), Phys. Rev. Lett. 113, 101101 (2014), arxiv:1405.5303 [3] M.G. Aartsen et al. (IceCube-Gen2), Generation 2 IceCube Digital Optical Module and DAQ, in Proc. of the 34th International Cosmic Ray Conference (The Hague, The Netherlands, 2015), [4] M.G. Aartsen et al. (IceCube-Gen2), A dual-pmt optical module (D-Egg) for IceCube-Gen2, in Proc. of the 34th International Cosmic Ray Conference (The Hague, The Netherlands, 2015), 01001-p.4

Very Large Volume Neutrino Telescope (VLVnT-2015) [5] M.G. Aartsen et al. (IceCube-Gen2), Multi-PMT optical modules for IceCube-Gen2, in Proc. of the 34th International Cosmic Ray Conference (The Hague, The Netherlands, 2015), [6] D. Hebecker, A wavelength-shifting optical module (WOM) for in-ice neutrino detectors, these proceedings [7] V.V. Borog et al., Measuring module for registration of Cherenkov radiation in the water, inproc. of the 16th International Cosmic Ray Conference (1979), Vol. 8, p. 380 [8] H. Löhner et al. (KM3NeT), Nucl. Inst. Meth. A718, 513 (2013) 01001-p.5