EXO-200 and nEXO - vip-doll.ru August/Session 21.08 A/34_talk-belov.pdf · EXO-200 and nEXO...

30
EXO-200 and nEXO Vladimir Belov, ITEP & MEPhI for EXO-200 and nEXO collaborations 17 th Lomonosov Conference, Moscow, 21 August 2013

Transcript of EXO-200 and nEXO - vip-doll.ru August/Session 21.08 A/34_talk-belov.pdf · EXO-200 and nEXO...

Page 1: EXO-200 and nEXO - vip-doll.ru August/Session 21.08 A/34_talk-belov.pdf · EXO-200 and nEXO Vladimir Belov, ITEP & MEPhI for EXO-200 and nEXO collaborations 17th Lomonosov Conference,

EXO-200 and nEXO

Vladimir Belov, ITEP & MEPhIfor EXO-200 and nEXO

collaborations

17th Lomonosov Conference, Moscow, 21 August 2013

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21.08.2015 V.Belov EXO-200 and nEXO 2

2ν mode: a conventional 2nd order process in Standard Model

0ν mode: a hypothetical process can happen only if: <mν> ≠ 0, ν = ν |ΔL|=2, |Δ(B-L)|=2

Simulated double beta decay spectrumP.Vogel. arXiv:hep-ph/0611243

To reach high measurement sensitivity for 0ν mode one requires, • High energy resolution• Large Isotope mass• Low background

Double beta decay

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21.08.2015 V.Belov EXO-200 and nEXO 3

Energy resolution is poorer than the crystalline devices (~ factor 10), but...Monolithic detector. Xenon can form detection medium, allow self shielding,

surface contamination minimized. Very good for large scale detectors.Has high Q value. Located in a region relatively free from natural

radioactivity.Isotopic enrichment is easier. Xe is already a gas & 136Xe is the heaviest

isotope.Xenon is “reusable”. Can be purified & recycled into new detector (no crystal

growth). Minimal cosmogenic activation. No long lived radioactive isotopes of Xe.Energy resolution in LXe can be improved. Scintillation light/ionization

correlation.Particle identification. Slightly limited, but can be used to tag alphas from Rn

chain.

… admits a novel coincidence technique. Background reduction by Ba daughter tagging.

Why xenon

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21.08.2015 V.Belov EXO-200 and nEXO 4

80.6% 136Xe T = 167 KP = 147 kPaρ = 3.0 g/cm3

High purity HFE7000 > 50 cm

25 cm

EXO-200 detector

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21.08.2015 V.Belov EXO-200 and nEXO 5

The EXO-200 TPC

• Field shaping rings: copper• Supports: acrylic• Light reflectors/diffusers: Teflon• APD support plane: copper; Au (Al) coated

for contact (light reflection)• Central cathode, U+V wires: photo-etched

phosphor bronze• Flex cables for bias/readout: copper on

kapton, no glue

Comprehensive material screening program

• 38 U triplet wire channels (charge)

• 38 V triplet wire channels, crossed at 60o (induction)

• 234 large area avalanche photodiodes (APDs, light in groups of 7)

• Wire pitch 3 mm (9 mm per channel)

• Wire planes 6 mm apart and 6 mm from APD plane

• All signals digitized at 1 MS/s, ±1024S around trigger

• Drift field 376 V/cm

40 cm40 cm

Two almost identical halves reading ionization and 178 nm scintillation, each with:

xz

y

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21.08.2015 V.Belov EXO-200 and nEXO 6

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21.08.2015 V.Belov EXO-200 and nEXO 7

● Signal finding. Digital filters are used on waveforms from U,V wires and APDs● Parameters of pulses (t, E) are estimated for both charge and light● Pulses are combined into clusters producing position, multiplicity (SS or MS) and energy.● Position is used in form of Standof Distance (SD) that is distance from any cluster to the nearest wall

Event reconstruction

V-wire signalsV-wire signals

U-wire signalsU-wire signals

APD signalsAPD signals

Charge clustersCharge clusters

Scintillation clustersScintillation clusters

Linked

tu

β

γ

SingleSiteEvents(SS)

tu

γ

MultipleSiteEvents(MS)

Efficiency to get into SS: 2β0ν ~90%γ 2.5MeV ~30%

But we don’t throw MS events away! We use them in the fit to help predict background

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21.08.2015 V.Belov EXO-200 and nEXO 8

APD denoising

1.53 % in SS at 0νββ Q-value

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21.08.2015 V.Belov EXO-200 and nEXO 9

Rotation angle chosen to optimize energy resolution at 2615 keV

Properties of xenon cause increased scintillation to be associated with decreased ionization (and vice-versa)

E. Conti et al. Phys. Rev. B 68 (2003) 054201

Use projection onto a rotatedaxis to determine event energy

Combining ionization and scintillation

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21.08.2015 V.Belov EXO-200 and nEXO 10

We used gamma sources Cs, Co, Th, Ra

Energy resolution model

Resolution is dominated by by constant term (noise)

At Qββ (2458 keV):σ/Ε = 1.53 % (SS)σ/Ε = 1.65 % (MS)

Energy calibration

Data with sources is fitted by model PDFs SS/MS ratio agrees with 10% accuracy Measured source activity is 4% accurate

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21.08.2015 V.Belov EXO-200 and nEXO 11

Data takingC

um

ula

tive

live

tim

e [d

ays]

Previous results

Accumulation of data in science «Run 2» from Oct'2011 till Sep'2013.«Golden» data is 447.60 ± 0.01 days livetimeThat corresponds to 100 kg y in⋅ 136Xe exposure.

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21.08.2015 V.Belov EXO-200 and nEXO 12

2β0ν measurement

Single site

Multi site

Efficiency to 2β events85 %

Full livetime477.6 d100.0 kg y

2β events~37000

The lowest background index among comparable detectorsBI = 1.7 ± 0.2 × 10-3 keV-1 kg-1 y-1

[Nature 510, 229 (2014)]

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13

2β0ν measurement

T1/20νββ > 1.1 x 1025 yr

〈 mββ 〉 < 190 – 450 meV (90% C.L.)

[Nature 510, 229 (2014)]

Pro

file

likel

ihoo

d

Backgrounds in ± 2σ ROI

Th chain 16.0

U chain 8.1

Xe-137 7.0

Total 31.1 ± 3.8

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21.08.2015 V.Belov EXO-200 and nEXO 14

Comparison of 2β0ν

EXO-200:Nature 510, 229 (2014)

GERDA Phase 1: PRL 111 (2013) 122503

KamLAND-Zen:PRL 110 (2013) 062502 KK&K Claim:Mod. Phys. Lett., A21 (2006) 1547

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21.08.2015 V.Belov EXO-200 and nEXO 15

Searching for majoron

Phys.Rev D90 9, 092004 (2014)

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21.08.2015 V.Belov EXO-200 and nEXO 16

EXO-200 results● Operated a 100 kg scale LXe TPC for 2 years● Discovered a double beta decay of 136Xe● Made the most precise measurement of its halflife● Measured residual backgrounds are very low● Reached design (anticorrelated) energy resolution, σ/E(Q)=1.5%● Achieved stable electron lifetime of ~3 ms or better● Utilized self-shielding in monolithic detector● Demonstrated power of β/γ discrimination (SS/MS)

● Implemented novel detector solutions and analysis techniques● 500 LAAPDs for VUV (175 nm) scintillation detection● Photo- etched, charge collection wires, cathode, and fasteners● Epoxy- poned, kapton flat cable feedthroughs● HFE- 7000 thermal bath and radiation shield● Ultra- light design, no solder joints

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21.08.2015 V.Belov EXO-200 and nEXO 17

nEXO concept

● 5 tonnes of enriched LXe● Monolithic design dramatically improves

performance with size● Using enhanced self- shielding● x100 better T

1/2 sensitivity

● < 1% energy resolution● no central cathode● *no* Ba tagging (initially)

Conceptual design for SNOLab150 kg

5000 kg

2.5MeV γ attenuation length (8.5cm)

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21.08.2015 V.Belov EXO-200 and nEXO 18

nEXO R&D: TPC

Charge readout tiles

Silicon Photo Multipliers

TCP: ~ 1.3 m x 1.3 m

Key features:● single drift volume● thin Copper or Carbon vessel● minimal use of plastics● charge collected by pads on top● 10 ms electron lifetime● scintillation collected by SIPMs on side barrel behind the field cage● VUV reflection● Optimization of fiducial volume

nEXO R&D in full swing

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21.08.2015 V.Belov EXO-200 and nEXO 19

nEXO R&D: Charge• Charge readout structures on low background substrates• SS/MS discrimination (readout pitch)● No tension and microphonics (not wires)

Prototype Charge Readout Quartz Tile LXe Test Apparatus

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21.08.2015 V.Belov EXO-200 and nEXO 20

nEXO R&D: Light• High light collection efficiency (>15% at 175 nm)• Ultra‐low background (~ppt levels for Th & U)• VUV sensitive SiPMs from FBK, Hamatsu, Ketek or Hamamatsu MEG devices or Wave-Length-Shifters• Already measuring samples

FBK SiPMs, 1st gen Hamamatsu MEG

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21.08.2015 V.Belov EXO-200 and nEXO 21

nEXO R&D: Electronics• Cold electronics close to the detector• improve energy resolution to 1%• low background, low noise• keep required power low enough• deliver all the signals without much loss• multiplexing to reduce cabling/feedthroughs

Cold charge readout ASIC Prototype circuit for SiPMs

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21.08.2015 V.Belov EXO-200 and nEXO 22

EXO-200 and nEXO projected sensitivities

Combining all ourexperience and thebest technologies

we plan

T1/2

= 6 · 1027 yr

in 5 years of

counting

Majorana

neutrino mass

<mββ

> sensitivity

of 7- 18 meV

nEXO is an active international R&D program for a x100 the sensitivity of EXO- 200!

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University of Alabama, Tuscaloosa AL, USA - T. Didberidze, M. Hughes, A. Piepke, R. TsangUniversity of Bern, Switzerland - S. Delaquis, R. Gornea, T. Tolba, J-L. Vuilleumier California Institute of Technology, Pasadena CA, USA - P. Vogel Carleton University, Ottawa ON, Canada - V. Basque, M. Dunford, K. Graham, C. Hargrove, R. Killick, T. Koffas, C. Licciardi, D. SinclairColorado State University, Fort Collins CO, USA - C. Chambers, A. Craycraft, W. Fairbank, Jr., T. WaltonDrexel University, Philadelphia PA, USA - M.J. Dolinski, Y.H. Lin, E. Smith, Y.-R YenDuke University, Durham NC, USA - P.S. BarbeauIHEP Beijing, China - G. Cao, W. Cen, X. Jiang, L. Wen, J. ZhaoUniversity of Illinois, Urbana-Champaign IL, USA - D. Beck, M. Coon, S. Homiller, J. Ling, J. Walton, L. Yang Indiana University, Bloomington IN, USA - J. Albert, S. Daugherty, T. Johnson, L.J. Kaufman, T. O’ConnerUniversity of California, Irvine, Irvine CA, USA - M. MoeITEP Moscow, Russia - V. Belov, A. Burenkov, M. Danilov, A. Dolgolenko, A. Karelin, A. Kuchenkov, V. Stekhanov, O. ZeldovichLaurentian University, Sudbury ON, Canada - B. Cleveland, A. Der Mesrobian-Kabakian, J. Farine, B. Mong, U. WichoskiUniversity of Maryland, College Park MD, USA - C. Davis, C. Hall University of Massachusetts, Amherst MA, USA - J. Abdollahi, S. Feyzbakhsh, S. Johnston, A. Pocar, D. ShyIBS Center for Underground Physics, Daejeon, South Korea - D.S. LeonardSLAC National Accelerator Laboratory, Menlo Park CA, USA - M. Breidenbach, R. Conley, T. Daniels, J. Davis, A. Dragone, K. Fouts, R. Herbst, A. Johnson, K. Nishimura, A. Odian, C.Y. Prescott, A. Rivas, P.C. Rowson, J.J. Russell, K. Skarpaas, M. Swift, A. Waite, M. WittgenUniversity of South Dakota, Vermillion SD, USA, – R. MacLellanStanford University, Stanford CA, USA - T. Brunner, J. Chaves, R. DeVoe, D. Fudenberg, G. Gratta, M. Jewell, S.Kravitz, D. Moore, I. Ostrovskiy, A. Schubert, K. Twelker, M. WeberStony Brook University, SUNY, Stony Brook, NY, USA – K. Kumar, O. Njoya, M. TarkaTechnical University of Munich, Garching, Germany - W. Feldmeier, P. Fierlinger, M. MarinoTRIUMF, Vancouver BC, Canada – J. Dilling, R. Krücken, F. Retière, V. Strickland

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21.08.2015 V.Belov EXO-200 and nEXO 24

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21.08.2015 V.Belov EXO-200 and nEXO 25

What else from EXO-200?

Following 2 accidents at the WIPP mine, EXO- 200 personnel is

now granted regular access to the site and recovery operations

are ongoing

● EXO-200 can still contribute to the leading set of experiments

● Upgrades had bee installed before the accident:● Radon suppression system for air around the detector● Upgraded electronics (could get to 1% energy resolution)

● Approx. 2 years of data are still being worked on:● Cosmogenic backgrounds● Gamma, beta and alpha backgrounds

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Efficiency to 2β 58 % (87 %)

Full exposure127.6 сут23.14 кг л

2β events18984

Reanalyzed Run 2a data from (PRL 109, 032505, 2012)

2β2ν measurementThe most precise measurement of halflife of any isotope to date

T1/22νββ = 2.165 ± 0.016(stat) ± 0.059(sys) × 1021 yr

[PRC 89, 015502 (2014)]total relative uncertainty 2.85%

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21.08.2015 V.Belov EXO-200 and nEXO 27

Xenon purity

Непрерывная циркуляция ксенона через высокотемпературные очистители SAES с использованием специально сконструированного насоса.

Neilson et al. (2011) arXiv:1104.5041v1

Среднее время жизни электрона ~3 мс обеспечивает на максимальном времени дрейфа 110 мкс уменьшение сигнала <3%.

Восстановление после остановок занимает несколько дней

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21.08.2015 V.Belov EXO-200 and nEXO 28

nEXO expected backgrounds and signalsSimulated nEXO spectrum near single-site ROI:

Full 4.8 tonnes, 5 yr

Central 1 tonneonly, 5 yr

T1/20νββ=

1.8·1027 yr

● Have developed Geant4 simulation for nEXO, using experience gained from EXO-200

● Spectra on right show expected backgrounds in 5 yr exposure, and 0νββ at discovery threshold

● Background calculation assumes measured activity for detector materials

● This procedure was verified with EXO-200 data, and assumes several improvements for nEXO

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21.08.2015 V.Belov EXO-200 and nEXO 29

Ba tagging

2448 keV214Bi

2615 keV208Tl

Simulated nEXO spectrum near single-site ROI:

Full 4.8 tonnes, 5 yr

● In addition, R&D to develop techniques to identify Ba daughter nucleus of 0νββ decay (“Ba tagging”) is continuing

● Candidate 0νββ events would be identified in real time and daughter Ba ion collected by probe inserted into the TPC at the decay location

● Identity of Ba daughter can be confirmed spectroscopically

•This technology would eliminate all non-ββ backgrounds near ROI•Could extend ultimate reach of nEXO into the normal hierarchy since full 5 tonne mass would be background free

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21.08.2015 V.Belov EXO-200 and nEXO 30

Ba tagging

Twelker et al., arXiv:1407.0618

Several techniques are currently being pursued:

• Tagging from solid Xe by fluorescence spectrum

• Resonance ionization spectroscopy (RIS):

• Also studying ion extraction and tagging from high pressure Xe gas

389.7 nm553.5 nm1064 nm

To Time of FlightSpectrometer

Ba+

Wavelength (nm)

Typical time of flight spectrum:

Fluorescence of Ba in SXe:

Excited by 558 nm laser

<128 atoms

<28 atoms<18 atoms

<6 atoms

Cold probe

Solid Xe

Liquid Xe Ba+

Detect single ion or atom on the probe with

laser-induced fluorescence

Co

un

ts