Status report on Double Chooz Amanda Porta for the Double Chooz - - PowerPoint PPT Presentation

status report on double chooz
SMART_READER_LITE
LIVE PREVIEW

Status report on Double Chooz Amanda Porta for the Double Chooz - - PowerPoint PPT Presentation

Status report on Double Chooz Amanda Porta for the Double Chooz collaboration A. Porta, CEA-Saclay Rencontres de Moriond EW 2009 1 Overview 13 measurement at reactors Double Chooz detector and discovery potential Status of the


slide-1
SLIDE 1
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 1

Status report on Double Chooz

Amanda Porta for the Double Chooz collaboration

slide-2
SLIDE 2
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 2

Overview

  • θ13 measurement at reactors
  • Double Chooz detector and discovery potential
  • Status of the detector
slide-3
SLIDE 3
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 3

P(ν

e→ ν e ) = 1 - sin2(2θ 13) sin2(∆ m2 31L/4E)

θ13 measurement at reactors

Nuclear Power Station Near detector Far detector d=400 m 218 ev./day d=1050 m 40 ev./day ν

e,µ ,τ

ν

e

ν

e,µ,τ

115 mwe 115 mwe 300 mwe

1st source of systematic error in CHOOZ: uncertainties on reactor neutrino spectrum

The Double Chooz solution

Near detector Far detector

∆m2

31=2.5 10-3 eV2 ∆m2 31=2 10-3 eV2

Present limit from CHOOZ: R = 1.01 ± 2.8%(stat)± 2.7%(syst) sin2(2θ13) < 0.15 (90% C.L.) at ∆ m2

31 =2.5 10-3 eV2

slide-4
SLIDE 4
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 4

F a r d e t e c t

  • r

Calibration Glove-Box

Outer Veto: plastic scintillator panels ν -Target: 10.3 m3 liquid scintillator doped with 0.1% of Gd γ-Catcher: 22.6 m3 liquid scintillator Buffer: 114 m3 mineral oil with ~400 PMTs Inner Veto: 90 m3 liquid scintillator with 80 PMTs Shielding: 15 cm steel

4 Liquid Volumes

The detectors

Prompt e+ signal Eprompt = Eν -(Mn-Mp)+me Delayed n capture on Gd (τ ~30 ms) with emission

  • f γ cascade (E∼8MeV)
slide-5
SLIDE 5
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 5

Double Chooz sensitivity to θ13

Two phases: 1) Far detector only 10 x CHOOZ statistics sin22θ13<0.06 2) Far + Near detectors Shape Analysis sin22θ13<0.03 Phase 1 σsys=2.6% Phase 2 σsys=0.6%

Error description Absolute

Production cross section 1.9% / Reactor power 2.0% / Energy per fission 0.6% / Solid angle / 0.06% Detection cross Section 0.1% / Target mass 0.2% 0.2% Number of protons 0.5% 0.1% Particle identification 0.4% 0.4%

Realative

sin22θ13

slide-6
SLIDE 6
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 6

Far detector construction (1)

September 08: the steel shielding. November 08: the inner veto tank Dec 08 - Jan 09: painting and cleaning June 08: starting of the work

slide-7
SLIDE 7
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 7

Far detector construction (2)

February 09: the inner veto cleaning .... and the ISO6 tend mounting... ...and the inner veto PMT mounting Presently: Buffer tank installation

slide-8
SLIDE 8
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 8

Future

  • Spring 09: buffer PMT integration
  • Summer 09: acrylic target and γ-catcher integration
  • Autumn 09: DAQ installation and liquid filling
  • First neutrino event @ the end of this year
  • Beginning 2010: outer veto and glove box installation

High precision weight measurement

  • f target liquid
slide-9
SLIDE 9
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 9

Near laboratory

 Site engineering study completed  Starting of construction soon  End of construction middle 2011

slide-10
SLIDE 10
  • A. Porta, CEA-Saclay

Rencontres de Moriond EW 2009 10

Conclusions

  • Double Chooz is the first “new generation” reactor neutrino experiment

using 2 identical detectors

  • We reduce background and errors respect to CHOOZ
  • Far detector under construction
  • First data from far detector at the end of this year

If no oscillation measured: sin22θ 13<0.06 in 1.5 years (90% C.L.)

  • Data taking with far + near detectors from 2011

If no oscillation measured: sin22θ 13<0.03 in 3 years (90% C.L.)