{ Precision measurements of the beta neutrino correlation in the WI Electrostatic Ion Trap 3...

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{ { Precision measurements of the Precision measurements of the beta neutrino correlation in beta neutrino correlation in the WI Electrostatic Ion Trap the WI Electrostatic Ion Trap Sergey Vaintraub

Transcript of { Precision measurements of the beta neutrino correlation in the WI Electrostatic Ion Trap 3...

Page 1: { Precision measurements of the beta neutrino correlation in the WI Electrostatic Ion Trap 3 December 2012 Sergey Vaintraub.

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Precision measurements of the beta Precision measurements of the beta neutrino correlation in the WI neutrino correlation in the WI

Electrostatic Ion TrapElectrostatic Ion Trap

Sergey Vaintraub

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Where to search for beyond SM Physics?

Sergey Vaintraub

Brute force (“Swifter, Higher, Stronger”):•Go higher in energy/luminosity• LHC/Tevatron/ILC

Finesse:•High precision experiments•Detect the effect of beyond SM on low energy observables•For example βν correlation measurements

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6Li daughter nucleus e- Electron

eElectron anti-neutrino

New physics beyond the Standard Model’s V-A structure

Pure Gamow-Teller

6He beta decay

Sergey Vaintraub

βν correlation

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Trap chamber

30o

magnet

Neutron generator

EIBT

1 m

Setup scheme

Sergey Vaintraub

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Electrons detector

MCP MCP

Entrance mirrorExit mirror

Electrons collected at position sensitive plastic scintillator6Li ions collected at MCP detectors

6Li+

+

e-

6He beta decay at EIBT

Sergey Vaintraub

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Electrons detector

MCP MCP

Entrance mirrorExit mirror

Some of 6Li ions will miss MCP at its periphery

6Li+

+

e- -

e and are in the same direction, hence momentum of recoiling 6Li is maximum AND in the opposite direction.

Sergey Vaintraub

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Electrons detector

MCP MCP

Entrance mirrorExit mirror

Some of 6Li ions will go though MCP hole

6Li+

+

e-

-

e and are in opposite directions, hence momentum of recoiling 6Li is small.

Sergey Vaintraub

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Losses Mechanisms

Sergey Vaintraub

e

e

eSM E

pHedW cos

3

11)(6

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Statistical precision

In order to go below 1% statistical precision one should accumulate about one million coincidences Sergey Vaintraub

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Present SetupPresent Setup

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DT-NGfurnace

300 magnet

EBIT Beam optics

7 m

Trap chamber

Setup StatusSetup StatusSetup StatusSetup Status

A. Neutron GeneratorA. Neutron Generator

DT-NG

D + T → n + 4He   En = 14.2 MeV, Production rate~1010 n/s Ordered from VNIIA (Russia).

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DT-NGfurnace

300 magnet

EBIT Beam optics

7 m

Trap chamber

Setup StatusSetup StatusSetup StatusSetup Status

B. Furnace + BeO targetB. Furnace + BeO target

• The 14 MeV neutrons hit a hot (1500K) BeO target, as a result , 6He nuclei are produced.

• Ordered from HeatWave (USA). (ETA - Winter 2011).Porous BeO 80 mm x 2 mm discs delivered and stored

6He

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DT-NGfurnace

300 magnet

EBIT Beam optics

7 m

Trap chamber

Setup StatusSetup StatusSetup StatusSetup Status

C. Accumulator and BuncherC. Accumulator and Buncher

EBIT - DREBIT (Dresden, Germany)

Neutral 6He enter the EBIT, ionized, accumulated and bunched.

Custom made for efficient 6He injection

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DT-NGfurnace

300 magnet

EBIT Beam optics

7 m

Trap chamber

Setup StatusSetup StatusSetup StatusSetup Status

D. Trap ChamberD. Trap Chamber Stable isotopes trapping Detectors:

MCP’s Plastic Scintillator with

multiple photomultipliers

Electronics – ADC, TDC,…

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Summary

Sergey Vaintraub

Present setup offers significant advantages over other schemes:

• Large solid angle for recoils and electrons.

• Field-free inner region.

• Full reconstruction of the e-ν angle.

• Ease-of-operation and portability. • Complementary to other methods (different systematic errors)

• “Continuous” operation (no “beam time”…)

• Easily adapted for other radioactive species.

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Collaborations• Weizmann group

Michael HassOded HeberMichael RappaportAnukul DhalDirk SchwalmDavid MelnikAlexander Prygarin

• Soreq (SARAF) group Tsviki HirshDan BerkovitsIsrael Mardor

• MPIK groupKlaus BlaumAndreas Wolf

Sergey Vaintraub