The GSI Anomaly M. Lindner Max-Planck-Institut fr Kernphysik, - - PowerPoint PPT Presentation

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The GSI Anomaly M. Lindner Max-Planck-Institut fr Kernphysik, - - PowerPoint PPT Presentation

The GSI Anomaly M. Lindner Max-Planck-Institut fr Kernphysik, Heidelberg Sildes partially adopted from F. Bosch What is the GSI Anomaly? Periodically modualted exponential -decay law of highly charged, stored ions at GSI by


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SLIDE 1

The GSI Anomaly

  • M. Lindner

Max-Planck-Institut für Kernphysik, Heidelberg

Sildes partially adopted from F. Bosch

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SLIDE 2
  • M. Lindner

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What is the GSI Anomaly?

Periodically modualted exponential β β β β-decay law

  • f highly charged, stored ions at GSI by the FRS/ESR Collaboration

exponential decay periodic modulation !?!?

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SLIDE 3
  • M. Lindner

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Production of HCI’s

FRS fragment separator Target: Production

  • f secondary beams
  • f short-lived nuclei

ESR storage ring SIS heavy-ion synchrotron UNILAC linear accelerator

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SLIDE 4
  • M. Lindner

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Production and Selection of exotic Nuclei

cocktail of HCIs

  • in-flight separation
  • mono-isotopic beams
  • possibility to select single ions
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SLIDE 5
  • M. Lindner

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Initial momentum spread

  • cooling:
  • stochastic cooling for the first ~5 seconds
  • electron cooling (permanently on)

narrows velocity, size and divergence of stored ions

Beam Cooling

momentum exchange with 'cold‘ electron beam ions get the sharp velocity of the electrons, small size and divergence

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SLIDE 6
  • M. Lindner

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Schottky-Noise Detection

Continious digitizing and data storage for 1,2,3, … stored ions

Schottky Pick-ups

Stored ion beam

f ~ 2 MHz

FFT amplification summation

Schottky pick-ups

electron cooler gas target quadrupole- triplet Septum- magnet dipole magnet fast kicker magnet RF-cavity hexapole- magnets

from the FRS

Extraction

To the SIS

Quadrupole- dublet

ESR

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SLIDE 7

time

illustration: 4 particles with different M/q

ω1 ω2 ω3 ω4

FFT

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SLIDE 8
  • M. Lindner

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Observation of Decays of stored Ions

bound-state β-decay first observed at GSI in early 90‘s

a) normal β β β β-decay

  • different charge
  • different M/q

b) bound state β β β β-decay by electon capture

  • same q, slightly different M’ (binding energy, ν

ν ν ν-emission)

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SLIDE 9
  • M. Lindner

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Examples for Decay of Single Ions

  • ordinary β

β β β-decay and EC clearly separable

  • for few ions: intensity allows to see individual decays
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SLIDE 10
  • M. Lindner

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Spectroscopy of individual Particles

Pr

140 58+

Ce

140 58+

5 particles 4 particles 3 particles 2 particles 1 particle 6 particles

Q = 3388 keV

EC

13 117 65 169

Time [s] Frequency [kHz] - 61000.0

187.4 187.6 187.2 187.8

  • Int. J. Mass Spectr. 251 (2006) 212
  • sensitive to single ions
  • well-defined
  • creation time t0
  • charge states
  • two-body β-decay

monochromatic νe

  • observation of changes

in peak intensities of mother and daughter ions

  • investigation of a selected decay branch, e.g. pure EC decay
  • time-dependence of the detection efficiency is excluded
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SLIDE 11
  • M. Lindner

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Relevant Decays: H-like 140Pr and 142Pm

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SLIDE 12
  • M. Lindner

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Examples of measured Time-Frequency Traces

  • determine lifetime of individual ions
  • plot distribution of lifetimes
  • expect exponential decay law
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SLIDE 13
  • M. Lindner

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140Pr all Runs: 2650 EC Decays from 7102 Injections

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SLIDE 14
  • M. Lindner

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142Pm: 2740 EC Decays from 7011 Injections

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SLIDE 15
  • M. Lindner

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142Pm: Zoom on the first 35s after Injection

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SLIDE 16
  • M. Lindner

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Fits

1) exponential dNEC (t)/dt = N0 exp {- λt} λEC λ= λβ+ + λEC + λloss 2) exponential plus periodic oscillation dNEC (t)/dt = N0 exp {- λt} λEC(t) λEC(t)= λEC [1+a cos(ωt+φ)]

T = 7.06 (8) s φ = - 0.3 (3) T = 7.10 (22) s φ = - 1.3 (4)

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SLIDE 17
  • M. Lindner

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What causes the Oscillations?

  • explanations relating the effect to neutrino mixing
  • discussion of literature
  • see poster
  • why this is NOT related to neutrino mixing
  • Feynman diagram of neutrino oscillation:
  • energy momentum properties, quantum numbers
  • e.g. observation of solar neutrinos in ν

ν ν νe channel

x

solar fusion process

  • ν

ν ν νe

  • projection on ν

ν ν νe mass eigenstates

  • +MSW
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SLIDE 18
  • M. Lindner

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Kinematics: a) precise measurement of mother and daughter energies and momenta

  • emitted mass eigenstate known
  • ne contribution
  • no oscillation, but rate ~ |Uei|2
  • not realized here

b) Finite kinematical resolution much smaller than neutrino masses

  • all three mass eigenstates contribute incoherently
  • independent of flavour mixing

The EC Process

x

EC capture process

  • ν

ν ν νe undetected neutrino

  • mass eigenstates

mass eigenstates

Uei

(i=1..n)

mother ion daughter ion

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SLIDE 19
  • M. Lindner

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Checks / Questions / Problems

Carefully checks:

  • artefacts such as periodic coupling of the Schottky-noise to all sort
  • f backgrounds excluded
  • all EC decays are recorded; continuous information on the status of

mother- and daughter ion during the whole observation time

Questions / problems?

  • 3.5σ could be a statistical fluctuation
  • ? suppressed statistical bin-to-bin fluctuations 15
  • ? scaling of amplitude of the Schottky-signal 9
  • ! primary signal unobserved: noise >> individual ion signal 6
  • ? relative phase Pr / Pm 15+16
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SLIDE 20
  • M. Lindner

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Summary and Outlook

  • bservation of an unexplained periodic modulation
  • f the decay of H-like HCIs (3.5σ

σ σ σ)

  • *NOT* related to neutrino mixing
  • conceivable: tiny splitting of a 2 level mother system
  • how to explain such a tiny split?
  • coherence length?
  • many careful checks of all sort of systematics have

been performed

  • however: some unexplained statistical properties
  • f data
  • new run with different element approved ~fall