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Two-Photon emission Two-Photon emission from the first excited from the first excited state of state of 72 72 Ge Ge Robert Glover Robert Glover University of York

Two-Photon emission from the first excited state of 72 Ge

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Two-Photon emission from the first excited state of 72 Ge. Robert Glover. University of York. Contents. What is Two-photon emission??? Experiment Data Simulations Summary Acknowledgements. Introduction to two-photon emission. - PowerPoint PPT Presentation

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Two-Photon emission from Two-Photon emission from the first excited state of the first excited state of

7272GeGe

Robert GloverRobert Glover

University of York

ContentsContents

• What is Two-photon emission???What is Two-photon emission???

• ExperimentExperiment

• DataData

• SimulationsSimulations

• SummarySummary

• AcknowledgementsAcknowledgements

Introduction to two-photon Introduction to two-photon emissionemission

• An excited state decays via the An excited state decays via the spontaneous emission of two photonsspontaneous emission of two photons

• Competes with all other modes of Competes with all other modes of decaydecay

• High order decay mechanism, hence High order decay mechanism, hence has a very small branchhas a very small branch

• So improbable, it is very hard to So improbable, it is very hard to measuremeasure

How to spot two photon How to spot two photon emissionemission

• Impossible to observe in Impossible to observe in competition with rapid competition with rapid gamma ray emissiongamma ray emission

• Can occur between states of Can occur between states of any spin/parityany spin/parity

• Selection rules prohibit Selection rules prohibit gamma-ray emission gamma-ray emission between states of equal spin between states of equal spin and parity, owing to the and parity, owing to the photons intrinsic spin of S=1photons intrinsic spin of S=1

0+

0+

t1/2=200ns

2+

4+

5/2-

7/2-

9/2-

11/2-

13/2-

E0

Previous investigationsPrevious investigations• Experiments have Experiments have

been carried out on been carried out on 1616O, O, 4040Ca, Ca, 7272Ge and Ge and 9090Zr which all have Zr which all have 00++ –› 0 –› 0++ transitions transitions

• Best measurements Best measurements made on made on 1616O where O where photons were found photons were found to be two E1 or M1 to be two E1 or M1 transitions with equal transitions with equal probabilityprobability

• The energies were The energies were found to follow a found to follow a Gaussian distribution Gaussian distribution

Taken from Nucl. Phys. A474 412 (1987)

Branches vary around 6 x 10-4

ExperimentExperiment

• Uses germanium as Uses germanium as target and as detecting target and as detecting mediummedium

• Segmented detector is Segmented detector is capable of measuring capable of measuring both photons both photons simultaneously simultaneously

• Excite the low lying Excite the low lying states of germanium states of germanium nuclei by inelastic nuclei by inelastic scattering of 2.45 MeVscattering of 2.45 MeV

• Make use of the half-life Make use of the half-life of the first exited 0of the first exited 0++ state state

n

nn

690

835

00+

0+

2+

t1/2 = 444ns

e-E0

72Ge ~ 28% of Ge

Neutron Generator Neutron Generator

d + d 3He + n

ElectronicsElectronicsHardware Trigger generated whenever a core signal found in coincidence with a 200ns delayed neutron signal

Fast data cards write out the full pulse shapes for a period 4us before and 2us after the trigger condition is satisfied

SpectraSpectraSingles spectrum shows that the experiment successfully probed the transitions from the first excited state

Electron has a small probability of crossing a segment boundary and so the 690-keV peak is much smaller in the 2-fold spectrumIn folds 3 and 4, we see no 690 peak owing to the short range of the electron

Two-photon events are buried underneath the above spectrum

time

Pulse shape analysisPulse shape analysis

More pulse shapesMore pulse shapesWith the smaller amount of events we can carry out a more in depth analysis of the pulse shapes

Able to distinguish between real two-photon events and electrons crossing boundaries

Geant4Geant4

summarysummary

• Use Pulse-shape analysis to measure Use Pulse-shape analysis to measure number of two-photon eventsnumber of two-photon events

• Use efficiency from Geant4 to scale up Use efficiency from Geant4 to scale up measured number of counts to the real measured number of counts to the real number of two-photon eventsnumber of two-photon events

• Calculate branching ratio of two-photon Calculate branching ratio of two-photon emission for the first time in emission for the first time in 7272GeGe

Acknowledgements Acknowledgements

• Would like to thank:-Would like to thank:-

• David Jenkins (York)David Jenkins (York)

• Rodi Herzberg (Liverpool)Rodi Herzberg (Liverpool)

• Andy Boston (Liverpool)Andy Boston (Liverpool)

• Craig Gray-Jones (Liverpool)Craig Gray-Jones (Liverpool)

• Andrew Mather (Liverpool)Andrew Mather (Liverpool)

• Paul Stevenson (Surrey)Paul Stevenson (Surrey)