Pionic fusion: comparison of different spin/isospin channels

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13 december 2002 H.L. / KVI PAC Meeting 1 Pionic fusion: comparison of different spin/isospin channels Study coherence of pion production, role of clustering correlations in the pionic fusion process, production mechanism: s, p-wave dynamics

description

Pionic fusion: comparison of different spin/isospin channels. Study coherence of pion production, role of clustering correlations in the pionic fusion process, production mechanism: s, p-wave dynamics. Existing data and models. semi-phenomenological model: - PowerPoint PPT Presentation

Transcript of Pionic fusion: comparison of different spin/isospin channels

Page 1: Pionic fusion:  comparison of  different  spin/isospin  channels

13 december 2002 H.L. / KVI PAC Meeting 1

Pionic fusion: comparison of different spin/isospin channels

Studycoherence of pionproduction, role of clusteringcorrelations in thepionic fusion process, production mechanism:s, p-wave dynamics

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13 december 2002 H.L. / KVI PAC Meeting 2

Existing data and modelsLiHeHe 734 ),(

L. Bimbot et al., PL B 114(82)311

semi-phenomenological model:3-nucleon transfer by p-3He reaction,analytic expressions for transfer formfactors from HO wave functions

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13 december 2002 H.L. / KVI PAC Meeting 3

Interacting cluster modelKajino, Toki, Kubo, PRC 35(87)1370

correlated microscopic cluster wave functions using Resonating Group Method (RGM),NN effective interaction + Coulomb(check charge symmetry),

entrance channel distortions by local imaginary potential WD

between clusters (from DWBA)

compared toshell model wave functions

data suggest importance of cluster correlations

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13 december 2002 H.L. / KVI PAC Meeting 4

origin of enhancement in cluster modeldecomposition of contributions

inter-cluster (3H – 4He) relative motionabsorbs large momentum transferto fused system 7Li

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Prediction for 0 fusion to 7Bechance to separate g.s. and 0.429 excited state:excellent application of dual-range QDC´s

simulated CM distribution with 25000 acceptedevents using cos2() distribution for pions

experiment strategy:final-state slectivity by-decay tagging

calculationsbut now data

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13 december 2002 H.L. / KVI PAC Meeting 6

Inclusive d - fusionM. Andersson et al., PL B 481 (00)165

measured integrated cross section (230 nb and 140 nb at 1.2 and 1.9 MeV above threshold) and strong forward-backward asymmetry

data explained by process viaquasi-deuteron: overlap with quasi-d determines angular distribution

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Systematic study of cluster structuressimilar processes butwith increasingly complex cluster structure:decisive tool: angular distributionsfinal-state slectivity by-decay tagging

9Be

3Hen

12C*

0

10B

dd

12C*

0

6Lid 12C*

0

6Lid

4He

3Hen

7Be*

0

4He

3He

7Be*

0

?

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angle acceptance of fusion productsmax. 3.8 deg in B mode

pionic fusion

radiative fusion (capture)

ground stateexcited state (15.1 MeV)

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momentum acceptance of fusion products

array of ca. 50 phoswich detectors100 m plastic/CsI 1.3X4 cm2

in focal plane of BBSfor HI detection:fusion products of 10 – 30 A MeV

coverage of momentum distributionby HI detectors:all / accepted events

B

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Summary

)(

98

kinematicss-wavep-waves-wavep-wave

Reactions with increasing complexity in cluster structureand different pion kinematics

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acceptance of neutral pions

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13 december 2002 H.L. / KVI PAC Meeting 12

TAPS schedule

ELSA Bonn - 6/03 including 2 KVI proposals

MAMI-B Mainz 6/03 - 6/04 with Crystal Barrel

KVI 7/04 - 6/05 setup during part of Trimp setup

MAMI-C 7/05 - early 07 with Crystal Barrel

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Table of BBS parameters

Mode A B Cdistance to Q1 0.84 1.14 1.44 mmomentum bite

13 19 25 %

solid angle 13.0 9.2 6.7 msrhor. angle span 4.1 3.8 3.4 deg.vert. angle span

10.3 8.0 6.4 deg.

hor. magnific. -0.46 -0.45 -0.44vert. magnific. -14.3 -10.1 -6.7lat. dispersion 2.54 2.54 2.54 cm / %ang. dispersion 42 42 42 deg.

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Proposed reactions

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design of liquid He target as buffer cryostatby Vacuum Specials Co. and P. Dendooven, J. Mulder, H. Timersma, H.L.