In recent years, the development of high power laser systems led to focussed intensities of more than 1022 W/cm2 at high pulse energies. Furthermore, both, the advanced high power lasers and the development of sophisticated laser particle acceleration mechanisms facilitate the generation of high energetic particle beams at high fluxes. The challenge of imaging detector systems is to acquire the properties of the high flux beam spatially and spectrally resolved. The limitations of most detector systems are saturation effects. These conventional detectors are based on scintillators, semiconductors, or radiation sensitive films. We present a nuclear activation-based imaging spectroscopy method, which is called NAIS, for the characterization of laser accelerated proton beams. The offline detector system is a combination of stacked metal foils and imaging plates (IP). After the irradiation of the stacked foils they become activated by nuclear reactions, emitting gamma decay radiation. In the next step, an autoradiography of the activated foils using IPs and an analysis routine lead to a spectrally and spatially resolved beam profile. In addition, we present an absolute calibration method for IPs.
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July 2013
Research Article|
July 22 2013
NAIS: Nuclear activation-based imaging spectroscopy Available to Purchase
M. M. Günther;
M. M. Günther
a)
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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A. Britz;
A. Britz
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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R. J. Clarke;
R. J. Clarke
2Central Laser Facility,
Rutherford Appelton Laboratory
, Chilton, Didcot, Oxon OX11 0QX, United Kingdom
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K. Harres;
K. Harres
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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G. Hoffmeister;
G. Hoffmeister
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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F. Nürnberg;
F. Nürnberg
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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A. Otten;
A. Otten
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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A. Pelka;
A. Pelka
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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M. Roth;
M. Roth
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
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K. Vogt
K. Vogt
3
GSI – Helmholtzzentrum für Schwerionenforschung GmbH
, D-64291 Darmstadt, Germany
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M. M. Günther
1,a)
A. Britz
1
R. J. Clarke
2
K. Harres
1
G. Hoffmeister
1
F. Nürnberg
1
A. Otten
1
A. Pelka
1
M. Roth
1
K. Vogt
3
1Institut für Kernphysik, Schlossgartenstr. 9,
Technische Universität Darmstadt
, D-64289 Darmstadt, Germany
2Central Laser Facility,
Rutherford Appelton Laboratory
, Chilton, Didcot, Oxon OX11 0QX, United Kingdom
3
GSI – Helmholtzzentrum für Schwerionenforschung GmbH
, D-64291 Darmstadt, Germany
a)
Electronic mail: [email protected]. Current address: GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstrasse 1, D-64291 Darmstadt, Germany.
Rev. Sci. Instrum. 84, 073305 (2013)
Article history
Received:
April 04 2013
Accepted:
July 01 2013
Citation
M. M. Günther, A. Britz, R. J. Clarke, K. Harres, G. Hoffmeister, F. Nürnberg, A. Otten, A. Pelka, M. Roth, K. Vogt; NAIS: Nuclear activation-based imaging spectroscopy. Rev. Sci. Instrum. 1 July 2013; 84 (7): 073305. https://doi.org/10.1063/1.4815826
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