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024 7 _ |a 10.1140/epja/i2011-11088-1
|2 DOI
024 7 _ |a WOS:000293634100001
|2 WOS
024 7 _ |a arXiv:1011.2415
|c nucl-ex
|2 arXiv
024 7 _ |a 2128/10296
|2 Handle
035 _ _ |9 arXiv
|a arXiv:1011.2415
|c nucl-ex
035 _ _ |a LEX-10-01
037 _ _ |a PreJuSER-18235
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Nuclear
084 _ _ |2 WoS
|a Physics, Particles & Fields
084 _ _ |2 PACS
|a 36.10.Gv
084 _ _ |2 PACS
|a 25.80.Ls
084 _ _ |2 PACS
|a 07.85.Nc
100 1 _ |0 P:(DE-Juel1)VDB57599
|a Strauch, Th.
|b 0
|u FZJ
245 _ _ |a Pionic deuterium
260 _ _ |a Berlin
|b Springer
|c 2011
300 _ _ |a 88
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
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336 7 _ |a Journal Article
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336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |0 1981
|a European Physical Journal A
|v 47
|x 1434-6001
|y 7
500 _ _ |a We would like to thank N. Dolfus, B. Leoni, L. Stohwasser, and K.-P. Wieder for the technical assistance and V. Baru, C. Hanhart, A. Nogga, M. Hoferichter, and A. Rusetsky for continuous exchange of information on theoretical progress on the pi D system. The Bragg crystal was manufactured by Carl Zeiss AG, Oberkochen, Germany. Partial funding and travel support was granted by FCT (Lisbon) and FEDER (Grant No. SFRH/BD/18979/2004 and project PTDC/FIS/102110/2008) and the Germaine de Stael exchange program. LKB is Unite Mixte de Recherche du CNRS, de l'Ecole Normale Superieure et de UPMC No. 8552. This work is part of the PhD thesis of one of us (Th. S., University of Cologne, 2009).
520 _ _ |a The strong-interaction shift epsilon(pi D)(1s) and broadening Gamma(pi D)(1s) in pionic deuterium have been determined in a high statistics study of the pi D(3p-1s) X-ray transition using a high-resolution crystal spectrometer. The pionic deuterium shift will provide constraints for the pion-nucleon isospin scattering lengths extracted from measurements of shift and broadening in pionic hydrogen. The hadronic broadening is related to pion absorption and production at threshold. The results are epsilon(pi D)(1s) = (-2356 +/- 31) meV (repulsive) and Gamma(pi D)(1s) = (1171(-49)(+23)) meV yielding for the complex pi D scattering length apD = [-(24.99 +/- 0.33)+ i(6.22(-0.26)(+0.1)2)] x 10(-3) m(pi)(-1). From the imaginary part, the threshold parameter for pion production is obtained to be alpha = (251(-11)(+5))mu b. This allows, in addition, and by using results from pion absorption in He-3 at threshold, the determination of the effective couplings g(0) and g(1) for s-wave pion absorption on isoscalar and isovector NN pairs.
536 _ _ |0 G:(DE-Juel1)FUEK413
|2 G:(DE-HGF)
|a Physik der Hadronen und Kerne
|c P53
|x 0
588 _ _ |a Dataset connected to Web of Science
650 _ 7 |2 INSPIRE
|a deuterium: mesic atom
650 _ 7 |2 INSPIRE
|a pi: mesic atom
650 _ 7 |2 INSPIRE
|a scattering: (pi deuterium)
650 _ 7 |2 INSPIRE
|a pi: absorption
650 _ 7 |2 INSPIRE
|a pi: production
650 _ 7 |2 INSPIRE
|a spectrometer: crystal
650 _ 7 |2 INSPIRE
|a broadening
650 _ 7 |2 INSPIRE
|a scattering length
700 1 _ |0 P:(DE-HGF)0
|a Amaro, F.D.
|b 1
700 1 _ |0 P:(DE-HGF)0
|a Anagnostopoulos, D.F.
|b 2
700 1 _ |0 P:(DE-HGF)0
|a Bühler, P.
|b 3
700 1 _ |0 P:(DE-HGF)0
|a Covita, D.S.
|b 4
700 1 _ |0 P:(DE-HGF)0
|a Gorke, H.
|b 5
700 1 _ |0 P:(DE-Juel1)131168
|a Gotta, D.
|b 6
|u FZJ
700 1 _ |0 P:(DE-HGF)0
|a Gruber, A.
|b 7
700 1 _ |0 P:(DE-HGF)0
|a Hirtl, A.
|b 8
700 1 _ |0 P:(DE-HGF)0
|a Indelicato, P.
|b 9
700 1 _ |0 P:(DE-HGF)0
|a Le Bigot, E-O.
|b 10
700 1 _ |0 P:(DE-Juel1)VDB1136
|a Nekipelov, M.
|b 11
|u FZJ
700 1 _ |0 P:(DE-HGF)0
|a dos Santos, J.M.F.
|b 12
700 1 _ |0 P:(DE-HGF)0
|a Schmid, Ph.
|b 13
700 1 _ |0 P:(DE-HGF)0
|a Schlesser, S.
|b 14
700 1 _ |0 P:(DE-HGF)0
|a Simons, L.M.
|b 15
700 1 _ |0 P:(DE-HGF)0
|a Trassinelli, M.
|b 16
700 1 _ |0 P:(DE-HGF)0
|a Veloso, J.F.C.A.
|b 17
700 1 _ |0 P:(DE-Juel1)VDB1848
|a Zmeskal, J.
|b 18
|u FZJ
773 _ _ |0 PERI:(DE-600)1459066-9
|a 10.1140/epja/i2011-11088-1
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|p 88
|q 47<88
|t The @European physical journal / A
|v 47
|x 1434-6001
|y 2011
856 7 _ |u http://dx.doi.org/10.1140/epja/i2011-11088-1
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