000018235 001__ 18235
000018235 005__ 20200423203114.0
000018235 0247_ $$2DOI$$a10.1140/epja/i2011-11088-1
000018235 0247_ $$2WOS$$aWOS:000293634100001
000018235 0247_ $$2arXiv$$aarXiv:1011.2415$$cnucl-ex
000018235 0247_ $$2Handle$$a2128/10296
000018235 035__ $$9arXiv$$aarXiv:1011.2415$$cnucl-ex
000018235 035__ $$aLEX-10-01
000018235 037__ $$aPreJuSER-18235
000018235 041__ $$aeng
000018235 082__ $$a530
000018235 084__ $$2WoS$$aPhysics, Nuclear
000018235 084__ $$2WoS$$aPhysics, Particles & Fields
000018235 084__ $$2PACS$$a36.10.Gv
000018235 084__ $$2PACS$$a25.80.Ls
000018235 084__ $$2PACS$$a07.85.Nc
000018235 1001_ $$0P:(DE-Juel1)VDB57599$$aStrauch, Th.$$b0$$uFZJ
000018235 245__ $$aPionic deuterium
000018235 260__ $$aBerlin$$bSpringer$$c2011
000018235 300__ $$a88
000018235 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
000018235 3367_ $$2DataCite$$aOutput Types/Journal article
000018235 3367_ $$00$$2EndNote$$aJournal Article
000018235 3367_ $$2BibTeX$$aARTICLE
000018235 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000018235 3367_ $$2DRIVER$$aarticle
000018235 440_0 $$01981$$aEuropean Physical Journal A$$v47$$x1434-6001$$y7
000018235 500__ $$aWe would like to thank N. Dolfus, B. Leoni, L. Stohwasser, and K.-P. Wieder for the technical assistance and V. Baru, C. Hanhart, A. Nogga, M. Hoferichter, and A. Rusetsky for continuous exchange of information on theoretical progress on the pi D system. The Bragg crystal was manufactured by Carl Zeiss AG, Oberkochen, Germany. Partial funding and travel support was granted by FCT (Lisbon) and FEDER (Grant No. SFRH/BD/18979/2004 and project PTDC/FIS/102110/2008) and the Germaine de Stael exchange program. LKB is Unite Mixte de Recherche du CNRS, de l'Ecole Normale Superieure et de UPMC No. 8552. This work is part of the PhD thesis of one of us (Th. S., University of Cologne, 2009).
000018235 520__ $$aThe 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.
000018235 536__ $$0G:(DE-Juel1)FUEK413$$2G:(DE-HGF)$$aPhysik der Hadronen und Kerne$$cP53$$x0
000018235 588__ $$aDataset connected to Web of Science
000018235 650_7 $$2INSPIRE$$adeuterium: mesic atom
000018235 650_7 $$2INSPIRE$$api: mesic atom
000018235 650_7 $$2INSPIRE$$ascattering: (pi deuterium)
000018235 650_7 $$2INSPIRE$$api: absorption
000018235 650_7 $$2INSPIRE$$api: production
000018235 650_7 $$2INSPIRE$$aspectrometer: crystal
000018235 650_7 $$2INSPIRE$$abroadening
000018235 650_7 $$2INSPIRE$$ascattering length
000018235 7001_ $$0P:(DE-HGF)0$$aAmaro, F.D.$$b1
000018235 7001_ $$0P:(DE-HGF)0$$aAnagnostopoulos, D.F.$$b2
000018235 7001_ $$0P:(DE-HGF)0$$aBühler, P.$$b3
000018235 7001_ $$0P:(DE-HGF)0$$aCovita, D.S.$$b4
000018235 7001_ $$0P:(DE-HGF)0$$aGorke, H.$$b5
000018235 7001_ $$0P:(DE-Juel1)131168$$aGotta, D.$$b6$$uFZJ
000018235 7001_ $$0P:(DE-HGF)0$$aGruber, A.$$b7
000018235 7001_ $$0P:(DE-HGF)0$$aHirtl, A.$$b8
000018235 7001_ $$0P:(DE-HGF)0$$aIndelicato, P.$$b9
000018235 7001_ $$0P:(DE-HGF)0$$aLe Bigot, E-O.$$b10
000018235 7001_ $$0P:(DE-Juel1)VDB1136$$aNekipelov, M.$$b11$$uFZJ
000018235 7001_ $$0P:(DE-HGF)0$$ados Santos, J.M.F.$$b12
000018235 7001_ $$0P:(DE-HGF)0$$aSchmid, Ph.$$b13
000018235 7001_ $$0P:(DE-HGF)0$$aSchlesser, S.$$b14
000018235 7001_ $$0P:(DE-HGF)0$$aSimons, L.M.$$b15
000018235 7001_ $$0P:(DE-HGF)0$$aTrassinelli, M.$$b16
000018235 7001_ $$0P:(DE-HGF)0$$aVeloso, J.F.C.A.$$b17
000018235 7001_ $$0P:(DE-Juel1)VDB1848$$aZmeskal, J.$$b18$$uFZJ
000018235 773__ $$0PERI:(DE-600)1459066-9$$a10.1140/epja/i2011-11088-1$$gVol. 47, p. 88$$p88$$q47<88$$tThe @European physical journal / A$$v47$$x1434-6001$$y2011
000018235 8567_ $$uhttp://dx.doi.org/10.1140/epja/i2011-11088-1
000018235 8564_ $$uhttps://juser.fz-juelich.de/record/18235/files/1011.2415v2.pdf$$yOpenAccess
000018235 8564_ $$uhttps://juser.fz-juelich.de/record/18235/files/1011.2415v2.gif?subformat=icon$$xicon$$yOpenAccess
000018235 8564_ $$uhttps://juser.fz-juelich.de/record/18235/files/1011.2415v2.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000018235 8564_ $$uhttps://juser.fz-juelich.de/record/18235/files/1011.2415v2.jpg?subformat=icon-700$$xicon-700$$yOpenAccess
000018235 8564_ $$uhttps://juser.fz-juelich.de/record/18235/files/1011.2415v2.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000018235 909CO $$ooai:juser.fz-juelich.de:18235$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire
000018235 9131_ $$0G:(DE-Juel1)FUEK413$$aDE-HGF$$bStruktur der Materie$$kP53$$lPhysik der Hadronen und Kerne$$vPhysik der Hadronen und Kerne$$x0
000018235 9132_ $$0G:(DE-HGF)POF3-612$$1G:(DE-HGF)POF3-610$$2G:(DE-HGF)POF3-600$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Universum$$vCosmic Matter in the Laboratory$$x0
000018235 9141_ $$y2011
000018235 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000018235 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000018235 9201_ $$0I:(DE-Juel1)IKP-2-20111104$$gIKP$$kIKP-2$$lExperimentelle Hadrondynamik$$x0
000018235 970__ $$aVDB:(DE-Juel1)132891
000018235 980__ $$aVDB
000018235 980__ $$aConvertedRecord
000018235 980__ $$ajournal
000018235 980__ $$aI:(DE-Juel1)IKP-2-20111104
000018235 980__ $$aUNRESTRICTED
000018235 9801_ $$aUNRESTRICTED
000018235 9801_ $$aFullTexts