% IMPORTANT: The following is UTF-8 encoded. This means that in the presence % of non-ASCII characters, it will not work with BibTeX 0.99 or older. % Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or % “biber”. @ARTICLE{Adlarson:826388, author = {Adlarson, P. and Augustyniak, W. and Bardan, W. and Bashkanov, M. and Bergmann, F. S. and Berłowski, M. and Bhatt, H. and Bondar, A. and Büscher, M. and Calén, H. and Ciepał, I. and Clement, H. and Czerwiński, E. and Demmich, K. and Engels, Ralf W. and Erven, A. and Erven, W. and Eyrich, W. and Fedorets, P. and Föhl, K. and Fransson, K. and Goldenbaum, F. and Goswami, A. and Grigoryev, K. and Gullström, C.-O. and Heijkenskjöld, L. and Hejny, V. and Hüsken, N. and Jarczyk, L. and Johansson, T. and Kamys, B. and Kelkar, N. G. and Kemmerling, G. and Khatri, G. and Khoukaz, A. and Khreptak, O. and Kirillov, D. A. and Kistryn, S. and Kleines, H. and Kłos, B. and Krzemień, W. and Kulessa, P. and Kupść, A. and Kuzmin, A. and Lalwani, K. and Lersch, D. and Lorentz, B. and Magiera, A. and Maier, R. and Marciniewski, P. and Mariański, B. and Morsch, H.-P. and Moskal, P. and Ohm, H. and Perez del Rio, E. and Piskunov, N. M. and Prasuhn, D. and Pszczel, D. and Pysz, K. and Pyszniak, A. and Ritman, J. and Roy, A. and Rudy, Z. and Rundel, O. and Sawant, S. and Schadmand, S. and Schätti-Ozerianska, I. and Sefzick, T. and Serdyuk, V. and Shwartz, B. and Sitterberg, K. and Skorodko, T. and Skurzok, M. and Smyrski, J. and Sopov, V. and Stassen, R. and Stepaniak, J. and Stephan, E. and Sterzenbach, G. and Stockhorst, H. and Stroeher, Hans and Szczurek, A. and Trzciński, A. and Varma, R. and Wolke, M. and Wrońska, A. and Wüstner, P. and Yamamoto, A. and Zabierowski, J. and Zieliński, M. J. and Złomańczuk, J. and Żuprański, P. and Żurek, M.}, title = {{S}earch for η-mesic ${}^{4}\text{{H}e}$ in the $dd\to {}^{3}\text{{H}e}n{\pi }^{0}$ and $dd\to {}^{3}\text{{H}e}p{\pi }^{-}$ reactions with the {WASA}-at-{COSY} facility}, journal = {Nuclear physics / A}, volume = {959}, issn = {0375-9474}, address = {Amsterdam}, publisher = {North-Holland Publ. Co.}, reportid = {FZJ-2017-00616}, pages = {102 - 115}, year = {2017}, abstract = {The search for View the MathML sourceHe4-η bound states was performed with the WASA-at-COSY facility via the measurement of the excitation function for the View the MathML sourcedd→He3nπ0 and View the MathML sourcedd→He3pπ− processes. The deuteron beam momentum was varied continuously between 2.127 GeV/c and 2.422 GeV/c, corresponding to the excess energy for the View the MathML sourcedd→He4η reaction ranging from Q=−70 MeVQ=−70 MeV to Q=30 MeVQ=30 MeV. The luminosity was determined based on the View the MathML sourcedd→He3n reaction and the quasi-free proton–proton scattering via dd→ppnspectatornspectatordd→ppnspectatornspectator reactions. The excitation functions, determined independently for the measured reactions, do not reveal a structure which could be interpreted as a narrow mesic nucleus. Therefore, the upper limits of the total cross sections for the bound state production and decay in View the MathML sourcedd→(He4-η)bound→He3nπ0 and View the MathML sourcedd→(He4-η)bound→He3pπ− processes were determined taking into account the isospin relation between the both of the considered channels. The results of the analysis depend on the assumptions of the N⁎N⁎(1535) momentum distribution in the anticipated mesic-View the MathML sourceHe4. Assuming, as in the previous works, that this is identical with the distribution of nucleons bound with 20 MeV in View the MathML sourceHe4, we determined that (for the mesic bound state width in the range from 5 MeV to 50 MeV) the upper limits at $90\%$ confidence level are about 3 nb and about 6 nb for nπ0nπ0 and pπ−pπ− channels, respectively. However, based on the recent theoretical findings of the N⁎N⁎(1535) momentum distribution in the View the MathML sourceN⁎-He3 nucleus bound by 3.6 MeV, we find that the WASA-at-COSY detector acceptance decreases and hence the corresponding upper limits are 5 nb and 10 nb for nπ0nπ0 and pπ−pπ− channels respectively.}, cin = {IKP-1 / IKP-2 / IKP-4 / IKP-TA / ZEA-2 / PGI-6}, ddc = {530}, cid = {I:(DE-Juel1)IKP-1-20111104 / I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)IKP-4-20111104 / I:(DE-Juel1)IKP-TA-20111104 / I:(DE-Juel1)ZEA-2-20090406 / I:(DE-Juel1)PGI-6-20110106}, pnm = {612 - Cosmic Matter in the Laboratory (POF3-612)}, pid = {G:(DE-HGF)POF3-612}, experiment = {EXP:(DE-Juel1)WASA-at-COSY-20170712}, typ = {PUB:(DE-HGF)16}, UT = {WOS:000395211400007}, doi = {10.1016/j.nuclphysa.2017.01.001}, url = {https://juser.fz-juelich.de/record/826388}, }