kvi center for advanced radiation technology 22 06

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kvi - center for advanced radiation technology 22 -06 -2017 | Nuclear force studies

kvi - center for advanced radiation technology 22 -06 -2017 | Nuclear force studies in the pd break-up channel at 135 Me. V Hajar Tavakoli-Zaniani

22 -06 -2017 | outline › Introduction › Experimental setup › Results › Conclusion

22 -06 -2017 | outline › Introduction › Experimental setup › Results › Conclusion 2 2

22 -06 -2017 | 3 Two Nucleon Force (2 NF) 1935 Yukawa’s meson theory

22 -06 -2017 | 3 Two Nucleon Force (2 NF) 1935 Yukawa’s meson theory (2 NF) Theory : One Pion Exchange Model One Boson Exchange Model Heavier Meson Exchange e. g. r and w NN Force models ü ü ü Nijmegen II Reid 93 CD-Bonn Argonne V 18 with high precision, c 2 1 3

22 -06 -2017 | Where could we see 3 NF effects ? NN (AV

22 -06 -2017 | Where could we see 3 NF effects ? NN (AV 18) NN+3 NF (AV 18+IL 2) Exp. S. C. Pieper et al. PRC 64, 14001 (2001) 4 4

22 -06 -2017 | 5 W. P. Abfalterer et al. , PRL 81, 57

22 -06 -2017 | 5 W. P. Abfalterer et al. , PRL 81, 57 (1998) 5

22 -06 -2017 | 6 Three Nucleon Force (3 NF) 1957 Fujita and Miyazawa

22 -06 -2017 | 6 Three Nucleon Force (3 NF) 1957 Fujita and Miyazawa 3 NF theory Prog. Theor. Phys. 17, 360 (1957) 2 p-exchange 3 NF : D-isobar excitations in the intermediate 3 N Force models ü Tucson-Melbourn (TM) ü Urbana IX ü Brazil ü… 6

22 -06 -2017 | 7 Experimental setup AGOR KVI 7

22 -06 -2017 | 7 Experimental setup AGOR KVI 7

22 -06 -2017 | 8 BINA (Big Instrument for Nuclear-polarization Analysis) 8

22 -06 -2017 | 8 BINA (Big Instrument for Nuclear-polarization Analysis) 8

7 9 22 -06 -2017 | pd break-up at 135 Me. V (θ 1

7 9 22 -06 -2017 | pd break-up at 135 Me. V (θ 1 , φ1 , E 1 , θ 2 , φ2 , E 2 , θ 3 , φ3 , E 3) (θ 1 , φ1 , θ 2 , φ2 , S) φ2 p+d p+p+n 9

8 10 22 -06 -2017 | 10 Energy calibration of the E-detectors 10 9

8 10 22 -06 -2017 | 10 Energy calibration of the E-detectors 10 9 8 7 6 5 4 ∆θ 3 2 1

9 11 22 -06 -2017 | 11 Analysing power measurement

9 11 22 -06 -2017 | 11 Analysing power measurement

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14 16 22 -06 -2017 | 16 Conclusion ü For small azimuthal opening angles,

14 16 22 -06 -2017 | 16 Conclusion ü For small azimuthal opening angles, the calculation including 3 NF, the agreement is worse than calculation without the 3 NF. ü The effect of 3 NFs is predicted to be small, although adding a 3 NF to the NN potentials helps to bridge the gap between the data and the NN calculations.

22 -06 -2017 | 17 Our collaboration H. Tavakoli-Zaniani 1, 2, M. T. Bayat

22 -06 -2017 | 17 Our collaboration H. Tavakoli-Zaniani 1, 2, M. T. Bayat 1, M. Eslami-Kalantari 2, N. Kalantar-Nayestanaki 1 , St. Kistryn 3, A. Kozela 4, J. G. Messchendorp 1, M. Mohammadi-Dadkan 1, 5, R. Ramazani-Sharifabadi 1, 6, E. Stephan 7 1 KVI-Cart, University of Groningen, The Netherlands 2 Department of Physics, School of Science, Yazd University, Yazd, Iran 3 Institute of Physics, Jagiellonian University, Krakow, Poland 4 Institute of Nuclear Physics, PAN, Krakow, Poland 5 Department of Physics, University of Sistan and Baluchestan, Zahedan, Iran 6 Department of Physics, University of Tehran, Iran 7 Institute of Physics, University of Silesia, Chorzow, Poland Thanks

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22 -06 -2017 | 20 Data and calculations

22 -06 -2017 | 20 Data and calculations