Barabanov, M.Yu. ; Bedolla, M.A. ; Brooks, W.K. 
; Cates, G.D. ; Chen, C. ; Chen, Y. ; Cisbani, E. ; Ding, M. ; Eichmann, G. ; Ent, R. ; Ferretti, J. ; Gothe, R.W. ; Horn, T. ; Liuti, S. ; Mezrag, C. ; Pilloni, A. ; Puckett, A.J.R. ; Roberts, C.D. ; Rossi, P. ; Salmé, G. ; Santopinto, E. ; Segovia, J. ; Syritsyn, S.N. ; Takizawa, M. ; Tomasi-Gustafsson, E. ; Wein, P. ; Wojtsekhowski, B.B.
; Cates, G.D. ; Chen, C. ; Chen, Y. ; Cisbani, E. ; Ding, M. ; Eichmann, G. ; Ent, R. ; Ferretti, J. ; Gothe, R.W. ; Horn, T. ; Liuti, S. ; Mezrag, C. ; Pilloni, A. ; Puckett, A.J.R. ; Roberts, C.D. ; Rossi, P. ; Salmé, G. ; Santopinto, E. ; Segovia, J. ; Syritsyn, S.N. ; Takizawa, M. ; Tomasi-Gustafsson, E. ; Wein, P. ; Wojtsekhowski, B.B. Zusammenfassung
The last decade has seen a marked shift in how the internal structure of hadrons is understood. Modern experimental facilities, new theoretical techniques for the continuum bound-state problem and progress with lattice-regularised QCD have provided strong indications that soft quark+quark (diquark) correlations play a crucial role in hadron physics. For example, theory indicates that the ...
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