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S. Cederbaum, Phys. Rev. A 77, 033613 (2008) 29. K. I. E. S. Cederbaum, Phys. Rev. A 78, 023615 (2008) 30. I. E. S. Cederbaum, Phys. Rev. Lett. 100, 130401 (2008) 31. I. E. S. Cederbaum, Phys. Rev. A 80, 043616 (2009) 32. E. I. S. Cederbaum, Phys. Lett. A 373, 301 (2009) 33. J. Grond, J. Schmiedmayer, U. Hohenester, Phys. Rev. A 79, 021603(R) (2009) 34. J. Grond, von G. Winckel, J. Schmiedmayer, U. Hohenester, Phys. Rev. A 80, 053625 (2009) 35. J. Grond, J. Schmiedmayer, U. Hohenester, New J. Phys.

R p |r1 , . . , r p ; t), see Appendix B. Thus, the diagonal of g ( p) in momentum space provides information about the coherence of | (t) which is not contained in the diagonal of g ( p) in real space and vice versa. 9 First and Second Order RDMs, Correlations and Coherence The fact that many-body quantum systems interact generally via two-body interaction potentials makes the RDMs of first and second order particularly important. For example, the expectation value of any two-body operator can be represented by an integral involving the second-order RDM only, see Sect.

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