Hi,
Sorry, this is not yet described on the VASP Wiki in detail. Here is the description:
band No. > the band index enumerating the KS orbitals
KS-energies > the eigenenergies corresponding to the KS orbital computed within DFT E_nk^(0)
sigma(KS) > diagonal matrix elements of the self-energy <psi_nk^(0)|Sigma(w=Enk^(0))|psi_nk^(0)>
QP-e(linear) > quasiparticle energies obtained by linearizing the diagonal elements of the real-frequency self-energy around the DFT energies E_nk^(0), See Eq 76 in P. Liu, M. Kaltak, J. Klimes, and G. Kresse, Phys. Rev. B 94, 165109 (2016).
Z (column 5) > renormalization factor using linearization scheme. See Eq 77 in P. Liu, M. Kaltak, J. Klimes, and G. Kresse, Phys. Rev. B 94, 165109 (2016).
QP-e(zeros) > quasiparticle energies obtained by searching for roots of E_{nk}^{QP} = Re[ <psi_nk|T+V_{n-e}+V_H|psi_nk> + Sigma(w=E_{nk}^{QP}) ]
Z (column 7) > renormalization factor using roots scheme
occupation > occupation of KS orbital
Imag(E_QP) > Im[ Sigma(w=E_{nk}^{QP}) ]
QP_DIFF > difference of QP energies obtained by two methods for analytic continuation
TAG > Setting for the analytic continuation. TAG 1 is Thiele's method for Pade fitting. TAG 2 is a QR decomposition described in chapter 4 of
Manuel Grumet's master thesis
Does this help?
Marie-Therese