Hybridization of impurity states with the Shockley surface band versus bulk states

ANDREA BARRAL; ANA MARÍA LLOIS; ARMANDO ALIGIA

PHYSICAL REVIEW B - SOLID STATE

Año: 2004 vol. 70 p. 354161 - 354168

0556-2805

The characteristics of the Shockley surface states on Cus111d in the presence of Co impurity adsorbates are studied by means of one electron calculation performed using a well parametrized Hamiltonian in a local basis. Local densities of states in the spillover region as well as the relative hybridization strengths of Co "d" orbitals with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. studied by means of one electron calculation performed using a well parametrized Hamiltonian in a local basis. Local densities of states in the spillover region as well as the relative hybridization strengths of Co "d" orbitals with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. studied by means of one electron calculation performed using a well parametrized Hamiltonian in a local basis. Local densities of states in the spillover region as well as the relative hybridization strengths of Co "d" orbitals with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. s111d in the presence of Co impurity adsorbates are studied by means of one electron calculation performed using a well parametrized Hamiltonian in a local basis. Local densities of states in the spillover region as well as the relative hybridization strengths of Co "d" orbitals with bulk and surface states are obtained. We show that Co 3d orbitals hybridize mostly with Cu bulk conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. conduction states, thus giving ground to recent experimental results [N. Knorr, M. A. Schneider, L. Diekhoner, P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Lett. 88, 096804 (2002)] in the sense that the observed Kondo resonances are being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. being dominated by Cu bulk electrons. P. Wahl, and K. Kern, Phys. Rev. Let