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Spectroscopic features have been attributed to the Kondo resonance for systems other than a single, well-characterized magnetic impurity in a nonmagnetic host. See, for example, S. Gregory, Phys. Rev. Lett. 68, 2070 (1992); D. C. Ralph and R. A. Buhrman, ibid. 72, 3401 (1994); D. Goldhaber-Gordon et al., Nature 391, 156 (1998); E. L. Wolf, Principles of Electron Tunneling Microscopy (Oxford Univ. Press, New York, 1985). The pair-breaking effect of a single magnetic atom on a superconductor has also been observed [A. Yazdani, B. A. Jones, C. P. Lutz, M. F. Crommie, D. M. Eigler, Science 275, 1767 (1997)].
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Spectroscopic features have been attributed to the Kondo resonance for systems other than a single, well-characterized magnetic impurity in a nonmagnetic host. See, for example, S. Gregory, Phys. Rev. Lett. 68, 2070 (1992); D. C. Ralph and R. A. Buhrman, ibid. 72, 3401 (1994); D. Goldhaber-Gordon et al., Nature 391, 156 (1998); E. L. Wolf, Principles of Electron Tunneling Microscopy (Oxford Univ. Press, New York, 1985). The pair-breaking effect of a single magnetic atom on a superconductor has also been observed [A. Yazdani, B. A. Jones, C. P. Lutz, M. F. Crommie, D. M. Eigler, Science 275, 1767 (1997)].
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Spectroscopic features have been attributed to the Kondo resonance for systems other than a single, well-characterized magnetic impurity in a nonmagnetic host. See, for example, S. Gregory, Phys. Rev. Lett. 68, 2070 (1992); D. C. Ralph and R. A. Buhrman, ibid. 72, 3401 (1994); D. Goldhaber-Gordon et al., Nature 391, 156 (1998); E. L. Wolf, Principles of Electron Tunneling Microscopy (Oxford Univ. Press, New York, 1985). The pair-breaking effect of a single magnetic atom on a superconductor has also been observed [A. Yazdani, B. A. Jones, C. P. Lutz, M. F. Crommie, D. M. Eigler, Science 275, 1767 (1997)].
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Wolf, E.L.1
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9
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0030909823
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Spectroscopic features have been attributed to the Kondo resonance for systems other than a single, well-characterized magnetic impurity in a nonmagnetic host. See, for example, S. Gregory, Phys. Rev. Lett. 68, 2070 (1992); D. C. Ralph and R. A. Buhrman, ibid. 72, 3401 (1994); D. Goldhaber-Gordon et al., Nature 391, 156 (1998); E. L. Wolf, Principles of Electron Tunneling Microscopy (Oxford Univ. Press, New York, 1985). The pair-breaking effect of a single magnetic atom on a superconductor has also been observed [A. Yazdani, B. A. Jones, C. P. Lutz, M. F. Crommie, D. M. Eigler, Science 275, 1767 (1997)].
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note
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"Different tips" were obtained by changing the microscopic arrangement of the last few atoms on the STM tip through field emission and gentle collisions with the surface.
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23
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dI/dV traces taken with the tip displaced over the opposite side of the atom shown in Fig. 3 do not show as great a change in lineshape asymmetry. We attribute this to asymmetry in the particular STM tip used to acquire the data shown in Fig. 3.
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25
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Previous analysis of tunneling into an Anderson impurity [Y. Meir and N. S. Wingreen, Phys. Rev. Lett. 68, 2512 (1992)] can be generalized straightforwardly to include tunneling into the continuum.
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2642611370
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note
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We gratefully acknowledge M. El-Batanouny (who first noticed that the data suggest a Fano resonance), G. Murthy, and N. D. Lang for useful discussions. The work at Boston University was supported by NSF DMR-9457955, NSF DMR-9503837, the W. M. Keck Foundation, and the George I. Alden Trust.
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