2011
DOI: 10.1103/physrevb.84.075459
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Bistable behavior of silicon atoms in the (110) surface of gallium arsenide

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Cited by 21 publications
(35 citation statements)
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“…Their results are supported by the odd and even spatial symmetry, as well as similar spatial extent, of the two states appearing in the differential conductance maps at the corresponding energies [24]. Impurity states at the surface [40,41] are known to be quite different from those even a layer below the surface, which are much less sensitive to the influence of the surface [42,43]. The two states in our Figs.…”
Section: Discussionsupporting
confidence: 81%
“…Their results are supported by the odd and even spatial symmetry, as well as similar spatial extent, of the two states appearing in the differential conductance maps at the corresponding energies [24]. Impurity states at the surface [40,41] are known to be quite different from those even a layer below the surface, which are much less sensitive to the influence of the surface [42,43]. The two states in our Figs.…”
Section: Discussionsupporting
confidence: 81%
“…15 Electronic manipulation of dopant charge states has been predominately limited to ionization of Coulombically bound (shallow) donor and acceptor levels, 14,16 although switching a Si dopant between a substitutional and interstitial position with an associated charge change has also been demonstrated. 17 Electronic manipulation of tightly bound states, especially the spin-polarized core d electrons of transition-metal dopants, would permit a wider range of novel phenomena, including changing the core spin and magnetic interactions of a dopant. Such transitions have been measured optically for ensembles of transition-metal dopants in semiconductors, 18 and there is evidence of multiple d states associated with single transition-metal dopants embedded in the surface layer.…”
Section: Introductionmentioning
confidence: 99%
“…Switching to Si − i is strongly dependent on the tunneling current and reaches a frequency of about 1 Hz for I = 250 pA. 10 The switching depends on the availability of electrons, which is favored by a high current just below the tip. At the same time, local TIBB repels electrons, which is also highest just below the tip.…”
Section: Resultsmentioning
confidence: 99%
“…This is because the energy provided by the electrons is not enough to relax the atom into a different lattice position, probably by either inelastic excitation of phonons or quantum tunneling. 10 Therefore, scanning at low bias voltage allows us to determine the charge state of the Si atom without the STM tip affecting it.…”
Section: Resultsmentioning
confidence: 99%
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