1981
DOI: 10.1103/physrevb.24.244
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Low-temperature magnetic susceptibility of Si: P in the nonmetallic region

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Cited by 181 publications
(121 citation statements)
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“…The exchange is modelled as Heisenberg (σ · σ) interactions. Although in Si the true exchange is complicated by the indirect nature of the bandgap, and consequent intervalley interference and anisotropic effective mass effects, Andres et al (1981) and Koiller et al (2002aKoiller et al ( , 2002b show that the characteristic strength of the exchange interaction between defects can be related to the 'hydrogenic' value (Slater 1963, Herring andFlicker 1964), and this is what we assume. Thus, as we show in figure 2, there is a range of separations for which exchange between the ground states of A, B and C is negligible, and for which exchange between the excited state of C and A and C and B is usefully large.…”
Section: The Interaction Hamiltonianmentioning
confidence: 99%
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“…The exchange is modelled as Heisenberg (σ · σ) interactions. Although in Si the true exchange is complicated by the indirect nature of the bandgap, and consequent intervalley interference and anisotropic effective mass effects, Andres et al (1981) and Koiller et al (2002aKoiller et al ( , 2002b show that the characteristic strength of the exchange interaction between defects can be related to the 'hydrogenic' value (Slater 1963, Herring andFlicker 1964), and this is what we assume. Thus, as we show in figure 2, there is a range of separations for which exchange between the ground states of A, B and C is negligible, and for which exchange between the excited state of C and A and C and B is usefully large.…”
Section: The Interaction Hamiltonianmentioning
confidence: 99%
“…(At this separation the magnetic dipole-dipole interaction between the active electrons is ∼10 peV, and we ignore it.) Further details of exchange strengths in Si can be found in Herring and Flicker (1964), Cullis and Marko (1970), Stoneham (1975), Andres et al (1981), Koiller et al (2002aKoiller et al ( , 2002b.…”
Section: The Interaction Hamiltonianmentioning
confidence: 99%
“…Such control can presumably be achieved by fabrication of donor arrays with well-controlled positioning and surface gate potential (O'Brien et al 2001, Schofield et al 2003, Buehler et al 2002, Schenkel et al 2003. However, electron exchange in bulk silicon has spatial oscillations (Andres et al 1981, Koiller et al 2002 on the atomic scale due to valley interference arising from the particular six-fold degeneracy of the bulk Si conduction band. These exchange oscillations place heavy burdens on device fabrication and coherent control (Koiller et al 2002a), because of the very high accuracy and tolerance requirements for placing each donor inside the Si unit cell, and/or for controlling the external gate voltages.…”
Section: Electric-field Control Of Shallow Donor In Siliconmentioning
confidence: 99%
“…The effects of these properties have been considered elsewhere [16][17][18]. We have not estimated the overlap factors associated with the Bloch functions; these will give a factor that varies rapidly from one site to another, but the key analysis will not be affected [13,19].…”
Section: The Model Systemmentioning
confidence: 99%