“…A simple analytical expression for the magnetoresistance can be obtained for a quasi-ballistic one-dimensional SpinFET [125,126]. The effective Hamiltonian in the ferromagnetic regions has the following form in the one-band effective mass approximationĤ…”
Section: A Fin-based Quasi-ballistic Spinfet: Model Expressions For Tmentioning
confidence: 99%
“…For the one-dimensional semiconductor channel region the Hamiltonian has been formulated in [125][126][127]. The spin-orbit coupling for silicon is taken in the form (54).…”
Section: A Fin-based Quasi-ballistic Spinfet: Model Expressions For Tmentioning
confidence: 99%
“…To facilitate the injection of the spin-polarized current into the channel, one has to introduce, following [125] and [126], tunnel barriers at the interfaces between the contacts and the channel with the dimensionless strength…”
Section: Tunnel Barriers and Magnetoresistance At Elevated Temperaturementioning
“…A simple analytical expression for the magnetoresistance can be obtained for a quasi-ballistic one-dimensional SpinFET [125,126]. The effective Hamiltonian in the ferromagnetic regions has the following form in the one-band effective mass approximationĤ…”
Section: A Fin-based Quasi-ballistic Spinfet: Model Expressions For Tmentioning
confidence: 99%
“…For the one-dimensional semiconductor channel region the Hamiltonian has been formulated in [125][126][127]. The spin-orbit coupling for silicon is taken in the form (54).…”
Section: A Fin-based Quasi-ballistic Spinfet: Model Expressions For Tmentioning
confidence: 99%
“…To facilitate the injection of the spin-polarized current into the channel, one has to introduce, following [125] and [126], tunnel barriers at the interfaces between the contacts and the channel with the dimensionless strength…”
Section: Tunnel Barriers and Magnetoresistance At Elevated Temperaturementioning
“…To calculate the transport properties of the ballistic spin field-effect transistor we consider a model similar to (12) and (13). The Hamiltonian in the ferromagnetic regions has the following form in the one-band effective mass approximation: , 0 , 2…”
Section: Modelmentioning
confidence: 99%
“…where m * f is the effective mass in the contacts, h 0 =2PE F /(P 2 +1) is the exchange splitting energy with P defined as the spin polarization in the ferromagnetic regions, E F is the Fermi energy, and ı z is the Pauli matrix; ± in [5] stands for the parallel and anti-parallel configuration of the contact magnetization. For the semiconductor region the Hamiltonian reads ( 12), (13) , 2…”
We investigate the transport properties of ballistic spin field-effect transistors (SpinFET). We show that temperature exerts a significant influence on the device characteristics. For the InAsbased SpinFET an ambient temperature higher than T=150K leads to the absence of the ability to modulate the value of the tunneling magnetoresistance through changing the bandgap mismatch between the channel and the contacts. The length of the semiconductor channel impacts significantly the device characteristics. A shorter channel is preferred for potential operations at room temperature. For the silicon-based SpinFET the spin-orbit interaction has to be taken in the Dresselhaus form. We demonstrate that silicon fins with [100] orientation exhibit a stronger dependence on the value of the spin-orbit interaction and are thus preferable for practical realization of SpinFETs.
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