Patent ID: 7719071

Claim:
A method of changing spin polarization of electric current, comprising the steps of: (a) providing a bipolar transistor having a first semiconductor region, a single ferromagnetic layer, and a third semiconductor region comprising, (i) providing the first semiconductor region adjacent the single ferromagnetic layer, so as to form a first domain between the first semiconductor region and the single ferromagnetic layer, (ii) providing the third semiconductor region adjacent the single ferromagnetic layer, so as to form a second domain between the single ferromagnetic layer and the third semiconductor region, (iii) providing a first voltage between the first semiconductor region and the single ferromagnetic layer, so as to cause carriers having a first charge current spin polarization and first density spin polarization to move across the first domain from the first semiconductor region to the single ferromagnetic layer, and (iv) providing a second voltage between the single ferromagnetic layer and the third semiconductor region, so as to cause the carriers to move across the second domain from the single ferromagnetic layer to the third semiconductor region, wherein the second voltage has an amplitude different from that of the first voltage and the carriers have a second charge current spin polarization in the third semiconductor region that is greater than the first charge current spin polarization and the first density spin polarization, respectively, wherein said first semiconductor region is an emitter, said single ferromagnetic layer is a base, and said third semiconductor region is a collector, wherein said bipolar spin transistor is configured to create a spin-polarized current of highly spin-polarized electrons in the third semiconductor region by one of spin-split minority carrier bands in the single ferromagnetic layer, spin-selective minority carrier spin flipping in the single ferromagnetic layer, or spin selective recombination in the single ferromagnetic layer; and (b) providing a control adapted to be coupled to the bipolar transistor for controlling the spin-polarized current by-altering a magnetization associated with the single ferromagnetic layer by one of depleting the ferromagnetic layer and re-orienting the magnetization with a small fringe field, using spin current torque for switching the ferromagnetic layer, optically injecting real carriers into the single ferromagnetic layer, or using an optical Stark effect.