Spin injection electrode structure and spin transport element having the same
US-2015001601-A1 · Jan 1, 2015 · US
US2016169986A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2016169986-A1 |
| Application number | US-201514934240-A |
| Country | US |
| Kind code | A1 |
| Filing date | Nov 6, 2015 |
| Priority date | Dec 10, 2014 |
| Publication date | Jun 16, 2016 |
| Grant date | — |
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A method for directly electrically generating and detecting spin polarization in topological insulators comprising depositing a first and fourth contact on a layer of Bi 2 Se 3 and applying a current between the contacts, which creates a net spin polarization due to spin-momentum locking. A second (comprising ferromagnet/tunnel barrier) and third contact are deposited for detecting the spin polarization. A device for directly electrically generating and detecting the current-generated spin polarization in topological insulators, comprising a first and fourth contact on a layer of Bi 2 Se 3 and a second contact comprising a ferromagnet/oxide tunnel barrier contact as a detector, and a third contact comprising nonmagnetic metal as a reference contact, a current to the first and fourth contact to produce a net spin polarization, and the spin polarization manifesting as a voltage between the second (magnetic) and third (reference) contacts.
Opening claim text (preview).
What we claim is: 1 . A method of making a device for directly electrically generating and detecting spin polarization in topological insulators, comprising: depositing a first contact and fourth contact on a layer of Bi 2 Se 3 ; depositing a second contact and third contact wherein the second contact comprises a ferromagnet/oxide tunnel barrier contact and wherein the third contact comprises a nonmagnetic metal contact; applying a current between the first contact and fourth contact; creating a net spin polarization due to spin-momentum locking; and detecting the spin polarization between the second contact and the third contact. 2 . The method for directly electrically generating and detecting spin polarization in topological insulators of claim 1 wherein the ferromagnet/oxide tunnel barrier comprises a layer of Fe and a layer of Al 2 O 3 . 3 . The method for directly electrically generating and detecting spin polarization in topological insulators of claim 1 wherein the ferromagnet/oxide tunnel barrier comprises a layer of Co and a layer of MgO on top of a layer of graphene. 4 . The method for directly electrically generating and detecting spin polarization in topological insulators of claim 1 wherein the current is an unpolarized bias current. 5 . The method for directly electrically generating and detecting spin polarization in topological insulators of claim 1 wherein the step of detecting the spin polarization of the surface spin due to spin-momentum locking is its projection onto the detector contact magnetization manifests as a voltage. 6 . The method for directly electrically generating spin polarization in topological insulators of claim 1 wherein the step of detecting the spin polarization comprises detecting the voltage between the second ferromagnetic/oxide tunnel barrier contact and the third contact. 7 . The method for directly electrically generating spin polarization in topological insulators of claim 6 wherein the magnetization of the third contact determines the spin detection axis and the projection of the TI spin polarization onto the spin detection axis is detected electrically as a voltage. 8 . A method for direct electrical access to current-induced spin polarization due to spin-momentum locking of the topologically protected surface states in topological insulators comprising: applying an unpolarized bias current; creating a net spin polarization; creating a spin accumulation; creating spin polarized current flowing through surface states; detecting directly electrically the spin accumulation; and utilizing the spin polarized surface states for spintronic/electronic applications. 9 . The method for direct electrical access to current-induced spin polarization due to spin-momentum locking of the topologically protected surface states in topological insulators of claim 8 further comprising the step of: utilizing a ferromagnetic thin film surface contact to detect the spin polarization. 10 . The method for direct electrical access to current-induced spin polarization due to spin-momentum locking of the topologically protected surface states in topological insulators of claim 9 wherein the ferromagnetic thin film surface contact is magnetized and wherein the magnetization of the contact determines the spin detection axis. 11 . The method for direct electrical access to current-induced spin polarization due to spin-momentum locking of the topologically protected surface states in topological insulators of claim 10 further comprising the step of: detecting electrically as a voltage a projection of the topological insulator spin polarization onto the spin detection axis. 11 . A device for directly electrically generating and detecting the current-generated spin polarization in topological insulators, comprising: a first contact and fourth contact on a layer of Bi 2 Se 3 ; a second contact comprising a ferromagnet/oxide tunnel barrier contact on a layer of Bi 2 Se 3 ; wherein the second contact is a detector; a third contact on the layer of Bi 2 Se 3 ; wherein the third contact is a reference; a current to the first contact and the fourth contact; a net spin polarization; and the spin polarization manifesting as a voltage between the second contact and the third contact. 12 . The device for directly electrically generating and detecting the current-generated spin polarization in topological insulators of claim 11 wherein the ferromagnet/oxide tunnel barrier comprises a layer of Fe and a layer of Al 2 O 3 . 13 . The device for directly electrically generating and detecting the current-generated spin polarization in topological insulators of claim 12 wherein the ferromagnet/oxide tunnel barrier comprises a layer of Co and a layer of MgO on top of a layer of graphene. 14 . The device for directly electrically generating and detecting the current-generated spin polarization in topological insulators of claim 13 wherein the current is an unpolarized bias current. 15 . A device for directly electrically detecting current-generated spin polarization in topological insulators, comprising: a first contact and fourth contact on a layer of Bi 2 Se 3 to produce a spin; a second magnetic contact comprising a ferromagnet/oxide tunnel barrier contact as a detector; a third reference contact comprising nonmagnetic metal as the reference contact; a current to the first contact and fourth contact to produce a net spin polarization; and the spin polarization manifesting as a voltage between the second magnetic contact and third reference contact. 16 . The device for directly electrically detecting current-generated spin polarization in topological insulators of claim 15 wherein the ferromagnet/oxide tunnel barrier comprises a layer of Fe and a layer of Al 2 O 3 . 17 . The device for directly electrically detecting current-generated spin polarization in topological insulators of claim 15 wherein the ferromagnet/oxide tunnel barrier comprises a layer of Co and a layer of MgO on top of a layer of graphene. 18 . The device for directly electrically detecting current-generated spin polarization in topological insulators of claim 15 wherein the current is an unpolarized bias current. 19 . The device for directly electrically detecting current-generated spin polarization in topological insulators of claim 15 the spin polarization of the surface spin due to spin-momentum locking is its projection onto the detector contact magnetization manifests as a voltage.
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