Method and system for magnetic semiconductor solid state cooling
US-2015143817-A1 · May 28, 2015 · US
US11823974B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11823974-B2 |
| Application number | US-202017607823-A |
| Country | US |
| Kind code | B2 |
| Filing date | May 1, 2020 |
| Priority date | May 1, 2019 |
| Publication date | Nov 21, 2023 |
| Grant date | Nov 21, 2023 |
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Systems and/or methods can provide for solid-state refrigeration below 1 degree Kelvin. By applying a simple sequence of ac electrical signals to a gated semiconductor device, electrons are cooled in a refrigeration sequence that, in turn, provides cooling directly to the heat load of interest. Electrons in a single subband of a semiconductor quantum well are expanded adiabatically into several subbands, resulting in a temperature drop. Repeated application of this cycle at MHz-GHz frequencies results in a significant cooling power. The anticipated cooling powers can compete with today's standard cryogenic system, the dilution refrigerator, which represents the market standard for achieving cryogenic temperatures.
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I claim: 1. A device, comprising: a central reservoir configured to isolate electrons; a first reservoir in communication with the central reservoir; and a second reservoir in communication with the central reservoir, wherein the electrons are isolated in the central reservoir and expanded from a single subband state into a multi-subband state when the device is selectively operated at a first stage, wherein heat from the first reservoir is exchanged with the central reservoir when the device operates a second stage responsive to the device operating at the first stage, wherein the electrons are isolated and compressed in the central reservoir from the multi-subband state to the single subband state when the device is selectively operated at a third stage subsequent to the heat being exchanged between the first reservoir and the central reservoir, and wherein excess heat in the central reservoir generated during the second stage is ejected into the second reservoir when the device operates at a fourth stage responsive to the device operating at the third stage. 2. The device of claim 1 , wherein the device is configured to cyclically operate between the first stage and the fourth stage. 3. The device of claim 1 , wherein the device operates at frequencies in the Megahertz (MHz) range. 4. The device of claim 1 , wherein the device comprises a dimension in a range of 5 millimeters by 5 millimeters by 0.5 millimeters. 5. The device of claim 1 , wherein the electrons include a first temperature when the first stage begins and include a second temperature when the first stage ends. 6. The device of claim 5 , wherein the second temperature is one third of the first temperature. 7. The device of claim 1 , further comprising a gate associated with the second reservoir wherein a voltage is applied to the gate to selectively operate the device at the first stage. 8. The device of claim 1 , wherein the device comprises a layer formed of aluminum arsenide. 9. The device of claim 8 , wherein the layer formed of aluminum arsenide comprises a miscut angle. 10. The device of claim 1 , further comprising a cold load in communication with the first reservoir. 11. The device of claim 1 , further comprising a heat sink in communication with the second reservoir. 12. A method, comprising: selectively operating a device at a first stage to isolate electrons in a central reservoir and expand the electrons from a single subband state into a multi-subband state, wherein the central reservoir is in communication with a first reservoir; exchanging heat from the first reservoir to the central reservoir when the device operates at a second stage responsive to the device operating at the first stage; selectively operating the device at a third stage, subsequent to the second stage, to isolate the electrons in the central reservoir and compress the electrons in the central reservoir from the multi-subband state to the single subband state, wherein the central reservoir is in communication with a second reservoir; and ejecting excess heat in the central reservoir, generated during the third stage, into the second reservoir when the device operates at a fourth stage responsive to the device operating at the third stage. 13. The method of claim 12 , further comprising: cyclically operating the device between the first stage and the fourth stage. 14. The method of claim 12 , wherein the device operates at frequencies in the Megahertz (MHz) range. 15. The method of claim 12 , wherein the device comprises a dimension in a range of 5 millimeters by 5 millimeters by 0.5 millimeters. 16. The method of claim 12 , wherein the electrons include a first temperature when the first stage begins and include a second temperature when the first stage ends. 17. The method of claim 16 , wherein the second temperature is one third of the first temperature. 18. The method of claim 12 , wherein the device comprises a layer formed of aluminum arsenide. 19. The method of claim 18 , wherein the layer formed of aluminum arsenide comprises a miscut angle. 20. A device, comprising: a central reservoir configured to isolate electrons; a first reservoir in communication with the central reservoir; and a second reservoir in communication with the central reservoir, wherein the electrons are isolated in the central reservoir and expanded from a single-valley state into a triple-valley state when the device is selectively operated at a first stage, wherein heat from the first reservoir is exchanged with the central reservoir when the device operates a second stage responsive to the device operating at the first stage, wherein the electrons are isolated and compressed in the central reservoir from the triple-valley state to the single valley state when the device is selectively operated at a third stage subsequent to the heat being exchanged between the first reservoir and the central reservoir, and wherein excess heat in the central reservoir generated during the second stage is ejected into the second reservoir when the device operates at a fourth stage responsive to the device operating at the third stage.
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