Enhanced superconductivity of fullerenes
US-10418539-B2 · Sep 17, 2019 · US
US9685600B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9685600-B2 |
| Application number | US-201514625219-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 18, 2015 |
| Priority date | Feb 18, 2015 |
| Publication date | Jun 20, 2017 |
| Grant date | Jun 20, 2017 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
Methods for enhancing characteristics of superconductive fullerenes and devices incorporating the fullerenes are disclosed. Enhancements can include increase in the critical transition temperature at a constant magnetic field; the existence of a superconducting hysteresis over a changing magnetic field; a decrease in the stabilizing magnetic field required for the onset of superconductivity; and/or an increase in the stability of superconductivity over a large magnetic field. The enhancements can be brought about by transmitting electromagnetic radiation to the superconductive fullerene such that the electromagnetic radiation impinges on the fullerene with an energy that is greater than the band gap of the fullerene.
Opening claim text (preview).
What is claimed is: 1. A method for enhancing one or more superconductive characteristics of superconductive fullerenes comprising transmitting electromagnetic radiation comprising ultraviolet light, visible light, or infrared light to the superconductive fullerenes, the electromagnetic radiation impinging upon the superconductive fullerenes with an energy that is greater than the band gap of the superconductive fullerenes, wherein the superconductive fullerenes are hydrogenated and intercalated and have the general structure of: Cs a Rb b K c M y C n H x in which M=Hg, Bi, or Tl a, b, c=0-3, y=0-2, wherein at least one of a, b, y is at least 1 n is 20 or greater, and x=about 10 or more. 2. The method of claim 1 , wherein the one or more superconductive characteristics include an increase in the critical transition temperature of the superconductive fullerenes at a constant magnetic field; the existence of a superconducting hysteresis over a changing magnetic field; a decrease in the stabilizing magnetic field required for the onset of superconductivity; and/or an increase in the stability of superconductivity over a magnetic field. 3. The method of claim 2 , wherein the critical transition temperature of the superconductive fullerenes when in photonic communication with the electromagnetic radiation increases by about 10 K or more. 4. The method of claim 2 , wherein the critical transition temperature of the superconductive fullerenes when in photonic communication with the electromagnetic radiation increases by from about 10 K to about 25 K. 5. The method of claim 2 , wherein the critical transition temperature of the superconductive fullerenes when in photonic communication with the electromagnetic radiation is 77 K or greater. 6. The method of claim 2 , wherein a stabilizing magnetic field of the superconductive fullerenes when in photonic communication with the electromagnetic radiation is about 1000 Oe or less. 7. The method of claim 1 , wherein the superconductive fullerenes are halogenated. 8. The method of claim 1 , wherein the superconductive fullerenes are derivatized. 9. The method of claim 1 , wherein the electromagnetic energy impinges on the fullerenes at an energy of about 1 electron Volt or greater. 10. The method of claim 9 , wherein the electromagnetic energy impinges on the fullerenes at an energy of from about 1.3 electron Volts to about 2 electron Volts. 11. The method of claim 1 , wherein x=n−2. 12. A method for enhancing one or more superconductive characteristics of superconductive fullerenes comprising transmitting electromagnetic radiation to the superconductive fullerenes, the electromagnetic radiation impinging upon the fullerenes with an energy that is greater than the band gap of the superconductive fullerenes, wherein the superconductive fullerenes are hydrogenated and intercalated and have the general structure of: Cs a Rb b K c M y C n H x in which M=Hg, Bi, or Tl a, b, c=0-3, y=0-2, wherein at least one of a, b, y is at least 1 n is 20 or greater, and x=about 10 or more. 13. The method of claim 12 , wherein the one or more superconductive characteristics include an increase in the critical transition temperature of the superconductive fullerenes at a constant magnetic field; the existence of a superconducting hysteresis over a changing magnetic field; a decrease in the stabilizing magnetic field required for the onset of superconductivity; and/or an increase in the stability of superconductivity over a magnetic field. 14. The method of claim 13 , wherein the critical transition temperature of the superconductive fullerenes when in photonic communication with the electromagnetic radiation increases by about 10 K or more. 15. The method of claim 13 , wherein the critical transition temperature of the superconductive fullerenes when in photonic communication with the electromagnetic radiation increases by about 10 K to about 25 K. 16. The method of claim 13 , wherein the critical transition temperature of the superconductive fullerenes when in photonic communication with the electromagnetic radiation is 77 K or greater. 17. The method of claim 13 , wherein a stabilizing magnetic field of the superconductive fullerenes when in photonic communication with the electromagnetic radiation is about 1000 Oe or less. 18. The method of claim 12 , wherein the superconductive fullerenes are halogenated. 19. The method of claim 12 , wherein the superconductive fullerenes are derivatized. 20. The method of claim 12 , wherein the electromagnetic energy impinges on the fullerenes at an energy of about 1 electron Volt or greater. 21. The method of claim 12 , wherein the electromagnetic energy impinges on the fullerenes at an energy of from about 1.3 electron Volts to about 2 electron Volts.
Chemistry & Metallurgy · mapped topic
Electricity · mapped topic
Electricity · mapped topic
Fullerene superconductors, e.g. soccer ball-shaped allotropes of carbon, e.g. C60 or C94 · CPC title
After-treatment · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.