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'''H3LiIr2O6''' is a material considered to best fit the archetype for being a special type of [[quantum spin liquid]] called a [[Quantum spin liquid#Kitaev spin liquids|Kitaev spin liquid]]. Though known not to freeze at cold temperatures, H3LiIr2O6 is notoriously difficult to produce in a lab and is known to have disorder in it, muddying whether it was truly a spin liquid. <ref>{{Cite web |date=2024-06-10 |title=Researchers detail how disorder alters quantum spin liquids, forming a new phase of matter |url=https://www.brown.edu/news/2023-09-12/quantum-spin-liquids |access-date=2024-06-23 |website=Brown University |language=en}}</ref> |
'''H3LiIr2O6''' is a material considered to best fit the archetype for being a special type of [[quantum spin liquid]] called a [[Quantum spin liquid#Kitaev spin liquids|Kitaev spin liquid]]. Though known not to freeze at cold temperatures, H3LiIr2O6 is notoriously difficult to produce in a lab and is known to have disorder in it, muddying whether it was truly a spin liquid. <ref>{{Cite web |date=2024-06-10 |title=Researchers detail how disorder alters quantum spin liquids, forming a new phase of matter |url=https://www.brown.edu/news/2023-09-12/quantum-spin-liquids |access-date=2024-06-23 |website=Brown University |language=en}}{{Source-attribution-CC BY 4.0}}</ref> |
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H3LiIr2O6 is considered to be a spin liquid that is proximate to the Kitaev-limit quantum spin liquid. Its ground state shows no magnetic order or spin freezing as expected for the spin liquid state. However, hydrogen zero-point motion and stacking faults are known to be present. <ref>{{Cite journal |last=de la Torre |first=A. |last2=Zager |first2=B. |last3=Bahrami |first3=F. |last4=Upton |first4=M. H. |last5=Kim |first5=J. |last6=Fabbris |first6=G. |last7=Lee |first7=G.-H. |last8=Yang |first8=W. |last9=Haskel |first9=D. |last10=Tafti |first10=F. |last11=Plumb |first11=K. W. |date=2023-08-18 |title=Momentum-independent magnetic excitation continuum in the honeycomb iridate H3LiIr2O6 |url=https://www.nature.com/articles/s41467-023-40769-x |journal=Nature Communications |language=en |volume=14 |issue=1 |pages=5018 |doi=10.1038/s41467-023-40769-x |issn=2041-1723}}</ref> |
H3LiIr2O6 is considered to be a spin liquid that is proximate to the Kitaev-limit quantum spin liquid. Its ground state shows no magnetic order or spin freezing as expected for the spin liquid state. However, hydrogen zero-point motion and stacking faults are known to be present. <ref>{{Cite journal |last=de la Torre |first=A. |last2=Zager |first2=B. |last3=Bahrami |first3=F. |last4=Upton |first4=M. H. |last5=Kim |first5=J. |last6=Fabbris |first6=G. |last7=Lee |first7=G.-H. |last8=Yang |first8=W. |last9=Haskel |first9=D. |last10=Tafti |first10=F. |last11=Plumb |first11=K. W. |date=2023-08-18 |title=Momentum-independent magnetic excitation continuum in the honeycomb iridate H3LiIr2O6 |url=https://www.nature.com/articles/s41467-023-40769-x |journal=Nature Communications |language=en |volume=14 |issue=1 |pages=5018 |doi=10.1038/s41467-023-40769-x |issn=2041-1723}}</ref> |
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Revision as of 09:24, 23 June 2024
H3LiIr2O6 is a material considered to best fit the archetype for being a special type of quantum spin liquid called a Kitaev spin liquid. Though known not to freeze at cold temperatures, H3LiIr2O6 is notoriously difficult to produce in a lab and is known to have disorder in it, muddying whether it was truly a spin liquid. [1]
H3LiIr2O6 is considered to be a spin liquid that is proximate to the Kitaev-limit quantum spin liquid. Its ground state shows no magnetic order or spin freezing as expected for the spin liquid state. However, hydrogen zero-point motion and stacking faults are known to be present. [2]
References
- ^ "Researchers detail how disorder alters quantum spin liquids, forming a new phase of matter". Brown University. 2024-06-10. Retrieved 2024-06-23.
This article incorporates text from this source, which is under a CC BY 4.0 license.
- ^ de la Torre, A.; Zager, B.; Bahrami, F.; Upton, M. H.; Kim, J.; Fabbris, G.; Lee, G.-H.; Yang, W.; Haskel, D.; Tafti, F.; Plumb, K. W. (2023-08-18). "Momentum-independent magnetic excitation continuum in the honeycomb iridate H3LiIr2O6". Nature Communications. 14 (1): 5018. doi:10.1038/s41467-023-40769-x. ISSN 2041-1723.
