 | This article is an
orphan, as no other articles
link to it. Please
introduce links to this page from
related articles; try the
Find link tool for suggestions. (June 2024) |
| Identifiers | |
|---|---|
3D model (
JSmol)
|
|
| |
| Properties | |
| H3LiIr2O6 | |
Except where otherwise noted, data are given for materials in their
standard state (at 25 °C [77 °F], 100 kPa).
| |
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]
- ^ "Researchers detail how disorder alters quantum spin liquids, forming a new phase of matter". Brown University. 2024-06-10. Retrieved 2024-06-23.
-
^ 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.
PMC
10439105.
PMID
37596328.
This article incorporates text from this source, which is under a
CC BY 4.0 license.
| This article is an
orphan, as no other articles
link to it. Please
introduce links to this page from
related articles; try the
Find link tool for suggestions. (June 2024) |
| Identifiers | |
|---|---|
3D model (
JSmol)
|
|
| |
| Properties | |
| H3LiIr2O6 | |
Except where otherwise noted, data are given for materials in their
standard state (at 25 °C [77 °F], 100 kPa).
| |
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]
- ^ "Researchers detail how disorder alters quantum spin liquids, forming a new phase of matter". Brown University. 2024-06-10. Retrieved 2024-06-23.
-
^ 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.
PMC
10439105.
PMID
37596328. This article incorporates text from this source, which is under a
CC BY 4.0 license.