Research paper
Theoretical| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Energy Gap | single-particle direct gap at MBZ edge | 0.1meV | — | |||
| Phase Stability | ν = 1/3 FCI in CN scheme | unstable to charge density wave under small band mixing | — | |||
| Phase Stability | ν = 2/3 FCI in AVE scheme | more robust under similar band mixing but suppressed at stronger band mixing | — |
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Energy Gap | single-particle direct gap at MBZ edge | 0.1meV | — | |||
| Phase Stability | ν = 1/3 FCI in CN scheme | unstable to charge density wave under small band mixing | — | |||
| Phase Stability | ν = 2/3 FCI in AVE scheme | more robust under similar band mixing but suppressed at stronger band mixing | — |
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Energy Gap | single-particle direct gap at MBZ edge | 0.1meV | — | |||
| Phase Stability | ν = 1/3 FCI in CN scheme | unstable to charge density wave under small band mixing | — | |||
| Phase Stability | ν = 2/3 FCI in AVE scheme | more robust under similar band mixing but suppressed at stronger band mixing | — |
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Energy Gap | single-particle direct gap at MBZ edge | 0.1meV | — | |||
| Phase Stability | ν = 1/3 FCI in CN scheme | unstable to charge density wave under small band mixing | — | |||
| Phase Stability | ν = 2/3 FCI in AVE scheme | more robust under similar band mixing but suppressed at stronger band mixing | — |