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Structurally triggered orbital and charge orderings in TlMnO$_3$ and related compounds
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abstract
Rare earth perovskites ($R^{3+}$M$^{3+}$O$_3$), with $e_g^1$ electronic occupation of the M $d$ states, display different types of metal-insulator transition. For manganites (M=Mn), metal-insulator transition is usually induced by the Jahn-Teller ($JT$) distortions, which stabilize orbital orderings (OO) at Mn sites. Among them, LaMnO$_3$ shows a $C$ type OO and crystallizes with $Pbnm$ structure. Whereas, TlMnO$_3$ shows a very distinct $G$ type OO with an unusual $P\overline{1}$ structure. Employing first principles calculations, and symmetry mode analysis we rationalize structural and electronic origin of $G$-type OO in TlMnO$_3$. Going further, we consider nickelates (M=Ni), where metal-insulator transition is driven by a breathing distortion, which stabilizes the charge ordering (CO) at Ni sites. Interestingly, different $JT$ and breathing distortions are very similar MO$_6$ octahedral distortions and stem from high frequency phonon modes of ideal $Pm\overline3m$ structure. Our comparative study reveals that following a common triggering mechanism these modes appear in their respective ground states.
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Rational Control of Magnonic and Electronic Band Splittings
In MnF2, structural distortions along the A2u and A1g phonon modes tune and can switch off both electronic and magnon band splittings without changing the antiferromagnetic order.
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