Laser driving in systems with competing or coupled electronic orders can lead to the enhancement of orders or even to the appearance of hidden phases without an equilibrium analog. Here we consider a model for $A_3{\mathrm{C}}_{60}$ which exhibits a unique interplay between conventional and odd-frequency (or composite) orders. In particular, we show that photodoping of the antiferromagnetic Mott insulating phase, as realized in ${\mathrm{Cs}}_3{\mathrm{C}}_{60}$, results in a paramagnetic gapped state with broken orbital symmetry. This hidden phase, which does not exist under equilibrium conditions, can be interpreted as an odd-frequency orbital-ordered state and is conceptually related to the equilibrium Jahn-Teller metal in more weakly correlated compounds. Our study demonstrates the appearance of pure odd-frequency order via the nonthermal melting of magnetic order and provides an interesting example of nonequilibrium control of electronic orders in a multiorbital system.

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• Electronic structure
• Magnetism
• Phase transitions