Antiferromagnetic ground states, when doped, give rise to rich and complex phenomena, prompting detailed investigations in various spin systems. Here, we study the effect of doping on the one-dimensional $S=1$ antiferromagnetic Heisenberg model. Specifically, we investigate how the presence of holes affects the static and dynamic (frequency-dependent) spin-spin correlations of the two-orbital Hubbard-Kanamori chain. The latter, at half filling and in the strong-interaction limit, maps onto an $S=1$ Heisenberg model. For moderate interactions, an orbital resonating valence bond state emerges up to doping levels of $x\lesssim 0.3$. A detailed analysis of interaction strength $U$ and doping concentration $x$ reveals that this phase inherits the key features of spin excitations found in the half-filled case, namely, a gapped spin spectrum and “coherent” magnon behavior up to a wave vector $q$ determined by the Fermi vector, $2k_{\mathrm{F}}=\pi (1-x)$. Furthermore, our results uncover an additional broad, incoherent spectral weight for $q\gtrsim 2k_{\mathrm{F}}$ at high frequencies. Finally, we show that near the transition to a ferromagnetic phase, a previously unidentified spiral-like state emerges, characterized by spin excitations reminiscent of the $J_1\text{−}{J}_2$ Heisenberg model.

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• Spin dynamics
• Density matrix renormalization group
• Hubbard model
• Quantum spin chains