To overcome the limitations of existing algorithms for solving self-bound quantum many-body problems – such as those encountered in nuclear and particle physics – that access only a restricted subset of energy levels and provide limited structural information, we introduce and demonstrate a novel quantum-classical approach capable of resolving the complete bound-state spectrum. This method also provides the total angular momentum associated with each eigenstate. Our approach is based on expressing the Hamiltonian in second-quantized form within a novel input model combined with a scan scheme, enabling broad applicability to configuration-interaction calculations across diverse fields. We apply this hybrid method to compute, for the first time, the bound-state spectrum together with corresponding values of using a realistic strong-interaction Hamiltonian. Our approach applies to hadron spectra and values solved in the relativistic Basis Light-Front Quantization approach.

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