$\ensuremath{\Lambda}$-hypernuclear magnetic moments have been studied self-consistently in time-odd triaxial relativistic mean-field approach with newly proposed $\ensuremath{\Lambda}$-meson interactions. The $\ensuremath{\omega}\ensuremath{\Lambda}\ensuremath{\Lambda}$ tensor coupling highly reduces the polarized Dirac magnetic moment. The deviation of the magnetic moment from the Schmidt value $\ensuremath{\Delta}\ensuremath{\mu}$ is related to effective nucleon-meson interaction. A large deviation $\ensuremath{\Delta}\ensuremath{\mu}$ with ${l}_{\ensuremath{\Lambda}}\ensuremath{\ne}0$ is found to exist only in medium-mass hypernuclei.
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