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arXiv:2610.27223

Comparative Optical Spectroscopy of Er$^{3+}$, Tm$^{3+}$, and Eu$^{3+}$ Molecular Complexes at Cryogenic Temperature

Farhad Rasekh, Sahil, Arsalan Mansourzadeh, Diogo Alves Gálico, David Hunger, Muralee Murugesu, Daniel Oblak

quant-phSubmitted Oct 19, 2026• Announced Oct 21, 2026• 0 citations
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Abstract

Rare-earth molecular complexes are attracting increasing interest for quantum information applications because of their structural flexibility and chemical tunability. Here, we compare the cryogenic optical properties of Er$^{3+}$, Tm$^{3+}$, and Eu$^{3+}$ complexes in the same ligand environment. Optical spectroscopy shows differing behavior across the three systems: spectral hole burning is observed in the Eu$^{3+}$ complex, whereas no measurable hole is detected in the Er$^{3+}$ and Tm$^{3+}$ complexes. We measure laser-induced local heating and rethermalization in the Er$^{3+}$ and Tm$^{3+}$ powder-like samples, observing strong local heating and slow thermal relaxation in the cold-plate cryostat. The recovery occurs over several seconds and, for some Er$^{3+}$ excitation conditions, extends over tens of seconds. The comparison across the three ions nevertheless suggests that heating alone is unlikely to account for the full contrast. Rather, the different behaviors of Eu$^{3+}$, Tm$^{3+}$, and Er$^{3+}$ point to ion-dependent relaxation and decoherence processes associated with their electronic level structure and coupling to the molecular environment. Temperature-dependent linewidth and line-shift measurements are further consistent with phonon-mediated broadening through coupling to crystal-field levels.

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14 pages and 5 figures

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Comparative Optical Spectroscopy of Er3+^{3+}3+, Tm3+^{3+}3+, and Eu3+^{3+}3+ Molecular Complexes at Cryogenic Temperature
Rare-earth molecular complexes are attracting increasing interest for quantum information applications because of their structural flexibility and chemical tunability. Here, we compare the cryogenic optical properties of Er3+^{3+}3+, Tm3+^{3+}3+, and Eu3+^{3+}3+ complexes in the same ligand environment. Optical spectroscopy shows differing behavior across the three systems: spectral hole burning is observed in the Eu3+^{3+}3+ complex, whereas no measurable hole is detected in the Er3+^{3+}3+ and Tm3+^{3+}3+ complexes. We measure laser-induced local heating and rethermalization in the Er3+^{3+}3+ and Tm3+^{3+}3+ powder-like samples, observing strong local heating and slow thermal relaxation in the cold-plate cryostat. The recovery occurs over several seconds and, for some Er3+^{3+}3+ excitation conditions, extends over tens of seconds. The comparison across the three ions nevertheless suggests that heating alone is unlikely to account for the full contrast. Rather, the different behaviors of Eu3+^{3+}3+, Tm3+^{3+}3+, and Er3+^{3+}3+ point to ion-dependent relaxation and decoherence processes associated with their electronic level structure and coupling to the molecular environment. Temperature-dependent linewidth and line-shift measurements are further consistent with phonon-mediated broadening through coupling to crystal-field levels.
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ABSTRACT We present an optical study of near‐surface ensembles in waveguide‐integrated and , investigating how nanophotonic coupling modifies rare‐earth spectroscopy. In particular, we compare bulk excitation with evanescently coupled TE and TM waveguide modes. In , we observe a pronounced polarization‐dependent surface effect. TE‐coupled spectra closely reproduce bulk behavior. In contrast, TM coupling induces strong inhomogeneous broadening and an asymmetric low‐energy shoulder of the site S1 Y1Z1 transition, with linewidths exceeding those of the bulk by more than a factor of four. Temperature‐dependent measurements and surface termination studies indicate that surface charges are the dominant mechanism. remains largely unaffected by mode polarization, and surface termination leads only to minor spectral shifts. These observations suggest that non‐charge‐neutral rare‐earth systems are more susceptible to surface‐induced decoherence sources than charge‐neutral hosts.
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