Transmission Spectroscopy of Molecular Spin Ensembles in the Dispersive Regime

  • Claudio Bonizzoni
    CNR Istituto Nanoscienze Centro S3, via G. Campi 213/A Modena 41125 Italy
  • Alberto Ghirri
    CNR Istituto Nanoscienze Centro S3, via G. Campi 213/A Modena 41125 Italy
  • Shigeaki Nakazawa
    Department of Chemistry and Molecular Materials Science Graduate School of Science Osaka City University 3‐3‐138 Sugimoto Sumiyoshi‐ku Osaka 558‐8585 Japan
  • Shinsuke Nishida
    Department of Chemistry and Molecular Materials Science Graduate School of Science Osaka City University 3‐3‐138 Sugimoto Sumiyoshi‐ku Osaka 558‐8585 Japan
  • Kazunobu Sato
    Department of Chemistry and Molecular Materials Science Graduate School of Science Osaka City University 3‐3‐138 Sugimoto Sumiyoshi‐ku Osaka 558‐8585 Japan
  • Takeji Takui
    Department of Chemistry and Molecular Materials Science Graduate School of Science Osaka City University 3‐3‐138 Sugimoto Sumiyoshi‐ku Osaka 558‐8585 Japan
  • Marco Affronte
    CNR Istituto Nanoscienze Centro S3, via G. Campi 213/A Modena 41125 Italy

抄録

<jats:title>Abstract</jats:title><jats:p>The readout in the dispersive regime is originally developed—and it is now largely exploited—for non‐demolitive measurement of super‐ and semiconducting qubits. More recently it has been successfully applied to probe collective spin excitations in ferro(i)magnetic bulk samples or collections of paramagnetic spin centers embedded into microwave cavities. The use of this readout technique within a semiclassical limit of excitation is only marginally investigated although it holds for a wide class of problems, including advanced magnetic resonance techniques. In this work, the coupling between a coplanar microwave resonator and diphenyl‐nitroxide organic radical diluted in a fully deuterated benzophenone single crystal is investigated. Two‐tone transmission spectroscopy experiments demonstrate the possibility to reconstruct the spectrum of the spin system with little loss of sensitivity with respect to the resonant regime. Likewise, pulse sequences of detuned microwave frequency allow the measurement of the spin‐lattice relaxation time (<jats:italic>T</jats:italic><jats:sub>1</jats:sub>). The independent tunability of the probe and the drive power enables one to adjust the signal‐to‐noise ratio of the spectroscopy. These results suggest that electron spin dispersive spectroscopy can be used as a complementary tool of electron spin resonance to investigate the spin response.</jats:p>

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