4.6 Article

Resonant optical spectroscopy and coherent control of Cr4+ spin ensembles in SiC and GaN

Journal

PHYSICAL REVIEW B
Volume 95, Issue 3, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.95.035207

Keywords

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Funding

  1. U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Materials Sciences and Engineering Division (LDRD program at Argonne National Laboratory)
  2. Air Force Office of Scientific Research [AFOSR FA9550-14-1-0231, AFOSR MURI FA9550-15-1-0029]
  3. Army Research Office [W911NF-15-2-0058]
  4. National Science Foundation [DMR-1306300]
  5. Linkoping Linnaeus Initiative for Novel Functional Materials (LiLi-NFM) [VR 349-2006-176]
  6. Knut and Alice Wallenberg Foundation [KAW 2013.0300]

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Spins bound to point defects are increasingly viewed as an important resource for solid-state implementations of quantum information and spintronic technologies. In particular, there is a growing interest in the identification of new classes of defect spin that can be controlled optically. Here, we demonstrate ensemble optical spin polarization and optically detected magnetic resonance (ODMR) of the S = 1 electronic ground state of chromium (Cr4+) impurities in silicon carbide (SiC) and gallium nitride (GaN). Spin polarization is made possible by the narrow optical linewidths of these ensembles (<8.5 GHz), which are similar in magnitude to the ground state zero-field spin splitting energies of the ions at liquid helium temperatures. This allows us to optically resolve individual spin sublevels within the ensembles at low magnetic fields using resonant excitation from a cavity-stabilized, narrow-line width laser. Additionally, these near-infrared emitters possess exceptionally weak phonon sidebands, ensuring that >73% of the overall optical emission is contained with the defects' zero-phonon lines. These characteristics make this semiconductor-based, transition metal impurity system a promising target for further study in the ongoing effort to integrate optically active quantum states within common optoelectronic materials.

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