Early investigations on vanadium in the cubic 3C-SiC polytype concluded that the luminescence of the center is not possible because the excited state is degenerate with the conduction band. However, later work refuted this notion, demonstrating a doublet in photoluminescence (PL) at <^>1493-1495 nm, apparently associated with vanadium (V). In this work, we undertake a detailed experimental and theoretical study of the V center in 3C-SiC. We show that the vanadium PL can be seen as a recombination of an exciton bound to V, in contrast to the other two common hexagonal polytypes (4H-and 6H-SiC), where the PL is due to an interatomic transition of the 3d electron within the V center, according to a well-established model. We also show that the splitting observed in the PL lines is likely not inherent to the center and is due to stress present in the samples. Ideally, in a strain-free 3C-SiC material, the vanadium PL will comprise a single line, which makes the V center in this polytype attractive for applications as a qubit at moderate temperatures. This contrasts with the hexagonal polytypes where the splitting of the zero-phonon line is inherent to the center due to the crystal structure, which has a negative effect on the spin coherence at liquid helium temperature, and millikelvin temperatures are needed to improve the spin coherence.

The divacancy comprising two neighboring vacant sites in the SiC lattice is a promising defect for applications in quantum technology. So far, most research has focused on the divacancy in 4H-SiC, whereas the divacancies in 6H- and 3C-SiC have received much less attention. Here, we outline arguments showing that the neutral charge state of the divacancies in the latter two polytypes is intrinsically stable, in contrast to that in 4H-SiC, where the photoluminescence quenches in most materials for certain excitation energies (below approximately 1.3 eV). Divacancies in 6H- and 3C-SiC are anticipated to remain stable for all excitation energies above resonant excitation. We provide ab initio calculation results for the charge transfer levels of divacancies in 6H- and 3C-SiC. We also show that the luminescence from the divacancy in 3C-SiC vanishes with increasing temperature toward room temperature because of the proximity of the excited state to the conduction band.

Charge state instability is a common problem of color centers in silicon carbide (SiC). In this wide-bandgap semiconductor, which is naturally n-type due to incorporation of the N shallow donor during the crystal growth, deep defects and impurities are singly, doubly, or even triply negatively charged, that is, in optically inactive charge states (dark states). Optical excitation is commonly used for activation and stabilization of their bright state. In this chapter, an overview of charge state control of common color centers in SiC, such as the negative Si vacancy, neutral divacancy, and neutral vanadium, is given. The competition between processes of electron emissions from electron traps related to dominant defects in the upper half of the bandgap and electron trapping to the ground level of bright states under optical excitation is modeled to explain the photoluminescence decay. Charge state control of ensembles and single emitters of these centers in pure n-type and high-purity semiinsulating materials by optical excitation, defect engineering for tuning the Fermi level, and external electric field are discussed.

Nuclear spins with hyperfine coupling to single electron spins are highly valuable quantum bits. Here we probe and characterize the particularly rich nuclear-spin environment around single silicon vacancy color centers (V2) in 4H-SiC. By using the electron spin-3/2 qudit as a four level sensor, we identify several sets of Si29 and C13 nuclear spins through their hyperfine interaction. We extract the major components of their hyperfine coupling via optical detected nuclear magnetic resonance, and assign them to shells in the crystal via the density function theory simulations. We utilize the ground-state level anticrossing of the electron spin for dynamic nuclear polarization and achieve a nuclear-spin polarization of up to 98±6%. We show that this scheme can be used to detect the nuclear magnetic resonance signal of individual spins and demonstrate their coherent control. Our work provides a detailed set of parameters and first steps for future use of SiC as a multiqubit memory and quantum computing platform.

Spin-active color centers in solids show good performance for quantum technologies. Several transition-metal defects in SiC offer compatibility with telecom and semiconductor industries. However, whether their strong spin-orbit coupling degrades their spin lifetimes is not clear. We show that a combination of a crystal-field with axial symmetry and spin-orbit coupling leads to a suppression of spin-lattice and spin-spin interactions, resulting in remarkably slow spin relaxation. Our optical measurements on an ensemble of Mo impurities in SiC show a spin lifetime T-1 of 2.4 s at 2 K.

Although various defect centers have displayed promise as either quantum sensors, single photon emitters, or light-matter interfaces, the search for an ideal defect with multifunctional ability remains open. In this spirit, we study the dichroic silicon vacancies in silicon carbide that feature two well-distinguishable zero-phonon lines and analyze the quantum properties in their optical emission and spin control. We demonstrate that this center combines 40% optical emission into the zero-phonon lines showing the contrasting difference in optical properties with varying temperature and polarization, and a 100% increase in the fluorescence intensity upon the spin resonance, and long spin coherence time of their spin-3/2 ground states up to 0.6 ms. These results single out this defect center as a promising system for spin-based quantum technologies.

The identification of a microscopic configuration of point defects acting as quantum bits is a key step in the advance of quantum information processing and sensing. Among the numerous candidates, silicon-vacancy related centers in silicon carbide (SiC) have shown remarkable properties owing to their particular spin-3/2 ground and excited states. Although, these centers were observed decades ago, two competing models, the isolated negatively charged silicon vacancy and the complex of negatively charged silicon vacancy and neutral carbon vacancy [Phys. Rev. Lett. 115, 247602 (2015)], are still argued as an origin. By means of high-precision first-principles calculations and high-resolution electron spin resonance measurements, we here unambiguously identify the Si-vacancy related qubits in hexagonal SiC as isolated negatively charged silicon vacancies. Moreover, we identify the Si-vacancy qubit configurations that provide room-temperature optical readout.

By minority carrier transient spectroscopy on as-grown n-type bulk GaN produced by halide vapor phase epitaxy (HVPE) one hole trap labelled H1 (EV + 0.34 eV) has been detected. After 2 MeV-energy electron irradiation, the concentration of H1 increases and at fluences higher than 5×10¹⁴ cm^-2, a second hole trap labelled H2 is observed. Simultaneously, the concentration of two electron traps, labelled T1 (E_C - 0.12 eV) and T2 (E_C - 0.23 eV) increases. By studying the increase of the concentration versus electron irradiation fluences, the introduction rate of T1 and T2 using 2 MeV-energy electrons was determined to 7X10^-3 cm^-1 and 0.9 cm^-1, respectively. Due to the low introduction rate of T1 and the low threading dislocation density in the HVPE bulk GaN material, it is suggested that the defect is associated with a primary defect decorating extended structural defects. The high introduction rate of the trap H1 suggests that the H1 defect is associated with a primary intrinsic defect or a complex.

Using medium- and high-resolution multi-spectra fitting of deep level transient spectroscopy (DLTS), minority carrier transient spectroscopy (MCTS), optical O-DLTS and optical-electrical (OE)-MCTS measurements, we show that the EH_6∕7 deep level in 4H-SiC is composed of two strongly overlapping, two electron emission processes with thermal activation energies of 1.49 eV and 1.58 eV for EH₆ and 1.48 eV and 1.66 eV for EH₇. The electron emission peaks of EH₇ completely overlap while the emission peaks of EH₆ occur offset at slightly different temperatures in the spectra. OE-MCTS measurements of the hole capture cross section σ_{p 0}(T) in p-type samples reveal a trap-Auger process, whereby hole capture into the defect occupied by two electrons leads to a recombination event and the ejection of the second electron into the conduction band. Values of the hole and electron capture cross sections σ_n(T) and σ_p(T) differ strongly due to the donor like nature of the deep levels and while all σ_n(T) have a negative temperature dependence, the σ_p(T) appear to be temperature independent. Average values at the DLTS measurement temperature (∼600 K) are σ_{n 2}+(T) ≈ 1 × 10⁻¹⁴ cm², σ_n +(T) ≈ 1 × 10⁻¹⁴ cm², and σ_{p 0}(T) ≈ 9 × 10⁻¹⁸ cm² for EH₆ and σ_{n 2}+(T) ≈ 2 × 10⁻¹⁴ cm², σ_n +(T) ≈ 2 × 10⁻¹⁴ cm², σ_{p 0}(T) ≈ 1 × 10⁻²⁰ cm² for EH₇. Since EH₇ has already been identified as a donor transition of the carbon vacancy, we propose that the EH_6∕7 center in total represents the overlapping first and second donor transitions of the carbon vacancy defects on both inequivalent lattice sites.