The nitrogen-vacancy center in diamond

The prototype point-defect qubit is the nitrogen-vacancy (NV) center in diamond,^{Reference Davies and Hamer8,Reference Gali, Janzén, Deak, Kresse and Kaxiras14} which consists of a nitrogen impurity next to a carbon vacancy (Figure 1d); this center can be initialized, manipulated, and read out at room temperature using optical and microwave excitations, and electric and magnetic fields.^{Reference Manson, Harrison and Sellars15}Figure 2 illustrates the electronic structure of this center, as calculated using hybrid DFT.^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom16}

Figure 2.

(a) Electronic structure of the negatively charged nitrogen-vacancy (NV) center (NV^–1) in diamond, as calculated with hybrid density functional theory.^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom16} Optical excitation (vertical green arrow) can lift an electron out of the spin-down a₁(2) state into an e _x/e _y state. (b) Calculated configuration coordinate diagram for the NV center. The lower curve indicates the energy of the defect in its electronic ground-state configuration (³A₂) as a function of a generalized coordinate, which measures the displacements of atoms. The upper curve corresponds to the ³E excited state. The zero-phonon line (ZPL) represents a transition between the two configurations in their relaxed atomic configurations; the intensity of this ZPL tends to be weak if these atomic configurations are very different (i.e., if large relaxations occur). Peaks in the optical absorption and emission curves will correspond to the “vertical” transitions (green and red arrows) for which the atomic positions remain fixed. Adapted from Reference 16.

The positioning of the defect states within the gap follows the generic pattern of Figure 1d (with the addition of spin polarization), but quantitative differences occur. For instance, the a ₁(1) states are not located within the bandgap but are resonant in the valence band. These bonding states do not play a direct role in the functionality as a spin center, and hence their energy is not directly relevant. The states that are of key importance are the spin-down a ₁(2) and e _x, e _y states: Laser light of appropriate wavelength can cause a spin-conserving transition in which a spin-down electron is excited from an a ₁(2) state to an e _x/e _y state; this corresponds to excitation from an ³A₂ ground state to an ³E excited state. The details of the operation of the NV center require a description in terms of such multiparticle states; this is described in great detail in a series of articles in the February 2013 issue of MRS Bulletin.^{Reference Acosta and Hemmer17} However, the single-particle picture presented in Figure 2 is sufficient to discuss the basic features of the NV center that are key to designing similar point-defect centers. The defect states follow the pattern of Figure 1d, but spin polarization leads to different energies for spin-up and spin-down states. Six electrons need to be accommodated in the defect states: Each dangling bond on a C atom contributes one electron, while the dangling bond on the N atom contributes two electrons due to the higher valence of nitrogen. In addition, an extra electron (provided by donors elsewhere in the material) is present that puts the center in a negative charge state. Filling the electronic states in order of increasing energy leads to the occupation shown in the figure, resulting in a spin-1 (triplet) state for the center.

The optical excitation energy corresponding to the transition depicted by the arrow in Figure 2a is evaluated by constraining the occupation to that of the excited state while keeping the atomic positions fixed to those of the ground state. The calculated energy difference (2.27 eV) is expected to yield the peak energy of the absorption spectrum, since electronic transitions occur on a time scale much faster than atomic relaxations. If we subsequently allow the atomic positions to relax, maintaining the excited-state triplet electronic configuration, we obtain a relaxation energy of 0.25 eV (the “Frank–Condon shift”), as illustrated in the diagram in Figure 2b. This configuration coordinate diagram allows the assessment of key features of optical absorption and emission processes for a point defect in which there may be significant differences in the atomic configurations of ground state and excited state.^{Reference Van de Walle and Neugebauer11} The energy difference between the excited state and the ground state, both with relaxed atomic configurations, corresponds to the zero-phonon line, calculated here to be 2.02 eV, and compares well with experiment, which reported a value of 1.945 eV.^{Reference Davies and Hamer8} We also obtain the peak emission energy, at 1.80 eV, in good agreement with the experimental value of 1.76 eV.^{Reference Davies and Hamer8}

The good agreement with experiment (to within 0.1 eV) is particularly impressive given that the calculations are completely ab initio and involved no fitting to any experimental quantities. In addition to optical emission, a non-spin-conserving decay path also exists that includes a nonradiative transition to an intermediate spin-singlet ¹A₁ state. This transition plays a key role since it allows the center to be optically initialized into a specific spin sublevel. Recent calculations and experiments place the ¹A₁ state 1.19 eV above the ³A₂ ground state.^{Reference Toyli, Christie, Alkauskas, Buckley, Van de Walle and Awschalom18}

Criteria for point defects to function as qubits

The thorough and quantitative understanding achieved for the NV center in diamond renders it an ideal prototype for generating a list of design criteria that other qubit candidates should satisfy.^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom16} The highly localized nature of the bound states of the NV center is critical in making a robust qubit and isolating the center from sources of decoherence; indeed, coherence times of over half a second have recently been demonstrated.^{Reference Bar-Gill, Pham, Jarmola, Budker and Walsworth19} In combination with on-chip microwave-frequency waveguides that enable quantum-control operations on sub-nanosecond time scales,^{Reference Fuchs, Dobrovitski, Toyli, Heremans and Awschalom20} tens of millions of coherent operations can be performed within this spin coherence time.

The localized nature of the NV-center wave functions is directly related to the position of the relevant states within the bandgap: States that are close to, or resonant with, the conduction or valence bands of the host will more strongly interact with the extended states and be more delocalized. It is the energetic separation of band-to-band and defect-to-band from intra-defect optical transitions that allows the defect to be initialized and measured with high fidelity at room temperature and even well above room temperature.^{Reference Toyli, Christie, Alkauskas, Buckley, Van de Walle and Awschalom18} This offers significant advantages over qubit implementations that require initialization by thermal equilibration and need cryogenic temperatures to operate. The energy difference between ground and excited states must also be large to avoid thermal excitations, avoiding the destruction of spin information.

In addition to the energetic position of the defect states, the occupation of these states is also important. To function as a single-spin center, the defect must be stable in a paramagnetic ground state. As illustrated previously for the NV center (see Figure 2), this involves an exercise in electron counting: placing electrons in states of increasing energy and checking the spin state for each of those configurations. We saw that for the NV center, the desired S = 1 state required an overall negative charge state of the center; by fortunate coincidence, the Fermi level in nitrogen-doped diamond (which is determined by isolated N atoms acting as deep donors) occurs at the right energy to put the NV center in a singly negative charge state. However, for other defects being considered as qubits, one may not be so lucky, and obtaining the correct spin state (and hence charge state) may require separate manipulation of the Fermi level through judicious incorporation of donors or acceptors. An example in the case of SiC is mentioned later in the text.

In addition to the ground state, the electronic structure of the defect must allow for an excited state positioned within the bandgap and accessed via a spin-conserving intra-defect optical transition. As alluded to earlier, the presence of a non-spin-conserving decay path can be important for initialization; the nature of these nonradiative transitions is still a subject of active research, which currently renders it difficult to formulate specific criteria that would ensure that such a path be present. Finally, if the qubit is to be probed by the luminescence from an excited state, the transition should be spin-conserving, and the strength of this transition should be large enough to enable efficient, high fidelity measurement of individual defect states.

As for the host material, a wide bandgap is desirable if band-to-band and defect-to-band transitions are to be avoided. Bandgaps as well as other relevant properties of some tetrahedrally coordinated hosts are listed in Table I. The host should exhibit small spin-orbit coupling in order to avoid decoherence through spin flips of the defect states. The spin-orbit splitting of the valence-band maximum can be taken as indicative of the strength of the spin-orbit interaction. Also, the constituent elements should have naturally occurring isotopes of zero nuclear spin, making it possible to eliminate spin bath effects. Host materials that are available in single-crystal form are preferred, either as bulk crystals or epitaxial layers; high structural quality is essential to suppress interactions with point defects or extended defects, or with paramagnetic impurities that could affect the defect spin state. The ability to easily process the host material (e.g., with standard wet etching techniques) is also an asset when considering future device development.

Table I.

Relevant properties of potential host materials.

All experimental values are from Madelung,^{Reference Madelung21} unless explicitly cited otherwise. Spin-orbit splitting values are for low temperatures, except in cases where room temperature (RT) is indicated.

Defects with optical transitions in the near-infrared (0.89–1.65 eV) or visible (1.65–3.10 eV) regions of the spectrum are favored because of the ready availability of optical equipment compatible with these energies. The requirement that defect states lie well away from the band edges then points toward host materials that have sufficiently wide bandgaps. Such hosts will typically be fairly ionic and/or contain constituents taken from the first few rows of the periodic table. Diamond, with a bandgap of 5.5 eV, clearly fits; and staying with the Group IV elements, SiC is an obvious candidate. Among compounds, oxides tend to have large gaps and may satisfy a number of the other criteria such as zero nuclear spin. Nitrides such as GaN and AlN also have large bandgaps, and availability of these materials is rapidly increasing due to their use for solid-state lighting and power electronics. Nitrogen does not have zero nuclear spin, but this is not necessarily a strict requirement.

Qubits in SiC

Silicon carbide is closely related to diamond in structural and electronic properties. It is tetrahedrally coordinated, every C being surrounded by four Si atoms, and vice versa. A silicon vacancy in SiC is therefore surrounded by four C atoms and may be expected to exhibit behavior very similar to a vacancy in diamond. The most common polytypes, 4H- and 6H-SiC, have wide bandgaps of 3.27 eV and 3.02 eV, respectively.^{Reference Madelung21} The use of defects in SiC for spintronics was proposed by Gali in 2010,^{Reference Gali, Gällström, Son and Janzén22} and recent experiments have demonstrated that certain defects in SiC exhibit optically addressable spin states with long coherence times.^{Reference Falk, Buckley, Calusine, Koehl, Dobrovitski, Politi, Zorman, Feng and Awschalom23,Reference Koehl, Buckley, Heremans, Calusine and Awschalom24} Hybrid functional calculations for the Si vacancy and for an NV center in 4H-SiC have indicated that these defects are indeed promising qubit candidates.^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom16,Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom25}

NV center in SiC

Since a Si vacancy in SiC is expected to behave similarly to a vacancy in diamond, placing an N atom next to the Si vacancy should create a center similar to the NV center in diamond. To obtain a spin-triplet ground state, the (N_C-V_Si) center should be negatively charged.^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom16,Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom25} Hybrid functional calculations have indicated that in 4H-SiC, this requires the Fermi level to lie between 1.60 eV and 2.83 eV above the valence band. Unlike the fortuitously favorable situation in diamond, judicious Fermi-level engineering (through controlled doping) is required here to achieve the desired charge state.

The calculated configuration coordinate diagram for the NV center in 4H-SiC (from Reference 16) is shown in Figure 3. The optical transitions occur at about half the energy of those for the NV center in diamond; for instance, the zero-phonon line (ZPL) of the NV center in 4H-SiC occurs at 1.09 eV, compared with 2.02 eV for the NV in diamond. This difference is due to the larger lattice constant of SiC compared to diamond, which leads to a smaller overlap among the carbon sp³ dangling-bond orbitals, and hence smaller splitting between the a ₁(2) and e levels. This defect has not yet been observed experimentally.

Figure 3.

(a) Electronic structure of the negatively charged nitrogen-vacancy (NV) center (NV^–1) in 4H-SiC, as calculated with hybrid density functional theory. Adapted from Reference 16. The positions of the defect states are qualitatively similar to those in the NV center in diamond (Figure 2a), but they are located closer to the band edges. Filling the electronic states in order of increasing energy leads to the occupation shown in the figure, resulting in a spin-1 (triplet) state for the center. (b) Calculated configuration coordinate diagram for the NV center in 4H-SiC. ZPL, zero-phonon line.

Silicon vacancy in SiC

Silicon vacancies have also been detected in various polytypes of SiC. Three zero-phonon lines in the photoluminescence spectrum of 6H-SiC, located in the near infrared between 1.35 eV and 1.45 eV, have been attributed to silicon vacancies at the three inequivalent sites in 6H-SiC:^{Reference Wagner, Magnusson, Chen, Janźen, Söman, Hallin and Lindström26,Reference Orlinski, Schmidt, Mokhov and Baranov27} V_Si(h), V_Si(k1), and V_Si(k2); “k” and “h” indicate quasi-cubic and quasi-hexagonal sites, respectively. Various first-principles calculations^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom25,Reference Torpo, Nieminen, Laasonen and Pöykkö28} have indicated that V_Si incorporates in a high spin state in 3C- and 4H-SiC and may act as a suitable qubit for quantum computing in these and other polytypes of SiC. Specifically, recent calculations^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom25} show that V_Si^–2 is stable in n-type 4H-SiC and assumes a high spin state, due to the broken tetrahedral symmetry that splits the t₂ states. Calculations also indicate that the charge neutral V_Si is a spin-triplet center, stable in p-type as well as in insulating 4H-SiC (i.e., for Fermi level positions less than 1.4 eV above the valence band).^{Reference Weber, Koehl, Varley, Janotti, Buckley, Van de Walle and Awschalom25} Optical excitation of V_Si preferentially pumps the system into specific spin sublevels of the ground state, as experimentally demonstrated by Soltamov et al.^{Reference Soltamov, Soltamova, Baranov and Proskuryakov29} for 4H- and 6H-SiC.

Divacancy in SiC

The first paramagnetic defect to be coherently manipulated in any polytype of SiC was the divacancy in 4H-SiC.^{Reference Koehl, Buckley, Heremans, Calusine and Awschalom24} Photoluminescence spectra display a number of distinct zero-phonon lines between 1.09 eV and 1.20 eV. Photo-enhanced spin resonance and annealing experiments have indicated that the first four of these peaks, known by the singular label UD-2, can be attributed to the neutral divacancy.^{Reference Gali30,Reference Son, Carlsson, ul Hassan, Janzén, Umeda, Isoya, Gali, Bockstedte, Morishita, Ohshima and Itoh31} This is a charge-neutral defect complex consisting of a carbon vacancy adjacent to a silicon vacancy. Such a defect can assume four different configurations in 4H-SiC, as illustrated in Figure 4. These have been shown to form localized, paramagnetic electronic states that can be spin-polarized with incident light.^{Reference Koehl, Buckley, Heremans, Calusine and Awschalom24}

Figure 4.

Structure of divacancy in 4H-SiC. The complex consisting of a Si vacancy next to a carbon vacancy can occur in four different inequivalent configurations, two axial and two basal. The hh and kk forms of the divacancy are oriented along the c-axis of the crystal, while the hk and kh forms are oriented along the basal bond directions. Adapted from Reference 16.

The divacancy signals can be optically detected and coherently controlled. A pulse of light can polarize all the defect spins in the ensemble, and then the ensemble can be coherently manipulated with pulsed microwaves. Excitation with a second pulse of light and measurement of the photoluminescence intensity (a spin-dependent process) allow for a spin-dependent readout of the qubit state. This procedure can be applied to all four inequivalent forms of the divacancy. Very recently, it has been shown that analogous defect centers exist in 3C- and 6H-SiC, which can also be manipulated and optically measured.^{Reference Falk, Buckley, Calusine, Koehl, Dobrovitski, Politi, Zorman, Feng and Awschalom23} The microscopic nature of these defects is still unknown.