Abstract: A quantum processing system is disclosed. In one embodiment, a quantum processing system comprises: a plurality of donor atoms positioned in a silicon crystal substrate, each donor atom positioned at a donor site; and a plurality of conductive control electrodes arranged about the donor atoms to operate the donor atoms as qubits. Where, at least two pairs of nearest neighbour donor atoms of the plurality of donor atoms are arranged along the [110] direction of the silicon crystal substrate and are configured to operate as qubits.

Abstract: A quantum processing system is disclosed. In one embodiment, a quantum processing system comprises: a plurality of donor atoms positioned in a silicon crystal substrate, each donor atom positioned at a donor site; and a plurality of conductive control electrodes arranged about the donor atoms to operate the donor atoms as qubits. Where, at least two pairs of nearest neighbour donor atoms of the plurality of donor atoms are arranged along the [110] direction of the silicon crystal substrate and are configured to operate as qubits.

Abstract: This disclosure concerns photonics and in particular the addressing of individual targets in solids. In aspect one there is provided a device comprising a solid substrate with one or more atomic scale targets in the substrate. A laser light is focused on a region of the substrate that contains a single target to selectively cause photoionization of the target. A charge sensor with sub-electron charge sensitivity is focussed on measuring the charge in the region of the substrate that contains a single target. In use, the device operates such that the laser is turned on to cause photoionization of the target, and the charge sensor detects the change in charge in the region of the substrate that contains the single target. In another aspect is the method for optically investigating individual nuclear spin states of single atoms by investigating both the Zeeman effect and the hyperfine interaction of the single atoms.

Abstract: The present disclosure provides a quantum processor realized in a semiconductor material and method to operate the quantum processor to implement adiabatic quantum computation. The quantum processor comprises a plurality of qubit elements disposed in a two-dimensional matrix arrangement. The qubits are implemented using the nuclear or electron spin of phosphorus donor atoms. Further, the processor comprises a control structure with a plurality of control members, each arranged to control a plurality of qubits disposed along a line or a column of the matrix. The control structure is controllable to perform adiabatic quantum error corrected computation.

Abstract: The present disclosure provides a quantum processor realized in a semiconductor material and method to operate the quantum processor to implement error corrected quantum computation. The quantum processor comprises a plurality of qubit elements disposed in a two-dimensional matrix arrangement. The qubits are implemented using the nuclear or electron spin of phosphorus donor atoms. Further, the processor comprises a control structure with a plurality of control members, each arranged to control a plurality of qubits disposed along a line or a column of the matrix. The control structure is controllable to perform topological quantum error corrected computation.

Abstract: A quantum computer comprises of at least one qubit formed from holes created with acceptor atoms (10) in crystalline silicon (12) and a pair of gates (14, 16) located above the acceptor atoms (10) to apply direct electric field and alternating electric field for switching, manipulating the qubit such that quantum information resulting from being manipulated is stored from decoherence.

Abstract: A quantum computer comprises of at least one qubit formed from holes created with acceptor atoms (10) in crystalline silicon (12) and a pair of gates (14, 16) located above the acceptor atoms (10) to apply direct electric field and alternating electric field for switching, manipulating the qubit such that quantum information resulting from being manipulated is stored from decoherence.

Abstract: The present disclosure provides a quantum processor realised in a semiconductor material and method to operate the quantum processor to implement error corrected quantum computation. The quantum processor comprises a plurality of qubit elements disposed in a two-dimensional matrix arrangement. The qubits are implemented using the nuclear or electron spin of phosphorus donor atoms. Further, the processor comprises a control structure with a plurality of control members, each arranged to control a plurality of qubits disposed along a line or a column of the matrix. The control structure is controllable to perform topological quantum error corrected computation.

Abstract: The present disclosure provides a quantum processor realised in a semiconductor material and method to operate the quantum processor to implement adiabatic quantum computation. The quantum processor comprises a plurality of qubit elements disposed in a two-dimensional matrix arrangement. The qubits are implemented using the nuclear or electron spin of phosphorus donor atoms. Further, the processor comprises a control structure with a plurality of control members, each arranged to control a plurality of qubits disposed along a line or a column of the matrix. The control structure is controllable to perform adiabatic quantum error corrected computation.

Abstract: This disclosure concerns photonics and in particular the addressing of individual targets in solids. In aspect one there is provided a device comprising a solid substrate with one or more atomic scale targets in the substrate. A laser light is focused on a region of the substrate that contains a single target to selectively cause photoionization of the target. A charge sensor with sub-electron charge sensitivity is focussed on measuring the charge in the region of the substrate that contains a single target. In use, the device operates such that the laser is turned on to cause photoionization of the target, and the charge sensor detects the change in charge in the region of the substrate that contains the single target. In another aspect is the method for optically investigating individual nuclear spin states of single atoms by investigating both the Zeeman effect and the hyperfine interaction of the single atoms.