Quantum Computing with Trapped Ion Hyperfine Qubits.

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Presentation transcript:

Quantum Computing with Trapped Ion Hyperfine Qubits

General requirements A scalable system of well-defined qubits A method to reliably initialize the quantum system Long coherence times Existence of universal gates An efficient measurement scheme

Type of qubits for trapped ion Optical qubits - derived from ground state and an excited metastable state separated by an optical frequency Hyperfine qubits - derived from electronic ground-state hyperfine levels separated by a microwave frequency

Ion traps Quadrupole ion trap: using DC and radio frequency (RF) ~1 MHz oscillating AC electric fields Penning trap: using a constant magnetic field and a constant electric field

Ponderomotive pseudopotential Oscillation frequency of ion

Trapped ion hyperfine qubits Electric field perturbations are small Magnetic field perturbations can be reduced by coherence between two internal levels Extremely long radioactive lifetime

γeγe | e>

Standard optical pumping to initialize HF qubits to either or Polarized laser beam resonant with spacing level scatter either or Initialization and detection of qubits

HF Qubit Rotations: Single Qubit Gates Microwave with frequency ω HF Big wavelength ~cm - good for joint rotations of all qubits - difficult for individual qubits rotation. Stimulated Raman Transitions (STR) - two laser fields with detuning Δ from excited state and differing in frequency by ω HF, Δ>>γ e - SRT Rabi frequency: Ω SRT =g 1 g 2 * / Δ - individual qubits rotation can be achieved

Interactions between HF qubits: entangling qubit gates Interaction Hamiltonian Motion-sensitive stimulated Raman transitions Spin-dependent optical forces

Motion-sensitive stimulated Raman transitions Rotating wave approximation :

J-C Hamiltonian k=-1

Spin-dependent optical forces Laser beams’ dipole force depends upon the state of the qubit |S> and certain excited state (atomic selection rules). Appropriate polarization of the light. Use intensity gradient of a laser beam or standing wave to control the motion of ion.

With an intensity gradient (focusing or standing wave)