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Quantum Computing with Trapped Ion Hyperfine Qubits

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Optical qubits - derived from ground state and an excited metastable state ... Penning trap: using a constant magnetic field and a constant electric field ... – PowerPoint PPT presentation

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Title: Quantum Computing with Trapped Ion Hyperfine Qubits


1
Quantum Computing with Trapped Ion Hyperfine
Qubits
2
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

3
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

4
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

5
Ponderomotive pseudopotential
Oscillation frequency of ion
6
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7
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

8
?e
egt
9
Initialization and detection of qubits
  • Standard optical pumping to initialize HF qubits
    to either or
  • Polarized laser beam resonant with spacing level
    scatter either or

10
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11
HF Qubit Rotations Single Qubit Gates
  • Microwave with frequency ?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 ? from
    excited state and differing in frequency by
    ?HF, ?gtgt?e
  • - SRT Rabi frequency OSRTg1g2/ ?
  • - individual qubits rotation can be achieved

12
Interactions between HF qubits entangling qubit
gates
  • Interaction Hamiltonian
  • Motion-sensitive stimulated Raman transitions
  • Spin-dependent optical forces

13
Motion-sensitive stimulated Raman transitions
Rotating wave approximation

14
k-1
J-C Hamiltonian
15
Spin-dependent optical forces
  • Laser beams dipole force depends upon the state
    of the qubit Sgt 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.

16
With an intensity gradient (focusing or standing
wave)
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