LOQC State Generation
Step-by-Step LOQC State Generation
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Photon Source Preparation
Begin with spontaneous parametric down-conversion (SPDC) to generate entangled photon pairs:
\(|\psi\rangle = \frac{1}{\sqrt{2}}(|H\rangle_1|H\rangle_2 + |V\rangle_1|V\rangle_2)\) -
Polarization Encoding
Use wave plates to encode qubits in photon polarization states:
\(|0\rangle \equiv |H\rangle, \quad |1\rangle \equiv |V\rangle\) -
Beam Splitter Operation
Apply a 50:50 beam splitter transformation:
\(\hat{a}^\dagger \rightarrow \frac{1}{\sqrt{2}}(\hat{b}^\dagger + \hat{c}^\dagger)\)
\(\hat{d}^\dagger \rightarrow \frac{1}{\sqrt{2}}(\hat{b}^\dagger - \hat{c}^\dagger)\) -
Post-Selection
Detect photons in specific output modes to herald successful state creation (e.g., Bell state generation requires coincidence detection) -
Feed-Forward Correction
Apply conditional phase shifts based on measurement outcomes:
\(U_{ff} = e^{i\pi|1\rangle\langle 1|}\) -
Verification
Perform quantum state tomography to confirm the generated state’s fidelity
Key optical components required:
- Nonlinear crystals (BBO/PPKTP)
- Polarizing beam splitters
- Half-wave and quarter-wave plates
- Single-photon detectors
The entire process can be represented as a quantum circuit:
\(\text{SPDC} \rightarrow \text{BS} \rightarrow \text{PS} \rightarrow \text{PBS} \rightarrow \text{Det.}\)
Where BS = Beam Splitter, PS = Phase Shifter, PBS = Polarizing Beam Splitter, Det. = Detection. The exact sequence depends on the target state (e.g., GHZ, cluster, or graph states).