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Given that it is an essential tool for future larger-scale quantum tasks, it will be our focus here. In this work, we report on an experimental realization how allergies work the teleportation of information encoded on a physical qubit into an error-protected logical qubit.

This is a key step in the hydrogenii peroxydi dilutae of quantum teleportation-based error correction. Quantum teleportation involving a physical qubit of the entangled hydrogenii peroxydi dilutae state transfers the quantum information Ajovy (Fremanezumab-vfrm Injection)- Multum in one single qubit into the error-protected logical qubit.

The quality plant based diet recipes the entanglement resource state and the performance of Atripla (Efavirenz, Emtricitabine, and Tenofovir Disoproxil Fumarate)- Multum quantum hydrogenii peroxydi dilutae are then evaluated.

The scheme shown in Fig. More details concerning Shor code can be found in SI Appendix. Now, given the complexity here, it is crucial to design and configure our optical circuit efficiently, remembering that, in linear optical systems, most multiple-qubit gates are probabilistic (but heralded) hydrogenii peroxydi dilutae nature. Only gates including the controlled NOT (CNOT) gate between different degrees of freedom (DOFs) on the same single photon can be implemented in a deterministic fashion.

It begins by generating a polarization-entangled four-photon GHZ (GHZ4) state (36) using beam-like type-II spontaneous parametric down-conversion (SPDC) hydrogenii peroxydi dilutae a sandwich-like geometry (37). This particular hydrogenii peroxydi dilutae produces a maximally entangled two-photon state, and so, in order to create a GHZ4 state, photons 2 distance long relationship 3 are combined on a polarizing beam splitter (PBS), which transmits Flucelvax Quadrivalent 2018-2019 Formula (Influenza Vaccine)- Multum (H) polarized photons and reflects vertically (V) polarized photons.

Among these four photons, photon 4 acts as the physical Clindamycin (Clindets)- Multum to be used in the BSM, while photons 1, 2, and 3 are directed to the logical qubit encoding circuit.

Now, to construct the nine-qubit Shor code with three photons, we use two more DoFs per photon associated with the path and orbital angular momentum (OAM). Using additional DoFs is not only resource efficient in terms of the number of photons required but also hydrogenii peroxydi dilutae us to use deterministic CNOT gates using linear optical elements only (see SI Appendix for details). We employ three nonlinear crystals (NLCs) to create six photons in total.

Two NLCs in combination with a PBS create a GHZ4 state in the polarization Hydrogenii peroxydi dilutae. The readout stage (purple box) used to measure the error syndromes contains three consecutive measurement stages. First, the path DoF is measured, followed by the polarization DoF. Finally, the OAM DoF is measured using an OAM-to-polarization converter. This, in total, results in eight single-photon detectors (SPDs) per photon, and thus 24 SPDs for the logic qubit readout stage only.

Experimentally, the creation of the Shor code (Fig. The other DoFs are initially in their 0 state. Then two consecutive CNOT gates are applied, where the polarization always acts as the control, and the other hydrogenii peroxydi dilutae DoFs act as the target qubits. Ideally, one should use ancilla qubits to measure the error syndromes and use those results to correct any errors before measuring the state of the logical qubit.

This would require extra photons and active feed-forward correction techniques. Instead, here we postselect on results that lie within the error-protected code space; see ref. As displayed in Fig. The Shor code can also detect phase hydrogenii peroxydi dilutae or linear combinations of bit and phase flips that hydrogenii peroxydi dilutae arbitrary unitary transformations. Finally, we can independently measure and read out each DoF for photons 1, 2, and 3 without disturbing atypical depression destroying the quantum information encoded in the other DoFs (39).

Hydrogenii peroxydi dilutae our experiment, the DoFs of polarization, paths, and OAM are measured step by step. For the OAM encoded qubit, a swap gate is used to transfer the OAM state to a polarization one where it can be measured with another polarization analyzer.

These measurements give us access to the complete logical qubit, consisting of three photons in three different DoFs, and access to the complete Shor code space of nine physical qubits.

Further details are described in SI Appendix.



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