Efficient High-Dimensional Entangled State Analyzer with Linear Optics
1QuTech, Delft University of Technology, Delft 2628CJ, Zuid-Holland, The Netherlands
2Instituut-Lorentz, Universiteit Leiden, P.O. Box 9506, 2300 RA Leiden, The Netherlands
3$\langle \text{aQa}^\text{L} \rangle$ Applied Quantum Algorithms Leiden, The Netherlands
4Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA
| Published: | 2025-04-18, volume 9, page 1711 |
| Editor: | Aaron Goldberg |
| Eprint: | arXiv:2401.15066v3 |
| Doi: | https://doi.org/10.22331/q-2025-04-18-1711 |
| Citation: | Quantum 9, 1711 (2025). |
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Abstract
The use of higher-dimensional photonic encodings (qudits) instead of two-dimensional encodings (qubits) can improve the loss tolerance and reduce the computational resources of photonic-based quantum information processing. To harness this potential, efficient schemes for entangling operations such as the high-dimensional generalization of a linear optics Bell measurement will be required. We show how an efficient high-dimensional entangled state analyzer can be implemented with a linear optics interferometer and auxiliary photonic states. The degree of entanglement of the auxiliary state is much less than in previous protocols as quantified by an exponentially smaller Schmidt rank. In addition, the auxiliary state only occupies a single spatial mode, allowing it to be generated deterministically from a single quantum emitter coupled to a small qubit register. The reduced complexity of the auxiliary states results in a high robustness to imperfections and we show that auxiliary states with fidelities above 0.9 for qudit dimensions 4 can be generated in the presence of qubit error rates on the order of 10%. This paves the way for experimental demonstrations with current hardware.

Featured image: Overview of a $d$-dimensional entangled state analyzer (ESA) of time-bin encoded qudits in spatial modes $a$ and $b$. The protocol uses $d-2$ auxiliary photons in one input mode $x_0$ to the quantum Fourier transform (QFT), the other input modes $x_1, x_2, \ldots, x_{d-3}$ contain vacuum as indicated by $\emptyset$. The QFT of the spatial modes can be implemented with standard linear optical elements. Finally, the output modes are measured with $d$ single photon detectors labeled $0, 1, \ldots d-1$. The condition for a successful ESA is to measure all photons in different time-bins and the resulting entangled state projection is determined by the specific detection pattern of the detectors.
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