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Maximum efficiency of a linear-optical Bell-state analyzer
Quantum Physics · Submitted 18 Jul 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show, that within this subclass it is not possible to discriminate unambiguously four equiprobable Bell states with a probability higher than 50 %.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
In a photonic realization of qubits the implementation of quantum logic is rather difficult due the extremely weak interaction on the few photon level. On the other hand, in these systems interference is available to process the quantum states. We formalize the use of interference by the definition of a simple class of operations which include linear optical elements, auxiliary states and conditional operations. We investigate an important subclass of these tools, namely linear optical elements and auxiliary modes in the vacuum state. For this tools, we are able to extend a previous quantitative result, a no-go theorem for perfect Bell state analyzer on two qubits in polarization entanglement, by a quantitative statement. We show, that within this subclass it is not possible to discriminate unambiguously four equiprobable Bell states with a probability higher than 50 %.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In a photonic realization of qubits the implementation of quantum logic is rather difficult due the extremely weak interaction on the few photon level. | background 1.00 | 0.05 | 0.02 | asserted 1.00 |
| s1 | On the other hand, in these systems interference is available to process the quantum states. | background 1.00 | 0.06 | 0.02 | asserted 0.94 |
| s2 | We formalize the use of interference by the definition of a simple class of operations which include linear optical elements, auxiliary states and conditional operations. | method 0.55 | 0.89 | 0.03 | asserted 0.99 |
| s3 | We investigate an important subclass of these tools, namely linear optical elements and auxiliary modes in the vacuum state. | contribution 0.66 | 0.42 | 0.03 | asserted 0.71 |
| s4 | For this tools, we are able to extend a previous quantitative result, a no-go theorem for perfect Bell state analyzer on two qubits in polarization entanglement, by a quantitative statement. | contribution 0.94 | 0.79 | 0.12 | asserted 0.71 |
| s5 | We show, that within this subclass it is not possible to discriminate unambiguously four equiprobable Bell states with a probability higher than 50 %. | result 1.00 | 0.93 | 0.93 | asserted 1.00 |
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Original abstract
In a photonic realization of qubits the implementation of quantum logic is rather difficult due the extremely weak interaction on the few photon level. On the other hand, in these systems interference is available to process the quantum states. We formalize the use of interference by the definition of a simple class of operations which include linear optical elements, auxiliary states and conditional operations. We investigate an important subclass of these tools, namely linear optical elements and auxiliary modes in the vacuum state. For this tools, we are able to extend a previous quantitative result, a no-go theorem for perfect Bell state analyzer on two qubits in polarization entanglement, by a quantitative statement. We show, that within this subclass it is not possible to discriminate unambiguously four equiprobable Bell states with a probability higher than 50 %.
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