Experimental quantum state learning with pairs of photons

• URL: http://arxiv.org/abs/2606.16932v2
• Date: Thu, 18 Jun 2026 16:16:42 GMT
• Title: Experimental quantum state learning with pairs of photons
• Abstract summary: Tomography allows one to estimate the density matrix describing the state an ensemble of quantum systems are prepared in.<n>We experimentally demonstrate this learning-from-pairs concept using photons in the polarization degree of freedom.<n>We investigate our ability to discriminate between two equal mixtures of distinct pairs of polarization states.
• Score: 0.35132824436572685
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Tomography allows one to estimate the density matrix describing the state an ensemble of quantum systems are prepared in (for example, polarization tomography determines the polarization state of a beam of identically prepared photons). In general, it is not possible to uniquely decompose the density matrix into its pure state components. Agarwal et al. proposed a protocol which, for a mixture composed of any two pure states of a qubit (with arbitrary probabilities), allows an observer to infer not only the density matrix but the identity of those specific pure states and their weights - the additional requirement being that the qubits arrive in pairs, where both qubits in each pair are in the same state. We experimentally demonstrate this learning-from-pairs concept using photons in the polarization degree of freedom. We use tomography to measure a sequence of single photons and make use of their time-of-arrival information to 'pair up' the photons after the measurement. From here we are able to infer the photons' polarization states and their respective probabilities, and we demonstrate this for various different choices of polarization states and ratios. Finally, we investigate our ability to discriminate between two equal mixtures of distinct pairs of orthogonal polarization states. We find that on the order of approx. 10e4 photons is typically enough to achieve tomography fidelities of approximately 0.9999. This is sufficient to discriminate between two different preparations of the same mixed state, differing by angles of less than 5 degrees between the pure states used in the two preparations.

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