Abstract
As a model of a two-level quantum system interacting with a quantum field, the Unruh-DeWitt detector is introduced and physically motivated. Both the transition probability and transition rate of this detector model are defined and expressed to leading order in terms of the vacuum Wightman function for a scalar field living on a curved spacetime. The entanglement harvesting protocol is introduced in which two detectors begin in a separable state and as a result of their local interaction with the field become entangled. This entanglement is interpreted as being extracted from entanglement present in the vacuum state of the field and is quantified by various measures. The measurement model induced by a collection of such detectors is constructed, identifying the POVMs associated with the field that such a collection of detectors measures.
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Notes
- 1.
In the interaction picture, the interaction Hamiltonian is \(H_{I} := e^{iH_0t} H_{int}e^{-iH_0 t}\).
- 2.
The diagonal elements of H I vanish because \( \left < 0 | \mathbf {X} | 0 \right > = \left < 1 | \mathbf {X} | 1 \right > =0\), which comes from the fact that ψ 0(x) and ψ 1(x) are symmetric around x = 0 due to the Coulomb interaction between the nucleus and electron of the atom being symmetric around x = 0.
- 3.
As stated in [1], a local realist theory is one where physical properties are defined prior to and independent of measurement, and no physical influence can propagate faster than the speed of light.
- 4.
The Svetlichny inequality is a Bell-like inequality whose violation is sufficient but not necessary for genuine tripartite nonlocal correlations [47].
- 5.
The partial transpose of the state \(\rho _{AB} \in \mathcal {S} \left (\mathcal {H}_A \otimes \mathcal {H}_B\right )\) with respect to \(\mathcal {H}_A\) is \(\rho _{AB}^{\Gamma _A}:=\left [{T} \otimes \mathcal {I}\right ] \left ( \rho _{AB} \right )\), where \({T}:~\mathcal {S}(\mathcal {H}_A)~\to ~\mathcal {S}(\mathcal {H}_A)\) is the transposition map.
- 6.
An observable is defined on a measurable space \((\Omega ,\mathcal {F})\), where Ω is a sample space and \(\mathcal {F}\) is a collection of subsets of Ω (\(\mathcal {F}\) is a σ-algebra); \((\Omega ,\mathcal {F})\) is the outcome space of the observable. An observable A is a map \(A: \mathcal {F} \to \mathcal {E}\left (\mathcal {H}\right )\), where \(\mathcal {F}\) is the space of possible outcomes of a measurement of the observable A on a system associated with the Hilbert space \(\mathcal {H}\), such that A is a positive operator valued measure (POVM). A POVM is a map \(A: \mathcal {F} \to \mathcal {E}\left (\mathcal {H}\right )\) such that (a) A(∅) = 0, (b) A( Ω) = I, and (c) A(∪i X i) =∑i A(X i) for any sequence {X i} of disjoint sets in \(\mathcal {F}\); for \(X \in \mathcal {F}\), A(X) are referred to as POVM elements. In other words, a mapping \(A: \mathcal {F} \to \mathcal {E}\left (\mathcal {H}\right )\) is a POVM if and only if the mapping \(X \mapsto \operatorname {\mathrm {tr}} \left [ \rho A(X)\right ]\) defines a probability measure for every state \(\rho \in \mathcal {S}\left (\mathcal {H}\right )\).
- 7.
From [20]: A self-adjoint operator \(W \in \mathcal {L}_s \left (\mathcal {H}_A\otimes \mathcal {H}_B\right )\) is an entanglement witness if W is not a positive operator but \(\left < \psi \right |\left < \phi \right | W \left | \psi \right >\left | \phi \right > \geq 0\) for all factorized vectors \(\left | \psi \right >\left | \phi \right > \in \mathcal {H}_A\otimes \mathcal {H}_B\). We say that an entangled state ρ is detected by W if \( \operatorname {\mathrm {tr}}[\rho W] < 0\).
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Smith, A.R.H. (2019). The Unruh-DeWitt Detector and Entanglement Harvesting. In: Detectors, Reference Frames, and Time. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-030-11000-0_3
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