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Robust entanglement buffers based on SWAP interactions

Ye-Chao Liu, Otfried Gühne, Stefan Nimmrichter

Abstract

Quantum entanglement is the essential resource for quantum communication and distributed information processing in a quantum network. However, the remote generation over a network suffers from inevitable transmission loss and other technical difficulties. This paper introduces the concept of entanglement buffers as a potential primitive for preparing long-distance entanglement. We investigate the filling of entanglement buffers with either one Bell state or a stream of Bell states via SWAP interactions. We illustrate their resilience to imperfect interactions, noise, and losses, making the buffers suitable for a realistic quantum network scenario. Additionally, larger entanglement buffers can always enhance these benefits.

Robust entanglement buffers based on SWAP interactions

Abstract

Quantum entanglement is the essential resource for quantum communication and distributed information processing in a quantum network. However, the remote generation over a network suffers from inevitable transmission loss and other technical difficulties. This paper introduces the concept of entanglement buffers as a potential primitive for preparing long-distance entanglement. We investigate the filling of entanglement buffers with either one Bell state or a stream of Bell states via SWAP interactions. We illustrate their resilience to imperfect interactions, noise, and losses, making the buffers suitable for a realistic quantum network scenario. Additionally, larger entanglement buffers can always enhance these benefits.
Paper Structure (5 sections, 1 theorem, 45 equations, 17 figures)

This paper contains 5 sections, 1 theorem, 45 equations, 17 figures.

Key Result

Proposition 1

For iSWAP caching of entanglement from a sequence of Bell-$|\psi_1\rangle$ pairs into a $k$-pair buffer, the $k$-ebit buffer state $\hbox{$| \psi_2 \rangle$}^{\otimes k}$ is a steady state for every swap angle $\alpha$.

Figures (17)

  • Figure 1: Sketch of a multi-pair entanglement buffer caching Bell-pair entanglement through a sequence of partial swap operations between the subsequent qubit pairs of the buffer and either (a) a single Bell pair over one or more repetitions or (b) a sequence of Bell pair copies. Entanglement is shared between two distant parties $A$ (upper part) and $B$ (lower part).
  • Figure 2: Entanglement cached from a single Bell pair in a 1-pair buffer by means of (a) a partial SWAP unitary and (b) a partial iSWAP of varying angles $\alpha$. Both buffer qubits are initialized in a pure state $\cos\theta\hbox{$| 0 \rangle$}+\sin\theta\hbox{$| 1 \rangle$}$ of varying $\theta$. The entanglement is measured in ebits of logarithmic negativity.
  • Figure 3: (a) Entanglement buffering from a single caching unitary of SWAP type with a single Bell pair for buffer sizes up to $k=4$. We plot the cached $E$ ebits as a function of the swap angle. (b) Number $n$ of repeated caching operations required to reach $E=1$ as a function of buffer size $k$, given fixed weak swap angles $\alpha$. We plot $n$ in terms of the total operation time $\propto nk\alpha$, which grows like $\sqrt{k}$ (dashed line). All buffer qubits are initialized in $|0\rangle$.
  • Figure 4: (a) Steady-state entanglement $E_\infty$ (ebits) cached from a sequence of Bell pairs in a 1-pair buffer, using a caching unitary of varying interaction parameters $\alpha,\beta$. (b) Entanglement $E$ accumulated in a 1-pair buffer over $n$ subsequent iSWAP caching steps ($\beta=\alpha$) with independent source pairs, comparing various $\alpha$-values.
  • Figure 5: Steady-state entanglement $E_\infty$ cached by multi-copy protocols with varying interaction parameters $\alpha,\beta$, for (a) a $2$-pair and (b) a $3$-pair buffer. The solid line marks the parameter range (right of it) for which the buffer contains more than 1 ebit.
  • ...and 12 more figures

Theorems & Definitions (2)

  • Proposition 1
  • proof