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Multiphoton Scattering Tomography with Coherent States

Tomás Ramos and Juan José García-Ripoll
Phys. Rev. Lett. 119, 153601 – Published 11 October 2017
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Abstract

In this work we develop an experimental procedure to interrogate the single- and multiphoton scattering matrices of an unknown quantum system interacting with propagating photons. Our proposal requires coherent state laser or microwave inputs and homodyne detection at the scatterer’s output, and provides simultaneous information about multiple—elastic and inelastic—segments of the scattering matrix. The method is resilient to detector noise and its errors can be made arbitrarily small by combining experiments at various laser powers. Finally, we show that the tomography of scattering has to be performed using pulsed lasers to efficiently gather information about the nonlinear processes in the scatterer.

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  • Received 6 June 2017

DOI:https://doi.org/10.1103/PhysRevLett.119.153601

© 2017 American Physical Society

Physics Subject Headings (PhySH)

Atomic, Molecular & Optical

Authors & Affiliations

Tomás Ramos* and Juan José García-Ripoll

  • Instituto de Física Fundamental IFF-CSIC, Calle Serrano 113b, Madrid 28006, Spain

  • *t.ramos.delrio@gmail.com

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Issue

Vol. 119, Iss. 15 — 13 October 2017

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Images

  • Figure 1
    Figure 1

    (a) A quantum scatterer with scattering matrix U transforms an input state |Ψin of m photons with generic quantum numbers k1,,km into an outgoing state |Ψout=U|Ψin of n photons with labels, p1,,pn. (b) Our experimental protocol for determining U requires coherent state wave packets inputs |αk, prepared with a signal generator (), and homodyne measurements at the output. Prior to measurement, the output signal is split evenly by an N-port beam splitter (BS), so as to measure all possible filtered correlations Bp1Bpn.

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  • Figure 2
    Figure 2

    A possible implementation of the protocol that works for one- and two-photon scattering matrices.

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  • Figure 3
    Figure 3

    Reconstruction of the nonlinear two-photon scattering matrix for a two-level system weakly coupled to a 1D photonic channel. (a) Upper bound of the reconstruction error ϵb(Z)|ϵ2(Z)|, as derived in the Supplemental Material [30] when combining q=1,,Z scattering matrix estimates E(bq1|α|2) with b=1.05. The various curves show ϵb(Z) as a function of the smallest laser power |α|2 for Z=1,2,,12 (from top to bottom). (b) Predicted transmission measurement of |Tp1p2k1k2|2 for a qubit with decay rate γ and Gaussian wave packets of width σ=0.8γ/c. We vary the momentum differences Δk=(k2k1)/2 and Δp=(p2p1)/2, between incoming and outgoing photons, and fix the conserved average momentum to k^=(ω0+1.5γ)/c, with ω0 the qubit’s transition frequency. (c) Cross sections of |T|2 measured at different widths, σ=0.8γ/c (dashed blue) and σ=0.4γ/c (solid brown), give the same exact result for |γT¯/c|2 after deconvolution (blue and brown dotted line). As marked in (a) and (d), the cross sections correspond to |Δp|=1.5γ/c. (d) Deconvolution of the measurements according to Eq. (19), to recover the two-photon interaction strength |T¯p1p2k1k2|2 of the two-level scatterer derived in Refs. [11, 12, 30].

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