Abstract

We demonstrate an optically controlled polarizer at ~1323 nm using a ladder transition in a Rb vapor cell. The lower leg of the 5S(1/2),F = 1->5P(1/2),F = 1,2->6S(1/2),F = 1,2 transitions is excited by a Ti:Sapphire laser locked to a saturated absorption signal, representing the control beam. A tunable fiber laser at ~1323 nm is used to excite the upper leg of the transitions, representing the signal beam. When the control beam is linearly polarized, it produces an excitation of the intermediate level with a particular orientation of the angular momentum. Under ideal conditions, this orientation is transparent to the signal beam if it has the same polarization as the control beam and is absorbed when it is polarized orthogonally. We also present numerical simulations of the system using a comprehensive model which incorporates all the relevant Zeeman sub-levels in the system, and identify means to improve the performance of the polarizer. A novel algorithm to compute the evolution of large scale quantum system enabled us to perform this computation, which may have been considered too cumbersome to carry out previously. We describe how such a polarizer may serve as a key component for high-speed Stokesmetric imaging. We also show how such a polarizer, combined with an optically controlled waveplate, recently demonstrated by us, can be used to realize a high speed optical logic gate by making use of the Quantum Zeno Effect. Finally, we describe how such a logic gate can be realized at an ultra-low power level using a tapered nanofiber embedded in a vapor cell.

Highlights

  • All-optical logic gates are important for quantum information processing [1,2,3,4,5]

  • We have demonstrated an optically controlled polarizer at ~1323 nm using a ladder transition in a Rb vapor cell

  • We investigated two geometries – when the control and the signal beams are co-propagating and counter propagating

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Summary

Introduction

All-optical logic gates are important for quantum information processing [1,2,3,4,5]. Consider a specific situation where input quantum state is |V> When it passes through a wave plate with its fast/slow axis at an angle of 45° with respect to the vertical axis, the polarization state of the photon can be expressed as (ignoring an overall phase factor) ψ = cos(Δnwt / 2) V + i sin(Δnwt / 2) H ,. The process can be understood via the Quantum Zeno effect by considering a quantum model of a classical laser field (by which we mean a field with intensity much stronger than that of a single photon) Any such field (including, but not limited to the coherent state) can be expressed as a superposition of the Fock states: V = nα n. QZE applies even if one does not explicitly consider the optical field quantum mechanically

Optically controlled polarizer
QZE based all-optical logic gate
Stokesmetric imaging
Experimental set-up
Results
Model used for simulation and computational details
Improvements to system and future work
10. Conclusions
Findings
11. Appendix
Full Text
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