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Conference on Lasers and Electro-Optics

Quantum soliton generation via interference of nonlinear Schrodinger equation coherent solitonic fields

M.J. Werner, Stephen R. Friberg

Published Nov 27, 2002• 1 citation
Publisher

Abstract

Summary form only given. We have shown for the first time that large photon-number squeezing of coherent pulses can be produced by a Sagnac loop for a significant range of input energies and that it is larger than predicted for directly spectrally filtered optical fiber solitons. Despite this, we pointed out the similarities between the two schemes. In essence, a Sagnac fiber loop is capable of producing optical pulses closer to true quantum solitons than their coherent counterparts from modelocked lasers.

DOI
10.1109/iqec.1998.680278

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Conference on Lasers and Electro-Optics•Nov 27, 2002•1 citation
Summary form only given. We have shown for the first time that large photon-number squeezing of coherent pulses can be produced by a Sagnac loop for a significant range of input energies and that it is larger than predicted for directly spectrally filtered optical fiber solitons. Despite this, we pointed out the similarities between the two schemes. In essence, a Sagnac fiber loop is capable of producing optical pulses closer to true quantum solitons than their coherent counterparts from modelocked lasers.
Direct photon-number squeezing is demonstrated, for the first time to our knowledge, in a nonlinear fiber-optic interferometer. Launching 126-fs solitons into a highly asymmetric Sagnac loop, the maximum photocurrent noise reduction was $3.9\ifmmode\pm\else\textpm\fi{}0.2\mathrm{dB}$ below shot noise, corresponding to $6.0\ifmmode\pm\else\textpm\fi{}0.9\mathrm{dB}$, when corrected for linear losses. The loop is a model system for squeezing generated by the interference of two pulses after nonlinear propagation through a fiber.
For the first time a method for realizing macroscopic quantum optical solitons is presented. Simultaneous photon-number and momentum squeezing is predicted using soliton propagation in an interferometer. Extraction of soliton pulses closer to true quantum solitons than their coherent counterparts from mode-locked lasers is possible. Moreover, it is a general method of reducing photon-number fluctuations below the shot-noise level for nonsoliton pulses as well. It is anticipated that similar reductions in particle fluctuations could occur for other forms of interfering bosonic fields whenever self-interaction nonlinearities exist, for example, interacting ultracold atoms.
Convenient methods of generating amplitude-squeezed (sub-Poissonian) light have recently been discovered, which rely on the use of soliton-like pulses in fibers. The idea of squeezing solitons in fibers is; what is new, however, is the use of femtosecond pulses in conjunction with asymmetric Sagnac loops. Since femtosecond solitons have a correspondingly high peak power, much shorter fiber lengths are required to obtain a given amount of squeezing, which directly translates into lowering of the guided acoustic-wave Brillouin scattering noise in the system. The use of an asymmetric Sagnac loop leads to a robust, practically very stable configuration for generating amplitude squeezing. In a related development, spectral filtering of femtosecond solitons emerging from a straight piece of fiber has also been shown to generate sub-Poissonian light.
Summary form only given. Several schemes to generate squeezed light by use of the Kerr nonlinearity in optical fibers have been devised. The most recent experiments used asymmetric Sagnac loops to produce amplitude squeezing. In our experiment the Sagnac geometry is "unfolded" into a Mach-Zehnder, wherein the two arms of the interferometer correspond to the polarization modes of a single-mode PM fiber. This setup allows us to switch from an asymmetric to a symmetric interferometer, and gives us full control of the phase and amplitude of the two interfering pulses. With these degrees of freedom, we are able to maximize noise reduction and perform a full measurement of the noise properties of the soliton squeezed pulses.
Summary form only given.Recently, a novel way of generating an amplitude-squeezed state using the Kerr nonlinearity has been demonstrated. In this scheme, a pulse with an energy greater than that of the fundamental soliton is launched into an optical fiber with a length of several soliton periods. At the fiber output, the pulse is filtered and detected. The resulting photocurrent has a noise level lower then the shot noise, indicating an amplitude-squeezed state. Here, we demonstrate that soliton amplitude squeezing can be obtained without postfiltering.