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CRC Press eBooks

Instabilities and quantum noise reduction in nonlinear optical mixing

Massimo Brambilla, F. Castelli, A. Gatti, Luigi A. Lugiato, Franco Prati

Published May 4, 2018• 3 citations
Publisher

Abstract

Nondegenerate four-wave-mixing (fwm) is a process by which one or two pump fields generate two signal beams, with conservation of the total photon energy and momentum. The signal beams can be distinguished by their frequency, or by their wave vector, or by their polarization. When the nonlinear medium which creates the fwm process is contained in a resonant cavity, the signal generation is caused by an instability, because the signal fields experience gain (fwm gain), and when this gain overcomes the cavity losses the signal beams build up. This chapter discusses several static and dynamical instabilities which arise from nondegenerate fwm. It considers a cavity with plane mirrors and examines the properties of quantum noise reduction which arise in the intensity difference between the signal beams generated by the fwm process. The chapter illustrates the problem of Gauss-Laguerre transverse modes in a ring cavity with spherical mirrors.

DOI
10.1201/9781351075046-5

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Nondegenerate four-wave-mixing (fwm) is a process by which one or two pump fields generate two signal beams, with conservation of the total photon energy and momentum. The signal beams can be distinguished by their frequency, or by their wave vector, or by their polarization. When the nonlinear medium which creates the fwm process is contained in a resonant cavity, the signal generation is caused by an instability, because the signal fields experience gain (fwm gain), and when this gain overcomes the cavity losses the signal beams build up. This chapter discusses several static and dynamical instabilities which arise from nondegenerate fwm. It considers a cavity with plane mirrors and examines the properties of quantum noise reduction which arise in the intensity difference between the signal beams generated by the fwm process. The chapter illustrates the problem of Gauss-Laguerre transverse modes in a ring cavity with spherical mirrors.
The dynamics of optical nonlinearity in the presence of gain and feedback can be complex leading to chaos in certain regimes. Temporal, spectral, spatial, or polarization instability of optical fields can emerge from chaotic response of an optical [Formula: see text] or [Formula: see text] nonlinear medium placed between two cavity mirrors or before a single feedback mirror. The complex mode dynamics, high-order correlations, and transition to instability in these systems are not well known. We consider a [Formula: see text] medium with amplified four-wave mixing process and study noise and correlation between multiple optical modes. Although individual modes show intensity instability, we observe relative intensity noise reduction close to the standard quantum noise, limited by the camera speed. We observe a relative noise reduction of more than 20 dB and fourth-order intensity correlation between four spatial modes. More than 100 distinct correlated quadruple modes can be generated using this process.
Given one oscillating mode in a laser or an optical bistability cavity, can other modes build up, that is, is single-mode operation unstable? The answer depends on an interplay of spontaneous emission, saturated gain, and four-wave mixing processes that permit one or more sidemodes both to be resonant with cavity modes and to have more gain than loss. We discuss this problem for cavities containing one- or two-photon two-level media subjected to a classical wave of arbitrary intensity and one or two weak quantized sidemodes. While a single sidemode may have gain, two sidemodes symmetrically placed about a strong pump mode can have greater gain due to four-wave mixing contributions sometimes called combination tones. The theory is valid for the buildup of sidemodes from quantum noise until the sidemodes begin to saturate. Subsequent dynamics including chaos must be handled by a theory that allows all modes to saturate. The same physical mechanisms are important in saturation spectroscopy and control the generation of squeezed states in a cavity. However while the instabilities depend on sidemode gain and spontaneous emission, the generation of squeezed states of the vacuum avoids these phenomena, depending solely on quantum combination tones.
The authors present a quantum analysis of four-wave mixing in a non-resonant nonlinear medium inside a cavity which is driven by two driving fields. In this process a nonlinear medium couples two pump modes with a signal mode of the frequency equal to the half-sum of the two pump field frequencies. Three types of stable steady-state solutions of the deterministic problem, describing three regimes of oscillation, are found: one below threshold and two different above-threshold regimes. The spectra of fluctuations of the quadrature-phase amplitudes for all three modes are calculated. It is found that in the above-threshold regime each of three modes may display a squeezed noise reduction. Below threshold a squeezing is realized for the central mode.
We show that an optomechanical cavity pumped by a bichromatic light beam can generate a signal whose frequency lies halfway between the two driving frequencies. This process can be understood as a degenerate four-wave mixing, in which two pump photons (one from each frequency) are combined to yield two identical signal photons. This process takes place between a lower and an upper threshold in terms of the pump intensity, which depend on the pump frequency difference. Close to the signal oscillation threshold a clear noise reduction in one of its quadratures is shown numerically.
We give the analytical expressions for the transfer of amplitude noise from the mixing frequencies to the generated frequencies during a nondegenerate and partially degenerate four-wave mixing (FWM) process and verify them by comparing with the numerical simulation results. We use these analytical expressions to study the amplitude noise relationships between the mixing frequencies and the generated frequencies during an FWM process, for various conditions. We also study the variance, relative intensity noise (RIN), and signal-to-noise ratio (SNR) of the generated frequencies as a function of the power, RIN, and SNR of the input signal.
Nonlinear optical systems can transform a continuous wave input beam, if it is intense enough, into an oscillating light output. The system which has been most thoroughly studied is an optical resonator, usually of the ring type, containing either a Kerr medium1,2 or a two-level medium. Unfortunately, the mathematical approaches of these studies do not lend themselves to a tractable intuitive explanation of the self-pulsation phenomena, and do not identify the physical origin of instabilities. In this paper we consider a different approach, showing that optical instabilities stem from one source, namely, gain generated by four-wave mixing processes. This gain, together with feedback supplied by the resonator, leads to oscillation of sidebands of the input field. The beating between these sidebands and the input field causes the oscillating output intensity. The salient feature of our approach lies in its intuitive appeal, namely, it is possible to predict the behavior of the system for a wide range of parameters. Moreover, our model enables understanding of the system's evolvement beyond the first bifurcation, something usually not possible with the other approaches.