## Abstract

We report experimentally a bistability between two limit cycles (i.e. time-periodic dynamics) in a free-running vertical-cavity surface-emitting laser. The two limit cycles originate from a bifurcation on two elliptically polarized states which exhibit a small frequency difference and whose main axes are symmetrical with respect to the linear polarization eigenaxes at threshold. We demonstrate theoretically that this peculiar behavior can be explained in the framework of the spin-flip model model by taking into account a small misalignment between the phase and amplitude anisotropies.

© 2014 Optical Society of America

## 1. Introduction

Going from the standard edge-emitting heterostructure to the innovative vertical-cavity surface-emitting laser (VCSEL) was a major step forward in laser technology providing a circular beam, significant reduction of the threshold and possibilities for on-chip testing capability. However their circular geometry resulted in one of their main drawbacks: laser emission is accompanied by polarization instabilities inducing polarization switching [1–7], and polarization chaos [8]. For a recent review see Ref. [9]. These instabilities are attributed to the competition between the two preferred orthogonal and linearly polarized (LP) modes of the VCSEL. To explain the resulting dynamics, various mechanisms such as thermal lensing [10], gain dependency with the current [2], and spin-relaxation mechanisms (so-called spin-flip model or SFM) have been proposed [11–13].

Among these instabilities, the emergence of elliptically polarized (EP) states has been studied [5, 14], and they later appear to be the roots of chaotic mode hopping dynamics [6–8, 13]. Although the bifurcation scenarios observed experimentally are in complete agreement with the theoretical predictions, the mechanism selecting the EP states remains to be clarified. Indeed, we experimentally observe that EP states always appear with the same orientation [7], whereas in theory, e.g. in the SFM framework, symmetrical EP with respect to LP modes are strictly equivalent and the selection is made at random [12].

Here we report on a peculiar phenomenon calling for a closer look on the bifurcations from elliptically polarized states: we observe a bistability between two limit cycles (LCs) oscillating around two EPs with main axes symmetrical with respect to the LP at threshold. The two LCs exhibit slightly different frequencies and a clear hysteresis cycle is observed. Theoretically, we demonstrate that these features can, in fact, be accurately reproduced in the SFM framework when including a misalignment between phase and amplitude anisotropies [15,16]. In this contribution, we therefore bring new light about the importance of EP state asymmetry for VCSEL nonlinear dynamics and provide further evidence validating the SFM model.

The paper is organized as follows: we first present the setup and experimental observations in section 2. Then we describe the theoretical model we use including the anisotropy misalignment in section 3. In section 4, we give the simulation results and we conclude in section 5.

## 2. Experimental observation: bistability between two limit cycles

The VCSEL used in this experiment is a single longitudinal mode InGaAs submonolayer quantum dot laser emitting at 990 nm that has already been described in detail elsewhere [7]; the laser and its temperature are controlled by a Profile LDC 1000 controller. The laser beam is focused using an aspheric lens and coupled into a multimode fiber for the measurements. Reflections from the fiber-facet are avoided using an optical isolator and polarization resolved measurements are achieved by rotating a half-waveplate located just before the optical isolator. In this contribution, the axis of the linear polarization at threshold is considered as the reference for polarization orientation, and as such, will be identified as the polarization at 0°. To record time-series we use a fast-photodetector (NewFocus 1554-B, 10kHz – 12GHz bandwidth), an electronic amplifier (NewFocus 1422LF, 20 GHz) and an oscilloscope (Agilent DSOX92504A, 25 GHz, 80 GS/s). The frequency content of the measured time-series are obtained through a Fast Fourier Transform (FFT).

The device temperature is set to 22°*C* and, in this case, the laser turns into chaos at high injection current [8]. At threshold, around 0.3 mA, the laser emits LP light but, similarly to what is described in Ref. [17], it is quickly destabilized towards an EP state shown in Fig. 1(a). The first limit cycle (LC) then appears oscillating around this EP with a frequency of about 6.25*GHz*, see the time-series in Fig. 1(b) and the frequency evolution in Fig. 1(e). The amplitude of the LC increases along with the current but, around 1.95 mA, it is destabilized and a new limit cycle appears. The latter exhibits a slightly larger frequency around 6.55 *GHz* but, even more importantly, the cycle oscillates around the second, symmetrical EP with respect to the polarization of the laser at threshold, see the inversion of the +45° and −45° curves shown in Fig. 1(a). At this point, decreasing the current unveils the region of bistability between the two LCs - in Fig. 1(a), 1(d) and 1(f) - until the laser settles back on the first LC for currents below 1.77 mA. Moreover, before the switching, we observe that the cycle fades out to an EP steady-state as can be seen very clearly in Fig. 1(f) where the FFT peak vanishes before the switching. Due to a high sensitivity of the device to experimental conditions, e.g. stress from the probes, the range of current at which the bistability appear can change between different measurements. In particular the current value at which polarization switchings occur in Fig. 1(a) are slightly different from what can be concluded from panels 1(c)–1(d) or 1(e)–1(f).

## 3. Asymmetric SFM model: misaligned phase and amplitude anisotropies

To describe the behavior of the investigated VCSEL, we use the SFM model [11, 12]. In this framework we consider the left and circular polarizations as two competing emission processes with two separated carrier reservoirs coupled through the spin-flip relaxation processes. However, as will be shown in the following, to reproduce the reported behavior, we need to consider misaligned phase and amplitude anisotropies as described in Ref. [16]. As a result, the SFM model writes as follow:

With *E*_{±} the electrical field for the right (+) and left (−) circular polarization, *N* the normalized total carrier population and *n* the normalized carrier population difference between the two reservoirs. *κ* is the electric field decay rate in the cavity and *γ _{s}* the spin-flip relaxation rate that accounts for the spin homogenization of the spin up and spin down carrier populations.

*α*is the linewidth enhancement factor,

*μ*is the normalized injection current. Finally, the phase anisotropy or birefringence is

*γ*whereas

_{p}*γ*is the amplitude anisotropy.

_{a}*θ*is defined as the angle between the axis of maximum frequency and the axis of maximum losses. All parameters and variables are dimensionless and the time is normalized by the carrier lifetime.

At this point it is convenient to define:
$\overline{{\gamma}_{p}^{\pm}}={\gamma}_{p}\mp \mathit{sin}(2.\theta ).{\gamma}_{a}$ and
$\overline{{\gamma}_{a}}=\mathit{cos}(2.\theta ).{\gamma}_{a}$. Thus, similarly to what is done in Refs. [13, 18], we can transform Eq. 1 into three real equations for the amplitude of the two circular polarizations *R*_{+} and *R*_{−} and their phase difference *ϕ*:

*κ*= 600,

*α*= 3,

*γ*= 35,

_{p}*γ*= −10 and

_{a}*γ*= 100.

_{s}## 4. Simulation results: asymmetry impact on laser dynamics

With the given set of parameters and without any asymmetry, i.e. *θ* = 0, we obtain the dynamical evolution given in Fig. 2. At threshold the laser emits LP light - see Fig. 2(a) - but an increase of the injection leads to a pitchfork bifurcation at *μ* ∼ 3.4 which creates two symmetrical EP states - see Fig. 2(b). Because the system is completely symmetrical, the two EPs are strictly equivalent, the polarization selection is therefore only made at random depending on the noise and initial conditions. With a further increase of the current, these steady-states are both destabilized by two identical Hopf bifurcations at *μ* ∼ 3.5, hence creating two symmetrical LCs oscillating around the now unstable EP states - see Fig. 2(c). Finally, for *μ* > 5, the system experiences a cascade of period doubling bifurcation and enters a large region of chaotic dynamics [8,13]. In addition, we observe no difference for the described scenario when decreasing the injection current.

Thus, without asymmetries in the SFM model, we observe an identical scenario for both symmetrical EP states. In other words, we already have a bistability between the two elliptical steady-states and the limit cycles born on those states, but no deterministic switching can occur between them: the jumps between the two symmetrical evolution can only occur through a noise-induced process. The reproducible hysteresis loop and frequency splitting therefore cannot be explained in this framework.

On the other hand, when considering a small misalignment between the phase and amplitude anisotropies, i.e. considering a small asymmetry in the model, we observe a very different behavior. In Fig. 3, we present the results obtained with *θ* = −0.023; this very specific angle between the two anisotropies has been chosen to provide a good match with the features observed in the experiments. For simplicity, we call *EP*_{+} (*EP*_{−}) the EP state exhibiting a dominant emission at +45° (−45°). We also designate the two limit cycles oscillating around these states *LC*_{+} and *LC*_{−}.

First, we observe that the pitchfork bifurcation destabilizing the LP at threshold has disappeared. As a result, for low injection current the polarization is not linear anymore but slightly *EP*_{+} elliptical. For levels of current where the pitchfork bifurcation would appear when no asymmetry is considered, we observe a smooth transition towards an elliptical *EP*_{+} emission with increasing ellipticity, see Fig. 3(a). This observation clearly confirms that the two EP states are no longer equivalent as the asymmetry obviously strengthens the *EP*_{+} emission.

Secondly, we report an hysteresis cycle and therefore a bistability between *LC*_{+} and *LC*_{−}, as can be seen from Fig. 3(a)–3(b) and 3(d)–3(e). Despite the misalignment induced asymmetry, a Hopf bifurcation still occurs around *μ* = 3.5 hence creating *LC*_{+}. The amplitude of the cycle largely increases along with the current until it is destabilized by a cascade of period doubling bifurcations at *μ* ∼ 4.9 (Fig. 3(b)). Without asymmetry the system would then enter in a region of polarization chaos [8], but here we find a polarization switching towards a second limit cycle which appears to be *LC*_{−}. The FFT of the output power time-series confirms a slight frequency shift, about 0.07 between the two cycles - i.e. about 70 MHz for a carrier lifetime of 1 ns. From this point, decreasing the injection current unveils a large bistability region between the two time-periodic solutions oscillating with different polarization and delimited by the two vertical dashed lines of Fig. 3(b)–3(e). The amplitude decreases along with the current until it reaches a steady *EP*_{−} emission around *μ* = 3.5 (see inset of Fig. 3(e)). This transition is also visible on the FFT spectrum, Fig. 3(f), as the frequency peak vanishes close to the switching point. Indeed the *EP*_{−} is stable only in a small region and the system quickly settles back on *LC*_{+}. The frequency shift we observe here is slightly larger around 0.1, i.e. about 100 MHz for a carrier lifetime of 1 ns, i.e. the same order of magnitude than in the experiment.

These results clearly demonstrate that misalignment as small as *θ* = −0.023 - which makes the
$\overline{{\gamma}_{p}^{\pm}}$ differ by less than 3% - can induce completely different dynamical behavior than that of the aligned case. We described here only the bifurcation scenario that matches our experimental results but we also observed many other features that are left for discussions elsewhere.

## 5. Conclusion

To conclude, we experimentally unveil a peculiar behavior in a free-running VCSEL: bistability between two limit cycles. The two cycles exhibit different amplitudes, slightly different frequencies, and more importantly they oscillate around two symmetrical elliptically polarized states with respect to polarization at threshold. Theoretically we explain this behavior framework of the SFM model by taking into account a small misalignment between the phase and amplitude anisotropies. We clearly show that all the experimental features are reproduced, hence showing an excellent qualitative agreement between experiment and theory. This study therefore brings new light on the role and interplay of phase and amplitude anisotropies in the nonlinear dynamics of VCSELs.

## Acknowledgments

The authors acknowledge support from the Conseil Régional de Lorraine, Fondation Supélec, FWO-Vlaanderen, the METHUSALEM programme of the Flemish government, and the interuniversity attraction poles programme of the Belgian Science Policy Office (grant no. IAP P7-35 “Photonics@be”).

## References and links

**1. **K. D. Choquette, D. A. Richie, and R. E. Leibenguth, “Temperature dependence of gain-guided vertical cavity surface emitting laser polarization,” Appl. Phys. Lett. **64**, 2062–2064 (1994). [CrossRef]

**2. **K. D. Choquette, R. P. Schneider, K. L. Lear, and R. E. Leibenguth, “Gain-dependent polarization properties of vertical-cavity lasers,” IEEE J. Sel. Top. Quantum Electron. **1**, 661–666 (1995). [CrossRef]

**3. **M. van Exter, M. Willemsen, and J. Woerdman, “Polarization fluctuations in vertical-cavity semiconductor lasers,” Phys. Rev. A **58**, 4191–4205 (1998). [CrossRef]

**4. **T. Ackemann and M. Sondermann, “Characteristics of polarization switching from the low to the high frequency mode in vertical-cavity surface-emitting lasers,” Appl. Phys. Lett. **78**, 3574–3576 (2001). [CrossRef]

**5. **M. Sondermann, T. Ackemann, S. Balle, J. Mulet, and K. Panajotov, “Experimental and theoretical investigations on elliptically polarized dynamical transition states in the polarization switching of vertical-cavity surface-emitting lasers,” Opt. Commun. **235**, 421–434 (2004). [CrossRef]

**6. **L. Olejniczak, M. Sciamanna, H. Thienpont, K. Panajotov, A. Mutig, F. Hopfer, and D. Bimberg, “Polarization switching in quantum-dot vertical-cavity surface-emitting lasers,” IEEE Photon. Technol. Lett. **21**, 1008–1010 (2009). [CrossRef]

**7. **L. Olejniczak, K. Panajotov, H. Thienpont, M. Sciamanna, A. Mutig, F. Hopfer, and D. Bimberg, “Polarization switching and polarization mode hopping in quantum dot vertical-cavity surface-emitting lasers.” Opt. Express **19**, 2476–2484 (2011). [CrossRef] [PubMed]

**8. **M. Virte, K. Panajotov, H. Thienpont, and M. Sciamanna, “Deterministic polarization chaos from a laser diode,” Nat. Photonics **7**, 60–65 (2012). [CrossRef]

**9. **K. Panajotov and F. Prati, *Polarization dynamics of vcsels, in VCSELs* (Springer, 2013), 181–231.

**10. **K. Panajotov, B. Ryvkin, J. Danckaert, M. Peeters, H. Thienpont, and I. Veretennicoff, “Polarization switching in VCSEL’s due to thermal lensing,” IEEE Photon. Technol. Lett. **10**, 6–8 (1998). [CrossRef]

**11. **M. San Miguel, Q. Feng, and J. Moloney, “Light-polarization dynamics in surface-emitting semiconductor lasers,” Phys. Rev. A **52**, 1728–1739 (1995). [CrossRef] [PubMed]

**12. **J. Martin-Regalado, F. Prati, M. San Miguel, and N. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quant. Electron. **33**, 765–783 (1997). [CrossRef]

**13. **M. Virte, K. Panajotov, and M. Sciamanna, “Bifurcation to nonlinear polarization dynamics and chaos in vertical-cavity surface-emitting lasers,” Phys. Rev. A **87**, 013834 (2013). [CrossRef]

**14. **F. Prati, P. Caccia, M. Bache, and F. Castelli, “Analysis of elliptically polarized states in vertical-cavity-surface-emitting lasers,” Phys. Rev. A **69**, 033810 (2004). [CrossRef]

**15. **M. Travagnin, M. P. van Exter, A. K. Jansen van Doorn, and J. P. Woerdman, “Role of optical anisotropies in the polarization properties of surface-emitting semiconductor lasers.” Phys. Rev. A **54**, 1647–1660 (1996). [CrossRef] [PubMed]

**16. **M. Travagnin, “Linear anisotropies and polarization properties of vertical-cavity surface-emitting semiconductor lasers,” Phys. Rev. A **56**, 4094–4105 (1997). [CrossRef]

**17. **F. Hopfer, A. Mutig, M. Kuntz, G. Fiol, D. Bimberg, N. N. Ledentsov, V. a. Shchukin, S. S. Mikhrin, D. L. Livshits, I. L. Krestnikov, a. R. Kovsh, N. D. Zakharov, and P. Werner, “Single-mode submonolayer quantum-dot vertical-cavity surface-emitting lasers with high modulation bandwidth,” Appl. Phys. Lett. **89**, 141106 (2006). [CrossRef]

**18. **T. Erneux, J. Danckaert, K. Panajotov, and I. Veretennicoff, “Two-variable reduction of the San MiguelFeng-Moloney model for vertical-cavity surface-emitting lasers,” Phys. Rev. A **59**, 4660–4667 (1999). [CrossRef]