2019
DOI: 10.1103/physreva.100.023829
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Impact of desynchronization and drift on soliton-based Kerr frequency combs in the presence of pulsed driving fields

Abstract: Pulsed driving of Kerr microresonators represents a promising avenue for the efficient generation of soliton states associated with coherent optical frequency combs. The underlying physics has not, however, yet been comprehensively investigated. Here, we report on a numerical and theoretical study of the impact of de-synchronization between the periodic pump field and the train of solitons circulating in the cavity. We show that de-synchronization can affect the soliton configurations that can be sustained for… Show more

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Cited by 36 publications
(25 citation statements)
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References 46 publications
(108 reference statements)
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“…We observe the usual signatures of stable CS formation: a region of modulation instability (MI) is followed by the formation of unstable (breathing) CSs and then a low-noise step indicating the presence of stable CSs. (Note that, throughout our experiments, the precise pump repetition rate is chosen so as to maximise the length of the soliton step, which also ensures that one of the intensity trapping positions is highly favoured due to the presence of stimulated Raman scattering [38].) Thanks to the auxiliary CW laser, the soliton step can be accessed in steady-state simply by manually advancing the cavity detuning.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…We observe the usual signatures of stable CS formation: a region of modulation instability (MI) is followed by the formation of unstable (breathing) CSs and then a low-noise step indicating the presence of stable CSs. (Note that, throughout our experiments, the precise pump repetition rate is chosen so as to maximise the length of the soliton step, which also ensures that one of the intensity trapping positions is highly favoured due to the presence of stimulated Raman scattering [38].) Thanks to the auxiliary CW laser, the soliton step can be accessed in steady-state simply by manually advancing the cavity detuning.…”
Section: Resultsmentioning
confidence: 99%
“…Theories predict [29], however, that under conditions of perfect synchronisation [with respect to (m/n) FSR], each pump pulse actually possesses two stable trapping points (located on the pulse's leading and trailing edge respectively). Fortunately, this degeneracy can be lifted via appropriate desynchronization of the pump pulse train, forcing the system to favour only one of these two trapping points [38].…”
Section: Conceptmentioning
confidence: 99%
“…By changing into a reference frame where the pump is stationary, τ → τ − d × t, the LLE Eq. ( 1) develops a convective drift term (Coen et al 1999;Parra-Rivas et al 2014;Hendry et al 2019):…”
Section: Desynchronization and Locking Rangementioning
confidence: 99%
“…As discussed in (Parra-Rivas et al 2014;Hendry et al 2019), the pump-cavity desynchronization gives rise to a relative drift between the CS and the driving field which is in addition to the motion induced by phase or amplitude inhomogeneities. Therefore, using a PM (S 0 , ∆) = 2, the total CS drift velocity becomes…”
Section: Desynchronization and Locking Rangementioning
confidence: 99%
“…1(a). Our simulations use the wellknown Lugiato-Lefever equation (LLE) with the desynchronization modelled by means of a convective drift term [21,28,29] and parameters as quoted above. These simulations show the formation of spectrally flat combs with an extent that can be continuously tuned by controlling the cavity desynchronization.…”
mentioning
confidence: 99%