2020
DOI: 10.1364/aop.385184
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Transverse mode instability

Abstract: This work presents a review on the effect of transverse mode instability in high-power fiber laser systems and the corresponding investigations led worldwide over the past decade. This paper includes a description of the experimental observations and the physical origin of this effect, as well as some of the proposed mitigation strategies.

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Cited by 212 publications
(99 citation statements)
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“…This mainly involves comprehensive suppressions of the transverse mode instabilities (TMI) and nonlinear inelastic scattering effects, such as stimulated Brillouin scattering (SBS) and stimulated Raman scattering (SRS) [16][17][18]. Basic principles to increase the TMI and SBS/SRS thresholds in high-power fiber lasers have already been proposed based on the understanding of those effects [19,20].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…This mainly involves comprehensive suppressions of the transverse mode instabilities (TMI) and nonlinear inelastic scattering effects, such as stimulated Brillouin scattering (SBS) and stimulated Raman scattering (SRS) [16][17][18]. Basic principles to increase the TMI and SBS/SRS thresholds in high-power fiber lasers have already been proposed based on the understanding of those effects [19,20].…”
Section: Introductionmentioning
confidence: 99%
“…As for the SBS/SRS effect, the counter-pumped configuration is the most favorable one, because the high-power signal only propagates over a relatively short length of the fiber (at the end of the fiber), which reduces the effective fiber length of high-power fiber lasers [25]. As for the TMI effect, most of the theoretical studies coincide in pointing out that the bidirectional configuration might offer some advantage over the sole forward-pumped or backward pumped case [19,[26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…where N 1 /N 2 and N Yb are the lower/upper state population and Yb 3+ ion concentration, respectively; P + p/s,i and P − p/s,i represent the forward and backward pump/ith modal power; σ ap /σ ep and σ as /σ es are the absorption/emission crosssections at the pump and signal wavelengths; α p (z) and α s,i (z) are the pump loss and ith mode loss that can be calculated according to Equation (3), and the units for those losses are dB/m; the pump and ith mode power fill factor are denoted by Γ p (z) and Γ s,i (z); and A dope (z) is the effective ion-doped area that is mainly dependent on Equation (1). The rare-earth-doped core can act as a heat source under a high-power pump [32] , and thus the longitudinally varying core radius of T-SCF results in longitudinally varying heat load density that is…”
Section: Theory and Modelmentioning
confidence: 99%
“…Email: fanwh@opt.ac.cn (W. Fan); ypzhang@xjtu.edu.cn (Y. Zhang) evolution on the output power of fiber lasers in the past two decades [4] . However, the evolution is suffering from a sudden halt owing to mode degradation phenomena [5,6] .…”
Section: Introductionmentioning
confidence: 99%