I. Introduction
Nowadays high power fiber lasers (FLs) with their outstanding advantages have been widely used in many industrial, military and scientific applications [1]– [3]. For a FL, the pumping configuration is of critical importance, which can be divided into two major categories: direct-pumping configuration [4], [5] and tandem-pumping configuration [6] , [7]. As far as we know, the highest power of single output fiber was reported by IPG in 2009 based on the tandem-pumping, taking advantage of the relatively short wavelength (1000–1030 nm) FLs employed as the pump source in tandem-pumping to reduce the quantum defect in the active fiber, which leads to less thermal load and larger pumping capacity [8]. Hence, the tandem-pumped FLs have the potential to raise the output power limit [9] . Consequently, rising attention has been paid by researchers worldwide to achieve higher output power of these short wavelength FLs, especially 1018 nm ytterbium-doped fiber laser (YDFLs) [10]–[14].