“…I sat ~ 3kWcm -2 at 1480 nm, and as such creates a higher inversion and therefore higher gain. However, the lifetime of the 4 I 11/2 level is sufficiently long to allow a strong ESA transition, assisted by the excitation of two vibrational modes, promoting an Er 3+ ion to its 4 F 9/2 energy state, leading to reduced gain, or even additional loss, at the longer probe wavelengths, Figure 2 Instead for the in-band pumped gain spectrum, Figure 2(b), there appears to be a different ESA process, from 4 I 13/2 to 4 I 9/2 , where one vibrational phonon is excited along with the absorption of a photon with a wavelength that covers pretty much the entire investigated range. It is noteworthy that there is a small spike around 1572 nm, which again corresponds to the gap in the vibrational modes around 550cm -1 .…”