À3.43 dB) and À3.43 dB (À3.2 dB), respectively. The maximum value of amplitude unbalance, the difference in power of S 31 and S 21 between two output ports, is measured (simulated) at 0.7 dB (0.35 dB) in the operating band. Figure 7 shows the simulated and measured phase differences between two output ports. The simulated phase differences between two output ports of a conventional MSL Wilkinson balun are compared. The conventional MSL Wilkinson balun are designed using two branches of À90 and À270 phase shift MSL. The differential output phase is shown to be flat in the operation band of the proposed balun. The fractional 180 6 10 bandwidth of the balun based on the PLH TL is measured (simulated) at 71% (70%) from 1.47 GHz (1.44 GHz) to 3.09 GHz (2.99 GHz), whereas the bandwidth of the conventional MSL balun is only 10.8% from 2.36 GHz to 2.63 GHz. Consequently, the broadband Wilkinson balun based on a PLH TL has good properties, such as return loss, isolation, and through in the broad frequency range.Furthermore, a wideband balun based on modified PLH TL [6] having a wide LH bandwidth is designed by the full wave simulation. The illustration of Figure 7 shows the top view of the modified PLH TL. The other dimensions of modified PLH TL are exactly the same with those of Figure 1 except for dimensions in figure caption of Figure 7. In this case, to satisfy the Eq. (4), the lengths of L 1 and L 2 are determined as 20.8 mm (corresponding to 4-stage modified PLH TL) and 60.3 mm, respectively. The designed balun has the fractional bandwidth of 107.8% from 1.12GHz to 3.74GHz, as shown in Figure 7. Consequently, the PLH TL balun is well-suited for RF devices requiring a broadband balanced signal.
CONCLUSIONS
ABSTRACT:We have demonstrated a homemade high-efficient ytterbium-doped fiber laser with up to 1.75 kW of continuous-wave output power at 1.09 lm with a slope efficiency of 76%. The fiber is pumped by two laser diode array (LDA) sources launched through opposite ends. No undesirable effect is observed with increasing pump power, which suggests that the homemade fiber laser could produce higher power output by using more pump sources.