“…High power orange-red lasers in the 600 -650 nm region are strongly desirable visible laser sources can be utilized in such important applications as spectral analysis, biomedicine, optical pumping, and laser projection displays etc [1 -3]. Conventionally, high power orange-red lasers can be realized by intracavity sum-frequency generation (SFG) via various approaches, such as laser diode (LD) pumped Nd 3+ -doped crystals [4,5], Pr 3+ -doped crystals pumped by the intracavity frequency doubled Nd 3+ laser [6,7], GaInNAs/GaAs semiconductor disk laser based second-harmonic generation (SHG) [8,9], or Raman frequency shift technology [10,11]. However, such lasers usually output a single wavelength, which is not satisfied to the applications where wide band wavelength is required.…”