[1] Cutler C C,Newton S A,Shaw H J.Limitation of rotation sensing by scattering [J].Opt Lett, 1980,5(9): 488-491.
[2] Bergh R A,Culshaw B,Cutler C C,et al. Source statics and the Kerr effect in fiber-optic gyroscopes[J].Opt Lett,1982,7(11): 563-565.
[3] Shuma R F,Killian K M.Superfluorescent diode(SLD) wavelength control in high performance fiber optic gyroscopes[A].Proc SPIEFiber Gyros: 10th Anniversary Conference [C]. 1986,719.203 -207.
[4] Lefevre H C.The Fiber-Optic Gyroscope [M].Brian Culshaw:Artech House Inc, 1993.
[5] Bergh R A,Lefevre H C,Shaw H J.An overview of fiber-optic gyroscopes[J].J Lightwave Technol,1984,LT-2:91-107.
[6] Wyscocki P F,Fesler K,LIU K,et al.Spectrum thermal stability of Nd-and Er-doped fiber sources[A].Proc SPIE,Fiber Laser Sources and Amplifiers Ⅱ [C].1990,1373.202-206.
[7] Wyscocki P F,Digonnet M J F,Kim B Y.Wavelength stability of a high -output, broadband, Er -doped, superfluorescent fiber source pump near 980 nm [J].Opt Lett, 1991,16(20) : 961-963.
[10] Wang L A,Chen C D.Characteristics comparison of Er-doped double-pass superfluorescent fiber sources pumped near 980 nm [J].IEEE Photonics Technology Letters, 1997,9(4):446-448.