Cheo P K, Berak J M, Oshinsky W, Swindal J L
Appl Opt. 1973 Mar 1;12(3):500-9. doi: 10.1364/AO.12.000500.
Thin-film waveguide structures consisting of epitaxially grown low-carrier-concentration GaAs and having two distinct index profiles have been investigated with a 10.6-microm C0(2) laser. Results of Schottky barrier and Hall measurements show that the carrier concentration of some of these films is less than 10(12) cm(-3), and the resistivity can be as high as 1.4 x 10(5) ?-cm. Guided-wave modes were excited by means of a germanium prism or phase grating coupler. When the index difference Deltan between the undoped film and the substrate is approximately 0.3 (strong guide), a number of modes can be obtained with a typical angular full width at half maximum intensity Delta(theta) (1/2) of <0.5 degrees . For guides having thickness greater than 20 microm, the measured losses are <1 dB/cm for N <10(13) cm(-3) and 1.7 dB/cm for N = 4 x 10(15) cm(-3). Simultaneous excitation of two orthogonal guided-wave modes, i.e., TE(m) and TM(m) for m </= 2, is possible in this structure. For Deltan approximately 10(-3) (weak guide) only one mode can be excited by means of a phase grating coupler with a typical Deltatheta((1/2)) of approximately degrees . Measurements were also made of the transmission and cutoff characteristics of the TE and TM modes in weak guides as a function of the guide thickness that varied between 20 micro and 50 micro Results indicate that optical transmission decreases rapidly as the thickness of the weak guide decreases toward the cutoff value.
利用10.6微米的CO₂激光器对由外延生长的低载流子浓度砷化镓构成且具有两种不同折射率分布的薄膜波导结构进行了研究。肖特基势垒和霍尔测量结果表明,其中一些薄膜的载流子浓度小于10¹²厘米⁻³,电阻率可高达1.4×10⁵欧厘米。通过锗棱镜或相位光栅耦合器激发导波模式。当未掺杂薄膜与衬底之间的折射率差Δn约为0.3(强波导)时,可获得多个模式,其典型的半高角全宽Δθ(1/2) <0.5度。对于厚度大于20微米的波导,当N<10¹³厘米⁻³时,测得的损耗<1分贝/厘米,当N = 4×10¹⁵厘米⁻³时,损耗为1.7分贝/厘米。在这种结构中,可以同时激发两个正交的导波模式,即m≤2时的TE(m)和TM(m)。对于Δn约为10⁻³(弱波导)的情况,通过相位光栅耦合器只能激发一个模式,其典型的Δθ(1/2)约为 度。还测量了弱波导中TE和TM模式的传输和截止特性随波导厚度的变化,波导厚度在20微米至50微米之间变化。结果表明,随着弱波导厚度朝着截止值减小,光传输迅速降低。