Question 9.7: REFRACTIVE AND GROUP INDEX OF Si AT 1550 nm Silicon photonic...

REFRACTIVE AND GROUP INDEX OF Si AT 1550 nm    Silicon photonic endeavors to integrate various photonic functionalities such as light guiding, light modulation, detection, etc., into the silicon microelectronics. Calculate the refractive and group index of Si at 1550 nm, one of the main communication wavelengths.

The blue check mark means that this solution has been answered and checked by an expert. This guarantees that the final answer is accurate.
Learn more on how we answer questions.

The 1550 nm wavelength is equivalent to a photon energy in eV of

h f=h c  /  \lambda=\left(6.626 \times 10^{-34}\right)\left(3 \times 10^{8}\right) /\left(1550 \times 10^{-9}\right)\left(1.602 \times 10^{-19}\right)=0.800  eV

Using the Cauchy dispersion relation for Si with coefficients from Table 9.2,

\begin{aligned} n &=n_{-2}(h f)^{-2}+n_{0}+n_{2}(h f)^{2}+n_{4}(h f)^{4} \\ &=\left(-2.04 \times 10^{-8}\right)(0.800)^{-2}+3.4189+\left(8.15 \times 10^{-2}\right)(0.800)^{2}+\left(1.25 \times 10^{-2}\right)(0.800)^{4} \\ &=3.4711 \end{aligned}

We can obtain the group index through Equation 9.23. We can change this equation from wavelength λ dependence to photon energy hf dependence by using h f=h c  /  \lambda . From straightforward calculus, the result is

N_{g}=n-\lambda \frac{d n}{d \lambda}=n+(h f) \frac{d n}{d(h f)}

Differentiating the Cauchy relation and substituting it into the above, we obtain

N_{g}=-n_{-2}(h f)^{-2}+n_{0}+3 n_{2}(h f)^{2}+5 n_{4}(h f)^{4}

Substituting hf = 0.800 eV we find

\begin{aligned} N_{g} &=-\left(-2.04 \times 10^{-8}\right)(0.800)^{-2}+3.4189+3\left(8.15 \times 10^{-2}\right)(0.800)^{2}+5\left(1.25 \times 10^{-2}\right)(0.800)^{4} \\ &=3.5756 \end{aligned}

N_{g} is about 3 percent smaller than n. Sometimes the empirical expression for n is not as easy to differentiate analytically as above, in which case we can simply find N_{g} by numerically differentiating n by calculating n and n + \delta n at two very closely spaced wavelengths λ and λ + δλ.

Table 9.2 Sellmeier and Cauchy coefficients
Sellmeier
A_{1} A_{2} A_{3} \lambda _{1} (\mu m) \lambda _{2} (\mu m) \lambda _{3} (\mu m)
SiO_{2} (fused silica) 0.6967490 0.4082180 0.8908150 0.0690660 0.1156620 9.9005590
86.5% SiO_{2}–13.5%
GeO_{2}
0.711040 0.451885 0.704048 0.0642700 0.129408 9.425478
GeO_{2} 0.80686642 0.71815848 0.85416831 0.068972606 0.15396605 11.841931
Sapphire 1.023798 1.058264 5.280792 0.0614482 0.110700 17.92656
Diamond 0.3306 4.3356 0.1750 0.1060
Cauch
Range of hf (eV) n_{−2} (eV^{2} ) n_{0} n_{2} (eV^{−2}) n_{4} (eV^{−4})
Diamond 0.05–5.47 −1.07 × 10^{−5} 2.378 8.01 × 10^{−3} 1.04 × 10^{−4}
Silicon 0.002–1.08 −2.04 × 10^{−8} 3.4189 8.15 × 10^{−2} 1.25 × 10^{−2}
Germanium 0.002–0.75 −1.0 × 10^{−8} 4.003 2.2 × 10^{−1} 1.4 × 10^{−1}

Related Answered Questions