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Problem 10.1 Make a mindmap of the material covered in this chapter. For more information about mindmaps, see Wikipedia

Problem 10.2 Describe the (possible) relevance of fiber optics in your line of work.

Problem 10.3 Explain why for optical fiber communication lines the wavelength of choice are 1310 and 1550 nm1550~\text{nm}.

Problem 10.4 Show that the phase factor (m1)π(m-1)\pi in eq:fiber:down-propagating-wave indeed leads to a vanishing EE-field at the mirrors. Is this the only possible solution?

Problem 10.5 A plastic fiber has a core refractive index of n1=1.49n_1=1.49 and a cladding refractive index of n2=1.38n_2=1.38. Its core diameter is 1.00 mm1.00~\text{mm} and light with a wavelength of 633 nm633~\text{nm} is coupled into the fiber from air (ne=1.00n_{\text{e}}=1.00). Calculate: (a) the internal critical angle θi,c\theta_{\text{i,c}} (b) the (external) critical angle θˉe,c\bar{\theta}_{\text{e,c}} (c) the Δ\Delta-parameter (Can you use the approximation?) (d) the numerical aperture (e) the VV-number (Is this a singlemode or multimode fiber?) (f) the cut-off wavelength

Problem 10.6 Describe, in your own words, the effect of dispersion on a short pulse. What is the maximum length of fiber of a loss-less datalink, given that the dispersion parameter of the fiber D=20 ps/kmnmD=20~\text{ps/km}\cdot \text{nm} and the laser used to communicate has a spectral width of 1.0 nm1.0~\text{nm}? The laser can send light pulses at a rate of 10 GHz10~\text{GHz}.

Problem 10.7 What is the maximum length of fiber of a dispersion-less datalink, given that the loss of the fiber αdB=0.30 dB/km\alpha_{\text{dB}}=0.30~\text{dB/km} and a light pulse can no longer be discriminated from the background noise if 99%99\% of the light is lost?

Problem 10.8 Estimate the loss (in dB) due to the following situations in which two single mode fibers are coupled incorrectly:

(a) a fiber with a core diameter of 7.0 μm7.0~\mu\text{m} is coupled to a fiber with core diameter 6.0 μm6.0~\mu\text{m} (see figFiberCouplingLoss).

(b) a 500 μm500~\mu\text{m}-air gap exists in between two fibers (see figFiberCouplingLoss). Both have a numerical aperture equal to 0.12 and a core diameter of 6.0 μm6.0~\mu\text{m}.

To make your estimation, neglect reflection due to refractive index mismatch and assume the incoming light has a Gaussian beam profile with intensity

I(r,z)=I0(d/4d/4+NAz)2exp(2r2(d/4+NAz)2).\begin{align*} I(r,z)=I_0\left(\frac{d/4}{d/4+\mathrm{NA}\cdot z}\right)^2\exp\left(\frac{-2r^2}{(d/4+\mathrm{NA}\cdot z)^2}\right). \end{align*}

Here, rr is the radial coordinate in the (x,y)(x,y)-plane (see figFiberTIR). Integrate over the fiber core into which the light is coupled and divide by I0I_0.

Note that these calculations are simplified, but they give a rough estimate of coupling losses.