Understanding Lasers: Chapter 10 Quiz
Source: Jeff Hecht, Understanding Lasers: An Entry-Level Guide, fourth edition (2019), Chapter 10 quiz, printed pages 395–398. The questions are paraphrased.
Quick answers
Question |
Answer |
|---|---|
1 |
b, direct-bandgap semiconductor |
2 |
a, InGaAsP |
3 |
c, 40% Ga, 10% Al, 50% As |
4 |
d |
5 |
b |
6 |
e, all listed structures |
7 |
d, VCSEL |
8 |
a, InGaN diode |
9 |
c, \(827\ \mathrm{nm}\) |
10 |
d, distributed feedback |
11 |
e, AlGaN |
12 |
b, AlGaInP |
13 |
e, VCSEL |
14 |
d, stacked arrays |
15 |
e, \(3.1\ \mathrm{eV}\) |
Worked reasoning
Efficient diode-laser material: b. A direct bandgap lets an electron and hole recombine while conserving crystal momentum and emitting a photon. Indirect-gap materials usually lose energy nonradiatively through phonons.
Quaternary III–V compound: a. InGaAsP contains four elements, all drawn from periodic-table groups III and V. GaAlAs is ternary and GaAs is binary.
Atomic fractions in Ga0.8Al0.2As: c. One formula unit contains \(0.8+0.2+1=2\) atoms in normalized proportions. Therefore
\[x_{\mathrm{Ga}}=\frac{0.8}{2}=40\%,\quad x_{\mathrm{Al}}=\frac{0.2}{2}=10\%,\quad x_{\mathrm{As}}=\frac{1}{2}=50\%.\]Exciton: d. It is a bound electron–hole pair: the electron is excited relative to the filled valence band but has not recombined with the hole.
Double-heterostructure advantage: b. Higher-bandgap layers confine injected carriers to the thin active layer, increasing the probability of radiative recombination. They also help confine the optical mode.
Structures possible in GaAlAs: e. The material system supports Fabry–Perot and distributed-feedback edge emitters, VCSELs, and gain chips used in external cavities.
Shortest cavity: d. A VCSEL cavity runs vertically through only a few micrometres of epitaxial material, much shorter than edge-emitter or free-space cavities.
High-definition optical-disc source: a. InGaN diodes emit violet-blue light, whose shorter wavelength focuses to the small spot required for high-density Blu-ray data.
Bandgap wavelength: c. Using \(E(\mathrm{eV})\lambda(\mathrm{nm})\approx1240\),
\[\lambda=\frac{1240\ \mathrm{eV\,nm}}{1.5\ \mathrm{eV}} =827\ \mathrm{nm}.\]Single-longitudinal-mode diode: d. A distributed-feedback grating selects one cavity mode across the gain region.
Shortest-wavelength family: e. Wide-bandgap AlGaN reaches farther into the ultraviolet than GaInN, AlGaInP, GaAlAs, or InGaAsP.
Red pointer diode: b. AlGaInP is the standard material family for efficient visible-red diode emission.
Low-threshold, efficient, good-beam source: e. VCSELs combine a tiny active volume with strong mirrors and a circular, low-divergence output mode.
Maximum efficient power without beam-quality priority: d. Stacking multiple diode arrays combines many broad emitting stripes and scales total power, at the cost of poorer spatial quality.
Energy of a 400-nm photon: e.
\[E=\frac{1240\ \mathrm{eV\,nm}}{400\ \mathrm{nm}} =3.10\ \mathrm{eV}.\]Check: a shorter wavelength than \(1240\ \mathrm{nm}\) must have more than \(1\ \mathrm{eV}\) of energy.