Understanding Lasers: Chapter 8 Quiz
Source: Jeff Hecht, Understanding Lasers: An Entry-Level Guide, fourth edition (2019), Chapter 8 quiz, printed pages 297–299. The questions are paraphrased.
Quick answers
Question |
Answer |
|---|---|
1 |
c, GaAs diode laser |
2 |
b, flashlamp |
3 |
a, 808-nm diode |
4 |
c, chlorine |
5 |
e |
6 |
d, ytterbium |
7 |
a |
8 |
b, \(347\ \mathrm{nm}\) |
9 |
c, \(477\ \mathrm{nm}\) |
10 |
a, titanium–sapphire |
11 |
d |
12 |
e, erbium |
13 |
d, OPSL/VECSEL |
14 |
b, titanium–sapphire |
Worked reasoning
Not in the conventional solid-state category: c. This book treats electrically injected semiconductor diode lasers separately from lasers whose dopant ions are embedded in a dielectric solid host.
Best listed general pump: b. A flashlamp supplies intense broadband light overlapping absorption bands; a properly wavelength-matched diode would usually be better, but none is offered in this item.
Best neodymium pump: a. An \(808\ \mathrm{nm}\) diode overlaps a strong Nd absorption band, giving efficient, selective pumping.
Not an active ion: c. Neodymium, titanium, chromium, and ytterbium are established solid-state laser dopants; chlorine is not one of the active species described.
Glass-host advantage: e. Glass is readily fabricated in large rods, slabs, and fibres, although its thermal conductivity is generally poorer than that of crystalline hosts.
Quasi-three-level system: d. Ytterbium’s lower laser level is close enough to the ground state to be thermally populated, so reabsorption must be overcome.
Thin-disk pumping: a. Diode light enters through the broad disk face, often making multiple passes, while the thin geometry efficiently removes heat through the back surface.
Ruby second harmonic: b.
\[\lambda_2=\frac{694\ \mathrm{nm}}2=347\ \mathrm{nm}.\]Not a ready Nd:YAG harmonic: c. Nd:YAG directly gives \(1064\ \mathrm{nm}\); doubling, tripling, and quadrupling give about 532, 355, and \(266\ \mathrm{nm}\). The listed \(477\ \mathrm{nm}\) value is not one of those harmonics.
Broadest solid-state gain band: a. Titanium–sapphire couples its electronic transition to lattice vibrations and supports a very broad emission band.
Vibronic distinction: d. Strong interaction between electronic and vibrational states broadens gain, enabling wide tunability and short pulses.
Least retinal hazard: e. Erbium lasers around \(3\ \mathrm{\mu m}\) are strongly absorbed by water in the cornea and do not focus onto the retina as visible and near-infrared beams do. They remain hazardous to the eye surface.
Compact separate visible colours: d. Optically pumped semiconductor lasers, also called VECSELs, can be engineered and frequency converted for multiple visible wavelengths.
Femtosecond source: b. Titanium–sapphire’s broad gain bandwidth supports mode-locked pulses lasting only femtoseconds.