Download Fundamentals of Semiconductor Lasers by Takahiro Numai (auth.) PDF

By Takahiro Numai (auth.)

This e-book explains physics less than the working ideas of semiconductor lasers intimately in accordance with the adventure of the writer, facing the 1st production of phase-shifted DFB-LDs and up to date learn on transverse modes.

The booklet additionally bridges a large hole among magazine papers and textbooks, requiring basically an undergraduate-level wisdom of electromagnetism and quantum mechanics, and is helping readers to appreciate magazine papers the place definitions of a few technical phrases differ, counting on the paper. definitions of the photon density within the fee equations and definitions of the phase-shift within the phase-shifted DFB-LD are defined, and transformations within the calculated effects are indicated, looking on the definitions.

Readers can comprehend the physics of semiconductor lasers and analytical instruments for Fabry-Perot LDs, DFB-LDs, and VCSELs and should be encouraged to boost semiconductor lasers themselves.

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Extra resources for Fundamentals of Semiconductor Lasers

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08 m (solid line) and that for the bulk structures (broken line) 5 Density of states for the bulk ρ 0 4 ρ 3 ρ 13 12 2 ρ 11 1 0 0 2 4 6 8 Energy E (eV) Fig. 61), we obtain ρ1 (E) ≡ m∗ dn = . 62) Similarly, the densities of states for n z = 2, 3, . . are calculated, and the results are shown in Fig. 12. In Fig. 08 m where m is the electron mass in a vacuum, and ρ1 (E) for n z = 1, 2, 3 are indicated as ρ11 , ρ12 , ρ13 , respectively. It should be noted that the density of states for the one-dimensional quantum well is a step function.

10. For the design of the optical waveguides, the cutoff condition, in which the guided modes do not exist, is important. When the angle of incidence θf is equal to the critical angle θfs , the lightwave is not confined to the guiding layer anymore, and a fraction of the optical power is emitted to the substrate. 26). 30) Vm = mπ + tan−1 χc a. For Vm < V < Vm+1 , the guided modes from the zeroth order to the mth order exist as shown in Fig. 10, and a lower-order mode has a larger b for a common V value.

References 1. : Band structure of indium antimonide. J. Phys. Chem. Solids 1, 249 (1957) 2. : Quantum Theory of Solids, 2nd edn. John Wiley and Sons, New York (1987) 3. : Wave Mechanics Applied to Semiconductor Heterostructures. Halsted Press, New York (1988) 4. : Quantum Phenomena. Addison-Wesley, Reading (1989) 5. : Quantum Mechanics, 3rd edn. McGraw-Hill, New York (1968) 6. : Quantum Mechanics, vol. 2. 1 Introduction Among energy states, the state with the lowest energy is most stable. Therefore, the electrons in semiconductors tend to stay in low energy states.

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