Skip to main content

Electron Waves in Semiconductor Heterostructures

  • Chapter
  • First Online:
Basics of Laser Physics

Part of the book series: Graduate Texts in Physics ((GTP))

  • 120k Accesses

Abstract

We study electron waves in one-dimensional potentials and in semiconductor heterostructures.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 79.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 99.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 139.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Karl F. Renk .

Problems

Problems

30.1

Quantum well.

Estimate the eigenvalues \(E_1\) and \(E_2\) of an electron in an AlAs/GaAs/AlAs quantum well (barrier height 2.2 eV; \(m_\mathrm{GaAs} = 0.07\ m_0\); \(m_\mathrm{AlAs}\) \(\sim \) 3 \(m_\mathrm{GaAs}\)) if the well consists of films of different thickness.

  1. (a)

    Film thickness = 14 GaAs monolayers

  2. (b)

    Film thickness = 2 GaAs monolayers.

30.2

Double-quantum well.

  1. (a)

    Determine the eigenvalues of a one-dimensional double well, which correspond to the two lowest energy levels (s \(=\) 1, 2) of a single one-dimensional double well. [Hint: make use of the symmetry.]

  2. (b)

    Determine the energy level splitting \(E_1^- - E_1^+\) for the two lowest levels.

  3. (c)

    Sketch the wave functions that correspond to the four lowest levels.

  4. (d)

    Calculate the level splitting occurring in an AlAs/GaAs/AlAs/GaAs/AlAs double quantum well (Fig. 30.6) for \(a_1=10\) nm and \(a_2=2\) nm.

30.3

Dispersion of electrons in a periodic potential.

Derive the dispersion relation of electrons in a periodic potential by the use of the matrix method.

30.4

Interface.

  1. (a)

    Electrons (energy \(\epsilon \)) propagate toward a GaAs/AlAs interface and are reflected. Determine the average penetration depth of electrons. [Hint: take into account the difference between the penetration depth of the wave function and of the electrons.]

  2. (b)

    Determine the penetration depth for \(\epsilon = 10\,\mathrm {meV}\) and 100 meV.

  3. (c)

    Show that the reflectivity is \(R = |k_1-I\kappa |/|k_1-I\kappa _1|\).

  4. (d)

    Explain the electron total reflector used in a GaN quantum well laser (Sect. 24.3, Fig. 24.3a).

30.5

Tunneling.

  1. (a)

    Determine the transmissivity of an AlAs barrier in a GaAs/AlAs/GaAs heterostructure for electrons of energy \(\epsilon \).

  2. (b)

    Determine the transmissivity for electrons of energy \(\epsilon = 10\,\mathrm {meV}\) and 100 meV at a barrier width of 2 monolayers of AlAs and for a barrier of 10 monolayers of AlAs.

30.6

Resonance state.

  1. (a)

    Given is a GaAs/AlAs/GaAs/AlAs/GaAs heterostructure. Determine the energy dependence of the transmissivity for electron waves of different energies.

  2. (b)

    Design a heterostructure that is transparent for electrons of \(\epsilon = 10\) meV.

  3. (c)

    Design a heterostructure that is transparent for electrons of \(\epsilon \) 100 meV.

30.7

Injector of a quantum cascade laser.

  1. (a)

    Design a quantum cascade laser of AlAs/GaAs/AlAs/GaAs/AlAs heterostructures embedded in chirped GaAs/AlAs superlattices for a quantum cascade laser that may be able to generate radiation at a frequency of 4 THz.

  2. (b)

    Estimate the thicknesses of the different layers.

  3. (c)

    Discuss the role of the superlattice, especially in view of the result of the preceding problem.

30.8

Semiconductor superlattice.

  1. (a)

    Determine the effective mass \(m^*\) of an electron in a superlattice (for propagation along the superlattice axis) for an electron with k \(\sim \) 0.

  2. (b)

    Determine \(m^*\) of a GaAs/AlAs superlattice with 14 monolayers GaAs and 2 monolayers AlAs (\(\epsilon _\mathrm{m}\) \(\sim \) 140 meV).

  3. (c)

    Determine \(m^*\) of a GaAs/AlAs superlattice with 4 monolayers GaAs and 2 monolayers AlAs (\(\epsilon _\mathrm{m}\) \(\sim \) 40 meV).

  4. (d)

    Determine the effective mass \(m^*\) of an electron in a superlattice (for propagation along the superlattice axis) for arbitrary k and discuss the slope \(m^* (k)\) and \(m^* (\epsilon )\).

  5. (e)

    Determine the group velocity \(\mathrm v_\mathrm{g}(k)\) and the peak group velocity.

  6. (f)

    Sketch the wave functions of the lowest miniband for \(k \sim 0\) and \(k = \pi /a\).

  7. (g)

    Sketch the wave functions of the second miniband for \(k \sim 0\) and \(k = \pi /a\).

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Springer International Publishing AG

About this chapter

Cite this chapter

Renk, K.F. (2017). Electron Waves in Semiconductor Heterostructures. In: Basics of Laser Physics. Graduate Texts in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-50651-7_30

Download citation

Publish with us

Policies and ethics