Electron and hole wavefunctions in a semiconductor QW

In summary, optical transitions in quantum wells (QWs) involve both the energy levels of the electrons and holes, as well as the matrix elements that describe their interaction. The electric field plays a crucial role in determining the energy levels and allowed transitions. The selection rules for transitions between opposite parity states in QWs add an extra step in the transition process and affect the overall transition rate. The matrix elements also play a significant role in both stimulated emission and absorption.
  • #1
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Homework Statement


I'm attempting to understand better how optical transitions occur in a QW (more specifically quantum cascade lasers) with and without an electric field.

If an electron in the second excited state falls to the first, is it simply the transistion matrix between these two equations that determine the transistion rate or is the parity of the hole states also important? Does this matrix affect stimulated emission/absorption or is it only important because of the effect of spontaneous emision?

Homework Equations





The Attempt at a Solution


http://www.iop.org/EJ/abstract/0022-3719/20/19/010" explains that 'transitions between opposite-parity electron and hole levels are forbidden' which tells me I'm not understanding correctly. I assumed that the electron only recombines with the hole state when it falls to the ground state, am I wrong?
 
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  • #2


Hello,

Thank you for your question. Optical transitions in quantum wells (QWs) are a complex phenomenon that involve both the energy levels of the electrons and holes, as well as the matrix elements that describe the interaction between them. The electric field plays a crucial role in determining the energy levels and thus the possible transitions in a QW.

To answer your first question, it is not only the transition matrix elements that determine the transition rate, but also the selection rules that govern which transitions are allowed. In a QW, transitions between states with opposite parity (i.e. even-odd or odd-even) are forbidden, which means that the electron cannot directly transition from the second excited state to the first excited state. Instead, it must first transition to a state with the same parity (e.g. odd-odd or even-even) and then to the first excited state. This adds an extra step in the transition process and thus affects the overall transition rate.

Regarding your second question, the matrix elements do indeed affect both stimulated emission and absorption. In stimulated emission, the matrix element determines the strength of the interaction between the electron and hole, and thus the probability of the electron transitioning to a lower energy state. In absorption, the matrix element determines the probability of the electron absorbing a photon and transitioning to a higher energy state.

I hope this helps clarify the role of the transition matrix elements and parity in optical transitions in QWs. If you have any further questions, please don't hesitate to ask. Good luck with your studies!
 

1. What are electron and hole wavefunctions?

Electron and hole wavefunctions refer to the spatial distribution of the probability of finding an electron or hole in a specific location within a semiconductor quantum well (QW). These wavefunctions describe the quantum mechanical behavior of electrons and holes, which are the charge carriers in a semiconductor material.

2. What is a semiconductor QW?

A semiconductor quantum well (QW) is a thin layer of semiconductor material sandwiched between two layers of a different semiconductor material. This creates a potential well that confines electrons and holes within the thin layer, leading to quantum confinement effects and unique electronic properties.

3. How are electron and hole wavefunctions related in a QW?

In a QW, the electron and hole wavefunctions are coupled through the Coulomb interaction. This means that the spatial distribution of the electron wavefunction affects the spatial distribution of the hole wavefunction, and vice versa. This coupling is important for understanding the behavior of charge carriers in a QW.

4. What factors affect the shape and size of electron and hole wavefunctions in a QW?

The shape and size of electron and hole wavefunctions in a QW are primarily determined by the width and composition of the QW layer, as well as the energy level of the charge carriers. The shape and size can also be influenced by external factors such as temperature and electric fields.

5. How do electron and hole wavefunctions contribute to the electronic properties of a QW?

The shape and size of electron and hole wavefunctions in a QW determine the energy levels and transition probabilities of charge carriers, which in turn affect the electronic properties of the material. These properties include the bandgap, carrier mobility, and optical properties, making QWs important for a wide range of applications in optoelectronic devices.

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