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Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Carrier Generation and Recombination01:22

Carrier Generation and Recombination

Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
Biasing of P-N Junction01:16

Biasing of P-N Junction

The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
MOSFET Amplifiers01:17

MOSFET Amplifiers

The MOSFET, when operating in its active region, functions as a voltage-controlled current source. In this region, the gate-to-source voltage controls the drain current. This principle underlies the operation of the transconductance MOSFET amplifier. The output current is directed through a load resistor to convert this amplifier into a voltage amplifier. The output voltage is then obtained by subtracting the voltage drop across the load resistance from the supply voltage. This process results...

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Related Experiment Video

Updated: Jun 8, 2026

Laser-induced Forward Transfer for Flip-chip Packaging of Single Dies
08:21

Laser-induced Forward Transfer for Flip-chip Packaging of Single Dies

Published on: March 20, 2015

Gain coupling of class A semiconductor lasers.

Chris Hessenius1, Nathan Terry, Mahmoud Fallahi

  • 1College of Optical Sciences, University of Arizona, 1630 East University Boulevard, Tucson, Arizona 85721, USA. chessenius@optics.arizona.edu

Optics Letters
|September 18, 2010
PubMed
Summary
This summary is machine-generated.

We developed a novel semiconductor laser for dual-wavelength generation. This vertical external cavity surface emitting laser (VECSEL) technology enables simultaneous lasing at different wavelengths, offering new possibilities for optical switching applications.

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Area of Science:

  • Optics and Photonics
  • Semiconductor Lasers
  • Laser Engineering

Background:

  • Vertical External Cavity Surface Emitting Lasers (VECSELs) offer a flexible platform for high-power, high-brightness output.
  • Dual-wavelength generation is crucial for various applications, including optical communications and spectroscopy.
  • Controlling multiple laser cavities sharing a common gain region presents a significant challenge.

Purpose of the Study:

  • To develop a gain-coupled class A semiconductor laser capable of dual-wavelength generation.
  • To investigate the feasibility of optical switching between two VECSEL cavities.
  • To explore simultaneous lasing at different wavelengths within a single VECSEL structure.

Main Methods:

  • Utilized a VECSEL structure with two external cavities sharing a common gain region.
  • Employed birefringent filters within the external cavities to control laser cavity thresholds.
  • Conducted numerical simulations and experimental investigations to analyze laser behavior.

Main Results:

  • Demonstrated the possibility of optical switching between two VECSEL cavities operating at different wavelengths.
  • Showed that birefringent filters can manage carrier competition between cavities.
  • Confirmed, through numerical and experimental data, that simultaneous lasing at distinct wavelengths is achievable when considering spontaneous emission.

Conclusions:

  • The developed gain-coupled VECSEL is a viable platform for dual-wavelength generation and optical switching.
  • Simultaneous lasing at different wavelengths can be achieved by carefully managing cavity dynamics and spontaneous emission.
  • This research opens avenues for advanced laser sources with tunable and multiple wavelength outputs.