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Related Concept Videos

P-N junction01:11

P-N junction

1.1K
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
1.1K

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Well-aligned Vertically Oriented ZnO Nanorod Arrays and their Application in Inverted Small Molecule Solar Cells
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Radiation Tolerant Nanowire Array Solar Cells.

Pilar Espinet-Gonzalez1, Enrique Barrigón2, Gaute Otnes2

  • 1Department of Applied Physics and Materials Science , California Institute of Technology , Pasadena , California 91125 , United States.

ACS Nano
|October 19, 2019
PubMed
Summary
This summary is machine-generated.

III-V nanowire solar cells show significantly better radiation resistance than traditional planar cells. This breakthrough in space photovoltaics could lead to lighter, more durable solar panels for long-term space missions.

Keywords:
Monte Carlo simulationshigh specific powerirradiation-induced defectsnanowire solar cellsradiation hardspace environmentspace solar cells

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Area of Science:

  • Materials Science
  • Aerospace Engineering
  • Solid State Physics

Background:

  • Space power systems need lightweight, efficient, and reliable photovoltaics for long-duration missions.
  • Current planar III-V solar cells offer high efficiency but are limited by radiation shielding mass.
  • High-energy particle radiation in space degrades solar cell performance.

Purpose of the Study:

  • To evaluate the radiation tolerance of III-V nanowire-array solar cells compared to planar designs.
  • To investigate the potential of nanowire architectures for space photovoltaics.
  • To understand the mechanisms behind improved radiation resistance in nanowires.

Main Methods:

  • Irradiation of III-V nanowire and planar solar cells with protons (100-350 keV) and electrons (1 MeV).
  • Measurement of damage thresholds for different cell geometries and materials (GaAs, InP).
  • Monte Carlo simulations to analyze displacement density within nanowires.

Main Results:

  • Nanowire solar cells demonstrated 10-40 times higher damage thresholds than planar cells.
  • Improved radiation tolerance was observed across multiple nanowire geometries and materials.
  • Simulations indicated reduced displacement density in nanowires due to nanoscale dimensions.

Conclusions:

  • III-V nanowire-array solar cells offer superior radiation performance for space applications.
  • Nanowire architecture can significantly reduce the need for heavy radiation shielding.
  • This technology presents a pathway to high-specific-power, substrate-free space solar cells and may benefit other electronic devices.