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Related Concept Videos

Nuclear Fusion02:45

Nuclear Fusion

The process of converting very light nuclei into heavier nuclei is also accompanied by the conversion of mass into large amounts of energy, a process called fusion. The principal source of energy in the sun is a net fusion reaction in which four hydrogen nuclei fuse and ultimately produce one helium nucleus and two positrons.
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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.
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Atomic Nuclei: Nuclear Relaxation Processes

In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis. This...
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview01:19

Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview

In inductively coupled plasma–mass spectrometry (ICP–MS), an inductively coupled plasma (ICP) torch is used as an atomizer and ionizer. Solid samples are dissolved and volatilized before being introduced into the high-temperature argon plasma, while solution samples are nebulized and passed through the high-temperature argon plasma. Plasma dissociates the analytes and ionizes their component atoms to form a mixture of positive ions and molecular species. The positive ions are then passed on to...
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Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
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Published on: August 1, 2017

Kinetic processes in recombining H3+ plasmas.

Rainer Johnsen1

  • 1Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA 15260, USA. rj@pitt.edu

Philosophical Transactions. Series A, Mathematical, Physical, and Engineering Sciences
|October 3, 2012
PubMed
Summary

Recombination in hydrogen plasmas involves both binary and third-body mechanisms. Understanding these processes is crucial for modeling hydrogen discharges and analyzing plasma afterglow data accurately.

Area of Science:

  • Plasma Physics
  • Chemical Kinetics

Background:

  • Recombination is a key process in plasma chemistry.
  • Hydrogen plasmas contain trihydrogen cations (H3+).
  • Binary recombination is well-studied, but third-body effects are less understood.

Purpose of the Study:

  • Investigate third-body assisted recombination mechanisms in H3+ plasmas.
  • Analyze the impact of third-body effects on plasma modeling.
  • Improve the inference of binary recombination coefficients from afterglow data.

Main Methods:

  • Theoretical modeling of recombination processes.
  • Analysis of plasma discharge and afterglow data.
  • Focus on third-body assisted recombination pathways.

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Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
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Emission Spectroscopic Boundary Layer Investigation during Ablative Material Testing in Plasmatron
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Main Results:

  • Third-body mechanisms significantly influence recombination rates in H3+ plasmas.
  • These effects are critical for accurate hydrogen discharge simulations.
  • Quantified the contribution of third-body assisted recombination.

Conclusions:

  • Third-body effects are essential for understanding recombination in H3+ plasmas.
  • Accurate modeling of hydrogen discharges requires incorporating these mechanisms.
  • Improved methods for deriving binary recombination coefficients from experimental data.