Related Experiment Video
Updated: Apr 5, 2026

07:44
Resonance Raman Spectroscopy of Extreme Nanowires and Other 1D Systems
Published on: April 28, 2016
15.7K
Multiparticle Exciton Ionization in Shallow Doped Carbon Nanotubes
Jay D Sau1, Jared J Crochet, Stephen K Doorn
1†Department of Physics, Harvard University, Cambridge, Massachusetts, United States.
The Journal of Physical Chemistry Letters
|August 21, 2015
Summary
Shallow hole doping in carbon nanotubes causes excitons to ionize into electron-hole pairs. This process, dependent on chirality, enhances exciton decay and leads to fluorescence quenching at higher dopant densities.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanotechnology
Background:
- Semiconducting carbon nanotubes (CNTs) exhibit unique electronic properties.
- Exciton behavior in CNTs is crucial for their optoelectronic applications.
- Valley degeneracy in small-diameter CNTs presents opportunities for novel phenomena.
Purpose of the Study:
- To investigate the effect of shallow hole doping on excitons in small-diameter semiconducting CNTs.
- To elucidate the mechanism of exciton ionization and its dependence on dopant density and chirality.
- To explain the observed fluorescence quenching in doped CNTs.
Main Methods:
- Theoretical prediction of resonant ionization of excitons.
- Modeling the dependence of exciton decay rate on dopant density.
- Analysis of multiparticle exciton ionization for fluorescence quenching.
Main Results:
- Shallow hole doping induces resonant ionization of excitons into free electron-hole pairs.
- Exciton decay efficiency scales with the square of the dopant density.
- Multiparticle exciton ionization explains delocalized fluorescence quenching.
Conclusions:
- Resonant exciton ionization is a key mechanism in doped CNTs.
- Chirality plays a critical role in this doping-induced phenomenon.
- Understanding this mechanism is vital for designing CNT-based electronic and optoelectronic devices.
More Related Videos
Related Concept Videos
¹³C NMR: ¹H–¹³C Decoupling
2.1K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
2.1K
Chemical Ionization (CI) Mass Spectrometry
1.7K
The molecular ion peak of a molecule in the mass spectrum provides vital information for molecular identification. However, conventional electron impact ionization can lead to the rapid dissociation of some molecular ions before they reach the detector. A milder ionization method is required to increase the lifetime of such ionized analyte molecules. Chemical ionization (CI) is a gas-phase protonation reaction useful for mass-analyzing analyte molecules that are easily protonated to yield the...
1.7K
π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds
2.0K
In aromatic compounds, such as benzene, the circulation of (4n + 2) π-electrons sets up a diamagnetic or diatropic ring current around the perimeter of the molecule. This current induces a magnetic field that opposes the external field inside the ring and reinforces it on the outside. The protons in benzene are deshielded and exhibit high chemical shifts in the range 6.5–8.5 ppm. The shielding effect at the center of the ring is evident in complex aromatic molecules, such as...
2.0K
π Electron Effects on Chemical Shift: Overview
1.9K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.9K

