Related Experiment Video
Updated: Aug 22, 2025

Resonance Fluorescence of an InGaAs Quantum Dot in a Planar Cavity Using Orthogonal Excitation and Detection
Published on: October 13, 2017
Identity of the reversible hole traps in InP/ZnSe core/shell quantum dots
Anne Myers Kelley1, Paul Cavanaugh1, Haochen Sun1
1Department of Chemistry and Biochemistry, University of California Merced, 5200 North Lake Road, Merced, California 95343, USA.
Researchers identified a specific defect in indium phosphide/zinc selenide/zinc sulfide quantum dots (InP/ZnSe/ZnS QDs) responsible for reversible hole trapping. This defect, a substitutional indium next to a zinc vacancy, helps understand photoluminescence quenching in these nanomaterials.
Area of Science:
- Materials Science
- Quantum Dot Research
- Solid-State Physics
Background:
- Quantum dots (QDs) are crucial in optoelectronics, but defects can limit their performance.
- Reversible hole trapping in InP/ZnSe/ZnS QDs affects their photoluminescence properties.
- Understanding defect sites is key to improving QD stability and efficiency.
Purpose of the Study:
- To identify the specific defect responsible for reversible hole trapping in InP/ZnSe/ZnS QDs.
- To correlate experimental observations with theoretical calculations for defect identification.
- To elucidate the mechanism of hole trapping and its impact on QD behavior.
Main Methods:
- Combined density functional theory (DFT) calculations with time-resolved photoluminescence experiments.
- Investigated excess indium in the shell of InP/ZnSe/ZnS QDs.
- Analyzed the effect of additives like zinc oleate, acetate, and carboxylic acids on trapping.
Main Results:
- Identified a substitutional indium adjacent to a zinc vacancy (In³⁺/VZn²⁻) as the most likely hole trapping species.
- Demonstrated that excess indium is necessary for trapping, and its extent is modulated by additives.
- Calculations showed this defect's energy levels are suitable for trapping quantum-confined holes.
Conclusions:
- The In³⁺/VZn²⁻ defect is the primary cause of reversible hole trapping in these QDs.
- This finding provides critical insights into defect engineering for enhanced QD performance.
- The study clarifies the role of specific atomic configurations in QD photophysics.
Related Concept Videos
Types of Semiconductors
Insensitive Nuclei Enhanced by Polarization Transfer (INEPT)
P-N junction
Biasing of P-N Junction
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 Junctions
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...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...

