Abstract

This work focuses on the dependence of the features of PbS films deposited by pulsed laser deposition (PLD) subsequent to the variation of the background pressure of helium (PHe). The morphology of the PLD-PbS films changes from a densely packed and almost featureless structure to a columnar and porous one as the He pressure increases. The average crystallite size related to the (111) preferred orientation increases up to 20 nm for PHe ≥ 300 mTorr. The (111) lattice parameter continuously decreases with increasing PHe values and stabilizes at PHe ≥ 300 mTorr. A downshift transition of the Raman peak of the main phonon (1LO) occurs from PHe = 300 mTorr. This transition would result from electron–LO–phonon interaction and from a lattice contraction. The optical bandgap of the films increases from 1.4 to 1.85 eV as PHe increases from 50 to 500 mTorr. The electrical resistivity of PLD-PbS is increased with PHe and reached its maximum value of 20 Ω·cm at PHe = 300 mTorr (400 times higher than 50 mTorr), which is probably due to the increasing porosity of the films. PHe = 300 mTorr is pointed out as a transitional pressure for the structural and optoelectronic properties of PLD-PbS films.

Highlights

  • We report on a systematic study of the effect of the He background pressure (PHe ) on the structural, morphological, and optoelectronic properties of the PbS

  • It is clearly seen that deposition rate (Drt) increases with pressure of helium (PHe) and reaches a maximum

  • This increase in the apparent thickness of the PbS films is a consequence of an increase of their porosity, as it has been previously reported for both IrO2 and SnO2 deposited by pulsed laser deposition (PLD) under background gas pressures in the same range as in the present study [36,37,38]

Read more

Summary

Introduction

Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. Lead sulfide (PbS) continues to attract interest because of its unique optoelectronic properties and associated applications. It is a semiconductor having a narrow bulk direct bandgap of 0.41 eV at room temperature [1] and a large exciton Bohr radius of 18 nm [2]. It exhibits strong quantum confinement effects when synthesized under the form of nanoparticles (NPs) having an average size smaller than 18 nm.

Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call