Sabrine
Ayari
a,
Michael T.
Quick
b,
Nina
Owschimikow
b,
Sotirios
Christodoulou
c,
Guillaume H. V.
Bertrand
d,
Mikhail
Artemyev
e,
Iwan
Moreels
f,
Ulrike
Woggon
b,
Sihem
Jaziri
ag and
Alexander W.
Achtstein
*b
aLaboratoire de Physique des Materiaux, Faculte des Sciences de Bizerte, Universite de Carthage, Jarzouna 7021, Tunisia
bInstitute of Optics and Atomic Physics, Technische Universität Berlin, Strasse des 17. Juni 135, 10623 Berlin, Germany. E-mail: achtstein@tu-berlin.de
cICFO-Institut de Ciencies Fotoniques, 08860 Castelldefels, Barcelona, Spain
dCEA Saclay, 91191 Gif-sur-Yvette, France
eResearch Institute for Physical Chemical Problems of Belarusian State University, 220006 Minsk, Belarus
fDepartment of Chemistry, Ghent University, Krijgslaan 281 - S3, 9000 Gent, Belgium
gLaboratoire de Physique de la Matiere Condensee, Departement de Physique, Faculte des Sciences de Tunis, Campus Universitaire, 1060 Tunis, Tunisia
First published on 18th March 2021
Correction for ‘Tuning trion binding energy and oscillator strength in a laterally finite 2D system: CdSe nanoplatelets as a model system for trion properties’ by Sabrine Ayari et al., Nanoscale, 2020, 12, 14448–14458, DOI: 10.1039/D0NR03170D.
‘Actually, the electric force lines emerging from charges within a semiconductor nanoparticle pass through the surrounding medium, having a smaller dielectric constant than the semiconductor. Therefore, in order to take the dielectric screening of Coulomb interaction properly into account, the electron–hole direct Coulomb interaction is treated here using a Rytova–Keldysh potential according to the widely accepted approach (Ref. 7,31,32,51,74–77 in the original manuscript, published here as Ref. 1–8, respectively). However to avoid the divergence of the integral of the exponential function in the Keldysh potential, we can construct an approximate expression for
c(ρ) in terms of elementary functions
(See ref. 8 below for details). This potential is better than using an unscreened vacuum Coulomb potential together with envelope functions in z-direction, the standard approach for quantum wells. Here, rs = εcdSeZ0/(2εenv) is the dielectric screening length, Z0 = (a0/2) × 4.5 ML is the platelet thickness and γ is the Euler constant’.
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
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