Irradiation-driven molecular dynamics simulation of the FEBID process for Pt(PF₃)₄

• Alexey Prosvetov,
• Alexey V. Verkhovtsev,
• Gennady Sushko and
• Andrey V. Solov’yov

Beilstein J. Nanotechnol. 2021, 12, 1151–1172, doi:10.3762/bjnano.12.86

• distributions can be obtained by means of Monte Carlo (MC) simulations of electron transport [37]. There are several codes suitable for this purpose with different possibilities and limitations, for example, SEED [38], Geant4 [39], and PENELOPE [40]. The yield of SE generated in various materials can also be

Temperature-tunable lasing from dye-doped chiral microdroplets encapsulated in a thin polymeric film

• Gia Petriashvili,
• Mauro Daniel Luigi Bruno,
• Maria Penelope De Santo and
• Riccardo Barberi

Beilstein J. Nanotechnol. 2018, 9, 379–383, doi:10.3762/bjnano.9.37

• Gia Petriashvili Mauro Daniel Luigi Bruno Maria Penelope De Santo Riccardo Barberi Institute of Cybernetics of the Georgian Technical University, Tbilisi 0175, Georgia Physics Department, University of Calabria, Rende 87036, Italy CNR-Nanotec UOS di Cosenza , c/o University of Calabria, Rende

Simulation of electron transport during electron-beam-induced deposition of nanostructures

• Francesc Salvat-Pujol,
• Harald O. Jeschke and
• Roser Valentí

Beilstein J. Nanotechnol. 2013, 4, 781–792, doi:10.3762/bjnano.4.89

• during post-growth electron-beam treatments. Keywords: electron backscattering; electron transport; (F)EBID; Monte Carlo simulation; PENELOPE; Introduction Electron-beam-induced deposition (EBID) [1][2][3] is a suitable method for the template-free fabrication of nanostructures. Molecules of a

• -assisted electron-beam post-growth nanostructure treatments [5][6]. We consider various geometric settings as well as different materials relevant for the EBID growth of nanostructures. For our simulations we use the Monte Carlo code for radiation transport PENELOPE [7], in which a statistical set of

• method for the simulation of radiation transport is a numerical means of solving the Boltzmann transport equation in an arbitrary geometry. The computer code system PENELOPE yields trajectories of primary and secondary particles according to state-of-the-art interaction cross sections on sample