Abstract:Here, we present an integrated ultra-high-vacuum (UHV) apparatus for the growth of complex materials and heterostructures. The specific growth technique is the Pulsed Laser Deposition (PLD) by means of a dual-laser source based on an excimer KrF ultraviolet and solid-state Nd:YAG infra-red lasers. By taking advantage of the two laser sources—both lasers can be independently used within the deposition chambers—a large number of different materials—ranging from oxides to metals, to selenides, and others—can be s… Show more
“…Our system -named Dual-PLD -takes advantage of two independent laser sources -namely, an excimer KrF ultraviolet (UV) and a solid-state Nd:YAG infra-red (IR) one -focused on the same target position, thus allowing the deposition of different materials in the form of thin films and/or heterostructures with both the lasers. 12…”
We report on the progress of Pulsed Laser Deposition growth of thin films by using a high-power Nd:YAG laser source. We demonstrate that by using the fundamental wavelength at 1064 nm, the congruent ablation of a large number of materials can be successfully achieved. Even if the infra-red radiation of the fundamental harmonics of Nd:YAG lasers -corresponding to impinging photons with energy of about 1.16 eV -is unexpectedly proved to be also absorbed by insulating materials characterized by a large value of the band-gap (e.g. 3.0 eV for rutile TiO 2 ). Combined investigation of structural properties by transmission electron microscopy and scanning electron microscopy provides evidence of the very high-quality thin films grown by Nd:YAG lasers with no trace of precipitates and droplets over a scale of tens of micrometers.
“…Our system -named Dual-PLD -takes advantage of two independent laser sources -namely, an excimer KrF ultraviolet (UV) and a solid-state Nd:YAG infra-red (IR) one -focused on the same target position, thus allowing the deposition of different materials in the form of thin films and/or heterostructures with both the lasers. 12…”
We report on the progress of Pulsed Laser Deposition growth of thin films by using a high-power Nd:YAG laser source. We demonstrate that by using the fundamental wavelength at 1064 nm, the congruent ablation of a large number of materials can be successfully achieved. Even if the infra-red radiation of the fundamental harmonics of Nd:YAG lasers -corresponding to impinging photons with energy of about 1.16 eV -is unexpectedly proved to be also absorbed by insulating materials characterized by a large value of the band-gap (e.g. 3.0 eV for rutile TiO 2 ). Combined investigation of structural properties by transmission electron microscopy and scanning electron microscopy provides evidence of the very high-quality thin films grown by Nd:YAG lasers with no trace of precipitates and droplets over a scale of tens of micrometers.
“…16 We used the multipurpose PLD facility directly connected to the distribution chamber of the APE beamline to produce and characterize in situ undoped 2H-MoS 2 films and doped with Co (Co-MoS 2 ) and Mn (Mn-MoS 2 ) grown on an Nb:SrTiO 3 (NbSTO) substrate. 17 The in situ transfer technology offered by the NFFA-Trieste allowed measurements by surface sensitive X-ray photoemission (XPS) and X-ray absorption (XAS) techniques avoiding any surface contamination that may affect the sample properties. In this study, we performed resonant photoemission spectroscopy (RESPES) with photon energies across the Mn and Co absorption L-edges, and the Mo M-edge, to study the electronic occupation close to the Fermi level.…”
In the field of hydrogen production, MoS2 demonstrates good catalytic properties for hydrogen evolution reaction (HER), which improve when doped with metal cations. However, while the role of sulfur atoms...
“…Epitaxial Cr 1.6 Te 2 thin films were grown by pulsed laser deposition (PLD) utilizing a Nd:YAG laser source operating at its first harmonics (λ = 1064 nm) falling in the infrared regime. , Such a laser ablates a rotating stoichiometric polycrystalline Cr 1.6 Te 2 target (purity 99.99%) placed at a distance of 9.5 cm from the substrate (Figure a). This mechanism allows for a few-nanometers-thick material to be synthesized with the precision of a single monolayer.…”
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