58 research outputs found
Evolution of the interfacial structure of LaAlO3 on SrTiO3
The evolution of the atomic structure of LaAlO3 grown on SrTiO3 was
investigated using surface x-ray diffraction in conjunction with
model-independent, phase-retrieval algorithms between two and five monolayers
film thickness. A depolarizing buckling is observed between cation and oxygen
positions in response to the electric field of polar LaAlO3, which decreases
with increasing film thickness. We explain this in terms of competition between
elastic strain energy, electrostatic energy, and electronic reconstructions.
The findings are qualitatively reproduced by density-functional theory
calculations. Significant cationic intermixing across the interface extends
approximately three monolayers for all film thicknesses. The interfaces of
films thinner than four monolayers therefore extend to the surface, which might
affect conductivity
Unit cell of graphene on Ru(0001): a 25 x 25 supercell with 1250 carbon atoms
The structure of a single layer of graphene on Ru(0001) has been studied
using surface x-ray diffraction. A surprising superstructure has been
determined, whereby 25 x 25 graphene unit cells lie on 23 x 23 unit cells of
Ru. Each supercell contains 2 x 2 crystallographically inequivalent subcells
caused by corrugation. Strong intensity oscillations in the superstructure rods
demonstrate that the Ru substrate is also significantly corrugated down to
several monolayers, and that the bonding between graphene and Ru is strong and
cannot be caused by van der Waals bonds. Charge transfer from the Ru substrate
to the graphene expands and weakens the C-C bonds, which helps accommodate the
in-plane tensile stress. The elucidation of this superstructure provides
important information in the potential application of graphene as a template
for nanocluster arrays.Comment: 9 pages, 3 figures, paper submitted to peer reviewed journa
Study of the stability of the 5-aminolevulinic acid tyrosine ester in aqueous solution
Photodynamic therapy based on photoactivable porphyrins (PAPs) can treat various dermatological conditions. The side-effects as well as the non-selective or insufficient accumulation of PAPs in the targeted tissues limit performances. We studied the stability in solution at different temperatures (21 degrees C; 4 degrees C), different pH values (7.5; 2.0), and as a function of time of 5-aminolevulinic acid's Tyrosine-ester, a molecule presenting interesting properties to selectively produce PAPs in blood vessels after topical application. Solutions of this precursor can be kept up to 24 h at refrigerated temperatures and under acidic pH. At room temperature or physiological pH, they must be prepared minutes before their use
Graphene on Ru(0001): A corrugated and chiral structure
We present a structural analysis of the graphene/Ru(0001) system obtained by
surface x-ray diffraction. The data were fit using Fourier-series expanded
displacement fields from an ideal bulk structure, plus the application of
symmetry constraints. The shape of the observed superstructure rods proves a
reconstruction of the substrate, induced by strong bonding of graphene to
ruthenium. Both the graphene layer and the underlying substrate are corrugated,
with peak-to-peak heights of (0.82 +/- 0.15) A and (0.19 +/- 0.02) A for the
graphene and topmost Ru-atomic layer, respectively. The Ru-corrugation decays
slowly over several monolayers into the bulk. The system also exhibits
chirality, whereby in-plane rotations of up to 2.0 degrees in those regions of
the superstructure where the graphene is weakly bound are driven by elastic
energy minimization
Kinetics and thermodynamics of carbon segregation and graphene growth on Ru(0001)
We measure the concentration of carbon adatoms on the Ru(0001) surface that
are in equilibrium with C atoms in the crystal's bulk by monitoring the
electron reflectivity of the surface while imaging. During cooling from high
temperature, C atoms segregate to the Ru surface, causing graphene islands to
nucleate. Using low-energy electron microscopy (LEEM), we measure the growth
rate of individual graphene islands and, simultaneously, the local
concentration of C adatoms on the surface. We find that graphene growth is fed
by the supersaturated, two-dimensional gas of C adatoms rather than by direct
exchange between the bulk C and the graphene. At long times, the rate at which
C diffuses from the bulk to the surface controls the graphene growth rate. The
competition among C in three states - dissolved in Ru, as an adatom, and in
graphene - is quantified and discussed. The adatom segregation enthalpy
determined by applying the simple Langmuir-McLean model to the
temperature-dependent equilibrium concentration seriously disagrees with the
value calculated from first-principles. This discrepancy suggests that the
assumption in the model of non-interacting C is not valid
Laser-induced etching of few-layer graphene synthesized by Rapid-Chemical Vapour Deposition on Cu thin films
The outstanding electrical and mechanical properties of graphene make it very
attractive for several applications, Nanoelectronics above all. However a
reproducible and non destructive way to produce high quality, large-scale area,
single layer graphene sheets is still lacking. Chemical Vapour Deposition of
graphene on Cu catalytic thin films represents a promising method to reach this
goal, because of the low temperatures (T < 900 Celsius degrees) involved during
the process and of the theoretically expected monolayer self-limiting growth.
On the contrary such self-limiting growth is not commonly observed in
experiments, thus making the development of techniques allowing for a better
control of graphene growth highly desirable. Here we report about the local
ablation effect, arising in Raman analysis, due to the heat transfer induced by
the laser incident beam onto the graphene sample.Comment: v1:9 pages, 8 figures, submitted to SpringerPlus; v2: 11 pages,
PDFLaTeX, 9 figures, revised peer-reviewed version resubmitted to
SpringerPlus; 1 figure added, figure 1 and 4 replaced,typos corrected,
"Results and discussion" section significantly extended to better explain
etching mechanism and features of Raman spectra, references adde
Size Quantization in Planar Graphene-Based Heterostructures: Pseudospin Splitting, Interface States, and Excitons
A planar quantum-well device made of a gapless graphene nanoribbon with edges
in contact with gapped graphene sheets is examined. The size-quantization
spectrum of charge carriers in an asymmetric quantum well is shown to exhibit a
pseudospin splitting. Interface states of a new type arise from the crossing of
dispersion curves of gapless and gapped graphene materials. The exciton
spectrum is calculated for a planar graphene quantum well. The effect of an
external electric field on the exciton spectrum is analyzed.Comment: 15 pages, 14 figure
Optical spectroscopy of the bladder washout fluid to optimize fluorescence cystoscopy with Hexvix®.
Fluorescence cystoscopy enhances detection of early bladder cancer. Water used to inflate the bladder during the procedure rapidly contains urine, which may contain fluorochromes. This frequently degradesfluorescence images. Samples of bladder washout fluid (BWF) or urine were collected (15 subjects). We studiedtheir fluorescence properties and assessed changes induced by pH (4 to 9) and temperature (15°C to 41°C).A typical fluorescence spectrum of BWF features a main peak (excitation/emission: 320∕420 nm, FWHM =50∕100 nm) and a weaker (5% to 20% of main peak intensity), secondary peak (excitation/emission: 455∕525 nm, FWHM = 80∕50 nm). Interpatient fluctuations of fluorescence intensity are observed. Fluorescence intensity decreases when temperature increases (max 30%) or pH values vary (max 25%). Neither approach is compatible with clinical settings. Fluorescence lifetime measurements suggest that 4-pyridoxic acid/riboflavin is the most likely molecule responsible for urine's main/secondary fluorescence peak. Our measurements give an insight into the spectroscopy of the detrimental background fluorescence. This should be included in the optical design of fluorescence cystoscopes. We estimate that restricting the excitation range from 370-430 nm to 395-415 nm would reduce the BWF background by a factor 2
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