1,724 research outputs found
Surface Dipoles and Work Functions of Alkylthiolates and Fluorinated Alkylthiolates on Au(111)
We study the dipole formation at the surface formed by -CH3 and -CF3
terminated shortchain alkyl-thiolate monolayers on Au(111). In particular, we
monitor the change in work function upon chemisorption using density functional
theory calculations. We separate the surface dipole into two contributions,
resulting from the gold-adsorbate interaction and the intrinsic dipole of the
adsorbate layer, respectively. The two contributions turn out to be
approximately additive. Adsorbate dipoles are defined by calculating dipole
densities of free-standing molecular monolayers. The gold-adsorbate interaction
is to a good degree determined by the Au-S bond only. This bond is nearly
apolar and its contribution to the surface dipole is relatively small. The
surface dipole of the self-assembled monolayer is then dominated by the
intrinsic dipole of the thiolate molecules. Alkyl-thiolates increase the work
function of Au(111), whereas fluorinated alkyl-thiolates decrease it.Comment: 24 pages, 5 figures, 4 table
First-principles study of the interaction and charge transfer between graphene and metals
Measuring the transport of electrons through a graphene sheet necessarily
involves contacting it with metal electrodes. We study the adsorption of
graphene on metal substrates using first-principles calculations at the level
of density functional theory. The bonding of graphene to Al, Ag, Cu, Au and
Pt(111) surfaces is so weak that its unique "ultrarelativistic" electronic
structure is preserved. The interaction does, however, lead to a charge
transfer that shifts the Fermi level by up to 0.5 eV with respect to the
conical points. The crossover from p-type to n-type doping occurs for a metal
with a work function ~5.4 eV, a value much larger than the work function of
free-standing graphene, 4.5 eV. We develop a simple analytical model that
describes the Fermi level shift in graphene in terms of the metal substrate
work function. Graphene interacts with and binds more strongly to Co, Ni, Pd
and Ti. This chemisorption involves hybridization between graphene -states
and metal d-states that opens a band gap in graphene. The graphene work
function is as a result reduced considerably. In a current-in-plane device
geometry this should lead to n-type doping of graphene.Comment: 12 pages, 9 figure
Formal Model Engineering for Embedded Systems Using Real-Time Maude
This paper motivates why Real-Time Maude should be well suited to provide a
formal semantics and formal analysis capabilities to modeling languages for
embedded systems. One can then use the code generation facilities of the tools
for the modeling languages to automatically synthesize Real-Time Maude
verification models from design models, enabling a formal model engineering
process that combines the convenience of modeling using an informal but
intuitive modeling language with formal verification. We give a brief overview
six fairly different modeling formalisms for which Real-Time Maude has provided
the formal semantics and (possibly) formal analysis. These models include
behavioral subsets of the avionics modeling standard AADL, Ptolemy II
discrete-event models, two EMF-based timed model transformation systems, and a
modeling language for handset software.Comment: In Proceedings AMMSE 2011, arXiv:1106.596
Magnetic Order in the 2D Heavy-Fermion System CePt2In7 studied by muSR
The low-temperature microscopic magnetic properties of the quasi-2D
heavyfermion compound, CePt2In7 are investigated by using a positive muon-spin
rotation and relaxation (?muSR) technique. Clear evidence for the formation of
a commensurate antiferromagnetic order below TN=5.40 K is presented. The
magnetic order parameter is shown to fit well to a modified BSC gap-energy
function in a strong-coupling scenario.Comment: Accepted in Journal of Physics: Conference Series (2014
ΠΠΊΡΡΠ°Π»ΡΠ½ΠΎΡΡΡ ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠΈ ΡΡΠΎΠΌΠ±ΠΎΡΠΌΠ±ΠΎΠ»ΠΈΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ Π² ΠΏΡΠ΅Π΄-, ΠΈΠ½ΡΡΠ°- ΠΈ ΠΏΠΎΡΡΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅
Catedra Anesteziologie Εi Reanimatologie nr. 2, USMF βNicolae TestemiΕ£anuβThe purpose of this article is an informative analysis of the efficiency of prophylaxis of the pulmonary artery trombembolism. Out of 627 patients
monitored, 473 had the benefit of a perioperatory tromboprophylaxis, while the other 154 patients got only a postoperatory tromboprophylaxis.
The incidence of pulmonary artery trombembolism is 0.48%, this result refers only to patients operated on urgently. The incidence of lethal
cases is 0.16%. Pulmonary artery trombembolism incidence varies depending on the combination of predisposing factors. We studied several
combined methods of prophylaxis. Priority was the combination of mechanical methods (application of elastic bandages on the legs) with low
molecular mass heparins. From observation of the study we determined an increased efficiency using the combination of mechanical methods
with Enoxoparine (Klexan) in tromboprophylaxis of patients with moderate and high risk of pulmonary artery trombembolism. The priorities
of Enoxoparine, to other low molecular weight heparins do not require the determination of bleeding and clotting time during administration.
Also there was no change in platelet count in patients receiving Enoxoparine.Π¦Π΅Π»ΡΡ Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠΈ ΡΡΠΎΠΌΠ±ΠΎΡΠΌΠ±ΠΎΠ»ΠΈΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ Π² ΠΏΡΠ΅Π΄-,
ΠΈΠ½ΡΡΠ°- ΠΈ ΠΏΠΎΡΡΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅. ΠΠ· 627 ΠΎΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², 473 Π±ΠΎΠ»ΡΠ½ΡΠΌ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»Π°ΡΡ, ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ, ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠ°
ΡΡΠΎΠΌΠ±ΠΎΡΠΌΠ±ΠΎΠ»ΠΈΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ Π² ΠΏΡΠ΅Π΄-, ΠΈΠ½ΡΡΠ°- ΠΈ ΠΏΠΎΡΡΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅, 154 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌ - ΡΠΎΠ»ΡΠΊΠΎ Π² ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅.
ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠΉ ΡΠ΅Π·ΡΠ»ΡΡΠ°Ρ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π΅ΠΌΠΎΡΡΠΈ ΡΡΠΎΠΌΠ±ΠΎΡΠΌΠ±ΠΎΠ»ΠΈΠ΅ΠΉ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ - 0,48%, ΠΎΡΠ½ΠΎΡΠΈΡΡΡ ΡΠΎΠ»ΡΠΊΠΎ ΠΊ Π±ΠΎΠ»ΡΠ½ΡΠΌ, ΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ Π²
ΡΡΠΎΡΠ½ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅. Π‘ΠΌΠ΅ΡΡΠ½ΠΎΡΡΡ 0,16% Π²Π°ΡΡΠΈΡΡΠ΅Ρ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΡ ΠΏΡΠ΅Π΄ΡΠ°ΡΠΏΠΎΠ»Π°Π³Π°ΡΡΠΈΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ². ΠΡΠ»ΠΎ ΠΈΠ·ΡΡΠ΅Π½ΠΎ Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΎ
ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠΈ. ΠΡΠΈΠΎΡΠΈΡΠ΅ΡΠ½ΡΠΌ Π±ΡΠ»ΠΎ ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΠ΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² (ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ»Π°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ Π±ΠΈΠ½ΡΠ° Π½Π°
Π½ΠΎΠ³Π°Ρ
) Ρ Π³Π΅ΠΏΠ°ΡΠΈΠ½Π°ΠΌΠΈ Ρ Π½ΠΈΠ·ΠΊΠΎΠΉ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΎΠΉ ΠΌΠ°ΡΡΠΎΠΉ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΎΡΡ ΠΏΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² Ρ Π΅Π½ΠΎΠΊΡΠΈΠΏΠ°ΡΠΈΠ½ΠΎΠΌ (Klexan) Π² ΠΏΡΠΎΡΠΈΠ»Π°ΠΊΡΠΈΠΊΠ΅ ΡΡΠΎΠΌΠ±ΠΎΡΠΌΠ±ΠΎΠ»ΠΈΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΠΌΠ΅ΡΠ΅Π½Π½ΡΠΌ ΠΈ Π²ΡΡΠΎΠΊΠΈΠΌ
ΡΠΈΡΠΊΠΎΠΌ ΡΡΠΎΠΌΠ±ΠΎΡΠΌΠ±ΠΎΠ»ΠΈΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ. ΠΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²ΠΎΠΌ Π΅Π½ΠΎΠΊΡΠΈΠΏΠ°ΡΠΈΠ½Π° ΠΈ Π΄ΡΡΠ³ΠΈΡ
Π½ΠΈΠ·ΠΊΠΎΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
Π³Π΅ΠΏΠ°ΡΠΈΠ½ΠΎΠ² ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠΎ, ΡΡΠΎ
Π½Π΅ ΡΡΠ΅Π±ΡΠ΅ΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΊΡΠΎΠ²ΠΎΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΈ Π²ΡΠ΅ΠΌΡ ΡΠ²Π΅ΡΡΡΠ²Π°Π½ΠΈΡ ΠΊΡΠΎΠ²ΠΈ Π²ΠΎ Π²ΡΠ΅ΠΌΡ ΠΏΡΠΈΠ΅ΠΌΠ°. Π’Π°ΠΊΠΆΠ΅ Π½Π΅ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΡΡ Π½ΠΈΠΊΠ°ΠΊΠΈΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ Π²
ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅ ΡΡΠΎΠΌΠ±ΠΎΡΠΈΡΠΎΠ² Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΏΠΎΠ»ΡΡΠ°ΡΡΠΈΡ
Π΅Π½ΠΎΠΊΡΠΈΠΏΠ°ΡΠΈΠ½
Level-3 Calorimetric Resolution available for the Level-1 and Level-2 CDF Triggers
As the Tevatron luminosity increases sophisticated selections are required to
be efficient in selecting rare events among a very huge background. To cope
with this problem, CDF has pushed the offline calorimeter algorithm
reconstruction resolution up to Level 2 and, when possible, even up to Level 1,
increasing efficiency and, at the same time, keeping under control the rates.
The CDF Run II Level 2 calorimeter trigger is implemented in hardware and is
based on a simple algorithm that was used in Run I. This system has worked well
for Run II at low luminosity. As the Tevatron instantaneous luminosity
increases, the limitation due to this simple algorithm starts to become clear:
some of the most important jet and MET (Missing ET) related triggers have large
growth terms in cross section at higher luminosity. In this paper, we present
an upgrade of the Level 2 Calorimeter system which makes the calorimeter
trigger tower information available directly to a CPU allowing more
sophisticated algorithms to be implemented in software. Both Level 2 jets and
MET can be made nearly equivalent to offline quality, thus significantly
improving the performance and flexibility of the jet and MET related triggers.
However in order to fully take advantage of the new L2 triggering capabilities
having at Level 1 the same L2 MET resolution is necessary. The new Level-1 MET
resolution is calculated by dedicated hardware. This paper describes the
design, the hardware and software implementation and the performance of the
upgraded calorimeter trigger system both at Level 2 and Level 1.Comment: 5 pages, 5 figures,34th International Conference on High Energy
Physics, Philadelphia, 200
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