275 research outputs found
Local antimagic chromatic number of partite graphs
Let be a connected graph with and . A bijection
is called a local antimagic labeling of if
for any two adjacent vertices and , , where , and is the set of edges incident to . Thus,
any local antimagic labeling induces a proper vertex coloring of where the
vertex is assigned the color . The local antimagic chromatic number
is the minimum number of colors taken over all colorings induced by local
antimagic labelings of . Let . In this paper, the local antimagic
chromatic number of a complete tripartite graph , and copies of
a complete bipartite graph where are
determined
Wavelength-insensitive radiation coupling for multi-quantum well sensor based on intersubband absorption
Devices and techniques for coupling radiation to intraband quantum-well semiconductor sensors that are insensitive to the wavelength of the coupled radiation. At least one reflective surface is implemented in the quantum-well region to direct incident radiation towards the quantum-well layers
Wavelength-insensitive radiation coupling for multi-quantum well sensor based on intersubband absorption
Devices and techniques for coupling radiation to intraband quantum-well semiconductor sensors that are insensitive to the wavelength of the coupled radiation. At least one reflective surface is implemented in the quantum-well region to direct incident radiation towards the quantum-well layers
ADEPOS: Anomaly Detection based Power Saving for Predictive Maintenance using Edge Computing
In industry 4.0, predictive maintenance(PM) is one of the most important
applications pertaining to the Internet of Things(IoT). Machine learning is
used to predict the possible failure of a machine before the actual event
occurs. However, the main challenges in PM are (a) lack of enough data from
failing machines, and (b) paucity of power and bandwidth to transmit sensor
data to cloud throughout the lifetime of the machine. Alternatively, edge
computing approaches reduce data transmission and consume low energy. In this
paper, we propose Anomaly Detection based Power Saving(ADEPOS) scheme using
approximate computing through the lifetime of the machine. In the beginning of
the machines life, low accuracy computations are used when the machine is
healthy. However, on the detection of anomalies, as time progresses, the system
is switched to higher accuracy modes. We show using the NASA bearing dataset
that using ADEPOS, we need 8.8X less neurons on average and based on
post-layout results, the resultant energy savings are 6.4 to 6.65XComment: Submitted to ASP-DAC 2019, Japa
Tricarbonylrhenium(I) and Manganese(I) Complexes of 2-(pyrazolyl)-4-toluidine
A series of tricarbonyl rhenium(I) and manganese(I) complexes of the electroactive 2-(pyrazolyl)-4-toluidine ligand, H(pzAnMe), has been prepared and characterized including by single crystal X-ray diffraction studies. The reactions between H(pzAnMe) and M(CO)5Br afford fac-MBr(CO)3[H(pzAnMe)] (M = Mn, 1a; Re, 1b) complexes. The ionic species {fac-M(CH3CN)(CO)3[H(pzAnMe)]}(PF6) (M = Mn, 2a; Re, 2b) were prepared by metathesis of 1a or 1b with TlPF6 in acetonitrile. Complexes 1a and 1b partly ionize to {M(CH3CN)(CO)3[H(pzAnMe)]+}(Br−) in CH3CN but retain their integrity in less donating solvents such as acetone or CH2Cl2. Each of the four metal complexes reacts with (NEt4)(OH) in CH3CN to give poorly-soluble crystalline [fac-M(CO)3(μ-pzAnMe)]2 (M = Mn, 3a; Re, 3b). The solid state structures of 3a and 3b are of centrosymmetric dimeric species with bridging amido nitrogens and with pyrazolyls disposed trans- to the central planar M2N2 metallacycle. In stark contrast to the diphenylboryl derivatives, Ph2B(pzAnMe), none of the tricarbonyl group 7 metal complexes are luminescent
Preparation, Properties, and Reactivity of carbonylrhodium(I) Complexes of di(2-pyrazolylaryl)amido-pincer Ligands
A series of six carbonylrhodium(I) complexes of three new and three previously reported di(2-3R-pyrazolyl)-p-Z/X-aryl)amido pincer ligands, (RZX)Rh(CO), (R is the substituent at the 3-pyrazolyl position proximal to the metal; Z and X are the aryl substituents para- to the arylamido nitrogen) were prepared. The metal complexes were studied to assess how their properties and reactivities can be tuned by varying the groups along the ligand periphery and how they compared to other known carbonylrhodium(I) pincer derivatives. This study was facilitated by the discovery of a new CuI-catalyzed coupling reaction between 2-(pyrazolyl)-4-X-anilines (X = Me or CF3) and 2-bromoaryl-1H-pyrazoles that allow the fabrication of pincer ligands with two different aryl arms. The NNN-pincer scaffolds provide an electron-rich environment for the carbonylrhodium(I) fragment as indicated by carbonyl stretching frequencies that occur in the range of 1948–1968 cm−1. As such, the oxidative addition (OA) reactions with iodomethane proceed instantaneously to form trans-(NNN-pincer)Rh(Me)(CO)(I) in room temperature acetone solution. The OA reactions with iodoethane proceeded at a convenient rate in acetone near 45 °C which allowed detailed kinetic studies. The relative order of reactivity was found to be (CF3CF3)Rh(CO) \u3c (iPrMeMe)Rh(CO) \u3c (MeMeMe)Rh(CO) ∼ (CF3Me)Rh(CO) \u3c (MeH)Rh(CO) \u3c (MeMe)Rh(CO) with the second order rate constant of the most reactive in the series, k2 = 8 × 10−3 M−1 s−1, being about three orders of magnitude greater than those reported for [Rh(CO)2I2]− or CpRh(CO)(PPh3). After oxidative addition, the resultant rhodium(III) complexes were found to be unstable. Although a few trans-(RMeMe)Rh(E = Me, Et, or I)(CO)(I) could be isolated in pure form, all were found to slowly decompose in solution to give different products depending on the 3R-pyrazolyl substituents. Those with unsubstituted pyrazolyls (R = H) decompose with CO dissociation to give insoluble dimeric [(RMeMe)Rh(E)(μ-I)]2 while those with 3-alkylpyrazolyls (R = Me, iPr) decompose to give soluble, but unidentified products
Ultra compact spectrometer apparatus and method using photonic crystals
The present invention is directed to methods of photonic crystal formation, and to methods and apparatus for using such photonic crystals, particularly in conjunction with detector arrays. Photonic crystal parameters and detector array parameters are compared to optimize the selection and orientation of a photonic crystal shape. A photonic crystal is operatively positioned relative to a plurality of light sensors. The light sensors can be separated by a pitch distance and positioned within one half of the pitch distance of an exit surface of the photonic crystals
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