9 research outputs found
Melanocortin-4 receptor gene: case-control study and transmission disequilibrium test confirm that functionally relevant mutations are compatible with a major gene effect for extreme obesity
We initially performed a mutation screen of the coding region of the MC4R in 808 extremely obese children and adolescents and 327 underweight or normal-weight controls allowing for a case-control study. A total of 16 different missense, nonsense, and frameshift mutations were found in the obese study group; five of these have not been observed previously. In vitro assays revealed that nine [the haplotype (Y35X; D37V) was counted as one mutation] of the 16 mutations led to impaired cAMP responses, compared with wild-type receptor constructs. In contrast, only one novel missense mutation was detected in the controls, which did not alter receptor function. The association test based on functionally relevant mutations was positive (P = 0.006, Fisher's exact test, one-sided). We proceeded by screening a total of 1040 parents of 520 of the aforementioned obese young index patients to perform transmission disequilibrium tests. The 11 parental carriers of functionally relevant mutations transmitted the mutation in 81.8% (P = 0.033; exact one-sided McNemar test). These results support the hypothesis that these MC4R mutations represent major gene effects for obesity
Nanostructured Submicron Block Copolymer Dots by Sacrificial Stamping: A Potential Preconcentration Platform for Locally Resolved Sensing, Chemistry, and Cellular Interactions
Classical
contact lithography involves patterning of surfaces by
embossing or by transfer of ink. We report direct lithographic transfer
of parts of sacrificial stamps onto counterpart surfaces. Using sacrificial
stamps consisting of the block copolymer polystyrene-<i>block</i>-poly(2-pyridine) (PS-<i>b</i>-P2VP), we deposited arrays
of nanostructured submicron PS-<i>b</i>-P2VP dots with heights
of ∼100 nm onto silicon wafers and glass slides. The sacrificial
PS-<i>b</i>-P2VP stamps were topographically patterned with
truncated-pyramidal contact elements and penetrated by spongy-continuous
nanopore systems. The spongy nature of the sacrificial PS-<i>b</i>-P2VP stamps supported formation of adhesive contact to
the counterpart surfaces and the rupture of the contact elements during
stamp retraction. The submicron PS-<i>b</i>-P2VP dots generated
by sacrificial stamping can be further functionalized; examples include
loading submicron PS-<i>b</i>-P2VP dots with dyes and attachment
of gold nanoparticles to their outer surfaces. The arrays of submicron
PS-<i>b</i>-P2VP dots can be integrated into setups for
advanced optical microscopy, total internal reflection fluorescence
microscopy, or Raman microscopy. Arrays of nanostructured submicron
block copolymer dots may represent a preconcentration platform for
locally resolved sensing and locally resolved monitoring of cellular
interactions or might be used as microreactor arrays in lab-on-chip
configurations
Ordered Topographically Patterned Silicon by Insect-Inspired Capillary Submicron Stamping
Insect-inspired capillary
submicron stamping and subsequent surface-limited metal-assisted chemical
etching (MACE) with ammonium bifluoride as a HF source are employed
for the high-throughput production of ordered topographically patterned
silicon (tpSi). Insect feet often possess hairy contact elements through
which adhesive secretion is deployed. Thus, arrays of adhesive secretion
drops remain as footprints on contact surfaces. Stamps for insect-inspired
capillary submicron stamping having surfaces topographically patterned
with contact elements mimic the functional principles of such insect
feet. They contain spongy continuous nanopore networks penetrating
the entire stamps. Any ink (organic or aqueous) may be supplied from
the backside of the nanoporous stamps to the contact elements. We
generated ordered arrays of submicron AgNO<sub>3</sub> dots extending
square millimeters on Si by manual stamping with cycle times of a
few seconds under ambient conditions; at higher load, ordered holey
AgNO<sub>3</sub> films were obtained. Surface-limited MACE correspondingly
yielded either macroporous tpSi or Si pillar arrays. Inkjet printing
of polymer solutions onto the tpSi yielded patterns of polymer blots
conformally covering the tpSi. Such blot patterns could potentially
represent a starting point for the development of persistent and scratch-resistant
identity labels or quick response codes on silicon surfaces
Calcium-Induced Molecular Rearrangement of Peptide Folds Enables Biomineralization of Vaterite Calcium Carbonate
Proteins
can control mineralization of CaCO<sub>3</sub> by selectively
triggering the growth of calcite, aragonite or vaterite phases. The
templating of CaCO<sub>3</sub> by proteins must occur predominantly
at the protein/CaCO<sub>3</sub> interface, yet molecular-level insights
into the interface during active mineralization have been lacking.
Here, we investigate the role of peptide folding and structural flexibility
on the mineralization of CaCO<sub>3</sub>. We study two amphiphilic
peptides based on glutamic acid and leucine with β-sheet and
α-helical structures. Though both sequences lead to vaterite
structures, the β-sheets yield free-standing vaterite nanosheet
with superior stability and purity. Surface-spectroscopy and molecular
dynamics simulations reveal that reciprocal structuring of calcium
ions and peptides lead to the effective synthesis of vaterite by mimicry
of the (001) crystal plane
How Gold Nanoparticles Influence Crystallization of Polyethylene in Rigid Cylindrical Nanopores
Even high amounts of gold nanoparticles (AuNPs) only
moderately
influence crystallization of bulk polyethylene (PE). However, under
the rigid two-dimensional confinement of aligned cylindrical nanopores
in anodic aluminum oxide (AAO) the presence of Au turns nucleation-dominated
crystallization of PE at high supercooling into growth-dominated crystallization
at lower supercooling. Transmission electron microscopy investigations
revealed formation of larger Au crystals from AuNPs by Ostwald ripening.
These larger Au crystals apparently acted as heterogeneous nucleation
sites initiating PE crystallization in AAO nanopores. Thus, PE/Au
composites in AAO exhibited significantly higher crystallization and
melting onset temperatures as well as significantly weaker dependence
of crystallization half-times on crystallization temperatures. X-ray
texture analysis revealed for pure PE in AAO the existence of two
copopulations of crystals with different orientations (indicative
of nucleation-dominated crystal growth); PE/Au composites showed uniform
alignment of the fastest growing PE crystal direction with the AAO
nanopore axes (indicative of growth-dominated crystallization). The
prevailing alignment of the [020] direction of orthorhombic PE with
the AAO nanopore axes suggests that properly oriented crystals may
form on pre-existing crystal surfaces by secondary nucleation. These
secondary crystals grow along the AAO nanopores if, under the conditions
of growth-dominated crystallization, competing crystals clogging the
growth path are absent while the confinement of the AAO nanopore walls
stabilizes the (020) growth faces
Surface Oxidation of Stainless Steel: Oxygen Evolution Electrocatalysts with High Catalytic Activity
The
cheap stainless commodity steel AISI 304, which basically consists
of Fe, Ni, and Cr, was surface-oxidized by exposure to Cl<sub>2</sub> gas. This treatment turned AISI 304 steel into an efficient electrocatalyst
for water splitting at pH 7 and pH 13. The overpotential of the anodic
oxygen evolution reaction (OER), which typically limits the efficiency
of the overall water-splitting process, could be reduced to 260 mV
at 1.5 mA/cm<sup>2</sup> in 0.1 M KOH. At pH 7, overpotentials of
500–550 mV at current densities of 0.65 mA/cm<sup>2</sup> were
achieved. These values represent a surprisingly good activity taking
into account the simplicity of the procedure and the fact that the
starting material is virtually omnipresent. Surface-oxidized AISI
304 steel exhibited outstanding long-term stability of its electrocatalytic
properties in the alkaline as well as in the neutral regime, which
did not deteriorate even after chronopoteniometry for 150 000
s. XPS analysis revealed that surface oxidation resulted in the formation
of Fe oxide and Cr oxide surface layers with a thickness in the range
of a few nanometers accompanied by enrichment of Cr in the surface
layer. Depending on the duration of the Cl<sub>2</sub> treatment,
the purity of the Fe oxide/Cr oxide mixture lies between 95% and 98%.
Surface oxidation of AISI 304 steel by chlorination is an easy and
scalable access to nontoxic, cheap, stable, and efficient electrocatalysts
for water splitting
SARS-CoV-2 vaccination modelling for safe surgery to save lives: data from an international prospective cohort study
Background Preoperative SARS-CoV-2 vaccination could support safer elective surgery. Vaccine numbers are limited so this study aimed to inform their prioritization by modelling. Methods The primary outcome was the number needed to vaccinate (NNV) to prevent one COVID-19-related death in 1 year. NNVs were based on postoperative SARS-CoV-2 rates and mortality in an international cohort study (surgical patients), and community SARS-CoV-2 incidence and case fatality data (general population). NNV estimates were stratified by age (18-49, 50-69, 70 or more years) and type of surgery. Best- and worst-case scenarios were used to describe uncertainty. Results NNVs were more favourable in surgical patients than the general population. The most favourable NNVs were in patients aged 70 years or more needing cancer surgery (351; best case 196, worst case 816) or non-cancer surgery (733; best case 407, worst case 1664). Both exceeded the NNV in the general population (1840; best case 1196, worst case 3066). NNVs for surgical patients remained favourable at a range of SARS-CoV-2 incidence rates in sensitivity analysis modelling. Globally, prioritizing preoperative vaccination of patients needing elective surgery ahead of the general population could prevent an additional 58 687 (best case 115 007, worst case 20 177) COVID-19-related deaths in 1 year. Conclusion As global roll out of SARS-CoV-2 vaccination proceeds, patients needing elective surgery should be prioritized ahead of the general population.The aim of this study was to inform vaccination prioritization by modelling the impact of vaccination on elective inpatient surgery. The study found that patients aged at least 70 years needing elective surgery should be prioritized alongside other high-risk groups during early vaccination programmes. Once vaccines are rolled out to younger populations, prioritizing surgical patients is advantageous
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Search for supersymmetry in hadronic final states with missing transverse energy using the variables αT and b-quark multiplicity in pp collisions at √s = 8 TeV
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Previous issue date: 2013-09-01
An inclusive search for supersymmetric processes that produce final states with jets and missing transverse energy is performed in pp collisions at a centre-of-mass energy of 8 TeV. The data sample corresponds to an integrated luminosity of 11.7 fb-1 collected by the CMS experiment at the LHC. In this search, a dimensionless kinematic variable, αT, is used to discriminate between events with genuine and misreconstructed missing transverse energy. The search is based on an examination of the number of reconstructed jets per event, the scalar sum of transverse energies of these jets, and the number of these jets identified as originating from bottom quarks. No significant excess of events over the standard model expectation is found. Exclusion limits are set in the parameter space of simplified models, with a special emphasis on both compressed-spectrum scenarios and direct or gluino-induced production of third-generation squarks. For the case of gluino-mediated squark production, gluino masses up to 950-1125 GeV are excluded depending on the assumed model. For the direct pair-production of squarks, masses up to 450 GeV are excluded for a single light first- or second-generation squark, increasing to 600 GeV for bottom squarks. © 2013 CERN for the benefit of the CMS collaboration.
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Yerevan Physics Institute, Yerevan
Institut für Hochenergiephysik der OeAW, Wien
National Centre for Particle and High Energy Physics, Minsk
Universiteit Antwerpen, Antwerpen
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Centro Brasileiro de Pesquisas Fisicas, Rio de Janeiro
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Universidade Estadual Paulista, São Paulo
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University of Sofia, Sofia
Institute of High Energy Physics, Beijing
State Key Laboratory of Nuclear Physics and Technology Peking University, Beijing
Universidad de Los Andes, Bogota
Technical University of Split, Split
University of Split, Split
Institute Rudjer Boskovic, Zagreb
University of Cyprus, Nicosia
Charles University, Prague
Academy of Scientific Research and Technology of the Arab Republic of Egypt Egyptian Network of High Energy Physics, Cairo
National Institute of Chemical Physics and Biophysics, Tallinn
Department of Physics University of Helsinki, Helsinki
Helsinki Institute of Physics, Helsinki
Lappeenranta University of Technology, Lappeenranta
DSM/IRFU CEA/Saclay, Gif-sur-Yvette
Laboratoire Leprince-Ringuet, Ecole Polytechnique IN2P3-CNRS, Palaiseau
Institut Pluridisciplinaire Hubert Curien, Universite de Strasbourg, Universite de Haute Alsace Mulh CNRS/IN2P3, Strasbourg
CNRS-IN2P3, Institut de Physique Nucléaire de Lyon Université de Lyon, Université Claude Bernard Lyon 1, Villeurbanne
Institute of High Energy Physics and Informatization Tbilisi State University, Tbilisi
I. Physikalisches Institut RWTH Aachen University, Aachen
III. Physikalisches Institut A RWTH Aachen University, Aachen
III. Physikalisches Institut B RWTH Aachen University, Aachen
Deutsches Elektronen-Synchrotron, Hamburg
University of Hamburg, Hamburg
Institut für Experimentelle Kernphysik, Karlsruhe
Institute of Nuclear and Particle Physics (INPP) NCSR Demokritos, Aghia Paraskevi
University of Athens, Athens
University of Ioánnina, Ioánnina
KFKI Research Institute for Particle and Nuclear Physics, Budapest
Institute of Nuclear Research ATOMKI, Debrecen
University of Debrecen, Debrecen
Panjab University, Chandigarh
University of Delhi, Delhi
Saha Institute of Nuclear Physics, Kolkata
Bhabha Atomic Research Centre, Mumbai
Tata Institute of Fundamental Research - EHEP, Mumbai
Tata Institute of Fundamental Research - HECR, Mumbai
Institute for Research in Fundamental Sciences (IPM), Tehran
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Politecnico di Bari, Bari
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Università di Bologna, Bologna
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Università di Catania, Catania
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Università di Firenze, Firenze
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Università di Genova, Genova
INFN Sezione di Milano-Bicocca, Milano
Università di Milano-Bicocca, Milano
INFN Sezione di Napoli, Napoli
Università di Napoli 'Federico II', Napoli
Università della Basilicata (Potenza), Napoli
Università G. Marconi (Roma), Napoli
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Università di Padova, Padova
Università di Trento (Trento), Padova
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Università di Perugia, Perugia
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Università di Pisa, Pisa
Scuola Normale Superiore di Pisa, Pisa
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Università di Roma, Roma
INFN Sezione di Torino, Torino
Università di Torino, Torino
Università del Piemonte Orientale (Novara), Torino
INFN Sezione di Trieste, Trieste
Università di Trieste, Trieste
Kangwon National University, Chunchon
Kyungpook National University, Daegu
Institute for Universe and Elementary Particles Chonnam National University, Kwangju
Korea University, Seoul
University of Seoul, Seoul
Sungkyunkwan University, Suwon
Vilnius University, Vilnius
Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City
Universidad Iberoamericana, Mexico City
Benemerita Universidad Autonoma de Puebla, Puebla
Universidad Autónoma de San Luis Potosí, San Luis Potosí
University of Auckland, Auckland
University of Canterbury, Christchurch
National Centre for Physics Quaid-I-Azam University, Islamabad
National Centre for Nuclear Research, Swierk
Institute of Experimental Physics, Faculty of Physics University of Warsaw, Warsaw
Laboratório de Instrumentação e Física Experimental de Partículas, Lisboa
Joint Institute for Nuclear Research, Dubna
Petersburg Nuclear Physics Institute, Gatchina (St. Petersburg)
Institute for Nuclear Research, Moscow
Institute for Theoretical and Experimental Physics, Moscow
P.N. Lebedev Physical Institute, Moscow
Skobeltsyn Institute of Nuclear Physics Lomonosov Moscow State University, Moscow
State Research Center of Russian Federation Institute for High Energy Physics, Protvino
Faculty of Physics and Vinca Institute of Nuclear Sciences University of Belgrade, Belgrade
Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid
Universidad Autónoma de Madrid, Madrid
Universidad de Oviedo, Oviedo
Instituto de Física de Cantabria (IFCA) CSIC-Universidad de Cantabria, Santander
European Organization for Nuclear Research CERN, Geneva
Paul Scherrer Institut, Villigen
Institute for Particle Physics ETH Zurich, Zurich
Universität Zürich, Zurich
National Central University, Chung-Li
National Taiwan University (NTU), Taipei
Chulalongkorn University, Bangkok
Cukurova University, Adana
Physics Department Middle East Technical University, Ankara
Bogazici University, Istanbul
Istanbul Technical University, Istanbul
National Scientific Center Kharkov Institute of Physics and Technology, Kharkov
University of Bristol, Bristol
Rutherford Appleton Laboratory, Didcot
Imperial College, London
Brunel University, Uxbridge
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Brown University, Providence
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California Institute of Technology, Pasadena
Carnegie Mellon University, Pittsburgh
University of Colorado at Boulder, Boulder
Cornell University, Ithaca
Fairfield University, Fairfield
Fermi National Accelerator Laboratory, Batavia
University of Florida, Gainesville
Florida International University, Miami
Florida State University, Tallahassee
Florida Institute of Technology, Melbourne
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Universidade Estadual Paulista, São Paul