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        OH (1720 MHz) MASERS: A MULTIWAVELENGTH STUDY OF THE INTERACTION BETWEEN THE W51C SUPERNOVA REMNANT AND THE W51B STAR FORMING REGION

        Brogan, C. L.,Goss, W. M.,Hunter, T. R.,Richards, A. M. S.,Chandler, C. J.,Lazendic, J. S.,Koo, B.-C.,Hoffman, I. M.,Claussen, M. J. IOP Publishing 2013 The Astrophysical journal Vol.771 No.2

        <P>We present a comprehensive view of the W51B H II region complex and the W51C supernova remnant (SNR) using new radio observations from the VLA, VLBA, MERLIN, JCMT, and CSO along with archival data from Spitzer, ROSAT, ASCA, and Chandra. Our VLA data include the first lambda = 400 cm (74 MHz) continuum image of W51 at high resolution (88 ''). The 400 cm image shows non-thermal emission surrounding the G49.2-0.3 H II region, and a compact source of non-thermal emission (W51B_NT) coincident with the previously-identified OH (1720 MHz) maser spots, non-thermal 21 and 90 cm emission, and a hard X-ray source. W51B_NT falls within the region of high likelihood for the position of TeV gamma-ray emission. Using the VLBA, three OH (1720 MHz) maser spots are detected in the vicinity of W51B_NT with sizes of 60-300 AU and Zeeman effect magnetic field strengths of 1.5-2.2 mG. The multiwavelength data demonstrate that the northern end of the W51B HII region complex has been partly enveloped by the advancing W51C SNR and this interaction explains the presence of W51B_NT and the OH masers. This interaction also appears in the thermal molecular gas which partially encircles W51B_NT and exhibits narrow pre-shock (Delta v similar to 5 km s(-1)) and broad post-shock (Delta v similar to 20 km s(-1)) velocity components. RADEX radiative transfer modeling of these two components yield physical conditions consistent with the passage of a non-dissociative C-type shock. Confirmation of the W51B/W51C interaction provides additional evidence in favor of this region being one of the best candidates for hadronic particle acceleration known thus far.</P>

      • First observation of the decay B@?<sub>s</sub><sup>0</sup>→D<sup>0</sup>K<sup>@?0</sup> and a measurement of the ratio of branching fractions B(B@?<sub>s</sub><sup>0</sup>→D<sup>0</sup>K<sup>@?0</sup>)B(B@?<sup>0</sup>→D<sup>0</sup>ρ<sup>0</sup>)

        LHCb Collaboration,Aaij, R.,Abellan Beteta, C.,Adeva, B.,Adinolfi, M.,Adrover, C.,Affolder, A.,Ajaltouni, Z.,Albrecht, J.,Alessio, F.,Alexander, M.,Alkhazov, G.,Alvarez Cartelle, P.,Alves, A.A.,Amato, North-Holland Pub. Co 2011 Physics letters: B Vol.706 No.1

        The first observation of the decay B@?<SUB>s</SUB><SUP>0</SUP>→D<SUP>0</SUP>K<SUP>@?0</SUP> using pp data collected by the LHCb detector at a centre-of-mass energy of 7 TeV, corresponding to an integrated luminosity of 36 pb<SUP>-1</SUP>, is reported. A signal of 34.4+/-6.8 events is obtained and the absence of signal is rejected with a statistical significance of more than nine standard deviations. The B@?<SUB>s</SUB><SUP>0</SUP>→D<SUP>0</SUP>K<SUP>@?0</SUP> branching fraction is measured relative to that of B@?<SUP>0</SUP>→D<SUP>0</SUP>ρ<SUP>0</SUP>: B(B@?<SUB>s</SUB><SUP>0</SUP>→D<SUP>0</SUP>K<SUP>@?0</SUP>)B(B@?<SUP>0</SUP>→D<SUP>0</SUP>ρ<SUP>0</SUP>)=1.48+/-0.34+/-0.15+/-0.12, where the first uncertainty is statistical, the second systematic and the third is due to the uncertainty on the ratio of the B<SUP>0</SUP> and B<SUB>s</SUB><SUP>0</SUP> hadronisation fractions.

      • Towards high performance unique microstructures of Co<sub>9</sub>S<sub>8</sub>//CoFe<sub>2</sub>O<sub>4</sub> for asymmetric supercapacitor

        Patil, S.J.,Lokhande, A.C.,Park, J.S.,Kim, J.H.,Kim, Y.B.,Choi, B.C.,Park, S.H.,Jung, S.H.,Lee, D.W. Elsevier 2018 Journal of industrial and engineering chemistry Vol.61 No.-

        <P><B>Abstract</B></P> <P>Herein, we have proposed asymmetric supercapacitor device to achieve empirical electrochemical performance based on binder-free Co<SUB>9</SUB>S<SUB>8</SUB> and CoFe<SUB>2</SUB>O<SUB>4</SUB> electrodes. The unique architecture and porous surface of the prepared electrodes were analyzed using electron microscopy and Brunauer–Emmett–Teller technique. Electrochemical properties of Co<SUB>9</SUB>S<SUB>8</SUB> and CoFe<SUB>2</SUB>O<SUB>4</SUB> electrode were employed in a three-electrode cell-configuration that exhibits a capacitance of 817 and 1203Fg<SUP>−1</SUP>, respectively. Co<SUB>9</SUB>S<SUB>8</SUB>//CoFe<SUB>2</SUB>O<SUB>4</SUB> asymmetric supercapacitor reveals a high capacitance of 79.11Fg<SUP>−1</SUP> with 28.88Whkg<SUP>−1</SUP> energy density and superior cyclic stability over 2500 cycles (∼87%). These results suggest that prepared electrodes have a great potential for practical applications.</P> <P><B>Highlights</B></P> <P> <UL> <LI> Unique-microstructures of C<SUB>o9</SUB>S<SUB>8</SUB> and CoFe<SUB>2</SUB>O<SUB>4</SUB> electrodes were prepared. </LI> <LI> C<SUB>o9</SUB>S<SUB>8</SUB>//CoFe<SUB>2</SUB>O<SUB>4</SUB> supercapacitor exhibits an energy density of 28.88Whkg<SUP>−1</SUP>. </LI> <LI> The assembled Co<SUB>9</SUB>S<SUB>8</SUB>//CoFe<SUB>2</SUB>O<SUB>4</SUB> supercapacitor delivers a superior rate capability. </LI> </UL> </P> <P><B>Graphical abstract</B></P> <P>The Ragone plot shows the electrochemical performance of the Co<SUB>9</SUB>S<SUB>8</SUB>//CoFe<SUB>2</SUB>O<SUB>4</SUB> asymmetric supercapacitor device, and inset shows the BET surface area plot.</P> <P>[DISPLAY OMISSION]</P>

      • Clinical efficacy and safety of abatacept in methotrexate-naive patients with early rheumatoid arthritis and poor prognostic factors

        Westhovens, R,Robles, M,Ximenes, A C,Nayiager, S,Wollenhaupt, J,Durez, P,Gomez-Reino, J,Grassi, W,Haraoui, B,Shergy, W,Park, S-H,Genant, H,Peterfy, C,Becker, J-C,Covucci, A,Helfrick, R,Bathon, J BMJ Group 2009 Annals of the Rheumatic Diseases Vol.68 No.12

        <P><B>Objectives:</B></P><P>To assess the efficacy and safety of abatacept in methotrexate-naive patients with early rheumatoid arthritis (RA) and poor prognostic factors.</P><P><B>Methods:</B></P><P>In this double-blind, phase IIIb study, patients with RA for 2 years or less were randomly assigned 1 : 1 to receive abatacept (∼10 mg/kg) plus methotrexate, or placebo plus methotrexate. Patients were methotrexate-naive and seropositive for rheumatoid factor (RF), anti-cyclic citrullinated protein (CCP) type 2 or both and had radiographic evidence of joint erosions. The co-primary endpoints were the proportion of patients achieving disease activity score in 28 joints (DAS28)-defined remission (C-reactive protein) and joint damage progression (Genant-modified Sharp total score; TS) at year 1. Safety was monitored throughout.</P><P><B>Results:</B></P><P>At baseline, patients had a mean DAS28 of 6.3, a mean TS of 7.1 and mean disease duration of 6.5 months; 96.5% and 89.0% of patients were RF or anti-CCP2 seropositive, respectively. At year 1, a significantly greater proportion of abatacept plus methotrexate-treated patients achieved remission (41.4% vs 23.3%; p<0.001) and there was significantly less radiographic progression (mean change in TS 0.63 vs 1.06; p = 0.040) versus methotrexate alone. Over 1 year, the frequency of adverse events (84.8% vs 83.4%), serious adverse events (7.8% vs 7.9%), serious infections (2.0% vs 2.0%), autoimmune disorders (2.3% vs 2.0%) and malignancies (0.4% vs 0%) was comparable for abatacept plus methotrexate versus methotrexate alone.</P><P><B>Conclusions:</B></P><P>In a methotrexate-naive population with early RA and poor prognostic factors, the combination of abatacept and methotrexate provided significantly better clinical and radiographic efficacy compared with methotrexate alone and had a comparable, favourable safety profile.</P>

      • Quadratic Derivations on non-Archimedean Banach Algebras

        Park, C.,Shagholi, S.,Javadian, A.,Savadkouhi, M.B.,Gordji, M.E. Eudoxus Press LLC 2014 Journal of computational analysis and applications Vol.16 No.3

        Let A be an algebra and X be an A-module. A quadratic mapping D : A X is called a quadratic derivation ifD(ab) = D(a)b(2) + a(2) D(b)for all a(1), a(2) is an element of A. We investigate the Hyers-Ulam stability of quadratic derivations from a non-Archimedean Banach algebra A into a non-Archimedean Banach A-module.

      • Creep and stress relaxation of a FeMnSi-based shape memory alloy at low temperatures

        Leinenbach, C.,Lee, W.J.,Lis, A.,Arabi-Hashemi, A.,Cayron, C.,Weber, B. Elsevier Sequoia 2016 Materials science & engineering. properties, micro Vol.677 No.-

        <P>The creep and stress relaxation behavior of a Fe-17Mn-5Si-10Cr-4Ni-1(V,C) (wt%) shape memory alloy at low homologous temperatures (-45 degrees C < T < 50 degrees C) was systematically studied in stress and strain controlled tensile tests. At constant stresses at -45 degrees C, the alloy exhibits pronounced creep up to 0.6% at 600 MPa after only 30 min holding time. If the strain is kept constant, a pronounced stress relaxation of up to 10% of the initial stress was observed. The final creep strains, the creep rates at a constant stress as well as the stress relaxation at a constant strain increase with decreasing temperature. In addition, the change of the recovery stress as a function of time in a restrained sample after 4% elongation and heating to different constant temperatures was monitored. It was observed that the increase of the final recovery stress is more pronounced when the holding temperature is increased. This behavior was explained with the time and temperature dependent formation of stress induced epsilon-martensite from the parent gamma-austenite phase during mechanical loading according to the model of Kajiwara et al. as well as with the increased number of stacking faults at lower temperatures, which serve as nucleation sites for the epsilon-martensite formation. (C) 2016 Elsevier B.V. All rights reserved.</P>

      • First observation ofγγ→pp¯K+K−and search for exotic baryons inpKsystems

        Shen, C. P.,Yuan, C. Z.,Adachi, I.,Aihara, H.,Asner, D. M.,Aulchenko, V.,Aushev, T.,Ayad, R.,Babu, V.,Badhrees, I.,Bakich, A. M.,Barberio, E.,Behera, P.,Bhardwaj, V.,Bhuyan, B.,Biswal, J.,Bobrov, A.,B American Physical Society 2016 Physical review. D Vol.93 No.11

        <P>The process gamma gamma -> p (p) over barK(+)K(-) and its intermediate processes are measured for the first time using a 980 fb(-1) data sample collected with the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. The production of p (p) over barK(+)K(-) and a Lambda(1520)(0) ((Lambda) over bar (1520)(0)) signal in the pK(-) ((p) over barK(+)) invariant mass spectrum are clearly observed. However, no evidence for an exotic baryon near 1540 MeV/c(2), denoted as Theta(1540)(0) ((Theta) over bar (1540)(0)) or Theta(1540)(++) (Theta(1540)(--)), is seen in the pK(-) ((p) over barK(+)) or pK(+) ((p) over barK(-)) invariant mass spectra. Cross sections for gamma gamma -> p (p) over barK(+)K(-), Lambda(1520)(0)(p) over barK(+) + c.c. and the products sigma(gamma gamma -> Theta(1540)(0)(p) over barK(+) + c.c.)B(Theta(1540)(0) -> pK(-)) and sigma(gamma gamma -> Theta(1540)(++)(p) over barK(-) + c.c.)B(Theta(1540)(++) -> pK(+)) are measured. We also determine upper limits on the products of the chi(c0) and chi(c2) two-photon decay widths and their branching fractions to p (p) over barK(+)K(-) at the 90% credibility level.</P>

      • Electrical properties and deep traps spectra of a-plane GaN films grown on r-plane sapphire

        Polyakov, A.Y.,Smirnov, N.B.,Govorkov, A.V.,Markov, A.V.,Sun, Q.,Zhang, Y.,Yerino, C.D.,Ko, T.S.,Lee, I.H.,Han, J. Elsevier 2010 Materials science & engineering. B, Advanced funct Vol.166 No.3

        Electrical properties, deep traps spectra and luminescence spectra were studied for two undoped a-plane GaN (a-GaN) films grown on r-plane sapphire using metalorganic chemical vapor deposition and differing by structural perfection. For sample A, the a-GaN film was directly deposited on AlN buffer. A two-step growth scheme was implemented for sample B, including an initial islanding growth stage and a subsequent enhanced lateral growth. Preliminary detailed X-ray analysis showed that the stacking faults density was 8x10<SUP>5</SUP>cm<SUP>-1</SUP> for sample A and 1.7x10<SUP>5</SUP>cm<SUP>-1</SUP> for sample B. Electrical properties of a-GaN films were largely determined by deep traps with a level near E<SUB>c</SUB> -0.6eV, with other prominent traps having the activation energy of 0.25eV. The Fermi level was pinned by the E<SUB>c</SUB> -0.6eV deep traps for sample A, but shifted to the vicinity of the shallower 0.25eV traps for sample B, most likely due to the reduced density of the 0.6eV traps. This decrease of deep traps density is accompanied by a very pronounced improvement in the overall luminescence intensity. A correlation of the observed improvement in deep traps spectra and luminescence efficiency with the improved crystalline quality of the films is discussed.

      • SCISCIESCOPUS

        Gut-Specific Delivery of T-Helper 17 Cells Reduces Obesity and Insulin Resistance in Mice

        Hong, C.P.,Park, A.,Yang, B.G.,Yun, C.H.,Kwak, M.J.,Lee, G.W.,Kim, J.H.,Jang, M.S.,Lee, E.J.,Jeun, E.J.,You, G.,Kim, K.S.,Choi, Y.,Park, J.H.,Hwang, D.,Im, S.H.,Kim, J.F.,Kim, Y.K.,Seoh, J.Y.,Surh, C. Elsevier North Holland [etc.] 2017 Gastroenterology Vol.152 No.8

        <P>BACKGROUND & AIMS: Obesity and metabolic syndrome have been associated with alterations to the intestinal microbiota. However, few studies examined the effects of obesity on the intestinal immune system. We investigated changes in subsets of intestinal CD4(+) T-helper (T-H) cells with obesity and the effects of gut-tropic T(H)17 cells in mice on a high-fat diet (HFD). METHODS: We isolated immune cells from small intestine and adipose tissue of C57BL/6 mice fed a normal chow diet or a HFD for 10 weeks and analyzed the cells by flow cytometry. Mice fed a vitamin A-deficient HFD were compared with mice fed a vitamin A-sufficient HFD. Obese RAG1-deficient mice were given injections of only regulatory T cells or a combination of regulatory T cells and T(H)17 cells (wild type or deficient in integrin beta 7 subunit or interleukin 17 [IL17]). Mice were examined for weight gain, fat mass, fatty liver, glucose tolerance, and insulin resistance. Fecal samples were collected before and after T cell transfer and analyzed for microbiota composition by metagenomic DNA sequencing and quantitative polymerase chain reaction. RESULTS: Mice placed on a HFD became obese, which affected the distribution of small intestinal CD4(+) T-H cells. Intestinal tissues from obese mice had significant reductions in the proportion of T(H)17 cells but increased proportion of T(H)1 cells, compared with intestinal tissues from nonobese mice. Depletion of vitamin A in obese mice further reduced the proportion of T(H)17 cells in small intestine; this reduction correlated with more weight gain and worsening of glucose intolerance and insulin resistance. Adoptive transfer of in vitro-differentiated gut-tropic T(H)17 cells to obese mice reduced these metabolic defects, which required the integrin beta 7 subunit and IL17. Delivery of T(H)17 cells to intestines of mice led to expansion of commensal microbes associated with leanness. CONCLUSIONS: In mice, intestinal T(H)17 cells contribute to development of a microbiota that maintains metabolic homeostasis, via IL17. Gut-homing T(H)17 cells might be used to reduce metabolic disorders in obese individuals.</P>

      • SCISCIE

        V994 Herculis: the multiple system with a quadruple-lined spectrum and a double eclipsing feature

        Lee, C.-U.,Kim, S.-L.,Lee, J. W.,Kim, C.-H.,Jeon, Y.-B.,Kim, H.-I.,Yoon, J.-N.,Humphrey, A. Blackwell Publishing Ltd 2008 MONTHLY NOTICES- ROYAL ASTRONOMICAL SOCIETY Vol.389 No.4

        <P>ABSTRACT</P><P>We report the discovery of a multiple system with a quadruple-lined spectrum and a double eclipsing feature. Our photometric and high-resolution spectroscopic data show that V994 Herculis (V994 Her; ADS 11373 AB) is composed of two pairs of double-lined eclipsing binaries, which we designate as A and B. System A consists of a B8V+A0V binary with an orbital period of 2.083 264 d and system B of a A2V+A4V binary with 1.420 033 d. Our light curves show that both of them have a detached binary configuration. We derive masses and radii of four components (Aa, Ab, Ba and Bb) from the synthetic analyses of light curves and radial velocity curves. The masses of systems A and B are <I>M</I><SUB>Aa</SUB>= 2.83 ± 0.20 M<SUB>⊙</SUB>, <I>M</I><SUB>Ab</SUB>= 2.30 ± 0.16 M<SUB>⊙</SUB>, <I>M</I><SUB>Ba</SUB>= 1.87 ± 0.12 M<SUB>⊙</SUB> and <I>M</I><SUB>Bb</SUB>= 1.86 ± 0.12 M<SUB>⊙</SUB>, with radii <I>R</I><SUB>Aa</SUB>= 2.15 ± 0.05 R<SUB>⊙</SUB>, <I>R</I><SUB>Ab</SUB>= 1.71 ± 0.04 R<SUB>⊙</SUB>, <I>R</I><SUB>Ba</SUB>= 1.59 ± 0.08 R<SUB>⊙</SUB> and <I>R</I><SUB>Bb</SUB>= 1.50 ± 0.08 R<SUB>⊙</SUB>, respectively. These masses and radii are well consistent with the empirical relation for double-lined eclipsing binaries.</P>

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