1,522 research outputs found

    Nicotinamide Riboside Augments Human Macrophage Migration via SIRT3-Mediated Prostaglandin E2 Signaling.

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    (i) NR supplementation protocol (NCT02812238) and (ii) healthy volunteer blood were obtained from the NIH Clinical Center Blood Bank. We thank and acknowledge the assistance of Dan Yan and Natalia Dmitrieva from Manfred Boehm’s group (NHLBI) for the IncuCyte live-cell analysis. We also thank Yun-Wei A. Hsu for her support with the metabolomics analysis at the Northwest Metabolomics Research Center (NIH grant 1S10OD021562-01).Peer reviewe

    N-arachidonylglycine is a caloric state-dependent circulating metabolite which regulates human CD4+T cell responsiveness

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    Acknowledgments We thank Drs. Zoe Hall and Sonia Liggi of the University of Cambridge Biochemistry Department for their contributions to metabolomics analysis and data processing. Shahin Hassanzadeh of the Laboratory of Mitochondrial Biology and Metabolism for developing the PBMC RNAseq library.Matthew Rodman of the Laboratory of Mitochondrial Biology and Metabolism for preparing lean/obese samples. Dr. Duck-Yeon Lee of the NHLBI Biochemistry Core for NAGly analysis in cell culture. Special thanks to the National Institutes of Health Oxford-Cambridge Scholars Program and the International Biomedical Research Alliance for their sponsorship and support. Funding: NHLBI Division of Intramural Research (MNS – ZIA-HL005199) and the UK MRC (JLG – MR/P011705/2; UKDRI-5002; MAPUK).Peer reviewedPublisher PD

    Arachidonic acid inhibition of the NLRP3 inflammasome is a mechanism to explain the anti-inflammatory effects of fasting.

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    For the purpose of open access, the author has applied a Creative Commons Attribution (CC BY) license to any author-accepted manuscript version arising from this submission.Peer reviewe

    Propionate functions as a feeding state-dependent regulatory metabolite to counter proinflammatory signaling linked to nutrient load and obesity.

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    The authors thank Drs. Antonio Murgia and Ben McNally of the University of Cambridge Biochemistry Department for their contributions to metabolomics and lipidomic data processing. They thank and acknowledge the assistance of the National Heart, Lung, and Blood Institute DNA Sequencing and Genomics Core in performing the RNA library sequencing and the National Heart, Lung, and Blood Institute Flow Cytometry Core for performing the flow cytometry.Peer reviewe

    Boosting NAD preferentially blunts Th17 inflammation via arginine biosynthesis and redox control in healthy and psoriasis subjects

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    Acknowledgments We thank Myron Waclawiw of the NHLBI Biostatistics Branch for assistance with the clinical protocol design, Chromadex for supplying NR and matching placebo capsules for the in vivo study and NR powder for the cell culture studies, and an NIH Bench-to-Bedside award for supplemental funding. We additionally thank Dr. Nina Klimova, formerly of the NHLBI, and Dr. Yun-Wei A. Hsu for their support of the metabolomics analysis at the Northwest Metabolomics Research Center of the University of Washington (NIH grant 1S10OD021562-01). We thank and acknowledge the assistance of the NHLBI DNA Sequencing and Genomics Core in performing the RNA library sequencing and Dr. Pradeep Dagur in the NHLBI Flow Cytometry Core for performing the immunophenotyping. Trial registration was as follows: ClinicalTrials.gov: NCT01934660, NCT02812238, and NCT01143454 and NIH Clinical Center blood bank (ClinicalTrials.gov: NCT00001846). This work was supported by the NHLBI Division of Intramural Research (ZIA-HL005102 to M.N.S.), NIH Bench-to-Bedside award (HL-129510-04S1 to M.N.S. and R.T.) and the NIH Office of Dietary Supplements (J.T.), the Spanish Ministry of Science and Innovation (RYC2018-026050-I and PID2019-105665RA-I00 to J.T.), and the UK MRC (MR/P011705/2 and UKDRI-5002 to J.L.G.; MAP UK).Peer reviewedPublisher PD

    Measurement of the quasi-elastic axial vector mass in neutrino-oxygen interactions

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    The weak nucleon axial-vector form factor for quasi-elastic interactions is determined using neutrino interaction data from the K2K Scintillating Fiber detector in the neutrino beam at KEK. More than 12,000 events are analyzed, of which half are charged-current quasi-elastic interactions nu-mu n to mu- p occurring primarily in oxygen nuclei. We use a relativistic Fermi gas model for oxygen and assume the form factor is approximately a dipole with one parameter, the axial vector mass M_A, and fit to the shape of the distribution of the square of the momentum transfer from the nucleon to the nucleus. Our best fit result for M_A = 1.20 \pm 0.12 GeV. Furthermore, this analysis includes updated vector form factors from recent electron scattering experiments and a discussion of the effects of the nucleon momentum on the shape of the fitted distributions.Comment: 14 pages, 10 figures, 6 table

    A Study of Time-Dependent CP-Violating Asymmetries and Flavor Oscillations in Neutral B Decays at the Upsilon(4S)

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    We present a measurement of time-dependent CP-violating asymmetries in neutral B meson decays collected with the BABAR detector at the PEP-II asymmetric-energy B Factory at the Stanford Linear Accelerator Center. The data sample consists of 29.7 fb1{\rm fb}^{-1} recorded at the Υ(4S)\Upsilon(4S) resonance and 3.9 fb1{\rm fb}^{-1} off-resonance. One of the neutral B mesons, which are produced in pairs at the Υ(4S)\Upsilon(4S), is fully reconstructed in the CP decay modes J/ψKS0J/\psi K^0_S, ψ(2S)KS0\psi(2S) K^0_S, χc1KS0\chi_{c1} K^0_S, J/ψK0J/\psi K^{*0} (K0KS0π0K^{*0}\to K^0_S\pi^0) and J/ψKL0J/\psi K^0_L, or in flavor-eigenstate modes involving D()π/ρ/a1D^{(*)}\pi/\rho/a_1 and J/ψK0J/\psi K^{*0} (K0K+πK^{*0}\to K^+\pi^-). The flavor of the other neutral B meson is tagged at the time of its decay, mainly with the charge of identified leptons and kaons. The proper time elapsed between the decays is determined by measuring the distance between the decay vertices. A maximum-likelihood fit to this flavor eigenstate sample finds Δmd=0.516±0.016(stat)±0.010(syst)ps1\Delta m_d = 0.516\pm 0.016 {\rm (stat)} \pm 0.010 {\rm (syst)} {\rm ps}^{-1}. The value of the asymmetry amplitude sin2β\sin2\beta is determined from a simultaneous maximum-likelihood fit to the time-difference distribution of the flavor-eigenstate sample and about 642 tagged B0B^0 decays in the CP-eigenstate modes. We find sin2β=0.59±0.14(stat)±0.05(syst)\sin2\beta=0.59\pm 0.14 {\rm (stat)} \pm 0.05 {\rm (syst)}, demonstrating that CP violation exists in the neutral B meson system. (abridged)Comment: 58 pages, 35 figures, submitted to Physical Review

    Measurement of the Branching Fraction for B- --> D0 K*-

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    We present a measurement of the branching fraction for the decay B- --> D0 K*- using a sample of approximately 86 million BBbar pairs collected by the BaBar detector from e+e- collisions near the Y(4S) resonance. The D0 is detected through its decays to K- pi+, K- pi+ pi0 and K- pi+ pi- pi+, and the K*- through its decay to K0S pi-. We measure the branching fraction to be B.F.(B- --> D0 K*-)= (6.3 +/- 0.7(stat.) +/- 0.5(syst.)) x 10^{-4}.Comment: 7 pages, 1 postscript figure, submitted to Phys. Rev. D (Rapid Communications

    Study of B0(s)→K0Sh+h′− decays with first observation of B0s→K0SK±π∓ and B0s→K0Sπ+π−

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    A search for charmless three-body decays of B 0 and B0s mesons with a K0S meson in the final state is performed using the pp collision data, corresponding to an integrated luminosity of 1.0 fb−1, collected at a centre-of-mass energy of 7 TeV recorded by the LHCb experiment. Branching fractions of the B0(s)→K0Sh+h′− decay modes (h (′) = π, K), relative to the well measured B0→K0Sπ+π− decay, are obtained. First observation of the decay modes B0s→K0SK±π∓ and B0s→K0Sπ+π− and confirmation of the decay B0→K0SK±π∓ are reported. The following relative branching fraction measurements or limits are obtained B(B0→K0SK±π∓)B(B0→K0Sπ+π−)=0.128±0.017(stat.)±0.009(syst.), B(B0→K0SK+K−)B(B0→K0Sπ+π−)=0.385±0.031(stat.)±0.023(syst.), B(B0s→K0Sπ+π−)B(B0→K0Sπ+π−)=0.29±0.06(stat.)±0.03(syst.)±0.02(fs/fd), B(B0s→K0SK±π∓)B(B0→K0Sπ+π−)=1.48±0.12(stat.)±0.08(syst.)±0.12(fs/fd)B(B0s→K0SK+K−)B(B0→K0Sπ+π−)∈[0.004;0.068]at90%CL
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