312 research outputs found

    Disparate MgII Absorption Statistics towards Quasars and Gamma-Ray Bursts : A Possible Explanation

    Full text link
    We examine the recent report by Prochter et al. (2006) that gamma-ray burst (GRB) sight lines have a much higher incidence of strong MgII absorption than quasar sight lines. We propose that the discrepancy is due to the different beam sizes of GRBs and quasars, and that the intervening MgII systems are clumpy with the dense part of each cloudlet of a similar size as the quasars, i.e. < 10^16 cm, but bigger than GRBs. We also discuss observational predictions of our proposed model. Most notably, in some cases the intervening MgII absorbers in GRB spectra should be seen varying, and quasars with smaller sizes should show an increased rate of strong MgII absorbers. In fact, our prediction of variable MgII lines in the GRB spectra has been now confirmed by Hao et al. (2007), who observed intervening FeII and MgII lines at z=1.48 to be strongly variable in the multi-epoch spectra of z=4.05 GRB060206.Comment: 12 pages, 2 figures; substantially revised model calculation; accepted for publication in Astrophysics & Space Science as a Lette

    More is the Same; Phase Transitions and Mean Field Theories

    Full text link
    This paper looks at the early theory of phase transitions. It considers a group of related concepts derived from condensed matter and statistical physics. The key technical ideas here go under the names of "singularity", "order parameter", "mean field theory", and "variational method". In a less technical vein, the question here is how can matter, ordinary matter, support a diversity of forms. We see this diversity each time we observe ice in contact with liquid water or see water vapor, "steam", come up from a pot of heated water. Different phases can be qualitatively different in that walking on ice is well within human capacity, but walking on liquid water is proverbially forbidden to ordinary humans. These differences have been apparent to humankind for millennia, but only brought within the domain of scientific understanding since the 1880s. A phase transition is a change from one behavior to another. A first order phase transition involves a discontinuous jump in a some statistical variable of the system. The discontinuous property is called the order parameter. Each phase transitions has its own order parameter that range over a tremendous variety of physical properties. These properties include the density of a liquid gas transition, the magnetization in a ferromagnet, the size of a connected cluster in a percolation transition, and a condensate wave function in a superfluid or superconductor. A continuous transition occurs when that jump approaches zero. This note is about statistical mechanics and the development of mean field theory as a basis for a partial understanding of this phenomenon.Comment: 25 pages, 6 figure

    Investigating the effects of vitreous humour (crude extract) on growth and differentiation of rat mesenchymal stem cells (rMSCs) and human NTERA2 cells

    No full text
    It is very well documented that retinoic acid (RA) reduces growth rate by induction of cell differentiation in certain conditions and cell lines. On the other hand, hyaluronic acid (HA) is known for its growth induction on cultured cells. A natural source of HA, rabbit vitreous humour (VH), was previously shown to promote wound repair in model animals. In search for its possible mechanisms, VH extract was tested on the cultured mesenchymal stem cells and NTERA2 as human embryonal carcinoma cells in the presence of RA. Changes in some cellular and molecular markers (A2B5, Oct4, Sox2) showed that VH and possibly HA interfere with differentiating effects of RA. Therefore, this reagent may affect cell proliferation and tissue regeneration by inhibition of cell differentiation.Đ„ĐŸŃ€ĐŸŃˆĐŸ ОзĐČĐ”ŃŃ‚ĐœĐŸ, Ń‡Ń‚ĐŸ Ń€Đ”Ń‚ĐžĐœĐŸĐ”ĐČая ĐșĐžŃĐ»ĐŸŃ‚Đ° (RA) ŃĐœĐžĐ¶Đ°Đ”Ń‚ Ń‚Đ”ĐŒĐżŃ‹ Ń€ĐŸŃŃ‚Đ°, ĐžĐœĐŽŃƒŃ†ĐžŃ€ŃƒŃ ĐŽĐžŃ„Ń„Đ”Ń€Đ”ĐœŃ†ĐžĐ°Ń†ĐžŃŽ ĐșĐ»Đ”Ń‚ĐŸŃ‡ĐœŃ‹Ń… Đ»ĐžĐœĐžĐč ĐČ ĐŸĐżŃ€Đ”ĐŽĐ”Đ»Đ”ĐœĐœŃ‹Ń… ŃƒŃĐ»ĐŸĐČоях. Đ’ĐŒĐ”ŃŃ‚Đ” с Ń‚Đ”ĐŒ ОзĐČĐ”ŃŃ‚ĐœĐŸ, Ń‡Ń‚ĐŸ ĐłĐžĐ°Đ»ŃƒŃ€ĐŸĐœĐŸĐČая ĐșĐžŃĐ»ĐŸŃ‚Đ° (HA) ĐžĐœĐŽŃƒŃ†ĐžŃ€ŃƒĐ”Ń‚ Ń€ĐŸŃŃ‚ ĐșŃƒĐ»ŃŒŃ‚ĐžĐČĐžŃ€ŃƒĐ”ĐŒŃ‹Ń… ĐșĐ»Đ”Ń‚ĐŸĐș. Đ Đ°ĐœĐ”Đ” Đ±Ń‹Đ»ĐŸ ĐżĐŸĐșĐ°Đ·Đ°ĐœĐŸ, Ń‡Ń‚ĐŸ ДстДстĐČĐ”ĐœĐœŃ‹Đč ĐžŃŃ‚ĐŸŃ‡ĐœĐžĐș НА, стДĐșĐ»ĐŸĐČĐžĐŽĐœĐŸĐ” Ń‚Đ”Đ»ĐŸ (VH) ĐșŃ€ĐŸĐ»ĐžĐșĐ°, ĐČŃ‹Đ·Ń‹ĐČаДт зажОĐČĐ»Đ”ĐœĐžĐ” Ń€Đ°Đœ у ĐŒĐŸĐŽĐ”Đ»ŃŒĐœŃ‹Ń… жОĐČĐŸŃ‚ĐœŃ‹Ń…. В ĐżĐŸĐžŃĐșах ĐČĐŸĐ·ĐŒĐŸĐ¶ĐœĐŸĐłĐŸ ĐŒĐ”Ń…Đ°ĐœĐžĐ·ĐŒĐ° ŃŃ‚ĐŸĐłĐŸ ĐżŃ€ĐŸŃ†Đ”ŃŃĐ° эĐșстраĐșт стДĐșĐ»ĐŸĐČĐžĐŽĐœĐŸĐłĐŸ тДла был ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°Đœ ĐœĐ° ĐșŃƒĐ»ŃŒŃ‚ĐžĐČĐžŃ€ŃƒĐ”ĐŒŃ‹Ń… ĐŒĐ”Đ·Đ”ĐœŃ…ĐžĐŒĐ°Đ»ŃŒĐœŃ‹Ń… стĐČĐŸĐ»ĐŸĐČых ĐșлДтĐșах Đž ĐșлДтĐșах NTERA2 ŃĐŒĐ±Ń€ĐžĐŸĐœĐ°Đ»ŃŒĐœĐŸĐč ĐșĐ°Ń€Ń†ĐžĐœĐŸĐŒŃ‹ Ń‡Đ”Đ»ĐŸĐČĐ”ĐșĐ° ĐČ ĐżŃ€ĐžŃŃƒŃ‚ŃŃ‚ĐČОО RA. Đ˜Đ·ĐŒĐ”ĐœĐ”ĐœĐžŃ ĐœĐ”ĐșĐŸŃ‚ĐŸŃ€Ń‹Ń… ĐșĐ»Đ”Ń‚ĐŸŃ‡ĐœŃ‹Ń… Đž ĐŒĐŸĐ»Đ”ĐșŃƒĐ»ŃŃ€ĐœŃ‹Ń… ĐŒĐ°Ń€ĐșĐ”Ń€ĐŸĐČ (A2B5, Oct4, Sox2) ĐżĐŸĐșазалО, Ń‡Ń‚ĐŸ VH Đž, ĐČĐŸĐ·ĐŒĐŸĐ¶ĐœĐŸ, HA ĐČĐ»ĐžŃŃŽŃ‚ ĐœĐ° ĐŽĐžŃ„Ń„Đ”Ń€Đ”ĐœŃ†ĐžŃ€ŃƒŃŽŃ‰ĐžĐ” ŃŃ„Ń„Đ”Đșты RA. йаĐșĐžĐŒ ĐŸĐ±Ń€Đ°Đ·ĐŸĐŒ, ŃŃ‚ĐŸ ĐČДщДстĐČĐŸ ĐŒĐŸĐ¶Đ”Ń‚ ĐČĐ»ĐžŃŃ‚ŃŒ ĐœĐ° ĐżŃ€ĐŸĐ»ĐžŃ„Đ”Ń€Đ°Ń†ĐžŃŽ ĐșĐ»Đ”Ń‚ĐŸĐș Đž Ń€Đ”ĐłĐ”ĐœĐ”Ń€Đ°Ń†ĐžŃŽ тĐșĐ°ĐœĐ”Đč, ĐžĐœĐłĐžĐ±ĐžŃ€ŃƒŃ ĐŽĐžŃ„Ń„Đ”Ń€Đ”ĐœŃ†ĐžĐ°Ń†ĐžŃŽ ĐșĐ»Đ”Ń‚ĐŸĐș.Đ”ĐŸĐ±Ń€Đ” ĐČŃ–ĐŽĐŸĐŒĐŸ, Ń‰ĐŸ Ń€Đ”Ń‚ĐžĐœĐŸŃ”ĐČĐ° ĐșĐžŃĐ»ĐŸŃ‚Đ° (RA) Đ·ĐœĐžĐ¶ŃƒŃ” Ń‚Đ”ĐŒĐżĐž Ń€ĐŸŃŃ‚Ńƒ, Ń–ĐœĐŽŃƒĐșуючо ĐŽĐžŃ„Đ”Ń€Đ”ĐœŃ†Ń–Đ°Ń†Ń–ŃŽ ĐșлітĐșĐŸĐČох Đ»Ń–ĐœŃ–Đč ĐČ ĐżĐ”ĐČĐœĐžŃ… ŃƒĐŒĐŸĐČах. Đ Đ°Đ·ĐŸĐŒ Đ· Ń‚ĐžĐŒ ĐČŃ–ĐŽĐŸĐŒĐŸ, Ń‰ĐŸ ĐłŃ–Đ°Đ»ŃƒŃ€ĐŸĐœĐŸĐČĐ° ĐșĐžŃĐ»ĐŸŃ‚Đ° (НА) Ń–ĐœĐŽŃƒĐșує ріст ĐșŃƒĐ»ŃŒŃ‚ĐžĐČĐŸ- ĐČĐ°ĐœĐžŃ… ĐșĐ»Ń–Ń‚ĐžĐœ. Đ Đ°ĐœŃ–ŃˆĐ” Đ±ŃƒĐ»ĐŸ ĐżĐŸĐșĐ°Đ·Đ°ĐœĐŸ, Ń‰ĐŸ ĐżŃ€ĐžŃ€ĐŸĐŽĐœĐ” ĐŽĐ¶Đ”Ń€Đ”Đ»ĐŸ НА, сĐșĐ»ĐŸĐżĐŸĐŽŃ–Đ±ĐœĐ” Ń‚Ń–Đ»ĐŸ (VH) ĐșŃ€ĐŸĐ»Ń, ĐČĐžĐșлОĐșає Đ·Đ°ĐłĐŸŃ”ĐœĐœŃ Ń€Đ°Đœ у ĐŒĐŸĐŽĐ”Đ»ŃŒĐœĐžŃ… тĐČĐ°Ń€ĐžĐœ. В ĐżĐŸŃˆŃƒĐșах ĐŒĐŸĐ¶Đ»ĐžĐČĐŸĐłĐŸ ĐŒĐ”Ń…Đ°ĐœŃ–Đ·ĐŒŃƒ Ń†ŃŒĐŸĐłĐŸ ĐżŃ€ĐŸŃ†Đ”ŃŃƒ Đ”ĐșстраĐșт сĐșĐ»ĐŸĐżĐŸĐŽŃ–Đ±ĐœĐŸĐłĐŸ тіла буĐČ ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐžĐč ĐœĐ° ĐșŃƒĐ»ŃŒŃ‚ĐžĐČĐŸĐČĐ°ĐœĐžŃ… ĐŒĐ”Đ·Đ”ĐœŃ…Ń–ĐŒĐ°Đ»ŃŒĐœĐžŃ… ŃŃ‚ĐŸĐČĐ±ŃƒŃ€ĐŸĐČох ĐșĐ»Ń–Ń‚ĐžĐœĐ°Ń… та ĐșĐ»Ń–Ń‚ĐžĐœĐ°Ń… NTERA2 Đ”ĐŒĐ±Ń€Ń–ĐŸĐœĐ°Đ»ŃŒĐœĐŸŃ— ĐșĐ°Ń€Ń†ĐžĐœĐŸĐŒĐž Đ»ŃŽĐŽĐžĐœĐž ĐČ ĐżŃ€ĐžŃŃƒŃ‚ĐœĐŸŃŃ‚Ń– RA. Đ—ĐŒŃ–ĐœĐž ĐŽĐ”ŃĐșох ĐșĐ»Ń–Ń‚ĐžĐœĐœĐžŃ… та ĐŒĐŸĐ»Đ”ĐșŃƒĐ»ŃŃ€ĐœĐžŃ… ĐŒĐ°Ń€ĐșДріĐČ (A2B5, Oct4, Sox2) ĐżĐŸĐșазалО, Ń‰ĐŸ VH і, ĐŒĐŸĐ¶Đ»ĐžĐČĐŸ, НА ĐČплОĐČають ĐœĐ° ĐŽĐžŃ„Đ”Ń€Đ”ĐœŃ†Ń–ŃŽŃŽŃ‡Ń– ДфДĐșто RA. йаĐșĐžĐŒ Ń‡ĐžĐœĐŸĐŒ, ця Ń€Đ”Ń‡ĐŸĐČĐžĐœĐ° ĐŒĐŸĐ¶Đ” ĐČплОĐČато ĐœĐ° ĐżŃ€ĐŸĐ»Ń–Ń„Đ”Ń€Đ°Ń†Ń–ŃŽ і Ń€Đ”ĐłĐ”ĐœĐ”Ń€Đ°Ń†Ń–ŃŽ тĐșĐ°ĐœĐžĐœ, Ń–ĐœĐłŃ–Đ±ŃƒŃŽŃ‡Đž ĐŽĐžŃ„Đ”Ń€Đ”ĐœŃ†Ń–Đ°Ń†Ń–ŃŽ ĐșĐ»Ń–Ń‚ĐžĐœ

    Search for a W' boson decaying to a bottom quark and a top quark in pp collisions at sqrt(s) = 7 TeV

    Get PDF
    Results are presented from a search for a W' boson using a dataset corresponding to 5.0 inverse femtobarns of integrated luminosity collected during 2011 by the CMS experiment at the LHC in pp collisions at sqrt(s)=7 TeV. The W' boson is modeled as a heavy W boson, but different scenarios for the couplings to fermions are considered, involving both left-handed and right-handed chiral projections of the fermions, as well as an arbitrary mixture of the two. The search is performed in the decay channel W' to t b, leading to a final state signature with a single lepton (e, mu), missing transverse energy, and jets, at least one of which is tagged as a b-jet. A W' boson that couples to fermions with the same coupling constant as the W, but to the right-handed rather than left-handed chiral projections, is excluded for masses below 1.85 TeV at the 95% confidence level. For the first time using LHC data, constraints on the W' gauge coupling for a set of left- and right-handed coupling combinations have been placed. These results represent a significant improvement over previously published limits.Comment: Submitted to Physics Letters B. Replaced with version publishe

    Search for the standard model Higgs boson decaying into two photons in pp collisions at sqrt(s)=7 TeV

    Get PDF
    A search for a Higgs boson decaying into two photons is described. The analysis is performed using a dataset recorded by the CMS experiment at the LHC from pp collisions at a centre-of-mass energy of 7 TeV, which corresponds to an integrated luminosity of 4.8 inverse femtobarns. Limits are set on the cross section of the standard model Higgs boson decaying to two photons. The expected exclusion limit at 95% confidence level is between 1.4 and 2.4 times the standard model cross section in the mass range between 110 and 150 GeV. The analysis of the data excludes, at 95% confidence level, the standard model Higgs boson decaying into two photons in the mass range 128 to 132 GeV. The largest excess of events above the expected standard model background is observed for a Higgs boson mass hypothesis of 124 GeV with a local significance of 3.1 sigma. The global significance of observing an excess with a local significance greater than 3.1 sigma anywhere in the search range 110-150 GeV is estimated to be 1.8 sigma. More data are required to ascertain the origin of this excess.Comment: Submitted to Physics Letters

    Measurement of the Lambda(b) cross section and the anti-Lambda(b) to Lambda(b) ratio with Lambda(b) to J/Psi Lambda decays in pp collisions at sqrt(s) = 7 TeV

    Get PDF
    The Lambda(b) differential production cross section and the cross section ratio anti-Lambda(b)/Lambda(b) are measured as functions of transverse momentum pt(Lambda(b)) and rapidity abs(y(Lambda(b))) in pp collisions at sqrt(s) = 7 TeV using data collected by the CMS experiment at the LHC. The measurements are based on Lambda(b) decays reconstructed in the exclusive final state J/Psi Lambda, with the subsequent decays J/Psi to an opposite-sign muon pair and Lambda to proton pion, using a data sample corresponding to an integrated luminosity of 1.9 inverse femtobarns. The product of the cross section times the branching ratio for Lambda(b) to J/Psi Lambda versus pt(Lambda(b)) falls faster than that of b mesons. The measured value of the cross section times the branching ratio for pt(Lambda(b)) > 10 GeV and abs(y(Lambda(b))) < 2.0 is 1.06 +/- 0.06 +/- 0.12 nb, and the integrated cross section ratio for anti-Lambda(b)/Lambda(b) is 1.02 +/- 0.07 +/- 0.09, where the uncertainties are statistical and systematic, respectively.Comment: Submitted to Physics Letters

    Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in pp collisions at sqrt(s) = 7 TeV

    Get PDF
    A search is presented for physics beyond the standard model (BSM) in final states with a pair of opposite-sign isolated leptons accompanied by jets and missing transverse energy. The search uses LHC data recorded at a center-of-mass energy sqrt(s) = 7 TeV with the CMS detector, corresponding to an integrated luminosity of approximately 5 inverse femtobarns. Two complementary search strategies are employed. The first probes models with a specific dilepton production mechanism that leads to a characteristic kinematic edge in the dilepton mass distribution. The second strategy probes models of dilepton production with heavy, colored objects that decay to final states including invisible particles, leading to very large hadronic activity and missing transverse energy. No evidence for an event yield in excess of the standard model expectations is found. Upper limits on the BSM contributions to the signal regions are deduced from the results, which are used to exclude a region of the parameter space of the constrained minimal supersymmetric extension of the standard model. Additional information related to detector efficiencies and response is provided to allow testing specific models of BSM physics not considered in this paper.Comment: Replaced with published version. Added journal reference and DO

    Measurement of isolated photon production in pp and PbPb collisions at sqrt(sNN) = 2.76 TeV

    Get PDF
    Isolated photon production is measured in proton-proton and lead-lead collisions at nucleon-nucleon centre-of-mass energies of 2.76 TeV in the pseudorapidity range |eta|<1.44 and transverse energies ET between 20 and 80 GeV with the CMS detector at the LHC. The measured ET spectra are found to be in good agreement with next-to-leading-order perturbative QCD predictions. The ratio of PbPb to pp isolated photon ET-differential yields, scaled by the number of incoherent nucleon-nucleon collisions, is consistent with unity for all PbPb reaction centralities.Comment: Submitted to Physics Letters

    Current and Future Prospects of Nitro-compounds as Drugs for Trypanosomiasis and Leishmaniasis

    Get PDF
    • 

    corecore