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Diluted aqueous solutions of some proteins (bovine serum albumin, β-Lactoglobubin, Peroxidase) show weak phosphorescence lasting over several minutes after they have been irradiated with light in the range 3500-4200 A. Addition of Eosin after the irradiation amplifies in some cases the intensity of luminescence to a value of about hundred. If Eosin is present at the irradiation process the excitation to phosphorescence is possible with light of the wavelength 5460 A.
After denaturation processes which destroy the configuration of proteins (Urea, Guanidine-HCI. detergents, heat at higher pH) the ability of phosphorescence disappears altogether; likewise after blocking the SH-groups by benzochinone or a total oxidation or reduction of the SS-groups which causes an complete unfolding of the peptide chain.
In solutions of bovine serum-albumin irradiated with 3650 Å at room temperature and afterwards frozen to -178°C no radicals could be observed by measurements of electron-spin-resonance but they were detectable if the irradiation took place in the presence of H2O2.
The reactions Xanthinoxidase-Xanthine-O2, Peroxidase-H2O2 and bovine serum-albumin-H2O2-Fe (II) EDTA are accompanied by chemiluminescence. By comparison with the behaviour of oxidised serum-albumin it could be shown that the chemical reaction produces an excited state of the native protein.
The observations lead to the conclusion that the weak phosphorescence of long duration originates from a triplet-state which is sufficiently populated only as the consequence of cooperative phenomena attending the undisturbed α-Helix-structure of the protein.
The ALICE experiment at the LHC has studied J/psi production at mid-rapidity in pp collisions at sqrt{s}=7 TeV through its electron pair decay on a data sample corresponding to an integrated luminosity L_int = 5.6nb-1. The fraction of J/psi from the decay of long-lived beauty hadrons was determined for J/psi candidates with transverse momentum p_t>1.3 GeV/c and rapidity |y|<0.9. The cross section for prompt J/psi mesons, i.e. directly produced J/psi and prompt decays of heavier charmonium states such as the Psi(2S) and Csi_c resonances, is sigma_prompt-J/psi(pt > 1.3 GeV/c, |y| < 0.9) = 8.3 +- 0.8(stat.) +- 1.1(syst.) + 1.5 - 1.4(syst. pol.) micro barn. The cross section for the production of b-hadrons decaying to J/psi with p_t>1.3 GeV/c and |y|<0.9 is sigma_{J/psi<-h_B} = 1.46 +- 0.38(stat.) + 0.26 -0.32(syst.) micro barn. The results are compared to QCD model predictions. The shape of the p_t and y distributions of b-quarks predicted by perturbative QCD model calculations are used to extrapolate the measured cross section to derive the b-bbar pair total cross section and dsigma/dy at mid-rapidity.
Long-range angular correlations on the near and away side in p–Pb collisions at √sNN=5.02 TeV
(2013)
Angular correlations between charged trigger and associated particles are measured by the ALICE detector in p–Pb collisions at a nucleon–nucleon centre-of-mass energy of 5.02 TeV for transverse momentum ranges within 0.5<pT,assoc<pT,trig<4 GeV/c. The correlations are measured over two units of pseudorapidity and full azimuthal angle in different intervals of event multiplicity, and expressed as associated yield per trigger particle. Two long-range ridge-like structures, one on the near side and one on the away side, are observed when the per-trigger yield obtained in low-multiplicity events is subtracted from the one in high-multiplicity events. The excess on the near-side is qualitatively similar to that recently reported by the CMS Collaboration, while the excess on the away-side is reported for the first time. The two-ridge structure projected onto azimuthal angle is quantified with the second and third Fourier coefficients as well as by near-side and away-side yields and widths. The yields on the near side and on the away side are equal within the uncertainties for all studied event multiplicity and pT bins, and the widths show no significant evolution with event multiplicity or pT. These findings suggest that the near-side ridge is accompanied by an essentially identical away-side ridge.