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We report measurements of the inclusive J/ψ yield and average transverse momentum as a function of charged-particle pseudorapidity density dNch/dη in p–Pb collisions at √sNN = 5.02 TeV with ALICE at the LHC. The observables are normalised to their corresponding averages in non-single diffractive events. An increase of the normalised J/ψ yield with normalised dNch/dη, measured at mid-rapidity, is observed at mid-rapidity and backward rapidity. At forward rapidity, a saturation of the relative yield is observed for high charged-particle multiplicities. The normalised average transverse momentum at forward and backward rapidities increases with multiplicity at low multiplicities and saturates beyond moderate multiplicities. In addition, the forward-to-backward nuclear modification factor ratio is also reported, showing an increasing suppression of J/ψ production at forward rapidity with respect to backward rapidity for increasing charged-particle multiplicity.
We present the first ever measurements of femtoscopic correlations between the K0 S and K± particles. The analysis was performed on the data from Pb–Pb collisions at √sNN = 2.76 TeV measured by the ALICE experiment. The observed femtoscopic correlations are consistent with final-state interactions proceeding via the a0(980) resonance. The extracted kaon source radius and correlation strength parameters for K0 SK− are found to be equal within the experimental uncertainties to those for K0 SK+. Comparing the results of the present study with those from published identical-kaon femtoscopic studies by ALICE, mass and coupling parameters for the a0 resonance are tested. Our results are also compatible with the interpretation of the a0 having a tetraquark structure instead of that of a diquark
First results on the longitudinal asymmetry and its effect on the pseudorapidity distributions in Pb–Pb collisions at √sNN = 2.76 TeV at the Large Hadron Collider are obtained with the ALICE detector. The longitudinal asymmetry arises because of an unequal number of participating nucleons from the two colliding nuclei, and is estimated for each event by measuring the energy in the forward neutron-ZeroDegree-Calorimeters (ZNs). The effect of the longitudinal asymmetry is measured on the pseudorapidity distributions of charged particles in the regions |η| < 0.9, 2.8 < η < 5.1 and −3.7 < η < −1.7 by taking the ratio of the pseudorapidity distributions from events corresponding to different regions of asymmetry. The coefficients of a polynomial fit to the ratio characterise the effect of the asymmetry. A Monte Carlo simulation using a Glauber model for the colliding nuclei is tuned to reproduce the spectrum in the ZNs and provides a relation between the measurable longitudinal asymmetry and the shift in the rapidity (y0) of the participant zone formed by the unequal number of participating nucleons. The dependence of the coefficient of the linear term in the polynomial expansion, c1, on the mean value of y0 is investigated.
This letter presents the first measurement of jet mass in Pb–Pb and p–Pb collisions at sNN=2.76 TeV and sNN=5.02 TeV, respectively. Both the jet energy and the jet mass are expected to be sensitive to jet quenching in the hot Quantum Chromodynamics (QCD) matter created in nuclear collisions at collider energies. Jets are reconstructed from charged particles using the anti-kT jet algorithm and resolution parameter R=0.4. The jets are measured in the pseudorapidity range |ηjet|<0.5 and in three intervals of transverse momentum between 60 GeV/c and 120 GeV/c. The measurement of the jet mass in central Pb–Pb collisions is compared to the jet mass as measured in p–Pb reference collisions, to vacuum event generators, and to models including jet quenching. It is observed that the jet mass in central Pb–Pb collisions is consistent within uncertainties with p–Pb reference measurements. Furthermore, the measured jet mass in Pb–Pb collisions is not reproduced by the quenching models considered in this letter and is found to be consistent with PYTHIA expectations within systematic uncertainties.
The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, ε2 and ε3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n > 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range |η| < 0.8 and the transverse momentum range 0.2 < pT < 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the initial conditions, including initial spatial geometry and its fluctuations, as well as the ratio of the shear viscosity to entropy density of the produced system.
Direct photon production at mid-rapidity in Pb–Pb collisions at √sNN=2.76 TeV was studied in the transverse momentum range 0.9<pT<14 GeV/c. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the ALICE detector material with the e+e− pair reconstructed in the central tracking system. The results of the two methods were combined and direct photon spectra were measured for the 0–20%, 20–40%, and 40–80% centrality classes. For all three classes, agreement was found with perturbative QCD calculations for pT≳5 GeV/c. Direct photon spectra down to pT≈1 GeV/c could be extracted for the 20–40% and 0–20% centrality classes. The significance of the direct photon signal for 0.9<pT<2.1 GeV/c is 2.6σ for the 0–20% class. The spectrum in this pT range and centrality class can be described by an exponential with an inverse slope parameter of (297±12stat±41syst) MeV. State-of-the-art models for photon production in heavy-ion collisions agree with the data within uncertainties.
G-protein-coupled receptors (GPCRs) from the largest family of receptors in the human body. They contain seven transmembrane helices. There are roughly 800-900 GPCR genes expressed in humans encoded by 4-5% of the human genome. These receptors are the most important signal transducers and play a crucial role in cell physiology and pathology, by using various extracellular stimuli to start complex intracellular signaling. GPCRs interact with a wide variety of stimuli from small molecules (photons, ions, amines) to large molecules (peptides, small proteins), and trigger downstream cascade effects by interacting with G-proteins, GPCR kinases, and ß-arrestin. Because of their crucial roles in many cellular functions, GPCRs are the most important drug targets for the pharmaceutical industry. Approximately 30% of the clinically approved drugs available in the market are against GPCRs. In this work achieved successful expression and purification of GPCRs from class-C and class-A families. Combined with biochemical experiments, DNP-ssNMR, and molecular simulation helped to decipher the mechanism of crosstalk between the allosteric modulator, and the orthosteric binding sites of the peptide receptor. The main findings and major highlights of this dissertation are outlined in the following paragraphs.
The calcium-sensing receptor (CaSR) belongs to the GPCR class-C family and contains a large extracellular domain. This receptor regulates Ca2+ homeostasis in blood and its absorption in the kidney and bone. To understand the molecular and structural mechanisms of these receptors their cDNAs were cloned into the pPICZ and pOET1 vectors to express them in Pichia pastoris and in Sf9 insect cells respectively. The CaSR was successfully expressed heterologously in Pichia pastoris and in the insect cell with high yield. The purified receptor purified in LMNG shows no aggregation in a monomeric state. Further optimization was performed to use it for cryo-EM sample preparation and structure determination. In 2nd part of the thesis, different mini G (mini Gs, mini Gi, mini Gqs, and mini Gsi) DNA constructs were made and expressed in E. coli. It's challenging to obtain active GPCR structures due to the instability of G-protein or G-protein-bound receptors. In this work, all mini-G proteins and chimera mini-G-protein-maltose binding protein (MBP) were cloned and expressed in E. coli and purified with a His-trap column with high purity.
In the last part of the thesis, to decipher the mechanism of allosteric modulation of orthosteric binding sites in the bradykinin receptor was produced and characterized in insect cells. Angiotensin I converting enzyme inhibitors (ACEIs), are very important drugs and are widely used for the treatment of hypertension, congestive heart failure, and diabetic neuropathy. These drugs target primarily the catalytic zinc center of the ACE. It has been shown that enalaprilat, a well-known ACEI, binds to a proposed zinc-binding site on hB1R and even directly activates the receptor. To obtain information on the influence of ACEIs on the receptor-peptide complex, and to have a better understanding of the molecular mechanism and structural plasticity of the bradykinin receptor and PAM, we used the three commercially available ACEIs captopril, enalaprilat, and lisinopril for our studies. An important result of this thesis is that though enalaprilat, captopril, and lisinopril all have similar functional properties in humans, each one regulates the orthosteric binding site of hB1R in a unique way. These findings provide atomic insights into the allosteric modulation of the bradykinin receptor. This study along with the effects of ACEI on the binding sites of receptors also deciphers the effects of the Zn2+ as well as the crosstalk between zinc binding sites and ACEI compounds. The binding of allosteric modulators induces distinct endogenous binding, which might aid in creating new possibilities in the pharmaceutical field.