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We present a study of the inclusive charged-particle transverse momentum (pT) spectra as a function of charged-particle multiplicity density at mid-pseudorapidity, dNch/dη, in pp collisions at s√ = 5.02 and 13 TeV covering the kinematic range |η|<0.8 and 0.15<pT<20 GeV/c. The results are presented for events with at least one charged particle in |η|<1 (INEL>0). The pT spectra are reported for two multiplicity estimators covering different pseudorapidity regions. The pT spectra normalized to that for INEL >0 show little energy dependence. Moreover, the high-pT yields of charged particles increase faster than the charged-particle multiplicity density. The average pT as a function of multiplicity and transverse spherocity is reported for pp collisions at s√=13 TeV. For low- (high-) spherocity events, corresponding to jet-like (isotropic) events, the average pT is higher (smaller) than that measured in INEL >0 pp collisions. Within uncertainties, the functional form of ⟨pT⟩(Nch) is not affected by the spherocity selection. While EPOS LHC gives a good description of many features of data, PYTHIA overestimates the average pT in jet-like events.
Pion-kaon femtoscopy and the lifetime of the hadronic phase in Pb-Pb collisions at √sNN = 2.76 TeV
(2021)
In this paper, the first femtoscopic analysis of pion–kaon correlations at the LHC is reported. The analysis was performed on the Pb–Pb collision data at √sNN = 2.76 TeV recorded with the ALICE detector. The non-identical particle correlations probe the spatio-temporal separation between sources of different particle species as well as the average source size of the emitting system. The sizes of the pion and kaon sources increase with centrality, and pions are emitted closer to the centre of the system and/or later than kaons. This is naturally expected in a system with strong radial flow and is qualitatively reproduced by hydrodynamic models. ALICE data on pion–kaon emission asymmetry are consistent with (3+1)-dimensional viscous hydrodynamics coupled to a statistical hadronisation model, resonance propagation, and decay code THERMINATOR 2 calculation, with an additional time delay between 1 and 2 fm/c for kaons. The delay can be interpreted as evidence for a significant hadronic rescattering phase in heavy-ion collisions at the LHC.
We report on the measurement of the size of the particle-emitting source from two-baryon correlations with ALICE in high-multiplicity pp collisions at √s = 13 TeV. The source radius is studied with low relative momentum p–p, p–p, p–, and p– pairs as a function of the pair transverse mass mT considering for the first time in a quantitative way the effect of strong resonance decays. After correcting for this effect, the radii extracted for pairs of different particle species agree. This indicates that protons, antiprotons, s, and s originate from the same source. Within the measured mT range (1.1–2.2) GeV/c2 the invariant radius of this common source varies between 1.3 and 0.85 fm. These results provide a precise reference for studies of the strong hadron–hadron interactions and for the investigation of collective properties in small colliding systems.
Multiplicity dependence of inclusive J/ψ production at midrapidity in pp collisions at √s = 13 TeV
(2020)
Measurements of the inclusive J/ψ yield as a function of charged-particle pseudorapidity density dNch/dη in pp collisions at √s = 13 TeV with ALICE at the LHC are reported. The J/ψ meson yield is measured at midrapidity (|y| < 0.9) in the dielectron channel, for events selected based on the charged-particle multiplicity at midrapidity (|η| < 1) and at forward rapidity (−3.7 < η < −1.7 and 2.8 < η < 5.1); both observables are normalized to their corresponding averages in minimum bias events. The increase of the normalized J/ψ yield with normalized dNch/dη is significantly stronger than linear and dependent on the transverse momentum. The data are compared to theoretical predictions, which describe the observed trends well, albeit not always quantitatively.
The polarization of Λ and Λ¯ hyperons along the beam direction has been measured relative to the second and third harmonic event planes in isobar Ru+Ru and Zr+Zr collisions at √sNN = 200 GeV. This is the first experimental evidence of the hyperon polarization by the triangular flow originating from the initial density fluctuations. The amplitudes of the sine modulation for the second and third harmonic results are comparable in magnitude, increase from central to peripheral collisions, and show a mild pT dependence. The azimuthal angle dependence of the polarization follows the vorticity pattern expected due to elliptic and triangular anisotropic flow, and qualitatively disagree with most hydrodynamic model calculations based on thermal vorticity and shear induced contributions. The model results based on one of existing implementations of the shear contribution lead to a correct azimuthal angle dependence, but predict centrality and pT dependence that still disagree with experimental measurements. Thus, our results provide stringent constraints on the thermal vorticity and shear-induced contributions to hyperon polarization. Comparison to previous measurements at RHIC and the LHC for the second-order harmonic results shows little dependence on the collision system size and collision energy.
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.
G protein-coupled receptors (GPCRs) constitute an important class of integral membrane proteins that are involved in several signaling pathways. About 50% of the currently available drugs are targeted against these receptors and high-resolution structures of these receptors will be of immense importance from the perspective of designing specific and potent drugs. However, structure determination of these receptors and of membrane proteins in general, has been a very challenging task till date. A major limitation in the structure determination of these proteins is that they are present in minute amounts in the native tissues and therefore, they must be produced heterologously. Additionally, crystallization of GPCRs is difficult owing to their flexible nature and limited hydrophilic surface area available for crystal contacts. The aim of my Ph.D. thesis work is two fold, first, to address the problem of GPCR crystallization by using a fusion protein complex approach and second, to tailor Rhodobacter sphaeroides as an expression system for the heterologous production of GPCRs. In the first approach, R. sphaeroides was used as an expression system to generate a fusion protein complex of the photosynthetic reaction center (RC) with a GPCR, expecting that such a complex would be easier to crystallize than the receptor alone. The notion behind this approach is that the RC will act as a scaffold in providing surface area to create crystal contacts and at the same time, it will also reduce the flexibility of the receptor, hopefully without perturbing the functionality of the receptor. Based on the computational modelling experiments, two ways to generate a fusion complex were assigned. Long linkers were inserted between the subunits of the RC and the GPCR. The linkers were designed with a possibility of straightforward alteration of their length as they contained a number of restriction enzyme sites. A series of these constructs were designed and expressed in R. sphaeroides deletion strain, which did not possess the chromosomal RC genes. Though most of these fusion constructs could be successfully expressed, as analyzed by western blot, majority of them were not functional in terms of ligand binding of the GPCR component of the fusion complex. Interestingly, one of these constructs, where the M subunit of RC was directly fused to the human angiotensin II type 1a receptor (AT1aR), exhibited significant functional expression. Based on saturation binding analysis using [125I] iodotyrosyl4Sar1Ile8-angiotensin II (an AT1aR subtype specific antagonist), an expression level of 40+5 pmol/mg of total membrane protein was calculated. This expression level corresponds to approximately 0.3 mg of functional receptor per liter culture and it is significantly higher than the AT1aR expression in native tissues. Additionally, the binding affinity of the recombinant receptor for its endogenous ligand angiotensin II was found to be 1±0.1 nM, which is similar to that observed for the AT1aR in native tissues. More interestingly, the RC part of the fusion complex was structurally assembled in other words, properly folded as judged by the presence of the characteristic peaks at 760 nm, 800 nm and 850 nm by absorption spectroscopy. However, a slight change in the intensity of the peak at 800 nm was observed while comparing the spectra of native RC with that in the fusion protein complex. This slight variation might be due to the change in the protein environment. The fusion protein complex RC-AT1aR was functionally solubilized and purified using a decahistidine tag fused at the c-terminus of the AT1aR. Subsequently, the monodispersity and integrity of the complex was confirmed by size exclusion chromatography, which revealed a homogeneous peak. Additionally, it was also possible to solubilize and purify this complex in the presence of a fluorescein tagged angiotensin II ligand which provides a nice tool to judge the functionality of the AT1aR and integrity of the complex at the same time. The purified RC-AT1aR fusion complex was then subjected to three-dimensional (3-D) crystallization trials and it was possible to obtain reproducible crystals of this complex. The crystals were fluorescent (as the complex was purified in presence of fluorescently labelled angiotensin II) and needle or tetragonal in shape, but produced a powdery diffraction pattern. Further attempts to improve the crystallization condition and to optimize the cryo-conditions are underway. In addition, attempts are also being made to obtain the crystals of this complex with the antagonist (e.g. losartan) bound to the receptor. In view of several limitations in the heterologous expression of GPCRs, as the second part of my Ph.D. thesis, I decided to explore the possibilities of developing a novel expression system based on R. sphaeroides for production of recombinant GPCRs. The notion behind using this host is that lack of inclusion bodies and high concentration of membranes in R. sphaeroides would result in efficient functional overexpression of recombinant membrane proteins. For this purpose, a R. sphaeroides strain, modified by the deletion of the genes encoding the RC and the light harvesting proteins LH1 and LH2, was used. The genes for RC and LHs constitute about 85-90% of total membrane proteins in a R. sphaeroides cell. These membranes are normally housed in special membrane vesicles called intracytoplasmic membranes (ICMs) that can fill almost the entire cell volume under certain growth conditions. Synthesis of a heterologous protein under the control of the moderately strong photosynthetic superoperonic promoter should be coordinated with the synthesis of new membranes to harbour these proteins, thus acting as a natural induction system. Moreover, as most of the native membrane proteins are absent in this deletion strain, heterologously produced protein should not experience a shortage of molecular chaperones for proper folding and insertion. Additionally, the absence of inclusion bodies in this host should enhance the functional and homogenous population of the recombinant proteins. Three human GPCRs, namely the adenosine A2a receptor (A2a), the angiotensin II type 1a receptor (AT1aR) and the bradykinin subtype 2 receptor (B2R) were tested for expression and functionality in this system. Two different constructs were used to determine the optimal position and ribosome-binding site (RBS) in the superoperon for the highest expression level. Of these three receptors, the AT1aR and B2R were successfully produced, while the A2aR failed to express, producing green carotenoid free R. sphaeroides mutants, for unknown reasons. For the recombinant B2R, [3H] bradykinin binding analysis revealed a low functional expression level of 0.7-0.8 pmol/mg of total membrane protein. This expression level corresponds to 0.01 mg functional receptor per liter of culture and is not sufficient for large-scale expression of this receptor. However, for the recombinant AT1aR, [125I] iodotyrosyl4Sar1Ile8- angiotensin II binding analysis revealed an expression level of 12±1 pmol/mg of total membrane protein. This expression level corresponds to approximately 0.1 mg functional receptor per liter culture and this is significantly higher than the AT1aR expression in native tissues. This expression system is still in the nascent stages of development and there are several parameters, which are still to be assessed for the optimal use of this system for the production of GPCRs and other membrane proteins. In conclusion, my Ph.D. work presents a novel fusion protein complex based approach for obtaining crystallizable GPCRs and a novel expression system for producing heterologous GPCRs. It was possible, for the first time, to produce a functional RC-GPCR complex that could easily be crystallized, though further finetuning of the system is required. R. sphaeroides based novel expression system was successfully used to produce functional human GPCRs under the control of a moderately strong photosynthetic superoperonic promoter. This expression system represents a naturally induced system where the expression of a heterologous protein is coordinated with the synthesis of new membranes to harbour the recombinant protein. The fusion protein complex approach and the expression system presented here can hopefully be used as a general method to facilitate the expression and crystallization of other membrane proteins.