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The production of strange pentaquark states (e.g., Theta baryons and Ξ−− states) in hadronic interactions within a Gribov–Regge approach is explored. In this approach the Θ+(1540) and the Ξ are produced by disintegration of remnants formed by the exchange of pomerons between the two protons. We predict the rapidity and transverse momentum distributions as well as the 4π multiplicity of the Θ+, Ξ−−, Ξ−, Ξ0 and Ξ+ for s=17 GeV (SPS) and 200 GeV (RHIC). For both energies more than 10−3 Θ+ and more than 10−5 Ξ per pp event should be observed by the present experiments.
The production of the ρ(770)0 meson has been measured at mid-rapidity (|y|<0.5) in pp and centrality differential Pb-Pb collisions at sNN−−−√ = 2.76 TeV with the ALICE detector at the Large Hadron Collider. The particles have been reconstructed in the ρ(770)→π+π− decay channel in the transverse momentum (pT) range 0.5−11 GeV/c. A centrality dependent suppression of the ratio of the integrated yields 2ρ(770)0/(π++π−) is observed. The ratio decreases by ∼40% from pp to central Pb-Pb collisions. A study of the pT-differential 2ρ(770)0/(π++π−) ratio reveals that the suppression occurs at low transverse momenta, pT<2 GeV/c. At higher momentum, particle ratios measured in heavy-ion and pp collisions are consistent. The observed suppression is very similar to that previously measured for the K∗(892)0/K ratio and is consistent with EPOS3 predictions that may imply that rescattering in the hadronic phase is a dominant mechanism for the observed suppression.
The production of the ρ(770)0 meson has been measured at mid-rapidity (|y|<0.5) in pp and centrality differential Pb-Pb collisions at sNN−−−√ = 2.76 TeV with the ALICE detector at the Large Hadron Collider. The particles have been reconstructed in the ρ(770)→π+π− decay channel in the transverse momentum (pT) range 0.5−11 GeV/c. A centrality dependent suppression of the ratio of the integrated yields 2ρ(770)0/(π++π−) is observed. The ratio decreases by ∼40% from pp to central Pb-Pb collisions. A study of the pT-differential 2ρ(770)0/(π++π−) ratio reveals that the suppression occurs at low transverse momenta, pT<2 GeV/c. At higher momentum, particle ratios measured in heavy-ion and pp collisions are consistent. The observed suppression is very similar to that previously measured for the K∗(892)0/K ratio and is consistent with EPOS3 predictions that may imply that rescattering in the hadronic phase is a dominant mechanism for the observed suppression.
The production of the ρ(770)0 meson has been measured at mid-rapidity (|y|<0.5) in pp and centrality differential Pb-Pb collisions at sNN−−−√ = 2.76 TeV with the ALICE detector at the Large Hadron Collider. The particles have been reconstructed in the ρ(770)→π+π− decay channel in the transverse momentum (pT) range 0.5−11 GeV/c. A centrality dependent suppression of the ratio of the integrated yields 2ρ(770)0/(π++π−) is observed. The ratio decreases by ∼40% from pp to central Pb-Pb collisions. A study of the pT-differential 2ρ(770)0/(π++π−) ratio reveals that the suppression occurs at low transverse momenta, pT<2 GeV/c. At higher momentum, particle ratios measured in heavy-ion and pp collisions are consistent. The observed suppression is very similar to that previously measured for the K∗(892)0/K ratio and is consistent with EPOS3 predictions that may imply that rescattering in the hadronic phase is a dominant mechanism for the observed suppression.
G protein-coupled receptors (GPCRs) comprise the largest membrane protein family and play an essential role in signal transduction through the cell membrane. They are currently the targets of approximately 50 % of the pharmaceuticals on the market (Klabunde and Hessler, 2002). However, only one high-resolution GPCR structure has been determined up to now, that of bovine rhodopsin (Palczewski et al., 2000). The GPCR activation and regulation mechanisms are still unknown and other GPCR structures are thus required. MePNet (Membrane Protein Network) was a European consortium dedicated to structural studies of GPCRs. The approach was to produce 100 GPCRs in three expression systems (Escherichia coli, Pichia pastoris and Semliki Forest Virus infected mammalian cells) in order to select at each step of the process (production, solubilization, purification) the constructs that fulfilled quantity and quality (functionality) requirements for crystallization trials. In our team, we screened 38 of the 100 targets in P. pastoris. For each receptor, the clone with the highest production level was identified by dot-blot. The size and homogeneity of each receptor were then analyzed by Western-blot. The human adenosine A2A receptor showed a well-defined and pronounced single band and was thus selected for further characterization. The adenosine A2A receptor is a GPCR mainly localized in the central nervous system and, as it antagonizes dopaminergic activity, it has great potential as a drug target for the treatment of Parkinson’s disease. Functional characterization by binding assays with the specific antagonist [3H]-ZM241385 demonstrated a Bmax of 56 +/- 3 pmol/mg i.e. pmol of binder per milligram of total membrane protein, and a KD of 0.40 +/- 0.02 nM. Receptor production was then improved by lowering the induction temperature, decreasing the induction time and adding DMSO to the medium. For large-scale production, fermention reached around 300 g cells (wet weight)/L culture, which provided 43 mg of functional receptor in membranes per liter of culture. Functional solubilization was achieved with dodecyl-β-D-maltoside and the soluble yield was increased to 70-80 % of the membrane content by addition of cholesteryl hemisuccinate and increasing the ionic strength. The receptor was successfully purified via Ni-NTA and monomeric avidin chromatography in the presence of the antagonist ZM241385. This strategy produced a pure, homogeneous and stable receptor preparation with functionality demonstrated by radioligand binding assays. The total receptor yield after purification was routinely around 20 % of the membrane functional receptor content and 2 g of membranes provided 4 mg of pure receptor for crystallization trials. GPCRs are very difficult targets for crystallization, and co-crystallization with antibody fragments has been shown to be a successful method for crystallization of membrane proteins. In order to develop such a tool for the adenosine A2A receptor, a single-chain Fv (scFv) fragment specific to the purified receptor was selected by phage display. The receptor was functionally immobilized on the surface of streptavidin beads and after two rounds of selection, 6 different phages were identified several times. After production in E. coli and purification via Ni-NTA affinity chromatography, 4 out of the 6 scFv fragments were sufficiently enriched to be tested by ELISA. For the ELISA, the receptor was functionally immobilized via the biotinylation domain of the construct in a 96-well streptavidin-coated plate. The antibody fragments binding to the receptor were identified based on interaction with HRP-conjugated protein L. One scFv fragment gave a positive ELISA signal 10 fold above background and titration of the scFv fragment binding to the receptor was specific and saturable. However no complex of scFv fragment and receptor was observed on gel filtration. In order to have a more sensitive detection method, the scFv fragment was labeled with fluorescein: a complex was then observed up on gel filtration but the binding appeared to be non-specific. A pull-down assay with immobilized non-labeled scFv fragment finally confirmed the specificity of the binding, but also the low affinity of the interaction. Affinity maturation of this specific scFv fragment by a random mutagenesis and selection process should improve this parameter in order to obtain an adapted tool for co-crystallization.
The endothelin B receptor belongs to the rhodopsin-like G-protein coupled receptors family. It plays an important role in vasodilatation and is found in the membranes of the endothelial cells enveloping blood vessels. During the course of this work, the production of recombinant human ETB receptor in yeast, insect and mammalian cells was evaluated. A number of different receptor constructs for production in the yeast P. pastoris was prepared. Various affinity tags were appended to the receptor N-and C-termini to enable receptor detection and purification. The clone pPIC9KFlagHisETBBio, with an expression level of 60 pmol/mg, yielded the highest amount of active receptor (1.2 mg of receptor per liter of shaking culture). The expression level of the same clone in fermentor culture was 17 pmol/mg, and from a 10L fermentor it was possible to obtain 3 kg of cells that contained 20-39 mg of the receptor. For receptor production in insect cells, Sf9 (S. frugiperda) suspension cells were infected with the recombinant baculovirus pVlMelFlagHisETBBio. The peak of receptor production was reached at 66 h post infection, and radioligand binding assays on insect cell membranes showed 30 pmoL of active receptor /mg of membrane protein. Subsequently, the efficiency of different detergents in solubilizing the active receptor was evaluated. N-dodecyl-beta-D-maltoside (LM), lauryl-sucrose and digitonine/cholate performed best, and LM was chosen for further work. The ETB receptor was produced in mammalian cells using the Semliki Forest Virus expression system. Radioligand binding assays on membranes from CHO cells infected with the recombinant virus pSFV3CAPETBHis showed 7 pmol of active receptor /mg of membrane protein. Since the receptor yield from mammalian cells was much lower than in yeast and insect cells, this system was not used for further large-scale receptor production. After production in yeast and insect cells, the ETB receptor was saturated with its ligand, endothelin-1, in order to stabilize its native form. The receptor was subsequently solubilized with n-dodecyl-beta-D-maltoside and subjected to purification on various affinity matrices. Two-step affinity purification via Ni2+-NTA and monomeric avidin proved the most efficient way to purify milligram amounts of the receptor. The purity of the receptor preparation after this procedure was over 95%, as judged from silver stained gels. However, the tendency of the ETB receptor produced in yeast to form aggregates was a constant problem. Attempts were made to stabilize the active, monomeric form of the receptor by testing a variety of different buffer conditions, but further efforts in this direction will be necessary in order to solve the aggregation problem. In contrast to preparations from yeast, the purification of the ETB receptor produced in insect cells yielded homogeneous receptor preparations, as shown by gel filtration analysis. This work has demonstrated that the amounts of receptor expressed in yeast and insect cells and the final yield of receptor, isolated by purification, represent a good basis for beginning 3D and continuing 2D crystallization trials.
The production of π±, K±, and (p¯¯¯)p is measured in pp collisions at s√=13 TeV in different topological regions. Particle transverse momentum (pT) spectra are measured in the ``toward'', ``transverse'', and ``away'' angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, RT=NT/⟨NT⟩, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and ⟨NT⟩ is the mean value over all the analysed events. The first measurements of identified particle pT spectra as a function of RT in the three topological regions are reported. The yield of high transverse momentum particles relative to the RT-integrated measurement decreases with increasing RT in both the toward and away regions, indicating that the softer UE dominates particle production as RT increases and validating that RT can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. The pT-differential particle ratios (p+p¯¯¯)/(π++π−) and (K++K−)/(π++π−) in the low UE limit (RT→0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e+e− results.
The production of π±, K±, and (p¯¯¯)p is measured in pp collisions at s√=13 TeV in different topological regions. Particle transverse momentum (pT) spectra are measured in the ``toward'', ``transverse'', and ``away'' angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, RT=NT/⟨NT⟩, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and ⟨NT⟩ is the mean value over all the analysed events. The first measurements of identified particle pT spectra as a function of RT in the three topological regions are reported. The yield of high transverse momentum particles relative to the RT-integrated measurement decreases with increasing RT in both the toward and away regions, indicating that the softer UE dominates particle production as RT increases and validating that RT can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. The pT-differential particle ratios (p+p¯¯¯)/(π++π−) and (K++K−)/(π++π−) in the low UE limit (RT→0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e+e− results.
The production of π±, K±, and (p¯¯¯)p is measured in pp collisions at s√=13 TeV in different topological regions. Particle transverse momentum (pT) spectra are measured in the ``toward'', ``transverse'', and ``away'' angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, RT=NT/⟨NT⟩, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and ⟨NT⟩ is the mean value over all the analysed events. The first measurements of identified particle pT spectra as a function of RT in the three topological regions are reported. The yield of high transverse momentum particles relative to the RT-integrated measurement decreases with increasing RT in both the toward and away regions, indicating that the softer UE dominates particle production as RT increases and validating that RT can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. The pT-differential particle ratios (p+p¯¯¯)/(π++π−) and (K++K−)/(π++π−) in the low UE limit (RT→0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e+e− results.
Production of pions, kaons, (anti-)protons and φ mesons in Xe–Xe collisions at √sNN = 5.44 TeV
(2021)
The first measurement of the production of pions, kaons, (anti-)protons and φ mesons at midrapidity in Xe–Xe collisions at √sNN = 5.44 TeV is presented. Transverse momentum (pT) spectra and pT-integrated yields are extracted in several centrality intervals bridging from p–Pb to mid-central Pb–Pb collisions in terms of final-state multiplicity. The study of Xe–Xe and Pb–Pb collisions allows systems at similar charged-particle multiplicities but with different initial geometrical eccentricities to be investigated. A detailed comparison of the spectral shapes in the two systems reveals an opposite behaviour for radial and elliptic flow. In particular, this study shows that the radial flow does not depend on the colliding system when compared at similar charged-particle multiplicity. In terms of hadron chemistry, the previously observed smooth evolution of particle ratios with multiplicity from small to large collision systems is also found to hold in Xe–Xe. In addition, our results confirm that two remarkable features of particle production at LHC energies are also valid in the collision of medium-sized nuclei: the lower proton-to-pion ratio with respect to the thermal model expectations and the increase of the φ-to-pion ratio with increasing final-state multiplicity.