Search results for "chiral [symmetry]"

showing 10 items of 134 documents

Infrared enhanced analytic coupling and chiral symmetry breaking in QCD

2005

We study the impact on chiral symmetry breaking of a recently developed model for the QCD analytic invariant charge. This charge contains no adjustable parameters, other than the QCD mass scale $\Lambda$, and embodies asymptotic freedom and infrared enhancement into a single expression. Its incorporation into the standard form of the quark gap equation gives rise to solutions for the dynamically generated mass that display a singular confining behaviour at the origin. Using the Pagels-Stokar method we relate the obtained solutions to the pion decay constant $f_{\pi}$, and estimate the scale parameter $\Lambda$, in the presence of four active quarks, to be about 880 MeV.

High Energy Physics - TheoryQuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsInfraredHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaInvariant (physics)Asymptotic freedomHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentPion decay constantChiral symmetry breakingScale parameter
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A Domino Ring‐Closure Followed by Retro‐Diels–Alder Reaction for the Preparation of Pyrimido[2,1‐ a ]isoindole Enantiomers

2016

A simple method was developed to prepare pyrimido[2,1-a]isoindole derivatives by using di-endo- and di-exo-ethyl 3-aminobicyclo[2.2.1]hept-5-ene-2-carboxylate enantiomers as chiral sources. The method is based on a domino ring-closure reaction of norbornene 2-aminohydroxamic acid followed by microwave-induced retro-Diels–Alder reaction. In the case of enantiomeric starting substances, the chirality is transferred from norbornene derivatives to pyrimido[2,1-a]isoindoles. The configurations of the synthesized compounds were determined by 1D and 2D NMR spectroscopy [based on 2D NOE cross-peaks and 3JH,H coupling constants] and X-ray crystallography.

Isoindoles010405 organic chemistryStereochemistryChemistrydomino reactionsOrganic Chemistry010402 general chemistryRing (chemistry)Retro-Diels–Alder reaction01 natural sciencesMedicinal chemistryChiral resolutionmicrowave chemistry0104 chemical scienceschemistry.chemical_compoundsynthetic methodschiral resolutionnitrogen heterocyclesPhysical and Theoretical ChemistryEnantiomerIsoindoleChirality (chemistry)ta116NorborneneEuropean Journal of Organic Chemistry
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Direct chromatographic study of the enantioselective biodegradation of ibuprofen and ketoprofen by an activated sludge

2018

[EN] The quantification of the enantiomeric fraction (EF) during the biodegradation process is essential for environmental risk assessment. In this paper the enantioselective biodegradation of ibuprofen, IBU, and ketoprofen, KET, two of the drugs most consumed, was evaluated. Biodegradation experiments were performed in batch mode using a minimal salts medium inoculated with an activated sludge (collected from a Valencian Waste Water Treatment Plant) and supplemented with the racemate of each compound. The inoculum activity was verified using fluoxetine as reference compound. The experimental conditions used (analyte concentration and volume of inoculum) were chosen according to OECD guidel…

KetoprofenAnalyteCalibration curveIbuprofenFraction (chemistry)Wastewater010501 environmental sciences01 natural sciencesBiochemistryAnalytical ChemistryPeak area based estimatesEnantioselective biodegradationmedicineChromatography High Pressure Liquid0105 earth and related environmental sciencesChromatographySewageChemistryBatch experiment010401 analytical chemistryOrganic ChemistryStereoisomerismGeneral MedicineBiodegradationIbuprofenChiral separation0104 chemical sciencesKineticsBiodegradation EnvironmentalActivated sludgeKetoprofenCalibrationEnantiomermedicine.drugJournal of Chromatography A
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Synthesis, photophysical properties and structures of organotin-Schiff bases utilizing aromatic amino acid from the chiral pool and evaluation of the…

2017

Abstract Five new organotin(IV) complexes of compositions [Me 2 SnL 1 ] ( 1 ), [Me 2 SnL 2 ] n ( 2 ), [Me 2 SnL 3 ] ( 3 ), [Ph 3 SnL 1 H] n ( 4 ) and [Ph 3 SnL 3 H] ( 5 ) (where L 1  = (2 S )-2-(( E )-(( Z )-4-hydroxypent-3-en-2-ylidene)amino)-3-(1 H -indol-3-yl)propanoate, L 2  = (2 S )-( E )-2-((2-hydroxybenzylidene)amino)-3-(1 H -indol-3-yl)propanoate and L 3  = (2 S )-( E )-2-((1-(2-hydroxyphenyl)ethylidene)amino)-3-(1 H -indol-3-yl)propanoate were synthesized and spectroscopically characterized. The crystal structures of 1 – 4 were determined. For the dimethyltin derivative 2 , a polymeric chain structure was observed as a result of a long Sn∙∙∙O contact involving the exocyclic carbony…

Models MolecularCell SurvivalStereochemistryAntineoplastic AgentsCrystal structureChiral Schiff baseCrystallography X-Ray010402 general chemistry01 natural sciencesBiochemistryInorganic ChemistryAmino Acids AromaticInhibitory Concentration 50chemistry.chemical_compoundBromideCell Line TumorRiboseOrganotin CompoundsHumansSchiff BasesSpectroscopyX-ray crystallographyCoordination geometrychemistry.chemical_classificationCyclodextrin010405 organic chemistryLigandA375 (human melanoma) cell lineTryptophanStereoisomerismPhotochemical ProcessesOrganotin(IV) compound0104 chemical sciencesMolecular Docking SimulationMonomerchemistrySettore CHIM/03 - Chimica Generale E InorganicaDerivative (chemistry)Journal of Inorganic Biochemistry
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Calix[4]arene-Based Bis[2]catenanes: Synthesis and Chiral Resolution

2007

The exclusive formation of hydrogen-bonded dimers between tetraaryl and tetratosylurea calix[4]arenes has been used to prepare a series of ten "bisloop" tetraurea calix[4]arenes 3, in which adjacent phenylurea groups are covalently linked through alpha,omega-dioxyalkane chains. This dimerization with tetratosylurea 2 as template preorganizes the alkenyl residues of tetra(m-alkenyloxyphenyl) ureas 1 and enables their selective connection in high yield (up to 95 %) by olefin metathesis followed by hydrogenation. The "bisloop" calixarenes 3 also exclusively form heterodimers with 1. Thus, in a separated metathesis/hydrogenation sequence, a series of 14 cyclic bis[2]catenanes 4, in which two ca…

Models MolecularMagnetic Resonance SpectroscopyMolecular StructurebiologyChemistryStereochemistryOrganic ChemistryCatenaneCatenanesStereoisomerismSequence (biology)General ChemistryCrystallography X-Raybiology.organism_classificationMetathesisCatalysisChiral resolutionCrystallographyCovalent bondYield (chemistry)CalixareneTetraCalixarenesChemistry - A European Journal
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Diquark correlations in hadron physics: Origin, impact and evidence

2020

The last decade has seen a marked shift in how the internal structure of hadrons is understood. Modern experimental facilities, new theoretical techniques for the continuum bound-state problem and progress with lattice-regularised QCD have provided strong indications that soft quark+quark (diquark) correlations play a crucial role in hadron physics. For example, theory indicates that the appearance of such correlations is a necessary consequence of dynamical chiral symmetry breaking, viz. a corollary of emergent hadronic mass that is responsible for almost all visible mass in the universe; experiment has uncovered signals for such correlations in the flavour-separation of the proton's elect…

Nuclear TheoryHigh Energy Physics::LatticeHadronNuclear Theoryhiukkasfysiikka01 natural sciencesHigh Energy Physics - ExperimentBroad spectrumHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysicsDiquark correlationsBaryon spectra and structureHigh Energy Physics - Lattice (hep-lat)symmetry breaking: chiralDyson-Schwinger equationsDiquarkbound statediquark: correlationHigh Energy Physics - PhenomenologyQuark modelsChiral symmetry breakingPhenomenology (particle physics)QuarkNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]diquark correlationsNuclear Theory (nucl-th)High Energy Physics - Latticehadron physics0103 physical sciencesquantum chromodynamics010306 general physicsBaryon spectra and structure; Diquark correlations; Dyson-Schwinger equations; Lattice quantum chromodynamics; Quantum chromodynamics; Quark modelskvarkit010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]hadron spectroscopyHigh Energy Physics::PhenomenologyLattice quantum chromodynamicsform factor: electromagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Generalized Polarizabilities and the Chiral Structure of the Nucleon

1997

We are studying the electron scattering process e p to e' p' gamma in order to obtain information on the genuine virtual Compton scattering (VCS) process gamma^* N to gamma N. In addition to the two kinematical variables of real Compton scattering, e.g. the scattering angle theta and the energy omega' of the outgoing photon, the invariant amplitude for VCS depends on a third kinematical variable, which we choose as the absolute value of the three-momentum transfer to the nucleon. The structure-dependent coefficients in the VCS amplitude therefore acquire a momentum dependence and are termed ``generalized polarizabilities'' of the nucleon in analogy to real Compton scattering. Utilizing the …

Nuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryStructure (category theory)General Physics and AstronomyFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)PolarizabilityQuantum mechanics0103 physical sciencesPerturbation theoryNuclear Experiment010306 general physicsPhysicsChiral symmetry010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyCompton scatteringHigh Energy Physics - PhenomenologyNucleonElectron scattering
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Meson Resonances at large Nc: Complex Poles vs Breit-Wigner Masses

2009

The rigorous quantum mechanical definition of a resonance requires determining the pole position in the second Riemann sheet of the analytically continued partial wave scattering amplitude in the complex Mandelstam s variable plane. For meson resonances we investigate the alternative Breit–Wigner (BW) definition within the large NC expansion. By assuming that the pole position is View the MathML source and exploiting unitarity, we show that the BW determination of the resonance mass differs from the pole position by View the MathML source terms, which can be extracted from ππ scattering data. For the case of the σ (f0(600)) pole, the BW scalar mass is predicted to occur at not, vert, simila…

Nuclear and High Energy PhysicsMesonScalar (mathematics)FOS: Physical sciences01 natural sciencesUnitarizationHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsScalar mesonChiral symmetriesScalar mesonPhysicsUnitarity010308 nuclear & particles physicsPlane (geometry)ScatteringLarge N-CResonanceFísicaScattering amplitudeHigh Energy Physics - PhenomenologyResonancesQuantum electrodynamics
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Chiral Symmetry of Baryons

2001

We study chiral symmetry aspects of the positive and negative parity baryons by identifying them with linear representations of the chiral group $SU(N_{f}) \otimes SU(N_{f})$. It is shown that there are two distinctive schemes: naive and mirror assignments. We construct linear sigma models for baryons in the two assignments and examine their physical implications. Then we investigate properties of the naive and mirror nucleons microscopically by using QCD interpolating fields. Finally, we propose experiments to distinguish the two chiral assignments for the nucleon.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryPhysics and Astronomy (miscellaneous)Spontaneous symmetry breakingmedia_common.quotation_subjectHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesAsymmetryGroup representationPionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelNuclear Experimentmedia_commonChiral anomalyQuantum chromodynamicsPhysicsChiral symmetryHigh Energy Physics::PhenomenologySigmaParity (physics)BaryonHigh Energy Physics - PhenomenologyChiral symmetry breakingNucleon
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Three-body hadron systems with strangeness

2013

Recently, many efforts are being put in studying three-hadron systems made of mesons and baryons and interesting results are being found. In this talk, we summarize the main features of the formalism used to study such three hadron systems with strangeness S = -1, 0 within a framework built on the basis of unitary chiral theories and solution of the Faddeev equations. In particular, we present the results obtained for the pi(K) over barN, K (K) over barN and KK (K) over bar systems and their respective coupled channels. In the first case, we find four Sigma's and two A's with spin-parity J(P) = 1/2(+), in the 1500-1800 MeV region, as two meson-one baryon s-wave resonances. In the second cas…

Nuclear and High Energy PhysicsParticle physicsFaddeev equationsMesonNuclear TheoryHadronNuclear TheoryFOS: Physical sciencesStrangenessFew-body systems01 natural sciencesNuclear physicsNuclear Theory (nucl-th)Few-body systemsHadron spectroscopy0103 physical sciences010306 general physicsNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaUnitary chiral theoriesBaryonHigh Energy Physics::Experiment
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