000453768 001__ 453768
000453768 005__ 20250729151210.0
000453768 0247_ $$2doi$$a10.1103/PhysRevD.102.072005
000453768 0247_ $$2INSPIRETeX$$aAbazov:2020xjb
000453768 0247_ $$2inspire$$ainspire:1808882
000453768 0247_ $$2ISSN$$a0556-2821
000453768 0247_ $$2ISSN$$a1089-4918
000453768 0247_ $$2ISSN$$a1538-4500
000453768 0247_ $$2ISSN$$a1550-2368
000453768 0247_ $$2ISSN$$a1550-7998
000453768 0247_ $$2ISSN$$a2470-0010
000453768 0247_ $$2ISSN$$a2470-0029
000453768 0247_ $$2arXiv$$aarXiv:2007.13420
000453768 0247_ $$2datacite_doi$$a10.3204/PUBDB-2021-00159
000453768 0247_ $$2altmetric$$aaltmetric:86652126
000453768 0247_ $$2WOS$$aWOS:000576892700002
000453768 0247_ $$2openalex$$aopenalex:W3048713416
000453768 037__ $$aPUBDB-2021-00159
000453768 041__ $$aEnglish
000453768 082__ $$a530
000453768 088__ $$2arXiv$$aarXiv:2007.13420
000453768 088__ $$2Fermilab$$aFERMILAB-PUB-20-363-E
000453768 1001_ $$0INSPIRE-00039200$$aAbazov, Victor Mukhamedovich$$b0
000453768 245__ $$aStudies of $X(3872)$ and $\psi(2S)$ production in $p\bar{p}$ collisions at 1.96 TeV
000453768 260__ $$aMelville, NY$$bInst.302363$$c2020
000453768 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2020-10-13
000453768 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2020-10-01
000453768 3367_ $$2DRIVER$$aarticle
000453768 3367_ $$2DataCite$$aOutput Types/Journal article
000453768 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1610464004_8279
000453768 3367_ $$2BibTeX$$aARTICLE
000453768 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000453768 3367_ $$00$$2EndNote$$aJournal Article
000453768 500__ $$aPhys. Rev. D 102, 072005 (2020). 14 pages, 14 figures, 3 tables, accepted by Phys. Rev. D
000453768 520__ $$aWe present various properties of the production of the $X(3872)$ and $ψ(2S)$ states based on $10.4  fb^{−1}$ collected by the D0 experiment in Tevatron $p\bar{p}$ collisions at $\sqrt{s}=1.96  TeV$. For both states, we measure the nonprompt fraction $f_{NP}$ of the inclusive production rate due to decays of $b$-flavored hadrons. We find the $f_{NP}$ values systematically below those obtained at the LHC. The fNP fraction for $ψ(2S)$ increases with transverse momentum, whereas for the $X(3872)$ it is constant within large uncertainties, in agreement with the LHC results. The ratio of prompt to nonprompt $ψ(2S)$ production, $(1−f_{NP})/f_{NP}$, decreases only slightly going from the Tevatron to the LHC, but for the $X(3872)$, this ratio decreases by a factor of about 3. We test the soft-pion signature of the $X(3872)$ modeled as a weakly bound charm-meson pair by studying the production of the $X(3872)$ as a function of the kinetic energy of the $X(3872)$ and the pion in the $X(3872)π$ center-of-mass frame. For a subsample consistent with prompt production, the results are incompatible with a strong enhancement in the production of the $X(3872)$ at the small kinetic energy of the $X(3872)$ and the π in the $X(3872)π$ center-of-mass frame expected for the $X$+soft-pion production mechanism. For events consistent with being due to decays of $b$ hadrons, there is no significant evidence for the soft-pion effect, but its presence at the level expected for the binding energy of 0.17 MeV and the momentum scale $Λ=M(π)$ is not ruled out. 
000453768 536__ $$0G:(DE-HGF)POF3-611$$a611 - Fundamental Particles and Forces (POF3-611)$$cPOF3-611$$fPOF III$$x0
000453768 542__ $$2Crossref$$i2020-10-13$$uhttps://creativecommons.org/licenses/by/4.0/
000453768 588__ $$aDataset connected to CrossRef, INSPIRE
000453768 650_7 $$2INSPIRE$$aanti-p p: scattering
000453768 650_7 $$2INSPIRE$$aanti-p p: colliding beams
000453768 650_7 $$2INSPIRE$$aenergy: kinetic
000453768 650_7 $$2INSPIRE$$aenergy dependence
000453768 650_7 $$2INSPIRE$$aX(3872): hadroproduction
000453768 650_7 $$2INSPIRE$$apsi(3685): hadroproduction
000453768 650_7 $$2INSPIRE$$aBatavia TEVATRON Coll
000453768 650_7 $$2INSPIRE$$aDZERO
000453768 650_7 $$2INSPIRE$$ahadron
000453768 650_7 $$2INSPIRE$$abottom
000453768 650_7 $$2INSPIRE$$ainclusive production
000453768 650_7 $$2INSPIRE$$atransverse momentum dependence
000453768 650_7 $$2INSPIRE$$adirect production
000453768 650_7 $$2INSPIRE$$abinding energy
000453768 650_7 $$2INSPIRE$$aenhancement
000453768 650_7 $$2INSPIRE$$asignature
000453768 650_7 $$2INSPIRE$$aexperimental results
000453768 650_7 $$2INSPIRE$$a1960 GeV-cms
000453768 650_7 $$2autogen$$aParticle Physics Experiments
000453768 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
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