Hauptseite > Workflowsammlungen > Öffentliche Einträge > Production of K^{+}K^{−} pairs in proton-proton collisions below the ϕ meson threshold > print |
001 | 137994 | ||
005 | 20250129092500.0 | ||
024 | 7 | _ | |a 10.1103/PhysRevC.87.065203 |2 doi |
024 | 7 | _ | |a 1089-490X |2 ISSN |
024 | 7 | _ | |a 0556-2813 |2 ISSN |
024 | 7 | _ | |a arXiv:1302.7210 |c nucl-ex |2 arXiv |
024 | 7 | _ | |a WOS:000320279400002 |2 WOS |
024 | 7 | _ | |a 2128/5397 |2 Handle |
024 | 7 | _ | |a altmetric:1274433 |2 altmetric |
035 | _ | _ | |9 arXiv |a arXiv:1302.7210 |c nucl-ex |
037 | _ | _ | |a FZJ-2013-04279 |
041 | _ | _ | |a English |
082 | _ | _ | |a 530 |
100 | 1 | _ | |a Ye, Q. J. |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
245 | _ | _ | |a Production of K^{+}K^{−} pairs in proton-proton collisions below the ϕ meson threshold |
260 | _ | _ | |a Woodbury, NY |c 2013 |b Inst. |
264 | _ | 1 | |3 online |2 Crossref |b American Physical Society (APS) |c 2013-06-12 |
264 | _ | 1 | |3 print |2 Crossref |b American Physical Society (APS) |c 2013-06-01 |
336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 137994 |2 PUB:(DE-HGF) |
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336 | 7 | _ | |a ARTICLE |2 BibTeX |
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336 | 7 | _ | |a article |2 DRIVER |
500 | _ | _ | |3 POF3_Assignment on 2016-02-29 |
500 | _ | _ | |a *Brief entry* |
500 | _ | _ | |9 arXiv |a 7 pages, 8 figures |
520 | _ | _ | |9 arXiv |a The pp -> ppK+K- reaction was measured below the phi threshold at a beam energy of 2.568 GeV using the COSY-ANKE magnetic spectrometer. By assuming that the four-body phase space is distorted only by the product of two-body final state interactions, fits to a variety of one-dimensional distributions permit the evaluation of differential and total cross sections. The shapes of the distributions in the Kp and Kpp invariant masses are reproduced only if the K-p interaction is even stronger than that found at higher energy. The cusp effect in the K+K- distribution at the K0K0bar threshold is much more clear and some evidence is also found for coupling between the K-p and K0bar n channels. However, the energy dependence of the total cross section cannot be reproduced by considering only a simple product of such pair-wise final state interactions. |
536 | _ | _ | |a 531 - Hadron Structure and Dynamics (HSD) (POF2-531) |0 G:(DE-HGF)POF2-531 |c POF2-531 |f POF II |x 0 |
536 | _ | _ | |a 53G - COSY (POF2-53G32) |0 G:(DE-HGF)POF2-53G32 |c POF2-53G32 |f POF II |x 1 |
542 | _ | _ | |i 2013-06-12 |2 Crossref |u http://link.aps.org/licenses/aps-default-license |
542 | _ | _ | |i 2014-06-12 |2 Crossref |u http://link.aps.org/licenses/aps-default-accepted-manuscript-license |
588 | _ | _ | |a Dataset connected to CrossRef, juser.fz-juelich.de |
650 | _ | 7 | |a channel cross section: energy dependence |2 INSPIRE |
650 | _ | 7 | |a K- p: scattering length |2 INSPIRE |
650 | _ | 7 | |a K: pair production |2 INSPIRE |
650 | _ | 7 | |a threshold |2 INSPIRE |
650 | _ | 7 | |a p p: exclusive reaction |2 INSPIRE |
650 | _ | 7 | |a final-state interaction |2 INSPIRE |
650 | _ | 7 | |a cusp effect |2 INSPIRE |
650 | _ | 7 | |a ANKE |2 INSPIRE |
650 | _ | 7 | |a K+ K-: mass spectrum |2 INSPIRE |
650 | _ | 7 | |a mass spectrum: (2p K-) |2 INSPIRE |
650 | _ | 7 | |a Lambda(1405) |2 INSPIRE |
650 | _ | 7 | |a Juelich COSY PS |2 INSPIRE |
650 | _ | 7 | |a experimental results |2 INSPIRE |
650 | _ | 7 | |a p p --> 2p K+ K- |2 INSPIRE |
650 | _ | 7 | |a 2.568 GeV-kin |2 INSPIRE |
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773 | _ | _ | |a 10.1103/PhysRevC.87.065203 |g Vol. 87, no. 6, p. 065203 |0 PERI:(DE-600)2844098-5 |n 6 |p 065203 |t Physical review / C |v 87 |y 2013 |x 0556-2813 |
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