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Journal articles on the topic 'Kaon form factor'

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Published: 10 December 2022
Last updated: 28 January 2023

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1

Zhi-gang, Wang, Wan Shao-long, and Wang Ke-lin. "Calculation of kaon electromagnetic form factor." Chinese Physics 10, no. 6 (June 2001): 497–500. http://dx.doi.org/10.1088/1009-1963/10/6/307.

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2

BEILIN, V. A., V. A. NESTERENKO, and A. V. RADYUSHKIN. "KAON FORM FACTOR FOR SMALL Q2." International Journal of Modern Physics A 03, no. 05 (May 1988): 1183–97. http://dx.doi.org/10.1142/s0217751x88000515.

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We calculate the electromagnetic charge radii of K± and K0 mesons using the QCD sum rule approach. The results agree with existing experimental data. The relation to the vector meson dominance model is briefly discussed.
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3

Baker, O. K. "The space-like kaon electromagnetic form factor." Nuclear Physics A 623, no. 1-2 (September 1997): 351–56. http://dx.doi.org/10.1016/s0375-9474(97)00454-5.

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4

Shaolong, Wan, Wang Kelin, Wang Yi, and Chen Qinghu. "Calculation of the Electromagnetic Form Factor of the Kaon." Communications in Theoretical Physics 29, no. 4 (June 15, 1998): 605–8. http://dx.doi.org/10.1088/0253-6102/29/4/605.

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5

BEILIN, V. A., V. A. NESTERENKO, and A. V. RADYUSHKIN. "KAON ELECTROMAGNETIC RADIUS." Modern Physics Letters A 03, no. 08 (July 1988): 767–72. http://dx.doi.org/10.1142/s0217732388000921.

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We obtain a QCD sum rule for the kaon form factor at small Q2. It determines, with a rather good accuracy, the kaon charge radius which is in agreement with the experimental value. We also discuss a sum rule for the difference [Formula: see text].
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6

Xiao, Bo-Wen, Xin Qian, and Bo-Qiang Ma. "The kaon form factor in the light-cone quark model." European Physical Journal A 15, no. 4 (December 2002): 523–27. http://dx.doi.org/10.1140/epja/i2002-10059-y.

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7

Pearce, B. C., K. Holinde, and J. Speth. "The scalar form factor of the pion, kaon and nucleon." Nuclear Physics A 541, no. 4 (May 1992): 663–74. http://dx.doi.org/10.1016/0375-9474(92)90226-a.

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8

Syukurilla, L., and T. Mart. "A combination of hadronic form factors for modeling the kaon photoproduction process γp → K+Λ." International Journal of Modern Physics E 24, no. 02 (February 2015): 1550008. http://dx.doi.org/10.1142/s0218301315500081.

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We have phenomenologically investigated the kaon photoproduction process γp → K+Λ by combining different types of hadronic form factors (HFFs) inside a covariant isobar model. We obtained the best model with the smallest χ2/N by using the dipole form factor in the Born terms and a combination of the dipole, Gaussian, as well as generalized dipole form factors in the hadronic vertices of the nucleon, kaon and hyperon resonances. By utilizing this model we found that the experimental data used in the analysis are internally consistent, whereas the behavior of differential cross-section at forward angles is not significantly affected by the variation of hadronic coupling constants (CCs) and form factor cutoffs in the model.
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9

AGAEV, SHAHIN S. "THE KAON ELECTROMAGNETIC FORM FACTOR AND EFFECTS OF RUNNING COUPLING CONSTANT." Modern Physics Letters A 11, no. 12 (April 20, 1996): 957–63. http://dx.doi.org/10.1142/s0217732396000977.

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The Borel transform and resummed expression for the kaon electromagnetic form factor Fk(Q2) are obtained in the context of QCD running coupling αs(Q2(1 − x)(1 − y)) approach. It is demonstrated that the effects of running coupling (ir renormalons) can be taken into account by scale-setting procedure αs(Q2)→αs(ef (Q2)Q2) in the leading order expression.
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10

Dias, O. A. T., V. S. Filho, and J. P. B. C. de Melo. "Kaon and Pion Electromagnetic Form Factor Ratios in the Light-Front." Nuclear Physics B - Proceedings Supplements 199, no. 1 (February 2010): 281–84. http://dx.doi.org/10.1016/j.nuclphysbps.2010.02.044.

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11

MART, T., and A. K. SARI. "HADRONIC FORM FACTORS IN THE γp→K+Λ PROCESS." Modern Physics Letters A 28, no. 14 (May 10, 2013): 1350054. http://dx.doi.org/10.1142/s0217732313500545.

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We have investigated the effects of different hadronic form factors on the performance of an isobaric model developed for kaon photo-production off the proton. We found that there is no ideal form factor in this case. The dipole and generalized dipole form factors can help to nicely reproduce the differential cross-section and hyperon polarization data. However, in the case of double polarization data Cx and Cz the Gaussian form factor is found to be superior.
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12

D’Ambrosio, Giancarlo. "Kaon decays at KLOE-2." EPJ Web of Conferences 166 (2018): 00010. http://dx.doi.org/10.1051/epjconf/201816600010.

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I review kaon decays. I introduce the flavor problem and possible solutions. Very rare kaon decays like [see formula in PDF] are very important to this purpose: we study also [see formula in PDF] where chiral dynamics is important to disentangle short distance effects. We have also studied lepton flavor (universality) violation in rare kaon decays and the Bardeen Buras Gerard approach to describe the [see formula in PDF] form factor.
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13

Wu, Xing-Gang, and Tao Huang. "Kaon electromagnetic form factor within thekTfactorization formalism and it's light-cone wave function." Journal of High Energy Physics 2008, no. 04 (April 14, 2008): 043. http://dx.doi.org/10.1088/1126-6708/2008/04/043.

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14

Carrasco, N., P. Lami, V. Lubicz, E. Picca, L. Riggio, S. Simula, and C. Tarantino. "Kaon semileptonic vector form factor with Nf=2+1+1 Twisted Mass fermions." Nuclear and Particle Physics Proceedings 273-275 (April 2016): 2602–4. http://dx.doi.org/10.1016/j.nuclphysbps.2015.10.003.

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15

Krivoruchenko, M. I. "Isovector kaon form factor in the dispersion theory and S-wave ? K-scattering lengths." Zeitschrift f�r Physik A Hadrons and Nuclei 350, no. 4 (December 1995): 343–47. http://dx.doi.org/10.1007/bf01291191.

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16

RAGGI, MAURO. "TESTS OF CHPT WITH ${\rm K}_{{\rm e}4}^{+-}$ AND ${\rm K}_{{\rm e}4}^{00}$ DECAYS AT THE NA48/2 EXPERIMENT AT CERN." International Journal of Modern Physics: Conference Series 35 (January 2014): 1460458. http://dx.doi.org/10.1142/s201019451460458x.

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The NA48/2 experiment has collected the largest samples to date of semi-leptonic charged kaon decays in the [Formula: see text] (K± → π+π-e±ν) and [Formula: see text] (K± → π0π0e±ν) modes. From 1.1 million [Formula: see text] decays, form factors in the S- and P-wave have been extensively studied. Branching ratio and form factors have been measured at unprecedented precision. From ~ 66000 [Formula: see text] decays, preliminary values of the Branching ratio and form factor have been obtained at a percent level precision. The comparison of Branching ratio and form factor values in both Ke4 modes sheds new light on isospin symmetry breaking effects. Form factor measurements are major inputs to the study of low energy QCD and are powerful tests of Chiral Perturbation Theory predictions.
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17

Koponen, Jonna, André Zimermmane-Santos, Christine Davies, G. Peter Lepage, and Andrew Lytle. "Light meson form factors at high Q2 from lattice QCD." EPJ Web of Conferences 175 (2018): 06015. http://dx.doi.org/10.1051/epjconf/201817506015.

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Measurements and theoretical calculations of meson form factors are essential for our understanding of internal hadron structure and QCD, the dynamics that bind the quarks in hadrons. The pion electromagnetic form factor has been measured at small space-like momentum transfer |q2| < 0.3 GeV2 by pion scattering from atomic electrons and at values up to 2.5 GeV2 by scattering electrons from the pion cloud around a proton. On the other hand, in the limit of very large (or infinite) Q2 = −q2, perturbation theory is applicable. This leaves a gap in the intermediate Q2 where the form factors are not known. As a part of their 12 GeV upgrade Jefferson Lab will measure pion and kaon form factors in this intermediate region, up to Q2 of 6 GeV2. This is then an ideal opportunity for lattice QCD to make an accurate prediction ahead of the experimental results. Lattice QCD provides a from-first-principles approach to calculate form factors, and the challenge here is to control the statistical and systematic uncertainties as errors grow when going to higher Q2 values. Here we report on a calculation that tests the method using an ηs meson, a ’heavy pion’ made of strange quarks, and also present preliminary results for kaon and pion form factors. We use the nf = 2 + 1 + 1 ensembles made by the MILC collaboration and Highly Improved Staggered Quarks, which allows us to obtain high statistics. The HISQ action is also designed to have small dicretisation errors. Using several light quark masses and lattice spacings allows us to control the chiral and continuum extrapolation and keep systematic errors in check.
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18

Zhi-Gang, Wang, Wan Shao-Long, and Wang Ke-Lin. "Calculation of Kaon Electromagnetic Form Factor in the Framework of Coupled Schwinger–Dyson and Bethe–Salpeter Formulation." Communications in Theoretical Physics 35, no. 6 (June 15, 2001): 697–702. http://dx.doi.org/10.1088/0253-6102/35/6/697.

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19

Seth, Kamal K., S. Dobbs, A. Tomaradze, T. Xiao, and G. Bonvicini. "First measurement of the electromagnetic form factor of the neutral kaon at a large momentum transfer and the effect of SU(3) breaking." Physics Letters B 730 (March 2014): 332–35. http://dx.doi.org/10.1016/j.physletb.2014.02.003.

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20

Nam, Seung-il. "Quasi-distribution amplitudes for pion and kaon via the nonlocal chiral-quark model." Modern Physics Letters A 32, no. 39 (December 21, 2017): 1750218. http://dx.doi.org/10.1142/s0217732317502182.

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We investigate the pseudoscalar (PS) meson ([Formula: see text] and [Formula: see text]) quasi-distribution amplitude (QDA), which is supposed to be an asymptotic analog to the meson distribution amplitude (DA) [Formula: see text] in the limit of the large longitudinal PS-meson momentum, i.e. [Formula: see text], in the non-perturbative (NP) region. For this purpose, we employ the nonlocal chiral-quark model (NLChQM) in the light-front (LF) formalism with a minimal Fock-state for the mesons [Formula: see text][Formula: see text][Formula: see text] at the low-energy scale parameter of the model [Formula: see text][Formula: see text][Formula: see text][Formula: see text]1 GeV. As a trial, we extract the transverse-momentum distribution amplitude (TMDA) from the light-front wave function (LFWF) within the model, and convert it to QDA with help of the virtuality-distribution amplitude (VDA). By doing that, we derive an analytical expression for the NP QDA with the current-quark mass correction up to [Formula: see text]. Numerically, we confirm that the obtained TMDA reproduces the experimental data for the photon-pion transition form factor [Formula: see text] at the low-[Formula: see text] qualitatively well. We also observe that the obtained QDA approaches to DA as [Formula: see text] increases, showing the symmetric and asymmetric curves with respect to [Formula: see text] for the pion and kaon, respectively, due to the current-quark mass difference [Formula: see text]. Assigning [Formula: see text], the moments [Formula: see text] are computed, using the pion and kaon QDAs, and there appear only a few percent deviations in the moments for [Formula: see text] in comparison to the values calculated directly from DAs. It turns out that the higher moments are more sensitive to the change of [Formula: see text], whereas the lower ones depend less on it.
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21

Bijnens, Johan, and Pere Talavera. "Pion and kaon electromagnetic form factors." Journal of High Energy Physics 2002, no. 03 (March 20, 2002): 046. http://dx.doi.org/10.1088/1126-6708/2002/03/046.

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22

GAO, JUN, and Bing An Li. "FORM FACTORS OF PION AND KAON." International Journal of Modern Physics A 16, supp01a (October 2001): 175–77. http://dx.doi.org/10.1142/s0217751x01006413.

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The form factors of pion and kaon are studied by an effective chiral theory of large NC QCD. Besides the vector meson poles an additional intrinsic form factors are found. Theory agrees well with data in both time-like and space-like regions. There is no adjustable parameter.
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23

Mart, T., and C. Bennhold. "Kaon and hyperon form factors in kaon electroproduction on the nucleon." Nuclear Physics A 639, no. 1-2 (August 1998): 237c—246c. http://dx.doi.org/10.1016/s0375-9474(98)00279-6.

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24

Afanasev, Andrei, and W. W. Buck. "Unified description of kaon electroweak form factors." Physical Review D 55, no. 7 (April 1, 1997): 4380–84. http://dx.doi.org/10.1103/physrevd.55.4380.

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25

Dubnicka, S., and A. Z. Dubnickov$aacute$. "Strange vector form factor of kaons." Journal of Physics G: Nuclear and Particle Physics 28, no. 8 (June 21, 2002): 2137–49. http://dx.doi.org/10.1088/0954-3899/28/8/301.

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26

LEŚNIAK, L., A. FURMAN, R. KAMIŃSKI, and P. ŻENCZYKOWSKI. "ANALYSIS OF B± → K+K-K± DECAYS." International Journal of Modern Physics A 26, no. 03n04 (February 10, 2011): 542–44. http://dx.doi.org/10.1142/s0217751x11051974.

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Rare B± decays to three charged kaons are analysed. The weak decay amplitudes are derived in the QCD factorization approach. The strong final state interactions between pairs of kaons are described using the kaon scalar and vector form factors. The scalar form factors at low K+K- effective mass distributions are constrained by chiral symmetry and are related to the coupled channel meson-meson amplitudes describing all the transitions between three channels consisting of two kaons, two pions and four pions. The vector form factors are fitted to the data on e+e- collisions. The model results are compared with the Belle and BaBar data.
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27

Nam, Seung-il, and Hyun-Chul Kim. "Generalized form factors and spin structures of the kaon." Physics Letters B 707, no. 5 (February 2012): 546–52. http://dx.doi.org/10.1016/j.physletb.2012.01.016.

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28

Jin, Dan, and Ya-Dong Yang. "Space- and time-like kaon electromagnetic form factors in perturbative QCD." Chinese Physics C 36, no. 10 (October 2012): 941–46. http://dx.doi.org/10.1088/1674-1137/36/10/004.

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29

Bijnens, J., and A. Khodjamirian. "Exploring light-cone sum rules for pion and kaon form factors." European Physical Journal C 26, no. 1 (November 2002): 67–79. http://dx.doi.org/10.1140/epjc/s2002-01042-1.

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30

Bruch, C., A. Khodjamirian, and J. H. Kühn. "Modeling the pion and kaon form factors in the timelike region." European Physical Journal C 39, no. 1 (January 2005): 41–54. http://dx.doi.org/10.1140/epjc/s2004-02064-3.

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31

Beloborodov, Konstantin, Vladimir Druzhinin, and Sergey Serednyakov. "Isoscalar and isovector kaon form factors from e+e− and τ data." EPJ Web of Conferences 212 (2019): 03006. http://dx.doi.org/10.1051/epjconf/201921203006.

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The recent precise measurements of the e+e−→ KS KL and e+e−→ K+K− cross sections and the hadronic spectral function of the τ−→ K−KS ντ decay are used to extract the isoscalar and isovector electromagnetic kaon form factors and their relative phase in a model independent way. The experimental results are compared with a fit based on the vector-meson-dominance model.
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32

Beloborodov, K. I., V. P. Druzhinin, and S. I. Serednyakov. "Isoscalar and Isovector Kaon Form Factors from e+e– and τ Data." Journal of Experimental and Theoretical Physics 129, no. 3 (September 2019): 386–90. http://dx.doi.org/10.1134/s1063776119080016.

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33

Meng, Zhaoxia. "Hadron Form Factors at BESIII." International Journal of Modern Physics: Conference Series 46 (January 2018): 1860027. http://dx.doi.org/10.1142/s2010194518600273.

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Form factors of hadron provide fundamental information about its structure and dynamics. They constitute a rigorous test of non-perturbative QCD as well as of phenomenological models. Based on data samples collected with BESIII detector at BEPCII collider, born cross section of [Formula: see text] and proton effective form factors are measured at 12 center-of-mass energies between 2.2324 and 3.671 GeV. The ratio [Formula: see text]s are extracted by fitting polar angle distribution of proton for data samples with large statistics. For data between 3.773 and 4.6 GeV, we use initial state radiation (ISR) method to study [Formula: see text] by tagged or un-tagged ISR photon, where the pair cross section, effective form factors and [Formula: see text]s are obtained from proton pair threshold to about 3 GeV. For [Formula: see text] and [Formula: see text], the pair cross section and [Formula: see text] form factors are measured near threshold. With data scanned in 2015 from 2-3.08 GeV, charged Kaon pair cross section and form factors are measured at 21 center-of-mass energies.
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34

Lamanna, G. "Charged Kaons semi-leptonic form factors from NA48/2." Journal of Physics: Conference Series 1526 (April 2020): 012005. http://dx.doi.org/10.1088/1742-6596/1526/1/012005.

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35

KIM, HYUN-CHUL, SEUNG-IL NAM, and HYUN-AH CHOI. "PION AND KAON STRUCTURES FROM THE INSTANTON VACUUM." Modern Physics Letters A 24, no. 11n13 (April 30, 2009): 887–90. http://dx.doi.org/10.1142/s0217732309000231.

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In this presentation, we briefly review recent investigations on pion and kaon structures from the instanton vacuum. Starting from the low-energy QCD partition function, we have computed the Gasser-Leutwyler low-energy constants, electromagnetic form factors of the pion and kaon, and semileptonic decay form factors of the kaon. The results are in good agreement with the experimental and empirical data.
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36

Serednyakov, S. I., K. I. Beloborodov, and V. P. Druzhinin. "Study of the kaon electromagnetic form factors in e + e − annihilation and τ decays." Journal of Physics: Conference Series 1526 (April 2020): 012038. http://dx.doi.org/10.1088/1742-6596/1526/1/012038.

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37

Chang Shin, Yun, Bong Soo Han, Myung Ki Cheoun, K. S. Kim, and Il-Tong Cheon. "Pion and kaon electromagnetic form factors in a SUL(3) ⊗ SUR(3) effective Lagrangian." European Physical Journal A 9, no. 2 (November 2000): 269–76. http://dx.doi.org/10.1007/s100500070044.

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38

Raya, K., Z. F. Cui, L. Chang, J. M. Morgado, C. D. Roberts, and J. Rodríguez-Quintero. "Revealing pion and kaon structure via generalised parton distributions *." Chinese Physics C 46, no. 1 (January 1, 2022): 013105. http://dx.doi.org/10.1088/1674-1137/ac3071.

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Abstract Clear windows onto emergent hadron mass (EHM) and modulations thereof by Higgs boson interactions are provided by observable measures of pion and kaon structure, many of which are accessible via generalised parton distributions (GPDs). Beginning with algebraic GPD Ansätze, constrained entirely by hadron-scale and K valence-parton distribution functions (DFs), in whose forms both EHM and Higgs boson influences are manifest, numerous illustrations are provided. They include the properties of electromagnetic form factors, impact parameter space GPDs, gravitational form factors and associated pressure profiles, and the character and consequences of all-orders evolution. The analyses predict that mass-squared gravitational form factors are stiffer than electromagnetic form factors; reveal that K pressure profiles are tighter than profiles, with both mesons sustaining near-core pressures at magnitudes similar to that expected at the core of neutron stars; deliver parameter-free predictions for and K valence, glue, and sea GPDs at the resolving scale GeV; and predict that at this scale the fraction of meson mass-squared carried by glue and sea combined matches that lodged with the valence degrees-of-freedom, with a similar statement holding for mass-squared radii.
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39

Pejatović, Aleksandra, and Tamara Kunić. "Obrazovanje odraslih kao faktor ostvarivanja koncepta fleksigurnosti." Obrazovanje odraslih/Adult Education 12, no. 2 2012 (2012): 9–26. http://dx.doi.org/10.53617/issn2744-2047.2012.12.2.9.

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The term, more frequently occurring in the last few years in the European documents dealing with different aspects and possible development trends of employment policy primarly aimed at reducing the growing unemployment rate, is ''flexicurity''. The essence of this concept, which is becoming more and more current with the world economic crisis, is the employees, in order to maintain this status, have to express, meaning that they have to be trained for flexibility reflected in readiness for, and thus largely for the possibility for frequent job changes and changes of institutions and organisations in which they work, as well as for continuous knowledge acqusition and development of skills and competences. In addition, the flexicurity concept also emphasises the necessity of providing security, through the role of the state in the form of providing sufficient job position, enabling the emloyment of a larger number of people under good conditions and providing strong support in case of unployment. The subject of this paper is studying the role of adult education in implementing the flexicurity concept. As a manifestation of lifelong learning, adult education has a key role in acquiring knowledge, skills and competences, which is why it has long become a strong factor of economic development, increase of competitiveness, employability and employment. In line with the aforementioned subject, the aim of this paper is to, by analysis of the relevant literature and European documents devoted in different ways and in varying degrees to the flexicurity concept, explore the role of adult education in implementing this concept.
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40

Alkofer, R., S. Ahlig, C. Fischer, and M. Oettel. "Kaon photoproduction and form factors in a covariant and confining diquark–quark model for baryons." Nuclear Physics A 680, no. 1-4 (January 2001): 70–75. http://dx.doi.org/10.1016/s0375-9474(00)00391-2.

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41

Ahlig, S., R. Alkofer, C. Fischer, M. Oettel, and H. Reinhardt. "Kaon photoproduction and form factors in a covariant and confining diquark-quark model for baryons." Progress in Particle and Nuclear Physics 44 (March 2000): 361–62. http://dx.doi.org/10.1016/s0146-6410(00)00083-1.

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42

Bramon, A. "Electromagnetic form-factors of pions and kaons in the time-like region." Nuclear Physics A 623, no. 1-2 (September 1997): 357–60. http://dx.doi.org/10.1016/s0375-9474(97)00455-7.

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43

AGAEV, SHAHIN S. "THE RUNNING COUPLING METHOD WITH NEXT-TO-LEADING ORDER ACCURACY AND PION, KAON ELM FORM FACTORS." Modern Physics Letters A 13, no. 33 (October 30, 1998): 2637–43. http://dx.doi.org/10.1142/s0217732398002801.

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The pion and kaon electromagnetic form factors FM(Q2) are calculated at the leading order of pQCD using the running coupling constant method. In calculations, the leading and next-to-leading order terms in αS((1-x)(1-y)Q2) expansion in terms of αS(Q2) are taken into account. The resummed expression for FM(Q2) is found. Results of numerical calculations for the pion (asymptotic distribution amplitude) are presented.
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44

Czyż, Henryk, and Agnieszka Grzelińska. "PHOKHARA 7.0 Monte Carlo generator: the narrow resonances implementation and new pion and kaon form factors." Nuclear Physics B - Proceedings Supplements 218, no. 1 (September 2011): 201–6. http://dx.doi.org/10.1016/j.nuclphysbps.2011.06.032.

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45

Shim, Sang-In, Atsushi Hosaka, and Hyun-Chul Kim. "Vector and Axial-vector form factors in radiative kaon decay and flavor SU(3) symmetry breaking." Physics Letters B 795 (August 2019): 438–45. http://dx.doi.org/10.1016/j.physletb.2019.06.046.

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46

Glomazić, Hajdana. "Karakteristike odraslih kao faktori procene obrazovne funkcije televizije." Obrazovanje odraslih/Adult Education 14, no. 1 (2014): 45–64. http://dx.doi.org/10.53617/issn2744-2047.2014.14.1.45.

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This paper proceeds from the assumption that educational features and television-media experience of adults determine their view regarding the educational function of the television. The study wants to get an answer to the question whether there is, to what degree and what is the connection between certain characteristics of respondents and their relation to the educational function of the television. The results showed that the level of education is a factor in the assessment of educational functions of television, and a positive attitude towards the educational value of television content increases with higher levels of education. It has been shown that the level of formal education is a determinant of evaluating the most appropriate form of presentation of educational content. Also, the results suggest the conclusion that the television-media status of spectators is a significant factor of the educational function of television assessment.
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47

Seth, Kamal K. "First Measurements of Form Factors of Pion, Kaon, Proton, and Hyperons for the Highest Timelike Momentum Transfers." Journal of Physics: Conference Series 556 (November 26, 2014): 012009. http://dx.doi.org/10.1088/1742-6596/556/1/012009.

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48

Rudy, T. E., H. W. Fearing, and S. Scherer. "Off-shell electromagnetic form factors of pions and kaons in chiral perturbation theory." Physical Review C 50, no. 1 (July 1, 1994): 447–59. http://dx.doi.org/10.1103/physrevc.50.447.

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49

Druzhinin, V. P. "Measurement of the proton and kaon time-like electromagnetic form factors at high energy with the BaBar detector." Nuclear and Particle Physics Proceedings 273-275 (April 2016): 2770–72. http://dx.doi.org/10.1016/j.nuclphysbps.2015.10.059.

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50

Ivashyn, S. A., and A. Y. Korchin. "Electromagnetic form factors of charged and neutral kaons in an extended vector-meson-dominance model." European Physical Journal C 49, no. 3 (December 6, 2006): 697–708. http://dx.doi.org/10.1140/epjc/s10052-006-0167-5.

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