The pp → ppη reaction near the kinematical threshold

Calén, H.; Carius, Staffan; Fransson, K.; Gustafsson, L.; Häggström, S.; Höistad, B.; Johansson, A.; Johansson, T.; Kullander, S.; Moehn, J.; Mörtsell, A.; Ruber, Roger; Schuberth, U.; Złomańczuk, J.; Ekström, C.; Kilian, K.; Oelert, W.; Waters, M.; Bondar, A.; Kuzmin, A.; Shwartz, B.; Sidorov, V.; Kupść, A.; Steṕaniak, J.; Morosov, B.; Povtorejko, A.; Суханов, А.; Zabierowski, J.; Wilhelmi, Z.

doi:10.1016/0370-2693(95)01313-x

Cited by 134 publications

(82 citation statements)

References 11 publications

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“…As an example, in Figure 5 we show this ratio as obtained from the amplitude |M pp→pp | 2 presented as the dotted line in Figure 2. Figure 5a shows an increasing strength of |M 0 | for the η production at low V ps , indicating a strong η-proton FSI, as was discussed previously for the cross section ratio by Calén et al [6]. Note also that the ratio for the η ′ meson is constant over the phase space range considered (Figure 5b).…”

Section: The Curves Insupporting

confidence: 77%

“…PACS: 13.60. Le, 13.85.Lg, 29.20.Dh Typeset using REVT E X 2 New results on η and η ′ meson production in the reaction pp → ppX, measured very recently at the COSY-11 facility [1,2], together with previous data [3,4,5,6,7,8], determine the energy dependence of the near-threshold total cross section with a precision comparable to the measurements of the reaction pp → ppπ 0 [9,10]. These new data encouraged us to perform a phenomenological analysis similar to those of references [11,12,13].…”

Section: Introductionmentioning

confidence: 90%

“…[1,2,3,4,6,7,8,9,10,36]. The proton-proton scattering amplitude was calculated according to equation (4), and the phase shifts were computed using equation (5) (see the solid line in Figure 2).…”

Section: The Curves Inmentioning

confidence: 99%

“…In general, the total cross section is presented as a function of the dimensionless parameter η M [9,10,12] 1 , which is defined as the maximum meson momentum in units of meson mass (η M = q max M ), or as a function of the center-of-mass excess energy Q [3,6,8], where nonrelativistically these variables are related by:…”

Section: Introductionmentioning

confidence: 99%

“…Consideration of the dependence of |M 0 | on phase space allows us to infer the η-proton and η ′ -proton interactions. To avoid large ambiguities due to differences in pp-FSI models, we normalize the |M 0 | for η and η ′ mesons to the one for the π 0 meson and show that the resulting η ′ -proton interaction is comparable to the π 0 -proton one.In general, the total cross section is presented as a function of the dimensionless parameter η M [9,10,12] 1 , which is defined as the maximum meson momentum in units of meson mass (η M = q max M ), or as a function of the center-of-mass excess energy Q [3,6,8], where nonrelativistically these variables are related by:with m p and M denoting the proton and meson mass, respectively. The above equation…”

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confidence: 99%

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S-wave η′-proton FSI; phenomenological analysis of near-threshold production of π0, η, and η′ mesons in proton-proton collisions

et al. 2000

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We describe a novel technique for comparing total cross sections for the reactions pp → ppπ 0 , pp → ppη, and pp → ppη ′ close to threshold. The initial and final state proton-proton interactions are factored out of the total cross section, and the dependence of this reduced cross section on the volume of phase space is discussed. Different models of the proton-proton interaction are compared. We argue that the scattering length of the S-wave η ′ -proton 1 interaction is of the order of 0.1 fm. PACS: 13.60. Le, 13.85.Lg, 29.20.Dh Typeset using REVT E X 2 New results on η and η ′ meson production in the reaction pp → ppX, measured very recently at the COSY-11 facility [1,2], together with previous data [3,4,5,6,7,8], determine the energy dependence of the near-threshold total cross section with a precision comparable to the measurements of the reaction pp → ppπ 0 [9,10]. These new data encouraged us to perform a phenomenological analysis similar to those of references [11,12,13]. Here we concentrate on π 0 , η, and η ′ meson production, and complete the analysis of these references by taking into account the interaction between the incident protons, and by introducing a new representation of the data. The production rates of π 0 , η, and η ′ mesons will be compared as a function of the available phase space. We will study the phase-space dependence of the quantity |M 0 | which is derived from the total cross section with the ISI and pp-FSI factored out. Consideration of the dependence of |M 0 | on phase space allows us to infer the η-proton and η ′ -proton interactions. To avoid large ambiguities due to differences in pp-FSI models, we normalize the |M 0 | for η and η ′ mesons to the one for the π 0 meson and show that the resulting η ′ -proton interaction is comparable to the π 0 -proton one.In general, the total cross section is presented as a function of the dimensionless parameter η M [9,10,12] 1 , which is defined as the maximum meson momentum in units of meson mass (η M = q max M ), or as a function of the center-of-mass excess energy Q [3,6,8], where nonrelativistically these variables are related by:with m p and M denoting the proton and meson mass, respectively. The above equationshows that the proportionality factor between the variables Q and η 2 M changes for different mesons, since the masses of the π 0 , η, and η ′ are distinct. Hence, depending which variable is selected, the relation between the cross section values changes for different mesons. For example, as shown in reference [4] the η meson production-cross-section exceeds the π 0 cross 1 In order to avoid ambiguities with the abbreviation for the eta-meson, we introduce an additional suffix M for this parameter, which usually is called η.3 section by about a factor of five using η M , whereas the π 0 meson cross section is always larger when employing the Q scale.The total cross section for pp → ppX is in general an integral over phase space, weighted by the square of the transition matrix element and normalized to the incoming fl...

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Section: The Curves Insupporting

confidence: 77%

Section: Introductionmentioning

confidence: 90%

Section: The Curves Inmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

mentioning

confidence: 99%

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S-wave η′-proton FSI; phenomenological analysis of near-threshold production of π0, η, and η′ mesons in proton-proton collisions

et al. 2000

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Meson Production Near Threshold

et al. 2000

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Near threshold production of the pseudoscalar mesons at the COSY-11 facility

et al. 2008

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We summarise measurements of the COSY-11 collaboration concerning the excitation functions of the near threshold pseudoscalar meson production in the proton-proton interaction. The results are discussed in the context of the meson-nucleon and hyperon-nucleon interactions. We conclude that the η-proton interaction is significantly stronger than the η ′ -proton interaction. Similarly, we found that the hyperon Λ interacts with the nucleon considerably stronger than the hyperon Σ, and that the interaction of K − -proton is much stronger than this of the K + -proton.

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The pp → ppη reaction near the kinematical threshold

Cited by 134 publications

References 11 publications

S-wave η′-proton FSI; phenomenological analysis of near-threshold production of π0, η, and η′ mesons in proton-proton collisions

S-wave η′-proton FSI; phenomenological analysis of near-threshold production of π0, η, and η′ mesons in proton-proton collisions

Meson Production Near Threshold

Near threshold production of the pseudoscalar mesons at the COSY-11 facility

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