1998
DOI: 10.1103/physrevlett.81.5287
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Calculation of theHΣ4eBound State in theH

Abstract: We examine phenomenologically the 4 He͑in-flight K 2 , p 2 ͒ spectrum at p K 2 600 MeV͞c and u Kp 4 ± within distorted-wave impulse approximation calculations by using a coupled ͑3N-L͒ 1 ͑3N-S͒ model. The result shows that there exists a pole of the 4 S He unstable bound state on the second Riemann sheet of the complex energy plane, and its complex eigenvalue is E ͑pole͒ S 1

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Cited by 61 publications
(73 citation statements)
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“…In a previous work [23], we examined these spectra of the 3 He(in-flight K − , n) reactions within a distorted-wave impulse approximation (DWIA) employing the Green's function method [24] which well describes unstable hadron systems [25]. It has been shown that the 3 He(in-flight K − , n) reaction provides a promising spectrum which contains a s-wave dominance in the K − bound region, where a strong nuclear distortion for K − is reduced [23].…”
Section: Introductionmentioning
confidence: 99%
“…In a previous work [23], we examined these spectra of the 3 He(in-flight K − , n) reactions within a distorted-wave impulse approximation (DWIA) employing the Green's function method [24] which well describes unstable hadron systems [25]. It has been shown that the 3 He(in-flight K − , n) reaction provides a promising spectrum which contains a s-wave dominance in the K − bound region, where a strong nuclear distortion for K − is reduced [23].…”
Section: Introductionmentioning
confidence: 99%
“…In Fig. 3(a), we show these spectra obtained with (N R , N I ) = (0.6, 0.9), which values were suggested by the theoretical analyzes of the HeBC data [10]. We find that the 1 − resonant state is favored rather than the 0 + ground state in the conversion spectrum due to the momentum transfer q Σ ≃ 286 MeV/c, so that a peak of the spectrum is seen at ω ≃ 275 MeV above the Σ threshold.…”
Section: Resultsmentioning
confidence: 99%
“…Now let us evaluate pole positions of the three-channel coupled system in a ( 3 He-Λ)+( 3 H-Σ + )+ ( 3 He-Σ 0 ) model [11], solving the multichannel Lippmann-Schwinger equation with a phenomenological 3N-Y potential determined by theoretical analyzes [10]. We obtain the trajectories of the poles with s and p waves by changing the strengths of the 3N-Σ potential,…”
Section: Resultsmentioning
confidence: 99%
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