S-wave resonance coupled-channel approach to the reactionsπ−+p→η+nandK−+p→η+Λ, and a determination of the ηnand ηΛ scattering lengths

1996 ◽  
Vol 53 (1) ◽  
pp. 385-389 ◽  
Author(s):  
V. V. Abaev ◽  
B. M. K. Nefkens
1974 ◽  
Vol 27 (1) ◽  
pp. 13
Author(s):  
DC Peaslee

An investigation is made of the relation between scattering lengths and resonances in a two-nucleon system. For resonances Eo near zero energy the usual determination of an effective optical potential in mesonic atoms is limited, and it is shown here that the scattering length can only be represented usefully as a sum over resonances of the compound system if the condition IEolDI ~ (PDo)! Is satisfied, where D is the average spacing of s-wave states, p the density of target nucleons and Do the Compton volume of the reduced system. This condition is seen to be valid for mr:, nK and KK interactions and these systems are considered in some detail. It is shown that knowledge of the level shifts of each of these examples can help resolve present uncertainties in associated boson structure.


2009 ◽  
Vol 24 (02n03) ◽  
pp. 214-221
Author(s):  
AKAKI RUSETSKY

We consider two ways of the experimental determination of the S-wave ππ scattering lengths: from K → 3π decays and from Ke4 decays. In both cases the unitary cusps, which emerge due to the difference in the charged and neutral pion masses, play a crucial role. We construct a systematic effective field theory framework which can be used to describe decay amplitudes in the cusp region.


2009 ◽  
Vol 64 (4) ◽  
pp. 589-608 ◽  
Author(s):  
J. R. Batley ◽  
A. J. Culling ◽  
G. Kalmus ◽  
C. Lazzeroni ◽  
D. J. Munday ◽  
...  
Keyword(s):  
S Wave ◽  

2009 ◽  
Vol 24 (02n03) ◽  
pp. 488-492
Author(s):  
◽  
ANDREA BIZZETI

Large samples of K± → 3π and K± → π+π-e±ν (Ke4) decays have been collected by the NA48/2 experiment at CERN SPS. At the π+π- threshold, the π0π0 invariant mass spectrum of the decay K± → π±π0π0 xhibits a Wigner cusp, from which the S-wave ππ scattering lengths are extracted with high precision. The same scattering lengths are also independently determined from the accurate measurement of the form factors in the Ke4 decay K± → π+π-e±ν.


1966 ◽  
Vol 19 (8) ◽  
pp. 715-719 ◽  
Author(s):  
G. Alexander ◽  
O. Benary ◽  
U. Karshon ◽  
A. Shapira ◽  
G. Yukutieli ◽  
...  

1997 ◽  
Vol 55 (5) ◽  
pp. R3299-R3302 ◽  
Author(s):  
E. R. I. Abraham ◽  
W. I. McAlexander ◽  
J. M. Gerton ◽  
R. G. Hulet ◽  
R. Côté ◽  
...  

Author(s):  
Hao Wang ◽  
Ning Li ◽  
Caizhi Wang ◽  
Hongliang Wu ◽  
Peng Liu ◽  
...  

Abstract In the process of dipole-source acoustic far-detection logging, the azimuth of the fracture outside the borehole can be determined with the assumption that the SH–SH wave is stronger than the SV–SV wave. However, in slow formations, the considerable borehole modulation highly complicates the dipole-source radiation of SH and SV waves. A 3D finite-difference time-domain method is used to investigate the responses of the dipole-source reflected shear wave (S–S) in slow formations and explain the relationships between the azimuth characteristics of the S–S wave and the source–receiver offset and the dip angle of the fracture outside the borehole. Results indicate that the SH–SH and SV–SV waves cannot be effectively distinguished by amplitude at some offset ranges under low- and high-fracture dip angle conditions, and the offset ranges are related to formation properties and fracture dip angle. In these cases, the fracture azimuth determined by the amplitude of the S–S wave not only has a $180^\circ $ uncertainty but may also have a $90^\circ $ difference from the actual value. Under these situations, the P–P, S–P and S–S waves can be combined to solve the problem of the $90^\circ $ difference in the azimuth determination of fractures outside the borehole, especially for a low-dip-angle fracture.


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