Cargando…
A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c
The authors have investigated the final states K*/sup 0/(890) Lambda , K*/sup 0/(890) Sigma /sup 0/ and K*/sup 0/(890) Y/sub 1/*/sup 0/(1385) produced in pi /sup -/p interactions at 3.93 GeV/c. They present the differential cross sections and spin density matrix elements for the resonances as functi...
Autores principales: | , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
1973
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0550-3213(74)90081-9 http://cds.cern.ch/record/413713 |
_version_ | 1780894691161538560 |
---|---|
author | Yaffe, D Abramovich, M Chaloupka, V Ferrando, A Korkea-Aho, M K Losty, Michael J Montanet, Lucien Paul, E Zatz, J Zieminski, Z |
author_facet | Yaffe, D Abramovich, M Chaloupka, V Ferrando, A Korkea-Aho, M K Losty, Michael J Montanet, Lucien Paul, E Zatz, J Zieminski, Z |
author_sort | Yaffe, D |
collection | CERN |
description | The authors have investigated the final states K*/sup 0/(890) Lambda , K*/sup 0/(890) Sigma /sup 0/ and K*/sup 0/(890) Y/sub 1/*/sup 0/(1385) produced in pi /sup -/p interactions at 3.93 GeV/c. They present the differential cross sections and spin density matrix elements for the resonances as functions of momentum transfer, as well as the Lambda and Sigma /sup 0/ polarizations. The Sigma /sup 0/ polarization is found to be positive and maximal. An amplitude analysis is performed for the K* Lambda and K* Sigma /sup 0/ reactions, and it is found that one natural parity transversity amplitude is dominant for the latter. (15 refs). |
id | cern-413713 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1973 |
record_format | invenio |
spelling | cern-4137132019-09-30T06:29:59Zdoi:10.1016/0550-3213(74)90081-9http://cds.cern.ch/record/413713engYaffe, DAbramovich, MChaloupka, VFerrando, AKorkea-Aho, M KLosty, Michael JMontanet, LucienPaul, EZatz, JZieminski, ZA study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/cParticle PhysicsThe authors have investigated the final states K*/sup 0/(890) Lambda , K*/sup 0/(890) Sigma /sup 0/ and K*/sup 0/(890) Y/sub 1/*/sup 0/(1385) produced in pi /sup -/p interactions at 3.93 GeV/c. They present the differential cross sections and spin density matrix elements for the resonances as functions of momentum transfer, as well as the Lambda and Sigma /sup 0/ polarizations. The Sigma /sup 0/ polarization is found to be positive and maximal. An amplitude analysis is performed for the K* Lambda and K* Sigma /sup 0/ reactions, and it is found that one natural parity transversity amplitude is dominant for the latter. (15 refs).CERN-D-Ph-II-PHYS-73-24-revoai:cds.cern.ch:4137131973-11-12 |
spellingShingle | Particle Physics Yaffe, D Abramovich, M Chaloupka, V Ferrando, A Korkea-Aho, M K Losty, Michael J Montanet, Lucien Paul, E Zatz, J Zieminski, Z A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c |
title | A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c |
title_full | A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c |
title_fullStr | A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c |
title_full_unstemmed | A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c |
title_short | A study of the reactions $\pi^{-}p\rightarrow K^{*}X, K^{*}\Sigma$ and $K^{*}Y1^{*}$ (1385) at 3.93 GeV/c |
title_sort | study of the reactions $\pi^{-}p\rightarrow k^{*}x, k^{*}\sigma$ and $k^{*}y1^{*}$ (1385) at 3.93 gev/c |
topic | Particle Physics |
url | https://dx.doi.org/10.1016/0550-3213(74)90081-9 http://cds.cern.ch/record/413713 |
work_keys_str_mv | AT yaffed astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT abramovichm astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT chaloupkav astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT ferrandoa astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT korkeaahomk astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT lostymichaelj astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT montanetlucien astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT paule astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT zatzj astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT zieminskiz astudyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT yaffed studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT abramovichm studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT chaloupkav studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT ferrandoa studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT korkeaahomk studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT lostymichaelj studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT montanetlucien studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT paule studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT zatzj studyofthereactionspiprightarrowkxksigmaandky11385at393gevc AT zieminskiz studyofthereactionspiprightarrowkxksigmaandky11385at393gevc |