) (')K('0) (pi)('+)(pi)('-)n are presented. The data derive from a 4 event/nanobarn exposure of the LASS (Large Aperture Superconduc'/> A STUDY OF THE STRANGE MESON SPECTRUM AS OBSERVED IN THE REACTION NEGATIVE KAON PROTON TO NEUTRAL KAON POSITIVE PION NEGATIVE PION NEUTRON AT 11 GEV/C (ELEMENTARY PARTICLES, PARTIAL WAVE ANALYSIS).
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A STUDY OF THE STRANGE MESON SPECTRUM AS OBSERVED IN THE REACTION NEGATIVE KAON PROTON TO NEUTRAL KAON POSITIVE PION NEGATIVE PION NEUTRON AT 11 GEV/C (ELEMENTARY PARTICLES, PARTIAL WAVE ANALYSIS).

机译:从11 GEV / C的反应性负质子质子到中性正质子正离子负性中子的奇偶子谱研究(基本粒子,部分波分析)。

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摘要

The results of a high statistics study of the reaction K('-)p (--->) (')K('0) (pi)('+)(pi)('-)n are presented. The data derive from a 4 event/nanobarn exposure of the LASS (Large Aperture Superconducting Solenoid) spectrometer to an 11 GeV/c K('-) beam. The (')K('0) (pi)('+)(pi)('-)n event sample consists of 34,000 events with (')K('0) (pi)('+)(pi)('-) invariant masses less than 2.4 GeV/c('2) and (VBAR)t'(VBAR) (LESSTHEQ) 0.3 (GeV/c)('2).; The forward-produced (')K('0) (pi)('+)(pi)('-) events arise predominantly through the production and subsequent strong decay of natural spin-parity strange meson states (J('P) = 1('-), 2('+), ...). Their production can be understood in the context of an exchange model, while their decay into the (')K('0) (pi)('+)(pi)('-) final state proceeds through intermediate two-body states such as K*(892)('-)(pi)('+), (')K('0)(rho)(770)('0), K*(1430)('-)(pi)('+), and (')K('0)f(1270)('0). A partial wave analysis employing the three-body isobar model successfully describes all of the features of the data.; The J('P) = 1('+), 2('+), and 3('-) partial waves show resonant behavior that is attributed to the production and decay of the 1('+) Q(1400), the 2('+) K*(1430), and the 3('-) K*(1780). The structure in the 1('-) amplitudes can be understood as arising from two vector states, one at (TURN)1.42 GeV/c('2) coupling only to K*(pi) and the other at (TURN)1.73 decaying to both K*(pi) and K(rho). The J('P) = 4('+) waves, required above a mass of 2.0 GeV/c('2), show structures that may arise from the production of the 4('+) K*(2060). There is a second enhancement in the J('P) = 2('+) waves at (TURN)2.0 GeV/c('2) that may be evidence for a new resonant state.; The t' dependences of the 2('+), 3('-), and the higher mass 1('-) partial waves are steep, whereas the t' dependence of the 1('-) amplitude at low mass is shallow. This indicates that the lower mass 1('-) state, unlike the other natural spin-parity resonances, does not couple strongly to the K(pi) system.; The observed properties of these resonant states can be used to test and further develop models of the strange meson spectrum. The implications of these data for the most successful of these, the non-relativistic quark model, are discussed.
机译:给出了反应K('-)p(--->)(')K('0)(pi)('+)(pi)('-)n的高统计研究的结果。数据来自LASS(大孔径超导螺线管)光谱仪在11 GeV / c K('-)射线下的4事件/纳米波曝光。 ('] K('0)(pi)('+)(pi)('-)n事件样本包含34,000个事件,其中(')K('0)(pi)('+)(pi)( '-)不变质量小于2.4 GeV / c('2)和(VBAR)t'(VBAR)(LESSTHEQ)0.3(GeV / c)('2)。前向产生的('] K('0)(pi)('+)(pi)('-)事件主要是通过自然自旋奇偶校验介子态(J('P) = 1('-),2('+),...)。可以在交换模型的背景下理解它们的产生,而它们的衰减成(')K('0)(pi)('+)(pi)('-)最终状态则通过中间的两体状态进行,例如如K *(892)('-)(pi)('+),(')K('0)(rho)(770)('0),K *(1430)('-)(pi)( '+)和(')K('0)f(1270)('0)。采用三体等压线模型的局部波分析成功地描述了数据的所有特征。 J('P)= 1('+),2('+)和3('-)分波显示出共振行为,这归因于1('+)Q(1400)的产生和衰减, 2('+)K *(1430)和3('-)K *(1780)。可以将振幅为1('-)的结构理解为由两个矢量状态引起,一个矢量处于(TURN)1.42 GeV / c('2)仅耦合到K *(pi),而另一个处于(TURN)1.73衰减到K *(pi)和K(rho)。在质量为2.0 GeV / c('2)以上时,所需的J('P)= 4('+)波显示出可能由于产生4('+)K *(2060)而产生的结构。在(TURN)2.0 GeV / c('2)处的J('P)= 2('+)波有第二个增强,这可能是新共振状态的证据。 2('+),3('-)和较高质量的1('-)分波的t'依赖性较陡,而低质量的1('-)振幅的t'依赖性较浅。这表明较低质量的1('-)状态与其他自然自旋奇偶共振不同,不会与K(pi)系统强烈耦合。这些共振态的观察特性可用于测试和进一步开发奇怪的介子谱模型。讨论了这些数据对于其中最成功的非相对论夸克模型的含义。

著录项

  • 作者单位

    Stanford University.;

  • 授予单位 Stanford University.;
  • 学科 Physics Elementary Particles and High Energy.
  • 学位 Ph.D.
  • 年度 1986
  • 页码 249 p.
  • 总页数 249
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 高能物理学;
  • 关键词

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