${{\mathit a}_{{{0}}}{(980)}}$ T-MATRIX POLE $\sqrt {\mathit s }$
INSPIRE search
Note that $\Gamma $ = $−$2 Im($\sqrt {s }$).
M036PP |
$\bf{
(970 - 1020) − {\mit i} (30 - 70)}$
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OUR ESTIMATE
(see Fig. 64.2 in the review)
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$(1002.4 \pm1.4 \pm6.6) − {\mit i}(63.5 \pm2.9)$ |
1 |
|
CBAR |
$(1000.7 {}^{+12.9}_{-0.7}) − {\mit i}(36.6 {}^{+12.7}_{-2.6})$ |
2 |
|
RVUE |
$(989 \pm5) − {\mit i}(40 \pm5)$ |
3 |
|
RVUE |
$(1117 {}^{+24}_{-320}) − {\mit i}(12 {}^{+43}_{-12})$ |
4 |
|
RVUE |
$(982 \pm3) − {\mit i}(46 \pm4)$ |
5 |
|
CBAR |
1
Pole mass on sheet closest to the physical axis - the more remote pole is extracted at ($1004.1$ $\pm1.5$ $\pm6.5$) $−$ ${\mit i}(48.6$ $\pm1.2$ $\pm3.4$) MeV.
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2
T-matrix pole on sheet II.
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3
T-matrix pole on sheet II. Parameterizes couplings to ${{\overline{\mathit K}}}{{\mathit K}}$, ${{\mathit \pi}}{{\mathit \eta}}$, and ${{\mathit \pi}}{{\mathit \eta}^{\,'}}$. Uses AMSLER 1994D and ABELE 1998.
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4
Reanalysis of data from LINGLIN 1973, ESTABROOKS 1978, and ASTON 1988 in the unitarized ChPT model.
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5
T-matrix pole on sheet II; the pole on sheet III is at (1006 $−$ ${\mit i}$ 49) MeV.
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References: |
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EPJ C80 453
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Coupled channel analysis of ${\bar{p}p}\,\rightarrow \,\pi ^0\pi ^0\eta $, ${\pi ^0\eta \eta }$ and ${K^+K^-\pi ^0}$ at 900 MeV/c and of ${\pi \pi }$-scattering data |
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EPJ C80 436
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The $\pi \eta $ interaction and $a_0$ resonances in photon?photon scattering |
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PR D78 074023
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Reanalysis of Data on ${{\mathit a}_{{{0}}}{(1450)}}$ and ${{\mathit a}_{{{0}}}{(980)}}$ |
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MPL A19 2879
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Light Scalars as Tetraquarks or Two-meson States from Large ${{\mathit N}_{{{c}}}}$ and Unitarized Chiral Perturbation Theory |
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PR D57 3860
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${{\overline{\mathit p}}}$ ${{\mathit p}}$ Annihilation at Rest into ${{\mathit K}_L^0}$ ${{\mathit K}^{\pm}}$ ${{\mathit \pi}^{\mp}}$ |
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