${{\mathit f}_{{{2}}}{(1950)}}$ T-MATRIX POLE $\sqrt {\mathit s }$
INSPIRE search
Note that $\Gamma $ = $−$2 Im($\sqrt {s }$).
M135PP |
$\bf{
(1830 - 2020) − {\mit i} (110 - 220)}$
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OUR ESTIMATE
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$(1955 \pm75) − {\mit i} (175 \pm57)$ |
1 |
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RVUE |
$(1978.2 \pm1.8 {}^{+28.4}_{-16.9}) − {\mit i} (118.8 \pm0.8 {}^{+20.8}_{-7.8})$ |
2 |
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RVUE |
$(1867 \pm46) − {\mit i} (193 \pm29)$ |
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CBAR |
1
T-matrix pole from coupled channel K-matrix fit to data on ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$ (ABLIKIM 2015AE) and ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit K}_S^0}$ ${{\mathit K}_S^0}$ (ABLIKIM 2018AA).
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2
T-matrix pole, 4 poles, 4 channels, including scattering data from HYAMS 1975 (${{\mathit \pi}}{{\mathit \pi}}$), LONGACRE 1986 (${{\mathit K}}{{\overline{\mathit K}}}$), BINON 1983 (${{\mathit \eta}}{{\mathit \eta}}$).
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References: |
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EPJ C82 80
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Scalar and tensor resonances in $J/\psi $ radiative decays |
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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 C23 29
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Proton-Antiproton Annihilation at 900 ${\mathrm {MeV}}/\mathit c$ into ${{\mathit \pi}^{0}}{{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$, ${{\mathit \pi}^{0}}{{\mathit \pi}^{0}}{{\mathit \eta}}$, and ${{\mathit \pi}^{0}}{{\mathit \eta}}{{\mathit \eta}}$ |
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