Results from a π−p slow proton trigger experiment at 12 GeV/c

Evangelista, C.; Ghidini, B.; Palano, A.; Picciarelli, V.; Zito, G.; Bröring, J.; Müller, K.; Paul, E.; Renneberg, W.; Rühmer, W.; Eades, J.; French, B. R.; Moebes, J.; Navach, F.; Edwards, M.; Smith, I.L.; Petzmezas, G.; Donald, R.A.; Edwards, David; Fry, J. R.; Cantore, A.; Corato, M. Di; Mandelli, L.; Perini, L.

doi:10.1016/0550-3213(81)90407-7

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The D(1285) and The E(1420)1

The 8 As a Hybrid Qqg1

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1981

2016

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Cited by 18 publications

(3 citation statements)

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“…A clear qOrtr-decay mode of the D(1285) has been observed: see, for example, figure 37 which reproduces the results obtained by Evangelista et a1 (1981) for the reaction (3.5) r -p + p 7 ~~r -q ' at 12 GeVlc.…”

Section: The D(1285) and The E(1420)supporting

confidence: 83%

The positive-parity mesons

Montanet¹

1983

Rep. Prog. Phys.

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Section: The D(1285) and The E(1420)supporting

confidence: 83%

The positive-parity mesons

Montanet¹

1983

Rep. Prog. Phys.

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“…The problem comes with the isovector state. Data on the A2 (Cleland 1982, Evangelista et a1 1981 show no sign of an I = 1 state nearby. (The A2 is not split!…”

Section: The 8 As a Hybrid Qqgmentioning

confidence: 99%

Gluonic hadrons

1988

Rep. Prog. Phys.

168

141

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The standard theory of colour forces (QCD) suggests that in addition to the familiar hadrons made of quarks, there should exist new states where coloured gluons play an essential dynamical role. I review the theoretical predictions for the properties of these 'glueballs' and of states containing resonating quarks and gluons (variously called 'hybrids', 'hermaphrodites' or 'meiktons'). I attempt to highlight those features which are common to several models in the literature. Experimental candidates are confronted with the models. No clearcut signal for a gluonic hadron yet exists; consequently I consider what future data are required to determine the constituency of some popular candidates.

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“…The axial-vector meson b 1 , which is identified as a 1 P 1 state in the quark model, was first observed by the HBC Collaboration in 1963 [7]. Before 1994, it was studied in pp [8,9], γp [10], and pπ [11][12][13][14][15][16][17][18][19] reactions, where the focus was on mass and width measurements. Later, it was widely observed in hadronic decays of D, B, and charmonium states [3].…”

mentioning

confidence: 99%

Measurement of the absolute branching fraction of D ⁺ → K̅ ⁰ e ⁺ ν _e via K̅ ⁰ → π ⁰ π ^0<

Ablikim¹,

Ачасов²,

Ai³

et al. 2016

Chinese Phys. C

35
0
38
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Results from a π−p slow proton trigger experiment at 12 GeV/c

Cited by 18 publications

References 35 publications

The positive-parity mesons

The positive-parity mesons

Gluonic hadrons

Measurement of the absolute branching fraction of D ⁺ → K̅ ⁰ e ⁺ ν _e via K̅ ⁰ → π ⁰ π ^0<

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Results from a π−p slow proton trigger experiment at 12 GeV/c

Cited by 18 publications

References 35 publications

The positive-parity mesons

The positive-parity mesons

Gluonic hadrons

Measurement of the absolute branching fraction of D + → K̅ 0 e + ν e via K̅ 0 → π 0 π 0<

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Measurement of the absolute branching fraction of D ⁺ → K̅ ⁰ e ⁺ ν _e via K̅ ⁰ → π ⁰ π ^0<