Spectrum of Heavy Mesons in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>Annihilation

Harrington, Barry J.; Park, Soo Yong; Yildiz, Asim

doi:10.1103/physrevlett.34.168

Cited by 174 publications

(8 citation statements)

References 18 publications

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“…The d a t a of the c h a r m o n i u m s p e c t r u m seem to fit to experiments quite well [1,2,3] when a eonfinement potential between c and ~ is supposed in the form: V(r) = 1 (~ + Ar + Kr2).…”

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confidence: 86%

Confinement potential produced by indefinite metric multipole fields of infinite order

Nagy

1977

Acta Physica

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The possibility of obtaining some type of confinement of particles is discussed in a field theory with multipole fields of the N-th order. The limiting case N -+ ~ yields various forros of Jtatic confincment potcntials.1. The d a t a of the c h a r m o n i u m s p e c t r u m seem to fit to experiments quite well [1, 2, 3] when a eonfinement potential between c and ~ is supposed in the form:r F o r e x a m p l e [2] gives the values of ~, A, K as = --0 , 2 , K = ----, a = 0 , 2 f m . a 2T h e value of A is irrelevant (actually A = 0 is taken), it is an additive constant only to the total energy. A great v a r i e t y of theoretical considerations predicts the forro (1). We quote two r a t h e r conservative field theoretical approaches only [4,5] (similar to ours [61), where other referenees can be found.In a previous work [6] we have ealled the attention to multipole fields as possible sourees of some kind of particle confinement. There the free L a g r a n g i a n has been proposed to possess the forroand it has been shown t h a t the fields A, B, C interacting vŸ ah interaction L a g r a n g i a n L I in the form L i = -~cq~, q~ = glA + g2B + gaC, * On leave of absence from the Institute of Theorctical Physics, Roland E6tv6s University,

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confidence: 86%

Confinement potential produced by indefinite metric multipole fields of infinite order

Nagy

1977

Acta Physica

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“…The striking appearance of these new states precipitated extensive theoretical analysis and further detailed experiments. [126][127][128][129][130]), The level spacings are much less than the mass scale, suggesting that the states may be treated nonrelativistically by the Schrödinger equation. [125] and interprets J /ψ as a charmonium system based on an atomic model of heavycc quarks bound in a static, confining potential.…”

Section: Charmmentioning

confidence: 99%

Electroweak Forces

2008

Gauge Field Theories

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“…Using the 13S1 and 23S1 masses as inputs to fix the strength of a linear potential and the quark mass, Harrington et al (97) calculate eigenvalues E(33Sd = 4.18 GeV, EWSd = 4.61 GeV, E(53S,) = 5.00 GeV, fo r the next three charmonium states accessible to e + e -annihilation in lowest order.…”

Section: Charmoniummentioning

confidence: 99%

Psionic Matter

Chinowsky¹

1977

Annu. Rev. Nucl. Sci.

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Spectrum of Heavy Mesons ine+e−Annihilation

Cited by 174 publications

References 18 publications

Confinement potential produced by indefinite metric multipole fields of infinite order

Confinement potential produced by indefinite metric multipole fields of infinite order

Electroweak Forces

Psionic Matter

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