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Single quark transition model analysis of electromagnetic nucleon resonance excitations in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mo>[</mml:mo><mml:mn>7</mml:mn><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>โˆ’</mml:mi></mml:mrow></mml:msup></mml:mrow><mml:mo>]</mml:mo></mml:math>supermultiplet

Single quark transition model analysis of electromagnetic nucleon resonance excitations in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mo>[</mml:mo><mml:mn>7</mml:mn><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>โˆ’</mml:mi></mml:mrow></mml:msup></mml:mrow><mml:mo>]</mml:mo></mml:math>supermultiplet

We apply the single quark transition model to resonance transition amplitudes extracted from photo-production and electroproduction data. We use experimental data on the ${S}_{11}(1535)$ and ${D}_{13}(1520)$ nucleon resonances to extract the amplitudes for the electromagnetic transition from the nucleon ground state $[56, {0}^{+}]$ to the $[70, {1}^{\ensuremath{-}}]$ supermultiplet, and make โ€ฆ