- Collaboration, Fermilab E835;
- Andreotti, M;
- Bagnasco, S;
- Baldini, W;
- Bettoni, D;
- Borreani, G;
- Buzzo, A;
- Calabrese, R;
- Cester, R;
- Cibinetto, G;
- Dalpiaz, P;
- Garzoglio, G;
- Gollwitzer, KE;
- Graham, M;
- Hu, M;
- Joffe, D;
- Kasper, J;
- Lasio, G;
- Vetere, M Lo;
- Luppi, E;
- Macrì, M;
- Mandelkern, M;
- Marchetto, F;
- Marinelli, M;
- Menichetti, E;
- Metreveli, Z;
- Mussa, R;
- Negrini, M;
- Obertino, MM;
- Pallavicini, M;
- Pastrone, N;
- Patrignani, C;
- Pordes, S;
- Robutti, E;
- Roethel, W;
- Rosen, J;
- Rumerio, P;
- Rusack, RW;
- Santroni, A;
- Schultz, J;
- Seo, SH;
- Seth, KK;
- Stancari, G;
- Stancari, M;
- Tomaradze, A;
- Uman, I;
- Vidnovic, T;
- Werkema, S;
- Zweber, P
We present new precision measurements of the ψ (2 S) total and partial widths from excitation curves obtained in antiproton-proton annihilations by Fermilab experiment E835 at the Antiproton Accumulator in the year 2000. A new technique of complementary scans was developed to study narrow resonances with stochastically cooled antiproton beams. The technique relies on precise revolution-frequency and orbit-length measurements, while making the analysis of the excitation curve almost independent of machine lattice parameters. We study the ψ (2 S) meson through the processes over(p, ̄) p → e+ e- and over(p, ̄) p → J / ψ + X → e+ e- + X. We measure the width to be Γ = 290 ± 25 (sta) ± 4 (sys) keV and the combination of partial widths Γe+ e- Γover(p, ̄) p / Γ = 579 ± 38 (sta) ± 36 (sys) meV, which represent the most precise measurements to date. © 2007 Elsevier B.V. All rights reserved.