Search Results - "Worstell, W.A"

Performance of Large Area Picosecond Photo-Detectors (LAPPDTM) by Lyashenko, A.V., Adams, B.W., Aviles, M., Cremer, T., Ertley, C.D., Foley, M.R., Minot, M.J., Popecki, M.A., Stochaj, M.E., Worstell, W.A., Elam, J.W., Mane, A.U., Siegmund, O.H. W., Frisch, H.J., Elagin, A.L., Angelico, E., Spieglan, E.

“…We report on performance results achieved for recently produced LAPPDs - largest commercially available planar geometry photodetectors based on microchannel…”
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Count-rate dependent event mispositioning and NEC in PET by Badawi, R.D., Domigan, P., Johnson, O., Kemp, B., Kudrolli, H., Rempel, T., Rohatgi, R., Romanov, L.V., Surti, S., Worstell, W.A., Zimmerman, R.E.

“…Most current PET detector designs suffer from event mispositioning at high count rates, as scintillation light from nearby and nearly simultaneous gamma ray…”
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Large Area Picosecond Photodetector (LAPPDTM) - Pilot production and development status by Minot, M.J., Adams, B.W., Aviles, M., Bond, J.L., Cremer, T., Foley, M.R., Lyashenko, A., Popecki, M.A., Stochaj, M.E., Worstell, W.A., Wetstein, M.J., Elam, J.W., Mane, A.U., Siegmund, O.H.W., Ertley, C., Frisch, H.J., Elagin, A., Angelico, E., Spieglan, E.

“…We report performance results achieved for fully functional sealed Large Area Picosecond Photodetectors (LAPPD™) in tests performed at Incom Inc., as well as…”
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The Brookhaven muon storage ring magnet by Danby, G.T., Addessi, L., Armoza, Z., Benante, J., Brown, H.N., Bunce, G., Cottingham, J.C., Cullen, J., Geller, J., Hseuh, H., Jackson, J.W., Jia, L., Kochis, S., Koniczny, D., Larsen, R., Lee, Y.Y., Mapes, M., Meier, R.E., Meng, W., Morse, W.M., O'Toole, M., Pai, C., Polk, I., Prigl, R., Semertzidis, Y.K., Shutt, R., Snydstrup, L., Soukas, A., Tallerico, T., Toldo, F., Lintig, D.Von, Woodle, K., Carey, R.M., Earle, W., Hazen, E.S., Krienen, F., Miller, J.P., Ouyang, J., Roberts, B.L., Sulak, L.R., Worstell, W.A., Orlov, Y., Winn, D., Grossmann, A., Jungmann, K., zu Putlitz, G., von Walter, P., Debevec, P.T., Deninger, W.J., Hertzog, D.W., Sedykh, S., Urner, D., Green, M.A., Haeberlen, U., Cushman, P., Giron, S., Kindem, J., Miller, D., Timmermans, C., Zimmerman, D., Druzhinin, V.P., Fedotovich, G.V., Grigorev, D.N., Khazin, B.I., Ryskulov, N.M., Serednyakov, S., Shatunov, Yu.M., Solodov, E., Endo, K., Hirabayashi, H., Mizumachi, Y., Yamamoto, A., Dhawan, S.K., Disco, A., Farley, F.J.M., Fei, X., Grosse-Perdekamp, M., Hughes, V.W., Kawall, D., Redin, S.I.

“…The muon g-2 experiment at Brookhaven National Laboratory has the goal of determining the muon anomalous g-value a μ (=(g−2)/2) to the very high precision of…”
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Measurement of φ meson parameters with CMD-2 detector at VEPP-2M collider by Akhmetshin, R.R, Aksenov, G.A, Anashkin, E.V, Aulchenko, V.M, Baibusinov, B.O, Banzarov, V.S, Barkov, L.M, Baru, S.E, Bondar, A.E, Danilov, V.V, Eidelman, S.I, Fedotovich, G.V, Gabyshev, N.I, Grebeniuk, A.A, Grigoriev, D.N, Ivanov, P.M, Khazin, B.I, Koop, I.A, Kuzmin, A.S, Logashenko, I.B, Lysenko, A.P, Maksimov, A.V, Merzlyakov, Yu.I, Monitch, V.A, Nesterenko, I.N, Okhapkin, V.S, Perevedentsev, E.A, Polumin, A.A, Popkov, E.V, Ptitzyn, V.I, Purlats, T.A, Redin, S.I, Root, N.I, Ruban, A.A, Ryskulov, N.M, Shatunov, Yu.M, Sher, A.E, Shubin, M.A, Shwartz, B.A, Sidorov, V.A, Skrinsky, A.N, Smakhtin, V.P, Snopkov, I.G, Solodov, E.P, Sukhanov, A.I, Titov, V.M, Yudin, Yu.V, Zavarzin, V.G, Brown, D.H, Miller, J.P, Roberts, B.L, Worstell, W.A, Thompson, J.A, Valine, C.M, Cushman, P.B, Dhawan, S.K, Hughes, V.W

“…Results of the measurement of the φ meson parameters with the general purpose detector CMD-2 at the upgraded e + e − collider VEPP-2M at Novosibirsk are…”
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The effects of pulse pile-up on point-source measurements performed on different PET scanning devices by Badawi, R.D., Surti, S., Kemp, B., Zimmerman, R.E., El Fakhri, G., Holdsworth, C.H., Worstell, W.A.

“…We have quantified resolution and contrast loss as a function of noise-equivalent count rate on the GSO-based Philips Allegro and the pixelated NaI CPET2 using…”
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Study of KK coupled decays and K-Be interactions with the CMD-2 detector at VEPP-2M collider by Akhmetshin, R.R, Aksenov, G.A, Anashkin, E.V, Aulchenko, V.M, Baibusinov, B.O, Banzarov, V.S, Barkov, L.M, Baru, S.E, Bondar, A.E, Chernyak, D.V, Danilov, V.V, Eidelman, S.I, Fedotovich, G.V, Gabyshev, N.I, Grebeniuk, A.A, Grigoriev, D.N, Ivanov, P.M, Khazin, B.I, Koop, I.A, Kuzmin, A.S, Logashenko, I.B, Lukin, P.A, Lysenko, A.P, Maksimov, A.V, Merzlyakov, Yu.I, Nesterenko, I.N, Okhapkin, V.S, Perevedentsev, E.A, Polunin, A.A, Popkov, E.V, Ptitzyn, V.I, Purlats, T.A, Redin, S.I, Root, N.I, Ruban, A.A, Ryskulov, N.M, Shatunov, Yu.M, Sher, A.E, Shubin, M.A, Shwartz, B.A, Sidorov, V.A, Skrinsky, A.N, Smakhtin, V.P, Snopkov, I.G, Solodov, E.P, Sukhanov, A.I, Titov, V.M, Yudin, Yu.V, Zavarzin, V.G, Brown, D.H, Miller, J.P, Roberts, B.L, Worstell, W.A, Thompson, J.A, Valine, C.M, Cushman, P.B, Dhawan, S.K, Hughes, V.W

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Study of KSKL coupled decays and K L-Be interactions with the CMD-2 detector at VEPP-2M collider by Akhmetshin, R.R, Aksenov, G.A, Anashkin, E.V, Aulchenko, V.M, Baibusinov, B.O, Banzarov, V.S, Barkov, L.M, Baru, S.E, Bondar, A.E, Chernyak, D.V, Danilov, V.V, Eidelman, S.I, Fedotovich, G.V, Gabyshev, N.I, Grebeniuk, A.A, Grigoriev, D.N, Ivanov, P.M, Khazin, B.I, Koop, I.A, Kuzmin, A.S, Logashenko, I.B, Lukin, P.A, Lysenko, A.P, Maksimov, A.V, Merzlyakov, Yu.I, Nesterenko, I.N, Okhapkin, V.S, Perevedentsev, E.A, Polunin, A.A, Popkov, E.V, Ptitzyn, V.I, Purlats, T.A, Redin, S.I, Root, N.I, Ruban, A.A, Ryskulov, N.M, Shatunov, Yu.M, Sher, A.E, Shubin, M.A, Shwartz, B.A, Sidorov, V.A, Skrinsky, A.N, Smakhtin, V.P, Snopkov, I.G, Solodov, E.P, Sukhanov, A.I, Titov, V.M, Yudin, Yu.V, Zavarzin, V.G, Brown, D.H, Miller, J.P, Roberts, B.L, Worstell, W.A, Thompson, J.A, Valine, C.M, Cushman, P.B, Dhawan, S.K, Hughes, V.W

“…An integrated luminosity ≈ 4000 nb −1 of around F meson mass (5.0 × 10 6 of F's) has been collected with the CMD-2 detector at the VEPP-2M collider. The latest…”
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Compensating hadron calorimeters with Cerenkov light by Winn, D.R., Worstell, W.A.

“…Because only a small fraction ( approximately 10%) of the energy deposition in the purely hadronic portion of a hadron shower is by minimum ionizing particles,…”
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Count-rate dependent event mispositioning and NEC in PET by Badawi, R.D., Domigan, P., Johnson, O., Kemp, B., Kudrolli, H., Rempel, T., Rohatgi, R., Romanov, L.V., Surti, S., Worstell, W.A., Zimmerman, R.E.

“…Most current PET detector designs suffer from event mispositioning at high count rates, as scintillation light from nearby and nearly simultaneous gamma ray…”
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Compact representation of PET 3D system response matrices by Worstell, W.A., Adler, S.S., Kudrolli, H.A., Nevin, J.D., Romanov, L.V.

“…We present a method for the compact storage of 3D geometric system response matrix coefficients in PET, using a separation into transaxial and axial…”
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