Adler, J.O.; Hansen, K.; Lindgren, K.R.
Lund Univ. (Sweden). Dept. of Physics1984
Lund Univ. (Sweden). Dept. of Physics1984
AbstractAbstract
[en] A magnetic electron spectrometer for tagged photon experiments at the accelerator system MAX has been designed and constructed. A small magnet of the inclined plane pole faces type with opening angle +-8 degree was choosen resulting in a time difference between different electron trajectories of less than 1ns. The focal properties of the spectrometer were investigated by ray-tracings showing that for an angular acceptance of /theta(sub)V/<=4 degree and /theta(sub)H/<=8 degree the astigmatic and aberrational effects will contribute less than 10% to the energy resolution of the focal plane detector array. (author)
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Jun 1984; 54 p
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Report
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AbstractAbstract
[en] It is generally recognized that at small wind energy penetration levels, the capacity credit of many widely dispersed wind turbines is about equal to their average power output. In systems with few wind turbines, however, wind power fluctuations are not averaging each other out, and the capacity credit must be reduced. A methodology for estimating the capacity credit taking into consideration the wind power fluctuations is described. The methodology utilizes the commonly applied loss of load expectation index for estimating the capacity credit. Calculations are made and presented for a number of power system configurations and wind power penetration levels. It is concluded that the described methodology gives a consistent approach for determining the capacity credit for small and large systems with a few or many dispersed wind turbines. (Author)
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Zervos, A. (ed.) (National Technical University of Athens (Greece)); Ehmann, H.; Helm, P. (WIP, Munich (Germany)) (eds.); 1111 p; ISBN 0 9521452 9 4; ; 1996; p. 1089-1092; 1996 European wind energy conference and exhibition; Goeteborg (Sweden); 20-24 May 1996; Available from H.S. Stephens and Associates, Pavenham Road, Felmersham, Bedford MK43 7EX, price pound 130.00
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Miscellaneous
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Conference
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S. Strauch; S. Dieterich; K.A. Aniol; J.R.M. Annand; O.K. Baker; W. Bertozzi; M. Boswell; E.J. Brash; Z. Chai; J.-P. Chen; M.E. Christy; E. Chudakov; A. Cochran; R. De Leo; R. Ent; M.B. Epstein; J.M. Finn; K.G. Fissum; T.A. Forest; S. Frullani; F. Garibaldi; A. Gasparian; O. Gayou; S. Gilad; R. Gilman; C. Glashausser; J. Gomez; V. Gorbenko; P.L.J. Gueye; J.O. Hansen; D.W. Higinbotham; B. Hu; C.E. Hyde-Wright; D.G. Ireland; C. Jackson; C.W. de Jager; X. Jiang; C. Jones; M.K. Jones; J.D. Kellie; J.J. Kelly; Cynthia E. Keppel; G. Kumbartzki; Michael Kuss; J.J. LeRose; K. Livingston; Nilanga Liyanage; R.W. Lourie; S. Malov; D.J. Margaziotis; D. Meekins; R. Michaels; J.H. Mitchell; S.K. Nanda; J. Nappa; C.F. Perdrisat; Vina A. Punjabi; R.D. Ransome; R. Roche; G. Rosner; M. Rvachev; R. Sabatie; A. Saha; A. Sarty; J.M. Udias; P.E. Ulmer; G.M. Urciuoli; J.F.J can den Brand; J.R. Vignote; D.P. Watts; L.B. Weinstein; K. Wijesooriya; B. Wojtsekhowski
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
AbstractAbstract
[en] We have measured the proton recoil polarization in the 4He(polarized-e, e-prime, p)3H reaction at Q2 = 0.5, 1.0, 1.6, and 2.6 (GeV/c)2. The measured ratio of polarization transfer coefficients differs from a fully relativistic calculation, favoring the inclusion of a predicted medium modification of the proton form factors based on a quark-meson coupling model. In contrast, the measured induced polarizations agree reasonably well with the fully relativistic calculation indicating that the treatment of final-state interactions is under control
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1 Nov 2002; 381 Kilobytes; DOE/ER--40150-2318; AC05-84ER40150; Available from PURL: https://www.osti.gov/servlets/purl/804051-ce3Rhe/native/; No Journal information given for this preprint
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M. Amarian; L. Auerbach; T. Averett; J. Berthot; P. Bertin; B. Bertozzi; T. Black; E. Brash; D. Brown; E. Burtin; J. Calarco; G. Cates; Z. Chai; J.P. Chen; Seon-ho Choi; E. Chudakov; E. Cisbani; C.W. de Jager; A. Deur; R. DiSalvo; S. Dieterich; P. Djawotho; M. Finn; K. Fissum; H. Fonvieille; S. Frullani; H. Gao; J. Gao; F. Garibaldi; A. Gasparian; S. Gilad; R. Gilman; A. Glamazdin; C. Glashausser; E. Goldberg; J. Gomez; V. Gorbenko; J.O. Hansen; B. Hersman; R. Holmes; G.M. Huber; E. Hughes; B. Humensky; S. Incerti; M. Iodice; S. Jensen; X. Jiang; C. Jones; G. Jones; M. Jones; C. Jutier; A. Ketikyan; I. Kominis; W. Korsch; K. Kramer; K. Kumar; G. Kumbartzki; M. Kuss; E. Lakuriqi; G. Laveissiere; J. Lerose; M. Liang; N. Liyanage; G. Lolos; S. Malov; J. Marroncle; K. McCormick; R. Mckeown; Z.E. Meziani; R. Michaels; J. Mitchell; Z. Papandreou; T. Pavlin; G.G. Petratos; D. Pripstein; D. Prout; R. Ransome; Y. Roblin; D. Rowntree; M. Rvachev; F. Sabatie; A. Saha; K. Slifer; P. Souder; T. Saito; S. Strauch; R. Suleiman; K. Takahashi; S. Teijiro; L. Todor; H. Tsubota; H. Ueno; G. Urciuoli; R. Van der Meer; P. Vernin; H. Voskanian; B. Wojtsekhowski; F. Xiong; W. Xu; J.C. Yang; B. Zhang; P. Zolnierczuk
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2004
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2004
AbstractAbstract
[en] We have measured the spin structure functions g1 and g2 of 3He in a double-spin experiment by inclusively scattering polarized electrons at energies ranging from 0.862 to 5.07 GeV off a polarized 3He target at a 15.5o scattering angle. Excitation energies covered the resonance and the onset of the deep inelastic regions. We have determined for the first time the Q2 evolution of Γ1(Q2)=/int01 g1(x,Q2) dx, Γ2(Q2)=/int01 g2(x,Q2) dx and d2 (Q2) = /int01 x 2[2g1(x,Q2) + 3g2(x,Q2)] dx for the neutron in the range 0.1 GeV2 /leq Q2 /leq 0.9 GeV2 with good precision. Γ1(Q2) displays a smooth variation from high to low Q2. The Burkhardt-Cottingham sum rule holds within uncertainties and d2 is non-zero over the measured range
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JLAB-PHY--03-21; DOE/ER--40150-2636; HEP-EX--0310003; AC--05-84ER40150
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Journal Article
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