participants
Stanford, C 010430
Excerpt: ... Participants Fabio Anulli Instituto Nazionale di Fisica Nucleare Laboratori Nazionali di Frascati David Aston Stanford Linear Accelerator Center Virginia Azzolini Universit degli studi di Ferrara Rinaldo Baldini Instituto Nazionale di Fisica Nucleare Laboratori Nazionali di Frascati Wander Baldini Instituto Nazionale di Fisica Nucleare Universit degli studi di Ferrara Teresa Barillari University of Colorado Diego Bettoni Instituto Nazionale di Fisica Nucleare Universit degli studi di Ferrara M.E. Biagini Instituto Nazionale di Fisica Nucleare Laboratori Nazionali di Frascati Vittorio Bidoli Instituto Nazionale di Fisica Nucleare Universit degli studi di Roma Gerard Bonneaud Ecole Polytechnique Peter Bosted University of Massachusetts Tullio Bressani Universit degli studi di Torino Stanley Brodsky Stanford Linear Accelerator Center Roberto Calabrese Instituto Nazionale di Fisica Nucleare Universit degli studi di Ferrara Carl Carlson College of William and Mary Gianluigi Cibinetto Universit degli studi ...
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slac-pub-0255
Stanford, PUBS 0250
Excerpt: ... SLAC-PUB-255 January 196 7 SYSTEMS FOR THE HUMMINGBIRD AT SIX* C . Dickens Stanford Linear Accelerator Stanford University Stanford, California Center (Presented at the International Planck Institute, Munich, Conference on Flying Spot Devices at the Max January 18 - 20, 1967) Germany, * Work supported by the U. S. Atomic Energy Commission. I. Late in 1965 a joint research Center, Palo Alto, California, INTRODUCTION effort between IBM's Scientific Research Center and the Stanford Linear Accelerator was begun. Included in this effort was an IBM 360/50 provided by the Scientific The Graphic Sttidy Group (hereinafter denoted GSG) conof SLAC as principal Research Center. sisting of both SLAC and IBM personnel with W. F. Miller investigator initiated several projects. to reach early fruition One of the projects incorporation was the building and subsequent I scanner. into tile IBM 360/50 system of the Hummingbird After looking at several scanning systems, as possible the following (1) (2) Ease ...
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Hastings
Cornell, WORKSHOP 2003
Excerpt: ... Linear Accelerator Based X-Ray Sources: Temporal and Spatial Coherence J. B. Hastings SSRL Stanford Linear Accelerator Center Accelerator based synchrotron radiation (SR) sources are now commonplace in the world with the USA (APS), Japan (Spring-8) and Europe (ESRF) each operating storage ring sources in the hard x-ray energy range that provide unique radiation for studies in the chemical, biological and materials sciences. These sources are critical to the understanding of complex static structures and through inelastic x-ray scattering the dynamics. They have also been applied to time resolved diffraction on the scale of the photon pulse length ~100 psec. Photon beams with all the properties of SR but with pulse lengths of ~100fsec are now available from linear accelerator based sources, for example the Sub-Picosecond Pulse Source (SPPS) at the Stanford Linear accelerator Center (SLAC). X-ray free electron lasers providing unprecedented pulse intensities, full transverse coherence, and pulse lengths of ~ 10 ...
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lecture
Stanford, C 020805
Excerpt: ... /ssi/2002/lect_program.html (1 of 2) [7/16/02 2:28:41 PM] Lecture Series 4:00 6:00 DISCUSSION IN ORANGE ROOM 6:00 DINNER Poster Session Light & Light Refreshments Light (3PM2AM) Refreshments & Soccer Refreshments Game LICK Observatory Tour DISCUSSION IN ORANGE ROOM Light Refreshments Poster Session & Light Refreshments . Contact: Maura Chatwell SSI 2002 Coordinator Stanford Linear Accelerator Center 2575 Sand Hill Road, MS#81 Menlo Park, CA 94025 USA Ph: (650) 926-4931 Fax: (650) 926-2525 Email: ssi@slac.stanford.edu http:/www-conf.slac.stanford.edu/ssi/2002/lect_program.html (2 of 2) [7/16/02 2:28:41 PM] ...
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slac-pub-10039
Stanford, PUBS 10000
Excerpt: ... SLAC-PUB-10039 KEK-PREPRINT-93-190 Submitted to the 6th Advancd ICFA Beam Dynamics Workshop, Funchal, Madeira, 24-30 Oct 1993. Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309, USA ...
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slac-pub-1807
Stanford, PUBS 1750
Excerpt: ... SLAC-PUB-1807 August 1976 (T/E) TRANSVERSE MOMENTUM INCLUSIVE LIMITATION IN ELECTROPRODUCTION PROCESSES* Namik K. Pak Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT We show that if the longitudinal statistically phase space is populated in a distribution), in an independent manner (Poisson-like fixed by the rapidity interval between the limits ticles, one being virtual of the leading par- photon, then the average transverse and this limit is momentum must be limited in the Bjorken limit, scale invariant. of particles a universal As a result we further show that the average density with In s) has (the rate of increase of average multiplicity upper bound independent of dynamical variables. (Submitted to Phys. Letters. ) *Work supported in part by the Energy Research and Development Administration. -2Recently there has been increasing lepton scattering theoretical [II interest in deep-inelastic processes in which one or more of the final hadron is de ...
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slac-pub-1993
Stanford, PUBS 1750
Excerpt: ... SLAC-PUB-1993 August 19 77 (T/E) SOME CONSEQUENCES OF A SCALE BREAKING MODEL IN ELECTRON AND NEUTRINO DEEP INELASTIC SCATTERING* A. Fernandez-Pachecot, J. A. Grifolst? and Ivan A. Schmidtttt Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT We analyze electron and neutrino deep inelastic processes, extending a simple parton model explanation of the approach to scaling observed in electroproduction experimental at large x. The model is successful in fitting the present effects from asymptotic freedom data without any explicit or new quarks. different This model has a large q2 behavior which is quite from that expected in asymptotic freedom (AF) theories and to data can be used to sharpen any experimental demon- comparisoas stration of AF effects. Of course, the model is consistent with AF and both effects could be present. (Submitted for publication. ) *Work supported in part by the Energy Research and Development Administration. TOn leave from Departam ...
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dahlstrom
Iowa State, REU 2001
Excerpt: ... Measuring Leptonic B Decays at BaBar Michael Dahlstrom Iowa State University REU Program August 3, 2001 Abstract Using data gathered from the BaBar experiment at the Stanford Linear Accelerator Center, I searched for B mesons that decay into two charged leptons, focusing on the dielectron, dimuon, and electron-muon decay channels. These decays are interesting because their branching fractions have only upper limits. Also, the existence of any electron-muon pair product, or e, would give strong support to several beyond the standard model theories. So far, the data is in agreement with the results from the CLEO and ARGUS collaborations. This analysis is still in progress, however, and this paper is merely a report on the preliminary details. Introduction 1.1 The BaBar Experiment The BaBar detector at Pep-II was designed to study B mesons produced in asymmetric electron-positron collisions. Asymmetric" refers to the fact that the colliding particles have different energies. This gives the resulting pa ...
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slac-pub-7330
Stanford, PUBS 7250
Excerpt: ... SLAC-PUB-7330 October 1996 Diffraction model of a step-out transition beam in planar geometry* F. Zimmerman and for a sheet A.W. Chao Stanford Linear Accelerator Center Stanford University, Stanford, California 94309 Using a diffraction model, we derive the longitudinal for a sheet impedance of a small step-out transition nar geometry. high-frequency beam in pla- Presented at the 1996 DPF/DPB Summer Study on New Directions for High-Energp Phgsics (Snowmass 96), Snowmass, Colorado, June 25- July 12, 1996 *Work supported by Department of Energy contract DE-AC03-76SFO0515. sLAc-Pm-7330 October 1996 Diffraction model of a step-out transition for a sheet beam in planar geomet~ 94300 F. Zimmerman and A. W. Chao Stanford Linear Accelerate< Stanford UniversiQ, Stanford, Cal#omia ABSTRACT Using a diffraction model, we derive the longitudinal highfrequency impedance of a small step-out transition for a sheet beam in planar geometry. III. Outlook 1. Sheet Beam and Planar Impedance Consider an infini ...
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slac-pub-1739
Stanford, PUBS 1500
Excerpt: ... SLAC-PUB-1739 April 1976 0) MODELFOR LOWENERGYKAON-NUCLEON INTERACTION IN THE I = 0 STATE* Pontiflcia Universidade S.C.B. Andrade Cato/lica, Rio de Janeiro, Brazil E. M. Ferreira Stanford Linear Accelerator Center Stanford University, Stanford, California and Pontifi<ia Universidade Catdlica, Rio de Janeiro, 94305 Brtizil (Contributed to the titernational Topical Conference on Meson Nuclear Carnegie-Mellon University, Pittsburgh, PA., May 24-28, 1976.) Physics, * Work supported by the Energy Research and Development Administration. MODEL FOR LOW ENERGY KAON-NUCLEON IN THE I = 0 STATE* CI INTERACTION S. C. B. Andrade and E. M, Ferreira* Pontiffcia Universidade Cat'olica, Rio de Janeiro, Brazil Unitary Pad6 approximants were recently used1 to build a model for the low energy kaon-nucleon interaction. The model is based on a Lagrangian 9 int = { -bzNAK Gy5AKf + &y5AKo) + h. c.} + ~-ig~K(-$5ZoK+&$5Zko C-K+)+h. c . } +h{ pp~`K'~n~K+~`K'+~p~oKo) (1) +iiy5~"Ko-$2iiy5 written in terms of nuc ...
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slac-pub-0966
Stanford, PUBS 0750
Excerpt: ... SLAC-PUB-966 WC) September 1971 RECIRCULATION OF THE SLAC BEAM* M. A. Allen, R. H. Helm, G. A. Loew, R. B. Neal and P. B. Wilson Stanford, California 94305 W. B. Herrmannsfeldt, Stanford Linear Accelerator Center, Stanford University, Abstract The intent of this proposal is to boost the energy of the SLAC beam into the 40 GeV range by recycling the electrons through the accelerator for a second pass. In order to use the normal klystron repetition rate (360 pps), the beam must be stored for the entire interpulse period (2.8 ms). Storage would be achieved in a 6.9 km-long path extending over the entire length of the accelerator housing. The direction of the beam would be reversed in magnet loops located at the ends of the accelerator. Beam energy losses due to synchrotron radiation would be made up by a room temperature linac operating at the accelerator frequency (2856 MHz). At the end of the storage interval, corresponding to about 122 revolutions, the beam would be reinjected into the accelerator to be a ...
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slac-pub-1089
Stanford, PUBS 1000
Excerpt: ... SLAC-PUB-1089 (TW August 1972 AXIAL VECTOR ANOMALIES AND THE SCALING PROPERTY OF FIELD THEORY* A. Zee The Rockefeller University New York, New York 10021 and Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT A proof of the Adler-Bardeen aid of the Callan-Symanzik theorem is given with the equation. (Submitted for publication. ) * Work supported in part by the U. S. Atomic Energy Commission. The recent realization basic informationI in this subject. normalized that the processes y - 3~ and 2y - 3n will provide anomaly2 has provoked new interest about the PCAC triangle If the anomaly is to provide a test of the relevance of the reseries to hadron physics, it is clearly essential that perturbation the value of the anomaly remains the same up to any finite order in perturbation n theory. Let us elaborate. RDpv (k, q) = i$d4x Consider a perturbative calculation of the amplitude d4y ei(kx+qy) <O ITaA(0) V;(x) Vz (Y) IO> (1) in any renormalizable ...
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Bozek_Abstract_SRC_UM2008
Wisconsin, UM 2008
Excerpt: ... Atomic and Molecular Science at the LCLS Free Electron Laser J. D. Bozek LCLS, Stanford Linear Accelerator Center, 2575 Sand Hill Rd., Menlo Park, CA 94025 The Linac Coherent Light Source (LCLS) at the Stanford Linear Accelerator Center (SLAC) is nearing completion with first light into the experimental areas anticipated in July 2009. The LCLS will be the first of several x-ray free electron lasers (xFELs) being built around the world to become operational. The LCLS will produce ultrafast (~100 fs) ultraintense (1012 1013 photons) pulses of radiation in the x-ray (1.5 15) range at a rate of 120 Hz. A suite of instruments is being built at SLAC to utilize this unique source of x-rays to study a wide variety of samples ranging from atoms to biological molecules and cells as well as solid materials. The first instrument scheduled to become operational at LCLS will be the Atomic, Molecular and Optical (AMO) science end-station which is designed to study the interaction of the intense LCLS ...
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iqa_filt_spec_1r3
Stanford, E 158
Excerpt: ... STANFORD LINEAR ACCELERATOR CENTER LC BANDPASS FILTER SPECIFICATION #1 Rev. 3 Center Frequency: 4.907 MHz +/-10 kHz, where 'center frequency' is the geometric mean of the upper 3dB frequency and the lower 3dB frequency. 3dB passband: 100 kHz minimum (see note below) 60dB passband: 1.00 MHz maximum (see note below) Insertion loss at center frequency: < 6dB Minimum return loss (S11) within the frequency band from 4.857 MHz to 4.957 MHz: > 15dB Impedance: 50 ohms Reliability: Will maintain specs at 0-70 deg. C operating temperature for more than 3 years. All components inside the filter are to be fixed value components, particularly, trimmer capacitors or variable resistors are not to be incorporated. RF shielding case must seal against standard P.C. board cleaning solvents. Package type: surface mount, to be same package as Bandpass Filter model: FN-2906 Filter shielding can ...
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iqa_filt_spec_2r3
Stanford, E 158
Excerpt: ... STANFORD LINEAR ACCELERATOR CENTER LC BANDPASS FILTER SPECIFICATION #2 Rev. 3 Center Frequency: 5.122 MHz +/-10 kHz, where 'center frequency' is the geometric mean of the upper 3dB frequency and the lower 3dB frequency. 3dB passband: 100 kHz minimum (see note below) 60dB passband: 1.00 MHz maximum (see note below) Insertion loss at center frequency: < 6dB Minimum return loss (S11) within the frequency band from 5.072 MHz to 5.172 MHz: > 15dB Impedance: 50 ohms Reliability: Will maintain specs at 0-70 deg. C operating temperature for more than 3 years. All components inside the filter are to be fixed value components, particularly, trimmer capacitors or variable resistors are not to be incorporated. RF shielding case must seal against standard P.C. board cleaning solvents. Package type: surface mount, to be same package as Bandpass Filter model: FN-2906 Filter shielding can ...
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2001-05-04-Arthur
Wisconsin, SRI 2001
Excerpt: ... Status of the LCLS X-Ray FEL Program John Arthur SSRL/SLAC, Stanford, CA 94309 USA The Linac Coherent Light Source (LCLS) program involves a collaboration of several US National Laboratories and universities with the goal of designing and building the first 4th-generation hard x-ray source, an x-ray free-electron laser (FEL). This FEL will utilize extremely short, intense, low-emittance electron pulses created by the high-energy linear accelerator at the Stanford Linear Accelerator Center. The FEL radiation produced will feature unprecedented peak brightness, short pulse length, and spatial coherence, tunable over an energy range of 0.8 - 8 keV. The LCLS program is now in the 3rd year of its initial R&D phase. With favorable funding, major construction will start in 2004 and the LCLS will be operating late in 2006. The LCLS facility will include experimental stations for carrying out groundbreaking experiments in several scientific fields, including atomic physics, plasma physics, chemistry, materials science ...
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slac-pub-1658
Stanford, PUBS 1500
Excerpt: ... I SLAC-PUB-1658 October 19 75 (T/E) MASSIVE PAIR PRODUCTION AND HADRONIC STRUCTURE" C. T. Sachrajdat and R. Blankenbecler Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT A brief review of the constituent theory of massive pair production for hadron, photon, and lepton beams is presented. to a physical description the classic Drell-Yan pairs from different of new production Emphasis is given mechanisms in addition to for hadron and lepton characterization of process, and to predictions A kinematic incident beams. the cross section arising from a general mechanism is given in terms of simple counting rules. ing the parameters regimes is stressed. The importance of experimentally in different determin- of the characterization kinematic A subtitle of this note could be "What to do with .your data when you don't find the D's. `I (Submitted to Nucl. Phys. B. ) *Work supported by the U. S. Energy Research and Development Administration. THarkness Fellow. ...
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slac-pub-1150
Stanford, PUBS 1000
Excerpt: ... &AC-PUB-1150 WC) November 19 72 BEAM FEEDBACK ELECTRONICS FOR THE SPEAR STORAGE RING* Jean-Louis Pellegrin Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT The two beams of the 2 GeV Stanford electron-positron ring can exhibit, under certain modes of operation, storage coherent oscil- lations which have a rate of growth proportional to the beam current. tiequency, Since this rate is much slower than the machine revolution it is possible to produce damping by means of negative feedback, the beam itself being part of the feedback loop. been built, two for the damping of transverse Three systems have oscillations at the oscilla- betatron frequency, and one for the damping of longitudinal frequency. The electronics tions at the synchrotron for these systems require wide band high power amplifiers and nanosecond circuitry. (Submitted to Nucl. Instr. and Methods. ) *Work supported by the U. S. Atomic Energy Commission. 2, Introduction The main parame ...
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slac-pub-0636
Stanford, PUBS 0500
Excerpt: ... SLAC -PUB-636 August 1969 (TH) and (EXP) RELATIONS BETWEEN CROSSING SYMMETRIC PROCESSES* E. A. Paschos Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT Relations between processes related by crossing are proposed as a test of (i) exchange degeneracy, (ii) dominance by trajectories of the same signature. Various possible experiments are discussed. * Work supported by the U.S. Atomic Energy Commission. The Regge analytic continuation of the u-channel amplitudes gives the high energy behavior for both the s- and t-channel processes in the neighborhood of u = 0. Therefore, both regions a r e mediated by the same Regge trajectories. For two general classes of exchanges the c r o s s sections of the two channels are identical in the high energy limit, except for known phase-space factors. We review here the argument that leads to these relations, and then discuss 1 processes which must obey them, a s well a s the kinematic regions where they are expected to hold. ...
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slac-pub-1867
Stanford, PUBS 1750
Excerpt: ... SLAC -PUB-l867 January 197 7 (T/E) BOUNDSTATESPECTROSCOPYOFSUPERHEAVYQUARKS" Amalio Fernandez-Pacheco? and J, A. Grifols$ Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT The transition to the exact positronium spectrum is studied as a potential function of quark mass. approach, It is shown that, in the nonrelativistic only for quarks as heavy as - 100 GeV might one expect to originally attributed to charmonium, It is also see the level structure noted that, in the hypothetical may directly case that superheavy quarks exist, one their 1+ bound states in produce, via the weak current, future e+e- experiments, (Submitted for publication) - *Supported in part by the Energy Research and Development Administration, -ton leave from Departamento de Fisica Nuclear, Universidad de Zaragoza, Spain, $On leave from Departamento de Fisica Teorica, Universidad Autonoma de Barcelona, Bellaterra, Spain. -2 By now it is clear that the very simple interpretation t ...
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slac-pub-0635
Stanford, PUBS 0500
Excerpt: ... SLAC- PUB- 635 July 1969 (TH) and (EXP) Photon-Photon Scattering Contribution to the Sixth Order Magnetic Moment of the Muon Janis Aldins t Laboratory of Nuclear Studies, Cornell University, Ithaca, New York Stanley J. Brodsky Stanford Linear Accelerator Center, Stanford University, Stanford, California Andrew J. Dufner Stanford Linear Accelerator Center, Stanford University, Stanford, California Toichiro Kinoshita Laboratory of Nuclear Studies, Cornell University, Ithaca, New York * ABSTRACT A calculation of the three photon exchange (electron loop) contribution to the sixth order anomalous magnetic moment of the muon is reported. The result, which contains a logarithmic dependence on the muon to electron mass ratio, brings the theoretical prediction into agreement with the CERN measurements, within the one standard deviation experimental accuracy. (Submitted to Physical Review Letters) q. Work supported in part by the U. S. Atomic Energy Commission and the U. S. Office of Naval Research. NDFA fellow. ...
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slac-pub-5588
Stanford, PUBS 5500
Excerpt: ... e in our theory, other CPT than a small number of bits used to insure charge conservation, invariance and the like; the "space-time simply structure" of these massless light cone) is, nec- quanta is represented by a string of l' (forward s light cone). Additional or a string of O' (backward s essarily, context dependent. structure This requires us to view the "Maxwell mathematically between the fields" as a simple way to interpolate motion theory of charges and currents meets Dombey' s in the sources and sinks. requirement, Thus our consistency and we can adopt limit" Feynman' s proof as providing a well-defined 5 "correspondence for a jnite and discrete relativistic equations. particle quantum mechanics in the classical Maxwell Details of our contention will be presented elsewhere. H. Pierre Noyesa Stanford Linear Accelerator Stanford Stanford, Center University 94309 California D Work supported by Department of Energy contract DE-AC03-76SF00515. 6 ` J. Dyson, Am. J. Phys. 58, ...
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slac-pub-0318
Stanford, PUBS 0250
Excerpt: ... s~c-~u~-318 June 1967 NEW JOINING TECHNIQUE FOR WATER-COOLED COPPER MAGNET COILS* Jack Gunnt Lawrence Radiation Laboratory University of California, Berkeley, California and Gerald Fritzke Stanford Linear Accelerator Center Stanford University, Stanford, California (Paper to be presented at the Second International Magnet Technology, Oxford, England, July 11-14, Conference on 1967) * Work supported by U. S. Atomic Energy Commission. J. `Formerly with Stanford Linear Accelerator Center, Stanford University, Stanford, California. New Joining Technique for Water-Cooled Magnet Coils The most widely used technique for joinin, r hollow copper magnet coil conductor is silver brazing. Although this is a highly-reliable technique, occasional water leaks have takes place and entire magnetoccurred at improperly-prepared joints. Short-circuiting coil assemblies have had to be removed for repair. The defect that occurs most frequently in silver-brazing is porosity in the joint. Thermal cycling of the coil ...
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slac-pub-1553
Stanford, PUBS 1500
Excerpt: ... THE PEP INJECTION SYSTEM+ K. L. Brown Stanford Linear Accelerator Center Stanford University, Stanford, California SLAC-PUB-1553 I=-3803 March 1975 94306 R. T. Avery, J. M. Peterson Lawrence Berkeley Laboratory Berkeley, California 94720 Smmary A system to transport lo-to-15-GeV electron and positron beams from the Stanford Linear Accelerator and to inject them into the PEP storage ring under a wide variety of lattice configurations has been designed. Optically, the transport line consists of three 360' phase-shift sections of FODO lattice, with bending magnets interspersed in such a way as to provide achromaticity, convenience in energy and emittance definition, and independent tuning of the various optical parameters for matching into the ring. The last 360' of phase shift has 88 milliradians of bend in a vertical plane and deposits the beam at the injection septum via a Lambertson magnet. Injection is accomplished by launching the beam with several centimeters of radial betatron amplitude in a fast bump ...
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slac-pub-1436
Stanford, PUBS 1250
Excerpt: ... . Rev. Letters 14, 670 (1965), and Phys. Rev. 143' 1269 (1966); K. J. Barnes, P. Carruthers, and F. von , Hippel, Phys.R.ev. Letters 14, 82 (1965). For a discussion of the constituent quark model states and the assignment of observed hadrons see F. J. Gilman in Experimental Meson Spectroscopy - 1972, AIP Conference Proceedings No. 8, edited by A.H. Rosenfeld and K.W. Lai (American Institute of Physics, New York, 1972); p. 460; R. H. Dalitz, invited paper presented at the Triangle Meeting on Low Energy Hadron Physics, Nov. 5-7, 1973 and Oxford preprint, 1974 (unpublished); J. L. Rosner, Phys. Reports (to be published) and Stanford Linear Accelerator Center Report No. SLAC-PUB-1391, 1974 (unpublished); M. Bowler, invited talk at this conference. Older work on current algebra renresentation mixing is reviewed bv H. Harari in Spectroscopic and Group Theoretical Methods in Physics (North Holland, Amsterdam, 1968), p. 363, particularly for baryons, and in F. J. Gilman and H. Harari, Phys. Rev. 165, 1863 (1968)for m ...
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