A Classic Thesis Style - Johannes Gutenberg-Universität Mainz

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144 bibliography [98] S. Nozawa and T. S. H. Lee. Electroproduction of pions on the nucleon (ii). polarization observables. Nuclear Physics A, 513:543–556, 1990. [99] V. Dmitrasinovic and F. Gross. Polarization observables in deuteron photodisintegration and electrodisintegration. Phys. Rev. C, 40(6), 1989. [100] N. Dombey. Hadronic interactions of electrons and photons. In J. Cumming, editor, Proceedings of the eleventh session of the scottish universities summer school in Physics,1970, pages 17,45, Glasgow, 1970. Academic Press London and New York.
L I S T O F F I G U R E S Figure 1 Predicted resonances 5 Figure 2 The electron scattering and hadronic reaction planes in the lab frame 9 Figure 3 Born and extended born terms 12 Figure 4 Resonant contributions 13 Figure 5 Contributions of the different resonances to the total cross-section 17 Figure 6 photon 19 Figure 7 Old data 20 Figure 8 DESY spectrometers 21 Figure 9 Saphir data 22 Figure 10 Rastered beam profile in calibration screen 26 Figure 11 Plan of accelerator facilities and experimental halls 27 Figure 12 Cryo target scheme 28 Figure 13 Experimental hall of the A1 collaboration 30 Figure 14 Detectors equipping KAOS spectrometer 31 Figure 15 Elastically scattered electrons of 450 MeV energy, back-traced from the detector system of the Kaos spectrometer to the target. 34 Figure 16 Electrodes and electric field configuration of MWPC 35 Figure 17 Efficiency MWPC 36 Figure 18 Scheme of scintillator walls electronics 37 Figure 19 Calibration ADC spectrum of a sample paddle 38 Figure 20 Absorption fits for F 39 Figure 21 FG trigger 40 Figure 22 Photographs of first (left) and second generation (right) FPGA logic modules: VULOM and VUPROM used in the tracking trigger for the positive-arm of the Kaos spectrometer. Both VME modules were equipped withs VIRTEX-4 FPGA chips and flash memory. Different trigger programs could be loaded into the FPGA via a JTAG connector or directly by means of the VME interface. VUPROM allowed a larger number of channels to be handled by the same module (256 I/O channels) by means of high density connectors. 42 Figure 23 KAOS-scheme 43 145
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M E A S U R E M E N T O F T H E U N
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A B S T R A C T The new stage of th
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C O N T E N T S i kaon electroprodu
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Part I K A O N E L E C T R O P R O
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4 introduction Lorentz invariance.
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6 introduction appear in the K + Λ
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8 introduction there was almost no
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10 introduction This allows us to w
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12 introduction K ¡p γ ∗ Λ(Σ
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14 introduction means of the isobar
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16 introduction amount of resonance
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18 introduction photo and electropr
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20 introduction 1.6 previous experi
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22 introduction Figure 9: Total cro
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E X P E R I M E N TA L S E T U P A
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2.3 target 27 Figure 11: Schematic
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2.4 kaos spectrometer 2.4 kaos spec
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M MWPC L F 2.4 kaos spectrometer 31
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Table 3: Spectrometers properties 2
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2.4 kaos spectrometer 35 Figure 16:
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2.4.5.1 Read out electronics 2.4 ka
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2.4 kaos spectrometer 39 channels.
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2.5 kaos single arm trigger 41 64MB
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2.6 spectrometer b 43 Figure 23: Sc
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2.7 coincidence setting 45 to be im
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2.8 data acquisition and analysis s
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2.9 kinematical setting 49 (GeV/c)
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52 detection efficiencies and data
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C O N C L U S I O N S The effort to
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cm [nb/sr] dσ v / dΩ K 1500 1000
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cm [nb/sr] dσ / dΩ K 500 400 300
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Part II F E A S I B I L I T Y S T U
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90 conclusions Figure 55: Emission
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92 prototyping and efficiency measu
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Page 148 and 149: 138 bibliography [16] J. C. David,
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Page 152 and 153: 142 bibliography [71] P. Achenbach
Page 156 and 157: 146 bibliography Figure 24 Spek B d
Page 158 and 159: Figure 73 Annealing at 80° of the
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