XV goals. We then discuss the baseline experimental facilities. Our baseline design is an accelerator of 500 GeV center-of-mass energy, with polarized e-beams, and with two interaction regions that share the luminosity. The design envisions a number of upgrade paths. These include low-energy precision measurements in one of the two regions and e+e-collisions at multi-TeV energies in the other. The logic of these plans is described in some detail. In the subsequent chapters, we discuss the possible options of positron polarization, operation of a yy collider by laser backscattering from electron beams, and operation for e-e-collisions. In each case, we review the promise and the technological problems of the approach.
The quasielastic (e,eЈp) reaction was studied on targets of deuterium, carbon, and iron up to a value of momentum transfer Q 2 of 8.1 (GeV/c) 2 . A nuclear transparency was determined by comparing the data to calculations in the plane-wave impulse approximation. The dependence of the nuclear transparency on Q 2 and the mass number A was investigated in a search for the onset of the color transparency phenomenon. We find no evidence for the onset of color transparency within our range of Q 2 . A fit to the world's nuclear transparency data reflects the energy dependence of the free-proton-nucleon cross section.
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Table S1: (ST1). PHREEQC inverse mixing modeling for the Mississippian Leadville Ls brine (Solution 3) assumed to be evolved from a mixture of the meteoric water endmember (Solution 1) and evaporated paleo-seawater endmember (Solution 2); Table S2: (ST2). PHREEQC inverse mixing modeling for the salt anticline brine (Solution 3) assumed to be evolved from a mixture of the meteoric water endmember (Solution 1) and evaporated paleo-seawater endmember (Solution 2).
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