Kaon-LT Experiment » History » Version 31
  Richard Trotta, 07/16/2018 11:09 AM 
  
| 1 | 15 | Richard Trotta | h1. *Welcome to the Kaon-LT redmine page!* | 
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| 2 | 5 | Richard Trotta | |
| 3 | 27 | Richard Trotta | h2. Overview | 
| 4 | 26 | Richard Trotta | |
| 5 | 31 | Richard Trotta | The simplest strongly bound quark-gluon systems in nature are the two lightest quarkantiquark | 
| 6 | pairs, pions and kaons, and the two lightest three-quark systems, protons and neutrons | ||
| 7 | - these also provide the building blocks for the atomic nuclei at the core of the atom. Gaining a | ||
| 8 | quantitative description of the nature of these systems, including a revealing of their inner | ||
| 9 | structure and an understanding of the dynamics that bind them, is thus of great importance for | ||
| 10 | our understanding of the fundamental structure of matter. This experiment is aimed to confirm | ||
| 11 | the potential of kaon measurements both for studies of the kaon structure itself and of the 3D | ||
| 12 | structure of the proton, in terms of spatial imaging (tomography). In particular, E12-09-011 will | ||
| 13 | probe if the measurements to map the spatial extension of the charged pion can be extended to | ||
| 14 | those of the charged kaon, and if kaons can be utilized to enable 3D spatial tomography of | ||
| 15 | strange quarks. | ||
| 16 | The E12-09-011 experiment is an exclusive measurement of the L/T separated kaon | ||
| 17 | electroproduction cross section important for understanding the role of strangeness in GPD | ||
| 18 | studies and the kaon form factor. It will for the first time make precision measurements of the | ||
| 19 | L/T separated kaon electroproduction cross sections as a function of Q2 | ||
| 20 | above the resonance | ||
| 21 | region. These data will provide information about the onset of the Q2 evolution in kaon | ||
| 22 | production. A direct comparison of the scaling properties of the + and  separated cross | ||
| 23 | sections would provide an important tool for the study of the onset of factorization in the | ||
| 24 | transition from the hadronic to the partonic regime, and provide a possibility to study effects | ||
| 25 | related to SU(3). The L/T separated cross sections at low –t can further provide constraints of the | ||
| 26 | largely unknown kaon form factor. | ||
| 27 | 26 | Richard Trotta | |
| 28 | 1 | Richard Trotta | h2. Physics Motivation | 
| 29 | 30 | Richard Trotta | * "PAC Proposal":https://redmine.jlab.org/documents/37 | 
| 30 | 28 | Richard Trotta | |
| 31 | h2. Collaboration | ||
| 32 | 29 | Richard Trotta | * [[Spokespersons]] | 
| 33 | 28 | Richard Trotta | * [[Collaboration List]] | 
| 34 | * [[Mailing List]] | ||
| 35 | |||
| 36 | h2. Data Analysis | ||
| 37 | * "Hall C Logbook":https://logbooks.jlab.org/book/hclog | ||
| 38 | * "Kaon LT Logbook":https://logbooks.jlab.org/book/kaonlt | ||
| 39 | 26 | Richard Trotta | |
| 40 | 9 | Richard Trotta | h2. Wiki Pages | 
| 41 | 25 | Richard Trotta | {{child_pages(depth=2)}} |