Browsing by Author "Thomas Schaefer, Committee Member"

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    Application of Perturbative and Lattice Techniques to the Analysis of Nuclear Matter.
    (2010-08-09) Thomson, Richard; Chueng Ji, Committee Chair; Albert Young, Committee Member; Dean Lee, Committee Member; Thomas Schaefer, Committee Member; Sarah Ash, Committee Member
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    The Spectrum and Decays of Scalar Mesons in the Light-Front Quark Model
    (2008-04-25) DeWitt, Martin Alan; Chueng Ji, Committee Chair; Thomas Schaefer, Committee Member; Dean Lee, Committee Member; Orlando Hankins, Committee Member
    We use the light-front quark model to investigate the structure of the scalar mesons, mainly focusing on the three heavy isoscalar states f0(1370), f0(1500), and f0(1710). We comput the spectrum of scalar mesons by diagonalizing a relativized, QCD-inspired model Hamiltonian written in a basis of 25 simple harmonic oscillator states. The masses are then used to perform a mixing analysis which assumes that the heavy isoscalars are mixtures of quarkonia and the scalar glueball. The resulting quark-glue content is used along with the meson wave functions determined from the spectrum to compute the decay rates to pairs of pseudoscalar mesons (two pions, two kaons, two eta mesons). We find that when the glueball contributions to the decays are ignored, the results are in poor agreement with the available data. However, when we estimate the effect of including the glueball contributions in the decays, a solution can be found that matches the data quite well. In this solution, the f0(1710) is mostly glueball (78%) while the f0(1500) and f0(1370) are mostly mixtures of quarkonia. Additionally, in this solution the glueball contributions to kaon and eta final states are significant, while the contributions to the pion final state is negligible. This finding is in agreement with Chanowitz who uses chiral perturbation theory to show that the amplitude for a scalar glueball to decay to a quark-antiquark pair is proportional to the quark mass. This results in a suppression of the pion decay channel compared to the kaon and eta decay channels.