
A set of exactly computable orthonormal basis functions that are useful in computations involving constituent quarks is presented. These basis functions are distinguished by the property that they fall off algebraically in momentum space and can be exactly Fourier-Bessel transformed. The configuration space functions are associated Laguerre polynomials multiplied by an exponential weight, and their Fourier-Bessel transforms can be expressed in terms of Jacobi polynomials in $��^2/(k^2 + ��^2)$. A simple model of a meson containing a confined quark-antiquark pair shows that this basis is much better at describing the high-momentum properties of the wave function than the harmonic-oscillator basis.
12 pages LaTeX/revtex, plus 2 postscript figures
wave function, Nuclear Theory, harmonic-oscillator basis, Completeness of eigenfunctions and eigenfunction expansions in context of PDEs, Nuclear physics, FOS: Physical sciences, quarks, Nuclear Theory (nucl-th), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Applications to the sciences, nuclear physics, Other elementary particle theory in quantum theory, particle physics, eigenfunction expansions, Fourier-Bessel transforms, PDEs in connection with quantum mechanics, orthonormal basis functions, quark-antiquark pair
wave function, Nuclear Theory, harmonic-oscillator basis, Completeness of eigenfunctions and eigenfunction expansions in context of PDEs, Nuclear physics, FOS: Physical sciences, quarks, Nuclear Theory (nucl-th), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Applications to the sciences, nuclear physics, Other elementary particle theory in quantum theory, particle physics, eigenfunction expansions, Fourier-Bessel transforms, PDEs in connection with quantum mechanics, orthonormal basis functions, quark-antiquark pair
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