Jamila Douari
TITLE: Unified Particles Algebra and Non-Commutative Geometry
ABSTRACT: The non-commutative geometry is redefined by referring to statistical
properties of our space. We consider an excitation operator on two-dimensional
space. Thus excited annihilation and creation operators are defined and an
excited particles algebra is given as unified symmetry of bosonic, fermionic and
anyonic algebras, depending on the kind of statistics of the space in
consideration. If the dimension of space d is greater than or equal to 3, and
the statistical parameter \nu=0,1, we refind the bosonic and fermionc algebras
respectively. For d=2, the unified algebra is the anyonic one, and it is
constructed by considering an excitation applied to ordinary particles living in
non-commutative 2-dimensional space. Then, the Heisenberg algebra is extended by
a polynomial in some disorder operator denoted K_i and deformed in terms of the
statistical parameter. By using the excited particles operators we realize a
deformed \omega_\infty-algebra depending on the statistical parameter that we
call in this work Excited Particles \omega_\infty-algebra. The Hamiltonian is
given as a deformed "free particles" Hamiltonian extended by some statistical
term.
References:
-A. H. Chamseddine and J. Fr\"ohlich, "Some elements of noncommutative
space-time
-A. Connes, M. R. Douglas and A. Schwarz, IHEP 9802 (1998) 003; M. R. Douglas
and C. Hull, JHEP 9802 (1998) 008; Y. K. E. Cheung and M. Krogh, Nucl. Phys.
B528 (1999) 185; C. -S. Chu and P. -M. Ho, Nucl. Phys. B528 (1999) 151.
-H. S. Snyder, Phys. Rev. 71 (1947) 38; Phys. Rev. 72 (1947) 68.
-A. Junussis, J. Phys. A26 (1982) L233; C. Quesne, N. Vansteenkiste, J. Phys.
A28 (1995) 7019; Helv. Phys. Acta 69 (1996) 141.
-J. M. Leinaas and J. Myrheim, Nuovo Cimento B37 (1977) 1.
-F. Wilczek, phys. rev. Lett. 48 (1982) 1144; 49 (1982) 957.