8 research outputs found
Spin Networks and Quantum Gravity
We introduce a new basis on the state space of non-perturbative quantum
gravity. The states of this basis are linearly independent, are well defined in
both the loop representation and the connection representation, and are labeled
by a generalization of Penrose's spin netoworks. The new basis fully reduces
the spinor identities (SU(2) Mandelstam identities) and simplifies calculations
in non-perturbative quantum gravity. In particular, it allows a simple
expression for the exact solutions of the Hamiltonian constraint
(Wheeler-DeWitt equation) that have been discovered in the loop representation.
Since the states in this basis diagnolize operators that represent the three
geometry of space, such as the area and volumes of arbitrary surfaces and
regions, these states provide a discrete picture of quantum geometry at the
Planck scale.Comment: 42 page
q-Quaternions and q-deformed su(2) instantons
We construct (anti)instanton solutions of a would-be q-deformed su(2)
Yang-Mills theory on the quantum Euclidean space R_q^4 [the SO_q(4)-covariant
noncommutative space] by reinterpreting the function algebra on the latter as a
q-quaternion bialgebra. Since the (anti)selfduality equations are covariant
under the quantum group of deformed rotations, translations and scale change,
by applying the latter we can generate new solutions from the one centered at
the origin and with unit size. We also construct multi-instanton solutions. As
they depend on noncommuting parameters playing the roles of `sizes' and
`coordinates of the centers' of the instantons, this indicates that the moduli
space of a complete theory will be a noncommutative manifold. Similarly, gauge
transformations should be allowed to depend on additional noncommutative
parameters.Comment: Latex file, 39 pages. Final version appeared in JM
Beauty photoproduction measured using decays into muons in dijet events in ep collisions at =318 GeV
The photoproduction of beauty quarks in events with two jets and a muon has
been measured with the ZEUS detector at HERA using an integrated luminosity of
110 pb. The fraction of jets containing b quarks was extracted from the
transverse momentum distribution of the muon relative to the closest jet.
Differential cross sections for beauty production as a function of the
transverse momentum and pseudorapidity of the muon, of the associated jet and
of , the fraction of the photon's momentum participating in
the hard process, are compared with MC models and QCD predictions made at
next-to-leading order. The latter give a good description of the data.Comment: 32 pages, 6 tables, 7 figures Table 6 and Figure 7 revised September
200
q - Difference Intertwining Operators for Uq(sl(4)) and q - Conformal Invariant Equations
Nonstandard Deformation U′ q (so n ): The Imbedding U′ q (so n ) ⊂ U q (sl n ) and Representations
κ - Deformed Poincaré Algebra and Some Physical Consequences
The κ-deformed D = 4 Poincaré algebra is obtained by a special contraction of the real quantum Lie algebra Uq(0(3, 2)). We describe this contraction and study the consequences of the κ-deformation of the relativistic energy formula for the kinematics of scalar massless and massive particules. The notion of κ-relativistic energy region is defined. The κ-deformed quantized Klein-Gordon scalar field is introduced
Measurement of the diffractive cross-section in deep inelastic scattering
Diffractive scattering of , where is either a
proton or a nucleonic system with ~GeV has been measured in deep
inelastic scattering (DIS) at HERA. The cross section was determined by a novel
method as a function of the c.m. energy between 60 and 245~GeV
and of the mass of the system up to 15~GeV at average values of
14 and 31~GeV. The diffractive cross section is,
within errors, found to rise linearly with . Parameterizing the
dependence by the form d\sigma^{diff}/dM_X \propto
(W^2)^{(2\overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}} -2)} the DIS data
yield for the pomeron trajectory
\overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}} = 1.23 \pm 0.02(stat) \pm
0.04 (syst) averaged over in the measured kinematic range assuming the
longitudinal photon contribution to be zero. This value for the pomeron
trajectory is substantially larger than
\overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}} extracted from soft
interactions. The value of \overline{\mbox{\alpha_{_{I\hspace{-0.2em}P}}}}
measured in this analysis suggests that a substantial part of the diffractive
DIS cross section originates from processes which can be described by
perturbative QCD. From the measured diffractive cross sections the diffractive
structure function of the proton F^{D(3)}_2(\beta,Q^2,
\mbox{x_{_{I\hspace{-0.2em}P}}}) has been determined, where is the
momentum fraction of the struck quark in the pomeron. The form F^{D(3)}_2 =
constant \cdot (1/ \mbox{x_{_{I\hspace{-0.2em}P}}})^a gives a good fit to
the data in all and intervals with $a = 1.46 \pm 0.04 (stat) \pmComment: 45 pages, including 16 figure