68 research outputs found
Massive twistor particle with spin generated by Souriau-Wess-Zumino term and its quantization
We present new model of D=4 relativistic massive particle with spin and we
describe its quantization. The model is obtained by an extension of standard
relativistic phase space description of massive spinless particle by adding new
topological Souriau-Wess-Zumino term which depends on spin fourvector variable.
We describe equivalently our model as given by the free two-twistor action with
suitable constraints. An important tool in our derivation is the spin-dependent
twistor shift, which modifies standard Penrose incidence relations. The
quantization of the model provides the wave function with correct mass and spin
eigenvalues.Comment: 1+15 page
Multiparticle mechanics with superconformal symmetry
We present a new multiparticle model of mechanics with
superconformal symmetry. The system is constructed in terms of two
matrix multiplets. One of them is a bosonic matrix multiplet and another is a fermionic one.
Off-diagonal bosonic components of the multiplet are chosen
to take values in the flag manifold and they
carry additional gauge symmetries. The explicit form of the
supersymmetry generators is found. We demonstrate that the superalgebra
constructed contains as subalgebras two different
superalgebras intersecting over the common
subalgebra.Comment: 1 + 23 pages, v2: minor corrections, new references and
acknowledgements adde
Extension of the Shirafuji model for Massive Particles with Spin
We extend the Shirafuji model for massless particles with primary spacetime
coordinates and composite four-momenta to a model for massive particles with
spin and electric charge. The primary variables in the model are the spacetime
four-vector, four scalars describing spin and charge degrees of freedom as well
as a pair of Weyl spinors. The geometric description proposed in this paper
provides an intermediate step between the free purely twistorial model in
two-twistor space in which both spacetime and four-momenta vectors are
composite, and the standard particle model, where both spacetime and
four-momenta vectors are elementary. We quantize the model and find explicitly
the first-quantized wavefunctions describing relativistic particles with mass,
spin and electric charge. The spacetime coordinates in the model are not
commutative; this leads to a wavefunction that depends only on one covariant
projection of the spacetime four-vector (covariantized time coordinate)
defining plane wave solutions.Comment: Latex, 27 pages, appendix.sty, newlfont.sty (attached
From Galilean superparticle to three-dimensional non-relativistic superfields
We consider the general Galilean superalgebra
with arbitrary central charges and study its dynamical realizations. Using the
nonlinear realization techniques, we introduce a class of actions for
three-dimensional non-relativistic superparticle, such that
they are linear in the central charge Maurer-Cartan one-forms. As a
prerequisite to the quantization, we analyze the phase space constraints
structure of our model for various choices of the central charges. The first
class constraints generate gauge transformations, involving fermionic
-gauge transformations. The quantization of the model gives rise to the
collection of free , Galilean superfields, which
can be further employed, e.g., for description of three-dimensional
non-relativistic supersymmetric theories.Comment: 1 + 39 pages; v2: minor corrections in few formulas and many language
corrections without any impact on the results; one reference and two
footnotes adde
OSp(4|2) Superconformal Mechanics
A new superconformal mechanics with OSp(4|2) symmetry is obtained by gauging
the U(1) isometry of a superfield model. It is the one-particle case of the new
N=4 super Calogero model recently proposed in arXiv:0812.4276 [hep-th].
Classical and quantum generators of the osp(4|2) superalgebra are constructed
on physical states. As opposed to other realizations of N=4 superconformal
algebras, all supertranslation generators are linear in the odd variables,
similarly to the N=2 case. The bosonic sector of the component action is
standard one-particle (dilatonic) conformal mechanics accompanied by an
SU(2)/U(1) Wess-Zumino term, which gives rise to a fuzzy sphere upon
quantization. The strength of the conformal potential is quantized.Comment: 1+20 pages, v2: typos fixed, for publication in JHE
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