We present general solutions to the equations of motion for a superconducting relativistic chiral string that satisfy the unit magnitude constraint in terms of products of rotations. From this result we show how to construct a general family of odd harmonic superconducting chiral loops. We further generalise the product of rotations to an arbitrary number of dimensions.PACS numbers: 11.27.+d,98.80.Cq
I. PRELIMINARIESParticle physics models where symmetry breaking is involved predict, in many cases, the existence of topological defects, which are formed when the topology of the vacuum manifold of the low energy theory is non-trivial [1]. Cosmic strings, in particular, are line-like objects that are formed when the the vacuum manifold contains unshrinkable loops. For a review see [2].In [3] it was shown that cosmic strings can be superconducting. In the case when the charge carriers on the string are not coupled to a gauge field the action for the string and the current can be taken to bewhere µ is the mass per unit length of the string, γ ab is the induced metric on the string worldsheet and φ is the field of the charge carriers living on the string. These strings were shown in [4] and [5] to have solutions in the case when γ ab φ ,a φ ,b = 0 of the formfor the string position andfor the field living on the string with the constraintsandwhere u = σ − τ and v = σ + τ and σ and τ are space-like and time-like parameters respectively that parametrise the string world-sheet. These strings are called chiral because the current only moves in one direction on the string.Comparing this to the usual Nambu-Goto case one can see that f (v) acts like a fourth component of the threevector b(v), making chiral superconducting strings behave like Nambu-Goto ones with chiral excitations in an extra fifth dimension. Indeed, this property was used in [6] in an investigation of the properties of superconducting cosmic string cusps.The right-and left-moving excitations, a ′ and b ′ , on a regular Nambu-Goto string in Minkowski space-time are arbitrary functions that satisfy the unit magnitude constraint, |a ′ | = |b ′ | = 1. Expressions for these functions are often given as Fourier sums and the unit magnitude constraint generally gives a non-linear set of equations involving the vector coefficients of the Fourier expansion. As a result, parametrising strings beyond the first few harmonics proves to be a difficult task. Fortunately, in that case, there exists a method to generate strings involving products of rotation matrices [7] that act on a starting unit vector so that the unit magnitude constraint is satisfied trivially.In a recent study of the properties of chiral cosmic strings [8] it was assumed that the current is constant. The work in [9] assumed that the current takes a very simple non-constant form. As was pointed out in the latter work one could expect to have loops with varying currents if the loops are formed by intersections involving different strings or if different segments of the loop or string were at some point i...