Abstract
Abstract
We study the collisions of elastic superconducting strings, also referred to as
current-carrying strings, formed in a U
local(1) × U
global(1) field-theory
model, using three-dimensional numerical field-theoretic simulations. The breaking of U
local
(1) leads to string formation via the Higgs mechanism, while the scalar field of the
second U
global(1) carries the current, which condenses onto the string. We construct
straight and static superconducting string solutions numerically and identify the regions in which
they exist in the model parameter space. We then perform dynamical simulations for colliding
superconducting strings with various collision angles and collision velocities. We explore the
kinematic parameter space for six sets of model parameters characterising the coupling between the
two scalar fields and the current on the string. The final states of the strings (after the
collision) are reported diagrammatically. We classify them into four categories: (i) regular
intercommutation, (ii) double intercommutation, (iii) bound state, and (iv) expanding string
solution. We find that the outcome of the collision process is the regular intercommutation of the
colliding strings in most of the kinematic parameter space while they form bound states for small
velocities and small angles. We also find that the strings undergo two successive
intercommutations and, therefore, pass through one other in a small region corresponding to
relatively small angles and velocities of order c/2. The string structure breaks down when there
is a relatively large coupling between the two scalar fields, even if each string is stable before
the occurrence of the collision.
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