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Further Results on Null and Force-free Electromagnetic Fields

Govind Menon, Rakshak Adhikari

Abstract

The theory of Force-Free Electrodynamics (FFE) provides a robust framework for modeling the magnetospheres of compact objects, where the electromagnetic field's energy density dominates the surrounding plasma. Central to this theory is the existence of two-dimensional integral submanifolds, or field sheets, which foliate the spacetime. While it is established that every null force-free field possesses an associated 2-D null geodesic foliation, the converse, identifying which null geodesic congruences can support a force-free solution, remains a non-trivial computational challenge. In this paper, we extend the foliation-based approach to null FFE by addressing two primary obstacles to the existence of a solution: the equipartition of null mean curvature and the involutivity of the field sheet distribution. We prove a general existence theorem demonstrating that for any given null geodesic congruence, there always exists a local rotation of a 2-D basis transverse to the geodesic congruence that satisfies the equipartition condition. Furthermore, we establish that a shear-free null geodesic congruence is sufficient to guaranty the existence of an arbitrary function of three variables such that any choice of such a function will generate a null field sheet foliation. Additionally, each unique foliation will be associated with a null force-free field that further contains an arbitrary function of two variables. These results are formally linked to the vanishing of the shear tensor, providing a coordinate-independent geometric criterion for the existence of null FFE solutions. We illustrate these theorems with explicit examples in Schwarzschild and Kerr geometries and present new, non-trivial exact null solutions in flat spacetime and for the C-metric.

Further Results on Null and Force-free Electromagnetic Fields

Abstract

The theory of Force-Free Electrodynamics (FFE) provides a robust framework for modeling the magnetospheres of compact objects, where the electromagnetic field's energy density dominates the surrounding plasma. Central to this theory is the existence of two-dimensional integral submanifolds, or field sheets, which foliate the spacetime. While it is established that every null force-free field possesses an associated 2-D null geodesic foliation, the converse, identifying which null geodesic congruences can support a force-free solution, remains a non-trivial computational challenge. In this paper, we extend the foliation-based approach to null FFE by addressing two primary obstacles to the existence of a solution: the equipartition of null mean curvature and the involutivity of the field sheet distribution. We prove a general existence theorem demonstrating that for any given null geodesic congruence, there always exists a local rotation of a 2-D basis transverse to the geodesic congruence that satisfies the equipartition condition. Furthermore, we establish that a shear-free null geodesic congruence is sufficient to guaranty the existence of an arbitrary function of three variables such that any choice of such a function will generate a null field sheet foliation. Additionally, each unique foliation will be associated with a null force-free field that further contains an arbitrary function of two variables. These results are formally linked to the vanishing of the shear tensor, providing a coordinate-independent geometric criterion for the existence of null FFE solutions. We illustrate these theorems with explicit examples in Schwarzschild and Kerr geometries and present new, non-trivial exact null solutions in flat spacetime and for the C-metric.
Paper Structure (8 sections, 9 theorems, 89 equations, 2 figures)

This paper contains 8 sections, 9 theorems, 89 equations, 2 figures.

Key Result

Theorem 1

Let ${\cal F}_{2,N}$ be a null foliation of a fixed, electrically neutral background spacetime ${\cal M}$, and let $(s, l, \alpha, n)$ be a null foliation adapted frame for ${\cal F}_{2,N}$. Then there exists a class of null force fields $F$ of the form if and only if ${\cal F}_{2,N}$ admits an equipartition of null mean curvature. Here $\kappa$ is given by the expression where Here $(x^1, \dot

Figures (2)

  • Figure 1: Null foliation generating a force-free field
  • Figure 2: Flowchart summarizing the geometric construction of null force-free electromagnetic fields from a prescribed null geodesic congruence. The procedure proceeds through shear check, frame rotation for equipartition, involutivity verification, and solution generation.

Theorems & Definitions (14)

  • Definition 1
  • Definition 2
  • Definition 3
  • Theorem 1
  • Definition 4
  • Corollary 1
  • Definition 5
  • Theorem 2
  • Theorem 3
  • Theorem 4
  • ...and 4 more