The solar wind interaction with Earth's intrinsic geomagnetic field creates a complex, highly dynamic geospace boundary layer consisting of the bow shock, the magnetosheath, the magnetopause, and the inner magnetosphere. Within the magnetosheath---the turbulent transition region between the supersonic bow shock and the magnetic cavity of the magnetopause---high-speed dynamic pressure pulses, commonly termed magnetosheath jets, frequently emerge.
These jets are characterized by kinetic energy densities several times larger than the ambient solar wind background and spatial scales spanning 0.5 to 2.0 Earth radii (RE ≈ 6,371 km). When traversing the sheath and colliding with the subsolar or high-latitude magnetopause, jets exert localized boundary forces that indent the magnetospheric shield, generate surface waves, trigger local magnetic reconnection, and excite field-aligned current (FAC) systems.
In the global hybrid framework, ions (protons) are treated as discrete kinetic superparticles governed by the relativistic Lorentz force equations:
$$\frac{d\mathbf{x}_i}{dt} = \mathbf{v}_i, \quad m_i \frac{d\mathbf{v}_i}{dt} = q_i \left( \mathbf{E} + \mathbf{v}_i \times \mathbf{B} \right)$$while electrons are modeled as a massless, charge-neutralizing fluid:
$$n_e \approx n_i, \quad \mathbf{E} = -\mathbf{V}_i \times \mathbf{B} + \frac{\mathbf{J} \times \mathbf{B}}{e n_e} - \frac{\nabla P_e}{e n_e} - \eta \mathbf{J}$$where J is the total current density, Pe is the electron scalar pressure, and η represents kinetic wave-particle resistivity.
In the baseline equilibrium state, the subsolar magnetopause standoff distance r0 follows the empirical Shue et al. (1998) model with r0 ≈ 9.8 RE and flaring exponent α = 0.56. Upon the arrival of the magnetosheath jet at t ≈ 60 s, the dynamic pressure surges from the ambient level of Pdyn ≈ 1.85 nPa to a peak of Pdyn ≈ 8.30 nPa, driving a localized inward boundary indentation of ΔX ≈ 1.8 RE.
The localized impact establishes steep pressure gradients and intense flow vorticity ω = ∇ × Vi. The resulting Field-Aligned Current density is evaluated as:
$$J_\parallel = \frac{\mathbf{J} \cdot \mathbf{B}}{\|\mathbf{B}\|} = \frac{(\nabla \times \mathbf{B}) \cdot \mathbf{B}}{\mu_0 \|\mathbf{B}\|}$$The boundary shear excites a distinct bipolar Birkeland current pair:
As the virtual MMS-1 probe traverses the dayside magnetosheath boundary (X ≈ 11.2 RE, Y ≈ 1.8 RE, Z ≈ 0.9 RE), it records:
The global hybrid simulation dataset analyzed in this study is publicly accessible via the Science Data Bank at DOI: 10.57760/sciencedb.space.03597. The complete interactive 4D visualization platform, Python analysis pipeline, and manuscript source files are openly deposited under the MIT and CC-BY-4.0 licenses on GitHub (https://github.com/dr-richard-barker/earth-magnetosphere-4d-viz) and archived with full FAIR compliance on Zenodo.