Related Experiment Video
Updated: Feb 20, 2026

11:47
A 100 KW Class Applied-field Magnetoplasmadynamic Thruster
Published on: December 22, 2018
9.7K
On-axis energy backflow in the focal fields of vector vortex beams with arbitrary initial phase
Optics Express
|February 18, 2026
Summary
Energy backflow in light beams is independent of initial phase. A condition involving polarization order (l) and phase topological charge (m) dictates its occurrence, enabling new light field control methods.
Area of Science:
- Optics and Photonics
- Electromagnetism
- Light Field Manipulation
Background:
- Energy backflow is a counterintuitive phenomenon observed in the focal region of light beams with singularities.
- Previous studies explored vector vortex beams with both polarization and phase singularities, but the role of initial phase was unclear.
Purpose of the Study:
- To theoretically prove and numerically demonstrate the independence of the longitudinal Poynting vector from the initial phase of light beams.
- To reveal the general conditions for on-axis energy backflow near the focus of light beams with arbitrary initial phases.
- To explore methods for achieving strong longitudinal electric fields on the optical axis.
Main Methods:
- Theoretical analysis of the Poynting vector in the focal plane.
- Numerical simulations to demonstrate energy backflow phenomena.
- Investigation of conditions relating polarization order (l) and phase topological charge (m).
Main Results:
- The longitudinal component of the Poynting vector is independent of the incident light beam's initial phase.
- On-axis energy backflow occurs when polarization order (l) and phase topological charge (m) satisfy l ± m = 2.
- Exceptional cases (l=1, m=±1) allow energy backflow by amplitude modulation; a method for strong longitudinal electric fields is proposed.
Conclusions:
- The initial phase of light beams does not influence on-axis energy backflow.
- A specific relationship between polarization and phase singularities (l ± m = 2) is the key condition for energy backflow.
- These findings provide new tools for controlling light fields and energy flow distributions in optical focal regions.
Related Concept Videos
Intensity Of Electromagnetic Waves
6.0K
The energy transport per unit area per unit time, or the Poynting vector, gives the energy flux of an electromagnetic wave at any specific time. For a plane electromagnetic wave with E0 and B0 as the peak electric and magnetic fields and traveling along the x-axis, the time-varying energy flux can be given by the following equation:
6.0K
Energy In A Magnetic Field
2.8K
If a magnetic field is sustained, there must be a current in a closed circuit or loop, implying some energy has been spent in creating the field. If this energy is not dissipated via the circuit's resistance, it is stored in the field.
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
Take an ideal inductor with zero resistance. Although it's practically impossible, assume that the coil's resistance is so small that it is practically negligible. The loss of the field's energy to dissipate thermal energy (or heat) is thus...
2.8K
Plane Electromagnetic Waves I
5.1K
The existence of combined electric and magnetic fields that propagate through space as electromagnetic (EM) waves is the most significant prediction of Maxwell's equations. As Maxwell's equations hold in free space, the predicted electromagnetic waves do not require a medium for their propagation. An EM wave comprises an electric field, defined as the force per charge on a stationary charge, and a magnetic field, which is the force per charge on a moving charge.
The EM field is assumed to be a...
The EM field is assumed to be a...
5.1K
Plane Electromagnetic Waves II
4.2K
Consider a plane wavefront traveling in position x-direction with a constant speed. This wavefront can be utilized to obtain the relationship between electric and magnetic fields with the help of Faraday's law.
4.2K
Magnetic Vector Potential
1.6K
In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
1.6K
Torque On A Current Loop In A Magnetic Field
6.0K
The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...
6.0K

