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Optical orbital angular momentum of evanescent Bessel waves
Optics Express
|June 16, 2015
Summary
Orbital angular momentum (OAM) in evanescent light differs significantly from traveling light. Its paraxial component vanishes, and OAM per unit energy is reduced in evanescent Bessel waves.
Area of Science:
- Optics and Photonics
- Electromagnetism
- Wave Phenomena
Background:
- Orbital angular momentum (OAM) is a key property of light.
- Evanescent waves are near-field phenomena with unique characteristics.
- Understanding OAM in evanescent fields is crucial for near-field optics.
Purpose of the Study:
- To investigate and quantify the orbital angular momentum (OAM) of evanescent light.
- To compare the OAM characteristics of evanescent Bessel waves with traveling waves.
- To analyze the impact of the evanescent decay rate on OAM.
Main Methods:
- Theoretical analysis of evanescent Bessel waves.
- Calculation of OAM for evanescent fields.
- Comparison with established results for traveling light waves.
Main Results:
- The paraxial contribution to OAM vanishes in evanescent Bessel waves when averaged azimuthally.
- OAM per unit energy is reduced by a factor of (1+κ²/k²) for evanescent Bessel fields compared to traveling fields.
- The reduction factor depends on the wave number (k) and evanescent decay rate (κ).
Conclusions:
- Evanescent light possesses distinct OAM properties compared to traveling light.
- The vanishing paraxial OAM component and reduced OAM per unit energy are significant findings for evanescent fields.
- These results have implications for near-field optical manipulation and microscopy.
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