Related Experiment Video
Updated: Jun 6, 2025

12:14
The Generation of Higher-order Laguerre-Gauss Optical Beams for High-precision Interferometry
Published on: August 12, 2013
21.7K
Gauge-flux-controlled orbital angular momentum mode conversion in silicon waveguides
Optics Letters
|November 27, 2024
Summary
We introduce a novel method to convert fundamental modes into orbital angular momentum (OAM) modes using chiral dynamics in silicon waveguides. This technique optimizes OAM mode conversion efficiency and enables on-chip OAM (de)multiplexing.
Area of Science:
- Photonics
- Integrated Optics
- Waveguide Technology
Background:
- Orbital Angular Momentum (OAM) modes offer unique properties for optical communications.
- Efficient on-chip generation and manipulation of OAM modes remain a challenge.
- Existing methods often require complex structures or are limited in efficiency.
Purpose of the Study:
- To propose a new method for converting fundamental modes into OAM modes using chiral dynamics.
- To demonstrate efficient OAM mode generation and control in silicon waveguides.
- To develop an on-chip OAM mode (de)multiplexer.
Main Methods:
- Integrating a trench into a few-mode silicon waveguide to induce chiral dynamics.
- Utilizing generated gauge fluxes for controlled rotation of TE modes (TE10 and TE01).
- Precisely controlling gauge flux to optimize OAM mode conversion efficiency.
Main Results:
- Successful conversion of fundamental modes to OAM modes with high efficiency.
- Demonstration of flux-controlled chiral dynamics for optimized OAM mode generation.
- Development of an on-chip OAM mode (de)multiplexer based on the proposed method.
- Overcoming challenges related to mode degeneracy through controlled gauge flux.
Conclusions:
- The proposed method offers a novel strategy for creating artificial gauge fluxes in straight waveguides.
- This approach enables efficient manipulation of OAM modes on photonic chips.
- The findings open new possibilities for advanced optical communication systems and integrated photonic devices.
Related Concept Videos
Conservation of Angular Momentum: Application
10.8K
A system's total angular momentum remains constant if the net external torque acting on the system is zero. Examples of such systems include a freely spinning bicycle tire that slows over time due to torque arising from friction, or the slowing of Earth's rotation over millions of years due to frictional forces exerted on tidal deformations. However in the absence of a net external torque, the angular momentum remains conserved. The conservation of angular momentum principle requires a...
10.8K
Biasing of Metal-Semiconductor Junctions
215
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
215
Conservation of Angular Momentum
10.2K
A system's total angular momentum remains constant if the net external torque acting on the system is zero. Considering a system that consists of n tiny particles, the angular momentum of any tiny particle may change, but the system's total angular momentum would remain constant. The principle of conservation of angular momentum only considers the net external torque acting on the system. While there are internal forces exerted by different particles within the system that also produce...
10.2K
MOSFET: Enhancement Mode
294
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
294
Angular Momentum about an Arbitrary Axis
193
Imagine a rigid body with a mass denoted as 'm', which has its center of mass at point G and is rotating around an inertial reference frame. The angular momentum at an arbitrary point P can be calculated by taking the cross product of the position vector and linear momentum vector for each individual mass element.
The velocity of a mass element comprises its translational velocity and the relative velocity instigated by the body's rotation. Substituting the velocity equation into...
The velocity of a mass element comprises its translational velocity and the relative velocity instigated by the body's rotation. Substituting the velocity equation into...
193
Angular Momentum: Single Particle
6.1K
Angular momentum is directed perpendicular to the plane of the rotation, and its magnitude depends on the choice of the origin. The perpendicular vector joining the linear momentum vector of an object to the origin is called the “lever arm.” If the lever arm and linear momentum are collinear, then the magnitude of the angular momentum is zero. Therefore, in this case, the object rotates about the origin such that it lies on the rim of the circumference defined by the lever arm...
6.1K

