Minhui Xiong’s research while affiliated with University of Electronic Science and Technology of China and other places

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Publications (3)


Figure 2: Electric field vector and singularity line at focus (t = 0). (a) Shows electric field vector and singularity at the focusing time (t = 0). (b)-(d) Shows the singularity lines and electric field vectors at the planes of z = 2q 1 , q 1 , 0, and the red and blue arrows indicate the direction of the electric field. In (a), the color matching of electric field vector is related to its azimuth í µí¼™ in the x-y plane, and the polar angle binds with brightness intensity, as shown in the illustration. The red and blue curves are respectively connected by the right-handed vortex core and the left-handed vortex core.
Figure 3: Electric field and singularity lines of helical pulses. (b) This figure presents the streamline plot of the electric field in the plane of the singular point and z = −70q 1 , −15q 1 , 30q 1 , 70q 1 at the instant when t = −15q 1 ∕c. (a) And (c) are enlarged local images of the red and green dashed rectangles in (b), respectively. The spiral structure maintains topological invariance. (c1-c4) Displays the electric field vector and modulus contour lines on z = 25q 1 , z = 30q 1 , z = 35q 1 and z = 40q 1 . In the image, the red curved arrow represents vortices, the blue curved arrow represents antivortices, the position of the green arrow indicates that vortices and antivortices are about to be generated or have already been annihilated, and the direction of the green arrow indicates the direction of the electric field vector. The orange dashed arrow indicates the direction of motion of the singularity. (c1-c4) Reveal the variation of the singular points with different planes.
Double-helix singularity and vortex–antivortex annihilation in space-time helical pulses
  • Article
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October 2024

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135 Reads

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1 Citation

Shuai Shi

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Minhui Xiong

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Topological structures reveal the hidden secrets and beauty in nature, such as the double helix in DNA, whilst, the manipulation of which in physical fields, especially in ultrafast structured light, draw booming attention. Here we introduce a new family of spatiotemporal light fields, i.e. helical pulses, carrying sophisticated double-helix singularities in its electromagnetic topological structures. The helical pulses were solved from Maxwell’s equation as chiral extensions of toroidal light pulses but with controlled angular momentum dependence. We unveil that the double helix singularities can maintain their topological invariance during propagation and the field exhibits paired generation and annihilation of vortices and antivortices in ultrafast space-time, so as to be potential information carriers beating previous conventional vortex structured light.

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Double-Helix Singularity and Vortex-Antivortex Annihilation in Space-Time Helical Pulses

September 2024

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45 Reads

Topological structures reveal the hidden secrets and beauty in nature, such as the double helix in DNA, whilst, the manipula-tion of which in physical fields, especially in ultrafast struc-tured light, draw booming attention. Here we introduce a new family of spatiotemporal light fields, i.e. helical pulses, carry-ing sophisticated double-helix singularities in its electromag-netic topological structures. The helical pulses were solved from Maxwell's equation as chiral extensions of toroidal light pulses but with controlled angular momentum dependence. We unveil that the double helix singularities can maintain their topological invariance during propagation and the field exhibits paired generation and annihilation of vortices and antivortices in ultrafast space-time, so as to be potential information carriers beating previous conventional vortex structured light.


Figure 1 Spatiotemporal structure of TE STNEV: The spatial isosurfaces of the magnetic field Re(Hz) at normalized amplitude levels of Re(Hz)=±0.1 and the Rayleigh range of q2=50q1 and parameter l=1. a The y-z cross-section of the instantaneous magnetic field Re(Hz) at x=0 for t=0 and ±q2/(2c). b The x-z cross-section of the instantaneous magnetic
Figure 2 Intensity and phase distribution of TE STNEV and LG beam with different orders: with Rayleigh range q2=50q1 in the x-y plane at certain frequency.
Parameter comparison of various kinds of pulse. N-Fid., N-Conc., and N. EoF, fidelity, concurrence, and EoF in intensity-normalized measurement, respectively.
Space Time Nonseparable Electromagnetic Vortices

August 2022

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156 Reads

In structured light with controllable degrees of freedom (DoFs), the vortex beams carrying orbital angular momentum (OAM) give access to provide additional degrees of freedom for information transfer, and in classic field, the propagation invariant space time electromagnetic pulses are the possible approach to high dimensional states. This paper arose an idea that coupling the space polarization nonseparable states of vortex beams and space time nonseparable states of spatiotemporal pulse can generate numerous unique and beneficial effects. Here, we introduce an family of space time nonseparable electromagnetic vortices (STNEV). The pulses exhibit complex and robust spatiotemporal topological structure of the electromagnetic fields, multiple singularities in the Poynting vector maps and distributions of energy backflow. We apply a quantum-mechanics methodology for quantitatively characterizing space time nonseparability of the pulse. Our findings facilitate their applications in fields of information transfer, toroidal electrodynamics and inducing transient excitations in matter.

Citations (1)


... These solutions are given by ( ) In conventional electromagnetic vortices, singularities typically form along the central axis of propagation. However, in the case of SNHPs, the singularities can take on a double-helix shape and vortex-antivortex annihilation can occur during the propagation [39]. ...

Reference:

Observation of space-time nonseparable helical pulses
Double-helix singularity and vortex–antivortex annihilation in space-time helical pulses