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Tunable unidirectional crossed waveguide distributor based on PT symmetrical structure and magneto-photonic crystal

A technology of magnetophotonic crystal and symmetric structure, applied in the directions of instruments, optics, nonlinear optics, etc., can solve the problems of single signal output mode, the number of signal output channels cannot be controlled in the direction of signal output, etc., and achieve obvious effect and backscattering. Good suppression effect

Active Publication Date: 2019-11-26
NANJING FORESTRY UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

[0007] The Chinese patent 201410363260.5 with the publication date of October 15, 2014 discloses a cross-shaped circulator based on a photonic crystal waveguide. Signals can enter from 4 ports, but can only be output from orthogonal adjacent ports; the publication date The Chinese patent 201410515362.4 on April 29, 2015 discloses a compact six-port photonic crystal circulator. Although there are six ports, it can only enter from the port and output from the adjacent port, and the direction of the signal output cannot be controlled. And the number of signal output channels, can only enter in one direction, determine the direction of one-way output, and the signal output mode is single

Method used

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  • Tunable unidirectional crossed waveguide distributor based on PT symmetrical structure and magneto-photonic crystal
  • Tunable unidirectional crossed waveguide distributor based on PT symmetrical structure and magneto-photonic crystal
  • Tunable unidirectional crossed waveguide distributor based on PT symmetrical structure and magneto-photonic crystal

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Embodiment 1

[0064] In this embodiment, the signal is input from the second channel 6, and the point source frequency is 1.25e 14 Hz, the first array 1 and the second array 2 are applied with a positive direction magnetic field, and the third array 3 and the fourth array 4 are applied with a negative direction magnetic field. The calculated steady-state electric field Ez distribution is as follows: image 3 shown. It can be seen from the figure that due to the topological protection, the signal does not disperse to the longitudinal channel when it is transmitted to the intersection of longitudinal and transverse transmission, but continues along the transverse waveguide structure and is output from the third channel 7 .

Embodiment 2

[0066] In this embodiment, the setting of the point current source and its position is the same as that of Embodiment 1, the difference is: the third array 3 is applied with a magnetic field in a negative direction, and the remaining three arrays are applied with a magnetic field in a positive direction, and the obtained electric fields are as follows: Figure 4 shown. It can be seen that since the same magnetic field corresponds to the horizontal energy band without dispersion and the opposite magnetic field corresponds to the energy band of one-way transmission, the signal can be collimated and propagated at 90 degrees, and the signal is output from the fourth channel 8, and the signal is bent spontaneously under the action of the external magnetic field L-shaped transmission. Because it is protected by topology, the backscatter suppression effect is obvious. It can be seen that there is no leakage wave in channel 1 and channel 3, and there is no signal output.

Embodiment 3

[0068] In this embodiment, the settings of the point current source and its position are the same as those in Embodiment 1, the difference is that the first array 1 is applied with a positive direction magnetic field, and the other three arrays are applied with a negative direction magnetic field. The calculated steady-state magnetic field is as follows: Figure 5 shown.

[0069] For the second channel 6, an external magnetic field of upper positive and lower negative is applied, so the signal is transmitted to the right in one direction, and because the second array 2 and the fourth array 4 are also negative magnetic fields, the signal cannot be transmitted, and for the second channel For channel 5, a positive and negative magnetic field is also added, so the signal can be transmitted to the right (that is, transmitted in the first channel 5), which realizes the entry of light into a single channel and the output of a designated channel.

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Abstract

The invention discloses a tunable unidirectional crossed waveguide distributor based on a PT symmetrical structure and a magneto-photonic crystal, which belongs to the field of miniature optoelectronic devices. The distributor comprises a dielectric substrate. First, second, third and fourth arrays are located at four corners of the dielectric substrate respectively to form a crossed photonic crystal waveguide with four ports. A first gain column and a second gain column are set at the corners, which are close to the center of the crossed waveguide, of the first array and the fourth array respectively. A first loss column and a second loss column are set at the corners, which are close to the center of the crossed waveguide, of the second array and the third array respectively. The first gain column, the second gain column, the first loss column and the second loss column satisfy the parity-in-time symmetry condition. The first array, the second array, the third array and the fourth array apply an external magnetic field as required respectively. The waveguide distributor provided by the invention can realize the selective propagation of electromagnetic waves in any designed one tofour channels under different external magnetic fields, and can realize electromagnetic localization in any channel.

Description

technical field [0001] The invention belongs to the field of miniature optoelectronic devices, and in particular relates to a tunable unidirectional cross waveguide splitter based on a PT symmetry structure and a magneto-photonic crystal. Background technique [0002] In recent years, artificial bandgap materials, especially photonic crystals, have become the research focus of a new generation of smart materials due to their superior performance, especially the topological properties of artificial bandgap materials have attracted widespread attention. State, with defect immunity, backscattering suppression transmission characteristics, great potential application prospects. [0003] In a quantum mechanical system, if the Hamiltonian of the system Satisfy And with Operators have a common eigenvector, then the system has non-broken PT symmetry, that is, the potential function of Hamilton satisfies the even symmetry of the real part and the odd symmetry of the imaginary p...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): G02F1/09G02F1/095
CPCG02F1/09G02F1/095G02F2202/32Y02D30/70
Inventor 张晓萌余观夏梅长彤朱剑刚赵莉
Owner NANJING FORESTRY UNIV
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