On-chip optical field wavefront measurement system and method based on grating coupler
Technical Field
The invention belongs to the technical field of optical information measurement, and particularly relates to an on-chip optical field wavefront measurement system and method based on a grating coupler.
Background
The wavefront sensing has wide application in astronomical self-adaptive optics, micro-nano three-dimensional morphology measurement, laser communication, biological quantitative phase microscopic imaging and other fields. The traditional wave-front phase sensing method mainly comprises a shack-Hartmann wave-front sensor, digital holographic quantitative phase imaging and the like.
Conventional phase measurement techniques typically employ complex optics that are difficult to meet a number of practical application requirements. The traditional shack-Hartmann sensor based on the micro lens array has the advantages of simpler device, lower imaging resolution and smaller dynamic range, and can only meet the wavefront measurement requirement with low partial resolution requirement.
In recent years, silicon photonic chips have been widely used in the fields of optical communication, optical computing, optical sensing, and the like. The micro-nano optical device on the chip enables the miniaturization and microminiaturization of the traditional optical measurement equipment due to the flexible regulation and control of the optical polarization, the phase and the amplitude.
Disclosure of Invention
Aiming at the defects and improvement demands of the prior art, the invention provides an on-chip light field wavefront measurement system and method based on a grating coupler, which utilize the grating coupler to convert the angle information of the wavefront to be measured into the light intensity information in a waveguide, and measure the light intensity signals in the waveguide through an optical fiber array and a photoelectric detector to determine the angle information of the wavefront to be measured at each space position, so as to realize a wavefront measurement system with high resolution and high dynamic range.
In order to achieve the above object, according to a first aspect of the present invention, there is provided an on-chip optical field wavefront measurement system based on a grating coupler, including a grating coupler array, an optical fiber, and a photodetector connected in sequence;
The grating coupler array is arranged on the silicon photon chip and comprises a grating coupling unit array and a waveguide array which are positioned in the same plane, wherein the grating coupling unit array is used for receiving a wavefront to be detected, coupling the wavefront to be detected into the waveguide array and converting a wavefront angle signal into a light intensity signal in the waveguide array;
The optical fiber array is used for coupling the light intensity signals in the waveguide array into the optical fibers and transmitting the light intensity signals to the photoelectric detector through the optical fibers;
the photoelectric detector is used for carrying out photoelectric conversion processing on the light intensity signals to obtain characteristic parameters of the wavefront to be detected.
Further, the grating coupler unit array includes four grating couplers forming an included angle of 90 degrees with each other in the same plane, a waveguide is disposed at one end of each grating coupler far away from each other, each grating coupler couples the wavefront to be measured into the waveguide, and the waveguides are used for forming the waveguide array.
Further, the optical fiber array couples the light intensity signals in the waveguide into the optical fibers through an edge coupler or a vertical coupler.
Further, the photoelectric detector is a CMOS camera, a CCD camera or a multichannel optical power meter.
According to another aspect of the present invention, the present invention further provides a method for measuring a wavefront characteristic parameter to be measured by using the above measurement system, including:
S1, determining light intensity signals in the waveguide array according to the light intensity signals in the optical fiber array received by the photoelectric detector:
s2, calculating the normalized coupling power ratio of the grating coupler array in the plane according to the light intensity signals in the waveguide array;
S3, calculating a wavefront angle corresponding to the wavefront to be measured under the current normalized coupling power ratio according to a response curve of the normalized coupling power ratio calibrated in advance and the wavefront angle to be measured;
And S4, integrating the wave-front angle measured values at different positions by utilizing a regional wave-front reconstruction algorithm according to the wave-front angle to determine the wave-front distribution to be measured.
Further, in the step S2-S3, the plane is a plane formed by xy directions, the grating coupler array includes grating couplers distributed in the four directions of +x, -x, +y and y in the plane, the direction of the wavefront to be measured is a z direction perpendicular to the plane, and the normalized coupling power ratio of the grating couplers in the +x and-x directions is:
the normalized coupling power ratio of the grating coupler in the +y direction and the-y direction is as follows:
Wherein the normalized coupled power ratios in the x-direction and the y-direction, R x and R y, respectively, are monotonic functions with respect to the wavefront angle θ x and the wavefront angle θ y;
The power P +x in the waveguide is Gaussian distribution about a wave-front angle theta x, the coupling peak angle is theta 1, the wave-front angle theta x is an included angle between the wave-front to be measured projected into an xz plane and the x direction, P -x is a response curve about the wave-front angle theta x and symmetrical with P +x about a yz plane, P +y is Gaussian distribution about the wave-front angle theta y, wherein theta y is an included angle between the wave-front to be measured projected into the yz plane and the y direction, P -y is a response curve about the wave-front angle theta y and symmetrical with P +y about the xz plane.
Further, the grating coupler structure distributed along the +x direction is obtained by constructing an objective function of the grating coupler structure, so that when the wave front angle to be measured is theta 1, the power of the transmission waveguide along the +x direction is maximum, and solving and calculating by using an intelligent optimization algorithm to obtain the optimal grating coupling unit structure.
In general, through the above technical solutions conceived by the present invention, the following beneficial effects can be obtained:
1. the invention provides an on-chip light field wavefront measuring system and a novel method based on a grating coupler, which utilize the grating coupler to convert the angle information of the wavefront to be measured into light intensity information in a waveguide, and can uniquely determine the angle information of the wavefront to be measured at each spatial position by measuring the light intensity signals in the waveguide through an optical fiber array and a photoelectric detector.
2. The on-chip light field wavefront measurement system provided by the invention only depends on the size of the grating coupler, and can realize higher spatial resolution compared with the traditional wavefront sensor based on the micro lens array.
3. The optimal measurement method can uniquely determine the angle information of the wavefront to be measured by calculating the normalized coupling power ratios of four different directions in the same plane, has simple data processing process and small calculation amount, and further improves the measurement efficiency.
Drawings
FIG. 1 is a schematic diagram of an on-chip optical field wavefront measurement system based on a grating coupler according to an embodiment of the present invention;
FIG. 2 is a schematic diagram of a grating coupler array provided in an embodiment of the present invention;
FIG. 3 is a graph showing the variation of +x-direction and-x-direction waveguide coupling power with the measured wavefront angle θ x provided in an embodiment of the present invention;
Fig. 4 is a graph showing the variation of the x-direction normalized power ratio R x with the wavefront angle θ x to be measured, provided in an embodiment of the present invention.
The same reference numbers are used throughout the drawings to reference like elements or structures, wherein:
A grating coupler array 100, a grating coupler 101, a waveguide array 102, an optical fiber array 200, and a photodetector 300.
Detailed Description
The present invention will be described in further detail with reference to the drawings and examples, in order to make the objects, technical solutions and advantages of the present invention more apparent. It should be understood that the specific embodiments described herein are for purposes of illustration only and are not intended to limit the scope of the invention. In addition, the technical features of the embodiments of the present invention described below may be combined with each other as long as they do not collide with each other.
The first aspect of the present invention proposes an on-chip optical field measurement system based on a grating coupler, as shown in fig. 1, the system comprises a grating coupler array 100, an optical fiber array 200, an optical fiber and a photodetector 300 connected in sequence, wherein the direction of light propagation is the z-axis, and the grating coupler array 100 is located in the xy-plane, wherein:
The grating coupler array 100 is disposed on a silicon photonic chip, and comprises a grating coupling unit array 101 and a waveguide array 102, which are located in the same plane, wherein the grating coupling unit array 101 is used for receiving a wavefront to be measured, coupling the wavefront to be measured into the waveguide array 102, and converting a wavefront angle signal into a light intensity signal in the waveguide array 102.
The fiber array 200 is used to couple the light intensity signals within the waveguide array 102 into the optical fibers and to transmit to the photodetector 300.
The photodetector 300 is configured to receive the light intensity signal in the optical fiber array 200, and perform photoelectric conversion processing on the light intensity signal to obtain a characteristic parameter of the wavefront to be measured.
Further, as shown in fig. 2, the grating coupling unit 101 includes grating couplers distributed in the four directions of +x, -x, +y and y in the plane, one waveguide is disposed at one end of each grating coupler away from each other, each grating coupler couples the wavefront to be measured into the waveguide, the waveguides are used to form the waveguide array 102, and each grating coupler converts the angle of the wavefront to be measured into the power P +x,P-x,P+y,P-y in four independent waveguides at the same time. The grating couplers in the +x direction and the-x direction are used for measuring an included angle theta x between the projection of the wavefront to be measured and the x axis in the xz plane, and the grating couplers in the +y direction and the-y direction are used for measuring an included angle theta y.θx between the projection of the wavefront to be measured and the y axis in the yz plane, and the measuring structures and the measuring principles of theta y are the same, and the measuring principles of theta x are now described. The power P +x of the +x-direction grating coupler coupling the wavefront to be measured into the waveguide is a gaussian curve about the angle θ x of the wavefront to be measured, with a coupling peak angle of θ 1, as shown in fig. 3. The response curve of P -x and P +x are symmetrical about the yz plane. The normalized coupling power ratio of the grating coupler in +x and-x directions is:
As shown in fig. 4, the normalized coupled power ratio R x in the x-direction is a monotonic function with respect to θ x. The measuring principle of the angle theta x.θy of the wavefront to be measured can be uniquely determined by measuring R x is the same as that of the angle theta x, and the angle theta y of the wavefront to be measured can be uniquely determined by measuring R y.
Furthermore, the design of the grating coupler is optimized according to the performance requirement of wavefront detection and the wavelength of the wavefront to be detected. Since the grating couplers arranged in four directions are identical in size, only a single grating coupler needs to be optimally designed. Taking a grating coupler along the +x direction as an example, an objective function of the grating coupler structure is constructed so that the power of the transmission waveguide along the +x direction is maximum when the wave front angle to be measured is theta 1. And solving and calculating by using a common intelligent optimization algorithm, such as a particle swarm optimization and simulated annealing algorithm, so as to obtain the optimal grating coupling unit structure.
Further, the fiber array 200 may couple the light intensity signals within the waveguide into the array fibers through an edge coupler or a vertical coupler.
Further, the photodetector 300 may employ a CMOS camera, a CCD camera, or a multichannel optical power meter.
In specific implementation, the on-chip optical field wavefront measurement method provided by the invention comprises the following steps:
1. The light intensity signal in the waveguide 102 is determined by the light intensity signal received by the photodetector 300 in the optical fiber array 200, P +x,P-x,P+y,P-y;
2. Calculating normalized coupling power ratios R x and R y in the x-direction and the y-direction from the light intensity signals within the waveguide array 102;
3. According to a response curve of a pre-calibrated normalized coupling power ratio and a wavefront angle to be measured, calculating the wavefront angles theta x and theta y of corresponding wavefront to be measured under the current R x and R y;
4. and according to the wave front angles theta x and theta y to be measured, the wave front distribution condition to be measured can be determined by integrating wave front angle measurement values at different positions by utilizing a regional wave front reconstruction algorithm.
It will be readily appreciated by those skilled in the art that the foregoing description is merely a preferred embodiment of the invention and is not intended to limit the invention, but any modifications, equivalents, improvements or alternatives falling within the spirit and principles of the invention are intended to be included within the scope of the invention.