The present application belongs to the field of two-photon laser direct writing photoetching, in particular to a method and an apparatus for direct writing photoetching by parallel interpenetrating super-resolution high-speed laser.
Two-photon laser direct writing can realize the processing of mesoscopic objects of a mm-cm level while maintaining the high accuracy at the nm-um level. This ability allows people to realize micro-scale or even nano-scale functional characteristics on mesoscale objects, which is particularly important in the research field of high-precision new complex devices and structures, such as on-chip integrated systems, micro-nano optics, metamaterials and so on. At present, there are still some problems in two-photon laser direct writing photoetching technology, among which the difficulty in realizing high-speed writing at mesoscale is the main factor restricting its further popularization, and the main reasons are insufficient scanning speed and imperfect writing strategy.
Replacing the traditional galvanometer with higher-speed scanning elements, such as a polyhedral scanning mirror (PLS), also known as a rotating mirror, or an acousto-optic deflector (AOD), can effectively improve the writing speed. On the other hand, using multi-beam synchronous scanning is also an effective method to improve the writing speed. How to combine them effectively is a mainstream direction in the development of two-photon laser direct writing photoetching. At present, an AOD is difficult to be combined with multi-beam scanning because of the high requirement of light incident angle and group velocity dispersion, while the rotating mirror can achieve the same scanning speed as an AOD and is easy to be combined with multi-beam scanning. However, the rotating mirror can only scan in the same direction, so it is not flexible enough in use. At present, the method of multi-beam parallel laser direct writing using edge photoinhibition technology combined with the rotating mirror is relatively simple, and it is difficult to really play the advantages of multi-beam rotating mirror scanning.
In view of the shortcomings of the prior art, the present application aims to provide a method and an apparatus for direct writing photoetching by parallel interpenetrating super-resolution high-speed laser.
The purpose of the present application is realized by the following technical solution: a method for direct writing photoetching by parallel interpenetrating super-resolution high-speed laser, including the steps of:
In an embodiment, the step of generating multiple writing light beams propagating in different diffraction directions based on a writing light optical diffractometer includes: using a spatial light modulator to load a multipoint pattern hologram to generate multiple writing light beams, or using a diffractive optical element DOE to generate multiple writing light beams.
In an embodiment, the step of generating multiple inhibited light beams propagating in different diffraction directions based on an inhibited light optical diffractometer includes:
using a spatial light modulator to load a multipoint pattern hologram to generate multiple solid spot beams, and further superposing 0-2π vortex phases to generate multiple hollow inhibited light beams.
Further, in the step of modulating an arrangement direction of the combined multiple beams based on an image rotator, a modulation angle θr satisfies:
n×N
beams
×δd+δd=D|sin θr, |+D|cos θr|·δd/Lmax
where the modulation angle θr is defined as an included angle between a scanning direction of the rotating mirror and the arrangement direction of the multiple beams; δd indicates a line spacing (solution/um); n is an integer, which means that a first beam reaches a designated position after n times of scanning, a distance between the position and a first writing position of a last beam of the multiple beams being δd; Nbeams indicates the number of the beams, which is an integer; D indicates a distance between two adjacent beams of the multiple beams; Lmax indicates a maximum length that the rotating mirror can reach in a single scanning on a focal plane of an objective lens.
Further, in the step of moving at a constant speed in a longitudinal direction based
on a displacement stage, the moving direction is perpendicular to the scanning direction of the rotating mirror, and the moving speed vs satisfies:
v
s
=δd/L
max
·v
PLS
where vPLS indicates a scanning speed of the rotating mirror.
Further, in the step of outputting a multichannel writing waveform based on a multichannel high-speed optical switch, the output multichannel writing waveform satisfies the parallel interpenetrating algorithm, which includes the following steps of:
Further, during step-moving the displacement stage fro one time, the moving direction of step-moving the displacement stage for one time is parallel to the writing direction of the rotating mirror; a moving distance Lstep is: Lstep=Lmax−Luseless, where Luseless indicates an invalid writing area, Luseless=Lout+D×Nbeams|cos θr|, where a first term Lout indicates an invalid writing length caused by cutting a light spot by the edge of the rotating mirror, and a second term indicates the invalid writing length caused by inclination of the multiple beams.
An apparatus for implementing the above method, including:
In an embodiment, the laser uses a 780 nm femtosecond laser.
In an embodiment, the inhibited light laser uses a 532 nm continuous laser.
In an embodiment, the group velocity dispersion compensation unit includes a group velocity dispersion compensation element, several reflecting mirrors and a one-dimensional displacement stage; the femtosecond laser repeatedly passes through the group velocity dispersion compensation element guided by the reflecting mirror, for a total of four times; the compensation amount can be adjusted by adjusting the distance between the first incidence and the second incidence through a one-dimensional displacement stage.
In an embodiment, the group velocity dispersion compensation element includes, but is not limited to, the following elements: a grating and a prism.
In an embodiment, refer to the following literature for the calculation method of the compensation amount: Kim, D. U., et al., Two-photon microscopy using an Yb(3+)-doped fiber laser with variable pulse widths. Opt Express, 2012. 20(11): p. 12341-9.
In an embodiment, the calculation method of the positive group velocity dispersion generated in the subsequent optical path propagation is as follows:
In an embodiment, the optical diffractive apparatus includes but is not limited to the following devices: a spatial light modulator (SLM) and a diffractive optical element (DOE).
In an embodiment, the multichannel high-speed optical switch uses a multichannel acousto-optic modulator.
In an embodiment, the beam expanding apparatus comprises two lenses, and the focal points of the two lenses placed in front and back are coincident, and there is the following relationship between the focal lengths f1, f2 and the incident/emergent spot sizes
In an embodiment, on the basis of the beam expanding apparatus, the shaping apparatus places a pinhole at the focal position where the two lenses overlap, and the pinhole size D is determined by the following formula: D=λf/r, where λ indicates the wavelength, f indicates the focal length of the incident lens, and r indicates the radius at the energy 1/e2 of the incident beam.
In an embodiment, the image rotator apparatus includes, but is not limited to, the following devices: a Dowell prism and a three-sided reflecting mirror.
In an embodiment, the scanning lens system includes a scanning lens, a field lens and an objective lens. The scanning lens and the field lens form a 4f system, which is placed between the rotating mirror and the objective lens, and the rotating mirror and the objective lens are respectively placed at the front and rear focal planes of the 4f system.
In an embodiment, the sample translation movement mechanism includes, but is not limited to, the following devices: a piezoelectric displacement stage, an air bearing displacement stage, a mechanical electric displacement stage, a manual displacement stage, and a combination containing at least one of the above devices.
The present application has the following beneficial effects:
In order to explain the purpose, technical solution and advantages of the present application more clearly, the present application will be further described in detail with examples and drawings. It should be understood that the specific embodiments described here are only used to explain the present application, and are not used to limit the present application. Those skilled in the art who make modifications or equivalent substitutions on the basis of understanding the technical solution of the present application without departing from the principle and spirit of the technical solution of the present application shall be covered by the protection scope of the present application.
The present application relates to an apparatus for direct writing photoetching by parallel interpenetrating super-resolution high-speed laser, which consists of a writing light laser, a writing light group velocity dispersion compensation unit, a writing light/inhibited light beam expanding/shaping apparatus, a writing light/inhibited light optical diffractometer, a writing light/inhibited light multichannel high-speed optical switch apparatus, an image rotator apparatus, a high-speed rotating mirror, a scanning lens system and a sample translation motion mechanism.
As shown in
In addition, the 532 nm continuous light laser 36 (an inhibited light laser) generates a beam of 532 nm continuous light laser, which passes through the beam expanding lens groups 37-38 to complete beam expansion. The beam direction is adjusted by reflecting mirrors 39-40 and then the beam enters the 532 nm spatial light modulator 41. By loading a hologram on the spatial light modulator 41, a single beam is modulated into multiple beams, which are solid light spots at this time, and the solid light spots are modulated into hollow light spots by superimposing 0-2π vortex light phases on the hologram, thus generating the inhibited light of the hollow light spots. The beam is reflected by the reflecting mirror 42, and the hologram is Fourier-transformed by the lens 43, so that multiple focal points of hollow inhibited light are generated at the focal plane of the lens 43. A 532 nm multichannel acousto-optic modulator 44 is placed at the focal plane of the lens 43, and each channel passes through a focal point to realize independent modulation of each beam. The divergent light is collimated by the lens 45, combined with the writing light through the dichroic mirror 18, and enters the image rotator 19 together.
The writing light and the inhibited light are modulated by the image rotator 19, reflected by the mirror 20 and then enter the rotating mirror 21. The multiple beams are reflected by the rotating mirror 21, pass through the scanning lens 22 and the field mirror 23, and then are reflected by the dichroic mirror 24 into the high-NA objective lens 25 and are focused on the photoresist sample 26. The piezoelectric displacement stage 27 and the air bearing displacement stage 28 drive the photoresist sample 26 to scan under the program control. The lighting source 33 is an LED lamp, and the illuminating light emitted by the lighting source 33 is converted into parallel light by the condensing lens 31 after passing through the diaphragm 32, and then reflected by the equal-proportion beam splitter 30, and then passes through the imaging lens 29 and the dichroic mirror 24 in turn to be focused at the entrance pupil of the high-NA objective lens 25. In addition, the image at the photoresist sample 26 passes through the high-NA objective lens 25, the dichroic mirror 24, the imaging lens 29 and the equal-proportion beam splitter 30 in turn and is imaged at the camera 34 for writing observation. As shown in
As shown in
n×N
beams
×δd+δd=D|sin θr, |+D|cos θr|·δd/Lmax
where δd indicates the line spacing (parallel to the scanning direction of the displacement stage) and the resolution/um; n is an integer, which means that the beam 1 reaches the 1* position after n times of scanning, where the 1* position is defined as the position at a distance of δd from the beam 2; Nbeams indicates the number of beams, which is an integer;
D indicates the distance between the starting points of two adjacent beams (as shown in the figure, the distance between the black spots of beams 1 and 2); θr indicates the included angle between the arrangement direction of the multiple beams and the scanning direction of the rotating mirror; Lmax indicates the maximum length that the rotating mirror can reach in a single scanning on the focal plane of the objective lens. The displacement stage moves at a constant speed until the whole column of left areas is written. The optical switch is turned off and then the displacement stage is step-moved for one time as shown by the arrow at the bottom of
As shown in
Number | Date | Country | Kind |
---|---|---|---|
202111248686.2 | Oct 2021 | CN | national |
The present application is a continuation of International Application No. PCT/CN2022/096829, filed on Jun. 2, 2022, which claims priority to Chinese Application No. 202111248686.2, filed on Oct. 26, 2021, the contents of both of which are incorporated herein by reference in their entireties.
Number | Date | Country | |
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Parent | PCT/CN2022/096829 | Jun 2022 | WO |
Child | 18404934 | US |