• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    A two-photon absorption 3D printer comprising a laser source (43) and a focusing objective (53) providing a focused laser beam in at least one focal volume, characterized in that it further comprises a system of deformation of the wavefront (49) of the laser beam (61), this system being associated with control means adapted to modify the deformation of the wavefront being printed so as to modify the dimensions of said at least one a focal volume.
    公开号:FR3023012A1
    申请号:FR1455948
    申请日:2014-06-26
    公开日:2016-01-01
    发明作者:Patrice Baldeck；Michel Bouriau
    申请人:Centre National de la Recherche Scientifique CNRS；Universite Joseph Fourier (Grenoble 1)；
    IPC主号:
    专利说明:

    [0001] FIELD OF THE INVENTION The present application relates to a three-dimensional (3D) object printing device more commonly referred to as a 3D printer, and more particularly to a 3D printer using a photochemical reaction induced by at least two photon multiphoton absorption. Background of the Prior Art In a two-photon absorption 3D printer, a laser beam of appropriate wavelength and power is focused at successive points of a material so that the regions of the material located at the points of focus successive shifts of the beam are modified by a photochemical reaction induced by absorption at least two photons. The material to be modified can be of various types. This material may comprise a resin that solidifies by polymerization or photo-crosslinking, a resin whose solubility properties are modified by photochemistry, proteins solidifying by photo-crosslinking, or metal salts solidifying by photo-crosslinking. The excess of unmodified material being dissolved by an appropriate solvent after the modification. The yields of these photochemical reactions induced by two-photon absorption are proportional to the square of the intensity of the laser resulting that the modification of the material is very localized. Figure 1 schematically shows an example of a two-photon absorption 3D printer. The 3D printer comprises a laser source 1, a focusing lens 3, and a tray 5 resting on a table XYZ 7 can be moved in orthogonal directions (XY) and parallel (Z) to the direction of propagation of a beam laser 9 generated by the source 1. The tray 5 is filled with a material 11 of one of the aforementioned types.
    [0002] The following is an example of the case where the material is a resin which solidifies by photocrosslinking. In operation, the laser beam 9 is focused by the objective 3 at a focusing point 13 located in the material 11. At the focusing point 13, when the power of the laser is sufficient, the material 11 solidifies locally which forms a pixel (voxel) of this material. In the figure, the focusing point 13 is shown as being at the bottom of the tray 5. The XYZ table 7 is controlled so that the focusing point 13 of the beam 9 is moved in the material 11 to form other voxels until the entire volume of the object to be printed has been solidified. The use of such a 3D printer makes it possible to produce voxels with dimensions of less than one micrometer or even one hundred nanometers. These printers have essentially been developed for the manufacture of very small objects with micrometric or submicrometric patterns. When printing an object whose dimensions are of the order of a millimeter or centimeter, because of the very small dimensions of the voxels, the printing times become very long. There is therefore a need for a 3D printer solving at least some of the disadvantages of conventional two-photon absorption 3D printers.
    [0003] SUMMARY Thus, an embodiment provides a two-photon absorption 3D printer comprising a laser source and a focussing lens providing a focused laser beam in at least one focal volume, characterized in that it further comprises a deformation system. the wavefront of the laser beam, this system being associated with control means adapted to modify the deformation of the wavefront being printed so as to modify the dimensions of said at least one focal volume.
    [0004] According to one embodiment, said system comprises a plurality of blades each of which has an irregular thickness, the control means comprising a carousel placing one or other of the blades in the path of the laser beam. According to one embodiment, said system comprises a matrix of micro-mirrors, the control means comprising means for positioning the micromirrors. According to one embodiment, said system comprises a matrix of liquid crystal pixels, the control means comprising biasing means capable of orienting the liquid crystals of each pixel. According to one embodiment, the 3D printer comprises an enlarger beam upstream of said system. BRIEF DESCRIPTION OF THE DRAWINGS These and other features and advantages will be set forth in detail in the following non-limiting description of particular embodiments in connection with the accompanying figures in which: Figure 1 schematically illustrates an example two-photon absorption 3D printer; Figures 2A and 2B schematically show an example of an object to be printed in 3D, Figure 2B being a sectional view along a plane BB of Figure 2A; FIG. 3 is a schematic view of the focusing zone of a laser beam; Figure 4 schematically shows an embodiment of a 3D printer; FIGS. 5A and 5B show schematically an embodiment of a wavefront deformation system used in the 3D printer of FIG. 4, FIG. 5A being a sectional view along a plane AA of FIG. 5B. ; Figures 6A and 6B schematically show an embodiment of a phase mask; Figure 7 schematically shows an embodiment of a liquid crystal wavefront deformation system; and Figure 8 schematically shows an embodiment of a micro-mirror wavefront deformation system. For the sake of clarity, the same elements have been designated with the same references in the various figures and, in addition, the various figures are not drawn to scale. DETAILED DESCRIPTION FIGS. 2A and 2B schematically represent an example of an object to be printed in 3D, FIG. 2A being a top view of the object, and FIG. 2B being a sectional view along a plane BB of FIG. 2A. . The object to be printed is a filter 21 comprising a filtration grid 23 integral with a ring 25. The grid, or sieve, 23 comprises extremely fine patterns which must be made with a high definition while the ring 25 does not require not a very high definition. The gate 23 comprises a network of small bars having, for example, a width of 100 nm with an interval i between bars of 200 nm. The ring 25 has a height 30 h of 0.5 mm, a thickness e of 0.2 mm, and an internal diameter d of 0.5 cm. If it is desired to manufacture the filter 21 with the 3D printer of FIG. 1, it will be necessary, to print the grid 23 with the desired precision, to choose a printer such that the voxels 35 have dimensions less than or equal to a hundred nanometers, this which causes that, to print the ring 25 having dimensions at least 1000 times greater than those of the voxels, the printing time becomes very long. It is proposed here to modify a two-photon absorption 3D printer of the type described with reference to FIG. 1 to incorporate a system for adapting, during printing, the dimensions of the voxels according to the dimensions of the different regions of an object to print. Thus, the grid 23 of the filter 21 may be printed with voxels 10 whose dimensions are less than one hundred nanometers, and the ring 25 may be printed with voxels whose dimensions are about 100 times larger, for example 1 at 20 μm, for example from 2 to 10 μm. FIG. 3 is a sectional view schematically illustrating the shape of the focussing zone of a focused laser beam 31 at a focal point 33. At the focal point 33, the laser beam 31 has a maximum convergence zone for which the beam has a minimum diameter (waist) Dmin. The beam diameter increases as one moves away from the maximum convergence zone. In particular, at a distance LR (Rayleigh length) of the maximum convergence zone, the beam has a diameter DR equal to Dmin multiplied by root of 2, and its energy per unit area is equal to half of the energy per unit area at the maximum convergence area. The volume portion of the laser beam 31 centered on the maximum convergence zone and of length L equal to twice the length of Rayleigh LR is called the focal volume. In practice, the focal volume 35 corresponds to the volume portion of the laser beam 31 in which the energy per unit area is sufficient to induce a two-photon absorption photochemical reaction resulting in the solidification of a suitable material and forming a voxel. Thus, by modifying the dimensions of a focal volume, the dimensions of the corresponding voxel are modified. In the remainder of this application, DR, Dmin, and L respectively denote the maximum diameter, the minimum diameter, and the length of a focal volume or a voxel. In the case of a laser beam with a plane wave front, the diameter Dmin of a focal volume 35 is inversely proportional to the numerical aperture ON of the focusing lens used, and the length L of the focal volume is proportional. squared Dmin- If the numerical aperture ON is reduced by a factor k, the length L of this focal volume is increased by a factor k by the diameter Dmin and by a factor k2. So that the energy of the beam remains sufficient to induce a chemical reaction by two-photon absorption, the power of the laser beam is increased by a factor k2. For example, for a focal volume of diameter Dmin equal to 0.2 fun and length L equal 0.7 pin, if the numerical aperture ON is decreased by a factor of 5, Dmin is multiplied by 5 and becomes equal to 1 pm and L is multiplied by 25 and becomes equal to 17.5 pin. The voxels obtained are therefore strongly stretched in the direction of their length and the Z-definition of the print becomes much smaller than the XY definition which poses many problems when printing a 3D object.
    [0005] Figure 4 schematically shows an embodiment of a two-photon absorption 3D printer. The 3D printer successively comprises, on an optical axis 41, a laser source 43, a beam expander 45, a plane mirror 47, a wavefront deformation system 49, a diaphragm 51, and a focusing objective 53 In the example shown, the beam expander 45 comprises two lenses 55 and 57. As in the case of Figure 1, the printer comprises a tray 5 disposed on a table XYZ 7 and filled with a material 11 itself. solidifying by a photochemical reaction induced by two-photon absorption. The output laser beam 61 of the enlarger 45 converges in the material 11 at a focusing point 63. Before passing through the wavefront deformation system 49, the wavefront of the laser beam is plane and orthogonal 35 to the optical axis 41. The wavefront deformation system 49 makes it possible to apply to the rays of the laser beam 61 phase shifts that vary according to the position of these rays in the beam. This results in a deformation of the wavefront of the laser beam 61.
    [0006] It is used here that, during the focusing of a laser beam having undergone a deformation of its wavefront, the focal volume is even larger than the wavefront of this beam is more disturbed. Thus, the diameters Dmin and DR mentioned above can be increased without the length L increasing significantly. The wavefront deformation system 49 is associated with unrepresented control means. These control means make it possible to modify, during printing, the disturbance applied to the wavefront of the beam to adapt the dimensions of the voxels to the dimensions of the regions of the object being printed. FIGS. AA and 5B schematically represent an embodiment of a wavefront deformation system 49A, FIG. 5B being a view from above, and FIG. AA being a sectional view along the plane AA of FIG. 5B. . The wavefront deformation system 49A comprises a plurality of blades 65a, 65b, 65c and 65d of irregular thicknesses of a material transparent to the wavelength of a laser beam 61. When the laser beam 61 passes through one of the blades 65a, 65b, 65c or 65d, the thickness irregularities of the blade cause different phase shifts between the beams of the beam 61, which results in a deformation of the wavefront of this beam. The irregularities of thicknesses are different from one blade to another and each blade corresponds to a particular deformation of the wavefront. One of the blades 65a, 65b, 65c and 65d may have an even thickness not causing deformation of the wavefront of the beam 61. The blades 65a, 65b, 65c and 65d, also called phase masks, are arranged in a carousel 67 rotatable about an axis 69 parallel to the direction of propagation of the beam 61. Rotations of the carousel 67 about the axis 69 allow to arrange one or the other of the blades on the path of the laser beam 61. These rotations can be controlled during printing to obtain different dimensions of voxels.
    [0007] Figures 6A. and 6B schematically illustrate an embodiment of a phase mask, for example phase mask 65a, FIG. 6A. being a view from above, and FIG. 6B being a sectional view along the plane BB of FIG. 6A. The phase mask 65a consists of a disc 73 made of a material that is transparent to the wavelength of the laser, the diameter of the disc 73 being greater than the diameter of a laser beam 61 passing through this phase mask 65a. Disk 73 comprises a flat face and a face having steps 75 having steep edges. The choice of the dimensions and the positions of the steps 75 leads to a particular deformation of the wavefront, and therefore to a given modification of the dimensions of the voxels. It is possible, for example, to pass voxels having dimensions Dmin equal to 0.2 fun and L equal to 0.7 gm to voxels with similar Dmin and L dimensions and between 1 and 20 gm, for example equal to 7, respectively. , 5 gm and 10 gm. Fig. 7 is a sectional view schematically showing another embodiment of a wavefront deformation system 49B. The system 49B comprises a matrix of pixels 81 transparent to the wavelength of a laser beam 61, each pixel 81 comprising liquid crystals 83 arranged between two polarization electrodes, not shown. The device 49B is disposed in a plane orthogonal to the direction of propagation of a laser beam 61 so that this beam passes through the pixel matrix.
    [0008] The polarization electrodes make it possible to control the orientation of the liquid crystals 83 in each pixel 81, which leads to different phase shifts between the beams of the beam 61. The orientation of the liquid crystals of each of the pixels 81 is controlled during printing. to perform different deformations of the wavefront resulting in obtaining different dimensions of voxels. Fig. 8 is a sectional view schematically showing another embodiment of a wavefront deformation system 49C. The system comprises a matrix of micro-mirrors 91, each micro-mirror being linked to the same support 93 via micro-pistons 95 to change the position of each micro-mirror. The system 49C is arranged so that a laser beam 61 striking the micromirrors 93 is reflected towards a focusing lens 53. By way of example, the system 49C is disposed in place of the plane mirror 47 of the 3D printer of FIG. 4. When the laser beam 61 is reflected by the matrix of micro-mirrors, the differences in position of the micro-mirrors of the matrix cause phase difference differences between the beams of the beam 61 from which it results in a deformation of the wavefront of the beam. The micro-pistons 95 are controlled so as to make it possible to modify, during printing, the positions of the micro-mirrors 93 to obtain different deformations of the wavefront and therefore different dimensions of voxels. Particular embodiments have been described. Various variations and modifications will be apparent to those skilled in the art. In particular, although a 3D printer has been described in relation to FIG. 4 in which the position of the focusing point is modified by the displacement of an XYZ table, the position of the focusing point can be modified by other means, for example, with regard to the Z-displacement, by a displacement of the focusing objective, and as regards the displacement in XY, by the use of directional mirrors or an acousto-optical deflector . Although an embodiment of a phase mask having steps having steep edges has been described in connection with FIGS. 6A and 6B, the thickness irregularities of the phase mask may be obtained with steps having rounded profiles. The phase masks may be replaced by other optical elements introducing a deformation of the wavefront of a laser beam passing through them. For example, microlens matrices may be used. FIGS. 5A, 5B, 6A, 6B, 7 and 8 show three embodiments of a wavefront deformation system, these systems comprising means for discretely or continuously changing the deformation. of the wavefront being printed. Those skilled in the art can use any other known types of controlled wavefront deformation systems 10 of a laser beam. For example, SLMs (Spatial Light Modulator), DMDs (Digital Micromiror Device), deformable mirrors, and liquid crystal optical valves can be used. Although wavefront deformation systems 49A and 49B have been described disposed between the plane mirror 47 and the diaphragm 51 of the 3D printer described in connection with FIG. 4, and a system 49C disposed in FIG. Instead of the plane mirror 47, the position of the wavefront deformation system in the 3D printer of FIG. 4 may be modified by those skilled in the art. More generally, in a 3D printer of the type described in relation to FIG. 4, it will be possible to add or delete optical elements. In particular, it will be possible to remove the reflecting mirror 47, or to add other mirrors to make the device more or less compact. Although a printing process has been described in which the entire volume of an object to be printed is solidified by successively producing many voxels, it will be possible to choose to print only the envelope (the walls) of the object to be printed or part of this object (the ring in the example of the filter given above). In addition to what has been previously described, it will be possible to adapt the focusing conditions of the beam, for example by modifying the numerical aperture or the objective of focusing.
    [0009] We considered the case where the printer is designed so that there is at each moment a single point of focus of a laser beam. If several focal points coexist, the deformation of the aforementioned wavefront will apply to each, and only to each of these focal points. Embodiments of a 3D printer have been described in which the material to be modified at the focal volume of a laser beam is disposed in a tray 5. In other embodiments, this material may be directly disposed on a support such as a glass or silicon plate. Although embodiments of a two-photon absorption 3D printer have been described, what has been previously described applies to photochemical reactions induced by multiphoton absorption.
    权利要求:
    Claims (5)
    [0001]
    REVENDICATIONS1. A two-photon absorption 3D printer comprising a laser source (43) and a focusing lens (53) providing a focused laser beam in at least one focal volume (35), characterized in that it further comprises a deformation system of the wavefront (49, 49A, 49B, 49C) of the laser beam (61), this system being associated with control means (67, 95) capable of modifying the wavefront deformation during printing to modify the dimensions of said at least one focal volume.
    [0002]
    The 3D printer according to claim 1, wherein said system (49A) comprises a plurality of blades (65a, 65b, 65c, 65d) each of which has an irregular thickness, the control means comprising a carousel (67) placing one or the other of the blades in the path of the laser beam (61).
    [0003]
    The 3D printer according to claim 1, wherein said system (49C) comprises a matrix of micro-mirrors (91), the control means including means (95) for positioning the micro-mirrors.
    [0004]
    The 3D printer according to claim 1, wherein said system (49B) comprises a matrix of pixels (81) with liquid crystals (83), the control means comprising polarization means for orienting the liquid crystals of each pixel.
    [0005]
    A 3D printer according to any one of claims 1 to 4, comprising a beam extender (45) upstream of said system (49, 49A, 49B, 49C).
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    法律状态:
    2015-05-26| PLFP| Fee payment|Year of fee payment: 2 |
    2016-01-01| PLSC| Publication of the preliminary search report|Effective date: 20160101 |
    2016-06-17| PLFP| Fee payment|Year of fee payment: 3 |
    2017-03-10| TQ| Partial transmission of property|Owner name: CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE, FR Effective date: 20170207 Owner name: UNIVERSITE GRENOBLE ALPES, FR Effective date: 20170207 |
    2017-06-16| PLFP| Fee payment|Year of fee payment: 4 |
    2018-06-14| PLFP| Fee payment|Year of fee payment: 5 |
    2019-06-17| PLFP| Fee payment|Year of fee payment: 6 |
    2020-06-26| PLFP| Fee payment|Year of fee payment: 7 |
    2021-06-28| PLFP| Fee payment|Year of fee payment: 8 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1455948A|FR3023012B1|2014-06-26|2014-06-26|THREE DIMENSIONAL PRINTING DEVICE|FR1455948A| FR3023012B1|2014-06-26|2014-06-26|THREE DIMENSIONAL PRINTING DEVICE|
    PCT/EP2015/064459| WO2015197794A1|2014-06-26|2015-06-25|Three-dimensional printing device|
    EP15731923.7A| EP3160719B1|2014-06-26|2015-06-25|Three-dimensional printing device|
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