Mirror Device for an Interferometer Device, Interferometer Device and Method for Producing a Mirror Device
20220221709 ยท 2022-07-14
Inventors
- Christoph Schelling (Stuttgart, DE)
- Christoph Daniel Kraemmer (Malsch, DE)
- Reinhold Roedel (Reutlingen, DE)
Cpc classification
G02B5/0816
PHYSICS
G02B5/284
PHYSICS
G01J3/26
PHYSICS
International classification
G02B26/00
PHYSICS
G01J3/26
PHYSICS
Abstract
The disclosure relates to a mirror device for an interferometer device including a first mirror layer and a second mirror layer, which are arranged in parallel on top of one another and spaced apart from one another by a mirror layer spacing. The mirror layer spacing forms an intermediate space between the first and the second mirror layer. The intermediate space includes a gas or a vacuum, and at least one spacing structure which extends at least partially between the first and the second mirror layer. The spacing structure has a material that is the same as or different from the first and/or second mirror layer.
Claims
1. A mirror device for an interferometer device comprising: a first mirror layer and a second mirror layer, which are arranged parallel one above the other with a mirror layer distance between them, wherein the mirror layer distance forms an intermediate space between the first and the second mirror layer, and wherein the intermediate space includes a gas or a vacuum; and at least one spacing structure extending at least partially between the first and the second mirror layer, and wherein the spacing structure comprises a material that is the same as or different from the first and/or second mirror layer.
2. The mirror device as claimed in claim 1, in which the spacing structure comprises side walls that extend vertically from a planar direction of extent of the first and second mirror layer or extend in deviation from a vertical direction by a specific angle.
3. The mirror device as claimed in claim 1, in which the spacing structure projects into at least one of the first and second mirror layers.
4. The mirror device as claimed in claim 2, in which the spacing structure comprises a core between the side walls and a bottom, wherein the side walls and the bottom comprise a different material than the core.
5. The mirror device as claimed in claim 4, in which the side walls and the bottom comprise an electrically insulating material.
6. The mirror device as claimed in claim 1, in which the spacing structure projects through at least one of the first and second mirror layers and beyond an outer side of the at least one of the first and second mirror layer by at least one thickness of one of the first and second mirror layers.
7. The mirror device as claimed in claim 1, wherein: the at least one spacing structure is one of a plurality of spacing structures; and the plurality of spacing structures that, in a top view of a planar top side of the second mirror layer, a hexagonal grid.
8. The mirror device as claimed in claim 1, further comprising: at least one recess in at least one of the first and second mirror layers, wherein, in a region at least one of below and above the recess, the at least one of the first and second mirror layer projects perpendicularly from the planar direction of extent of the at least one of the first and a second mirror layer in a direction away from the recess.
9. An interferometer device comprising: a substrate; a first mirror device P and a second mirror device, wherein at least one of the first and second mirror devices is formed as claimed in claim 1, which are arranged over the substrate and one above the other, spaced apart from one another by a first spacing wherein at least the first mirror device is arranged movably in relation to the second mirror device; and an actuating device configured to move at least one of the first and the second mirror device.
10. A method for producing a mirror device, comprising: providing at least one of a first sacrificial layer and a substrate; applying a first mirror layer onto the at least one of the first sacrificial layer and the substrate; applying a second sacrificial layer on the first mirror layer; forming a recess at least in the second sacrificial layer, which extends at least to the first mirror layer; introducing a material for a spacing structure into the recess; applying a second mirror layer onto the second sacrificial layer and over the recess; and at least partially removing at least one of the first and the second sacrificial layer.
11. The method as claimed in claim 10, wherein introducing the material for the spacing structure into the recess comprises: arranging an electrical insulator layer in the recess and on the top side of the second sacrificial layer; and introducing the material into the recess such that the recess is filled thereby forming a core of the spacing structure.
12. The method as claimed in claim 11, wherein at least one of the electrical insulator layer and the core is back thinned before the second mirror layer is applied in order to produce a planar connection with regions that laterally adjoin the recess.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0026] The present invention will be explained in more detail below with reference to the exemplary embodiments specified in the schematic figures of the drawing.
[0027] In the drawings:
[0028]
[0029]
[0030]
[0031]
[0032]
[0033] In the figures, identical reference signs denote identical or functionally identical elements.
[0034]
[0035]
[0036] The spacing structures 4 shown can undergo lateral deformations, for example resulting from the inner tensile stress (mechanical) in the mirror layers. Since the spacing structures advantageously comprise a different material than the mirror layers, these can be mechanically and advantageously electrically adapted to the requirements of the spacing structure, for example in order to be able to better maintain a tensile stress that is advantageously set in the layers (due to the reduced relaxation of the spacing structures), as a result of which the optically usable surface (the planarity of the mirrors with a defined spacing) can also be increased.
[0037] Furthermore, the spacing structures can terminate substantially planar with a top side of the mirror layer, which cannot produce any elevation above the mirror layer (produces hardly any or no topography), which may be advantageous both for process control and also for the optical and mechanical properties of any further (mirror) layers that may follow (consequently, little or no bending of the following layers of a further mirror may occur). During filling of the recess, the material for the spacing structure can form a planar surface with a tolerance with a top side of the mirror layer that faces away from the first mirror layer. The tolerance for a planar termination can have a deviation of at most the thickness of the mirror layer.
[0038] In
[0039] Furthermore, a plurality of spacing structures 4 may also be present, which can form, in a top view of a planar top side 3b of the second mirror layer 3, a hexagonal grid or other geometric shapes (not shown).
[0040] According to
[0041] According to
[0042] The spacing structure can consequently be deposited separately from the mirror layers and form a base for depositing the second mirror layer. The embodiment can also be expanded to include further mirror layers, advantageously using further mirror layers and sacrificial layers.
[0043] The gas (mixture) in the intermediate space 5, for example air, or a vacuum can represent (replace) a low-index layer and have a refractive index of approximately one. The mirror layers 2 and 3 can have, for example, silicon as the high-index material having a refractive index of, for example, 3.5. Rather than silicon, germanium or silicon carbide can also be used, or different materials that can be compatible with (resistant to) sacrificial layer etching processes. If air is used as the low-index material, it is possible to achieve a large refractive index difference with respect to the high-index material and to produce a spectrally broadband, highly reflective mirror device.
[0044] The spacing structures 4 can stabilize the mirror layers relative to one another in order to ensure, via as large an optical region (aperture area) of the mirror device as possible, a spacing of the mirrors (mirror devices) of one quarter wavelength of the central wavelength (that is to be transmitted or filtered), that is to say that the low-index layer (air) has a thickness of a quarter wavelength.
[0045] The material of the spacing structure 4 can be, for example, a semiconductor material and/or the same material as at least one of the mirror layers. The deposition process of the material of the spacing structure can be adapted to the mechanical and electrical properties (conductivity electrical, thermal, vertical electrical insulation of the mirror layers) of the mirror layers and the production process. However, these properties can also be set independently of the requirements regarding the mirror layers. For example, the doping and/or crystallinity can be variable. The spacing structure and the mirror layers can differ in their materials in terms of doping or crystallinity, but can also comprise a different semiconductor material. The spacing structure can be electrically insulating, for example the material of the core. From a mechanical standpoint, this spacing structure can be highly stable and resistant to breakage and hardly permit any deformations of the mirrors (membranes/layers), in particular their separation, for example no or little notch effect under stress.
[0046] The spacing structures can be designed as at least partially laterally continuous wall structures and/or as column structures, for example as honeycomb structures.
[0047] A predetermined separation between the mirror layers can be maintained due to reduced yielding or no yielding. The spacing structures can be embodied, in a top view, nearly in the shape of points, resulting in minimization of optical losses.
[0048] The material in the core 4d can comprise a high-index material (as compared to the intermediate region with gas, gas mixture or vacuum), similar to one of the mirror layers.
[0049] In the event of contact between the mirror layer 2 and an underlying structure, the spacers AH (anti-stiction bumps) can reduce the contact area and thus the static friction, which can prevent the mirror layer from irreversibly sticking to an underlying structure. Any overhang of the spacers beyond the mirror layer can preferably be greater than a thickness of the mirror layer (first one) itself. With particular preference, the overhang is greater than a thickness of the second sacrificial layer. The spacers AH can thus be made from an electrically insulating material or surrounded by an electrically insulating layer in order to prevent fusion in the event of contact being made with an underlying structure that is at a different electrical potential.
[0050] In a mirror device of this type, reduced deformation of the spacing structures (lateral) and of a mirror region can be attained due to continuous mirror layers that remain substantially planar.
[0051]
[0052] The step of
[0053] A further method step can involve, according to
[0054] According to the further method, according to
[0055] In a further step, according to
[0056] After the method step of
[0057] In a further method, according to
[0058] The recess A or further recesses (smaller ones) can be, in a top view of a planar direction of extent, circular, elliptical or have a different shape, such as elongated.
[0059] The elliptical shape can be characterized by better optical properties, in particular by a reduction in optical losses.
[0060] Using a third mirror layer and further sacrificial layers and corresponding recesses, the process sequences shown can be modified and multilayer mirror devices having a plurality of low-index layers and high-index layers (mirror layers) can be formed. The spacing structures can then be formed continuously between the plurality of mirror layers.
[0061] Furthermore, the first and the second sacrificial layer can be removed, for example by way of a sacrificial layer etching process using etching holes. The etching holes can be distributed (selective etching) in the first and/or second mirror layer (not shown).
[0062]
[0063] The partial steps can relate to the production of a mirror device as shown in
[0064] According to
[0065] According to
[0066] In a further method step, according to
[0067]
[0068] The interferometer device 10 can comprise a substrate S; a first mirror device SP1 and a second mirror device SP2, wherein at least one of these mirror devices can comprise a mirror device according to the invention, as shown in
[0069] The mirror devices SP1 and/or SP2 can comprise spacing structures 4 according to the invention with or without an overhanging portion, that is to say the spacers AH, toward the top or the bottom (relative to the substrate). The spacers AH can be placed on the substrate or on different elements. The interferometer device can comprise a peripheral structure RS outside an optical region, wherein the mirror devices SP1 and SP2 may be clamped in the peripheral structure RS and be contacted thereby with a contact K. In the optical region, the mirror devices can be exposed and the light path can be influenced by aperture stops BL and antireflective layers AR on the substrate S. The interferometer device can be designed as a Fabry-Perot interferometer (FPI). The FPI can be produced by depositing a plurality of sacrificial layers, wherein a sacrificial layer can be deposited on the substrate S, then the first mirror device can be formed thereon, then a further sacrificial layer can be deposited on the first mirror device, and a second mirror device can in turn be produced thereon. The thickness of the further sacrificial layer can be used for setting the first distance d12 and be set independently of the actuation gap, with the actuation gap being formed by the actuation electrodes between the substrate S and the first mirror device SP1. An FPI of this type does not need to be advantageously limited to a travel (actuation spacing or first spacing) of a third of the original optical gap (first spacing in the deflected position).
[0070] The interferometer device can be formed as a micro-electromechanical device (MEMS), for example as a micro-spectrometer.
[0071]
[0072] The method for producing a mirror device involves providing S1 a first sacrificial layer and/or a substrate; applying S2 a first mirror layer onto the first sacrificial layer and/or onto the substrate; applying S3 a second sacrificial layer on the first mirror layer; forming S4 a recess at least in the second sacrificial layer, which extends at least up to the first mirror layer; introducing S5 a material for a spacing structure into the recess; applying S6 a second mirror layer onto the second sacrificial layer and over the recess; and at least partially removing S7 the first and the second sacrificial layer.
[0073] Even though the present invention has been described completely above with reference to the preferred exemplary embodiment, it is not limited thereto, but rather modifiable in multifarious ways.