The invention relates to a biochip comprising at least one coupling arrangement for electrical stimulation of biological material or for electrical measurements on the biological material.
EP 1 478 737 B1 discloses a biochip adapted for capacitive stimulation and/or detection of biological tissues. To improve the coupling efficiency of the purely capacitive coupling provided in this biochip, it is suggested to use a dielectric with the highest possible relative dielectric constant εr, namely TiO2.
Furthermore, semiconductor devices exist which have areas made of a ferroe-lectric material. Corresponding manufacturing processes are also known. An example of such a semiconductor device is the ferroelectric field effect transistor (FeFET). Such semi-conductor devices are used, for example, to manufacture non-volatile semiconductor memories.
Despite the progress achieved in the field of biochips with pure capacitive coupling, their stimulation efficiency is usually not sufficient to realize, for example, microelectrode arrays (MEAs) or electrically active implants with a high spatial density of electrodes. The stimulation efficiency determines the minimum area of individual electrodes for which effective electrical stimulation of the biological material, which may comprise neurons, is practical.
It would among other objects be desirable to provide a biochip with improved stimulation efficiency, with which, for example, microelectrode arrays or electrically active implants with a high density of electrodes can be realized, whereby electrochemical degradation processes at the electrodes should also be prevented.
According to an embodiment of the present disclosure, a biochip comprising at least one coupling arrangement for electrical stimulation of biological material or for electrical measurements on the biological material, is provided, the biochip comprising: a support structure arranged at and/or in the at least one coupling arrangement; and a layer, a layer surface of which is arranged at the coupling arrangement and an opposite layer surface of which forms a coupling surface for electrical stimulation of the biological material and/or for electrical measurements on the biological material; wherein the layer has ferroelectric properties. In other words, the layer of such a biochip exhibits a nonlinear and/or hysteretic relationship between an electric field E within the layer and an electric displacement density D which is caused by the presence of a ferroelectric polarization P(FE) within the layer. This nonlinear and hysteretic behavior of this relationship D(E) is also referred to as ferroelectric behavior. In this sense, materials with ferroelectric properties also include antiferroelectric materials, ferrielectric materials, multiferroic materials or relaxor ferroelectric materials. Thus, the layer may comprise ferroelectric, antiferroelectric, ferrielectric, and/or relaxor-ferroelectric materials, or may consist of any of these materials.
The inventors have recognized that the layer with ferroelectric properties causes an additional contribution to the electrical stimulation of the biological material, which comes from the ferroelectric polarization in the layer. This additional contribution occurs in addition to a contribution due to the known purely capacitive stimulation. In many cases, the additional contribution can even be higher than the contribution of the purely capacitive coupling.
For example, the layer may comprise or be formed from hafnium oxide (HfO2) with ferroelectric properties. Such ferroelectric hafnium oxide is compatible with known semiconductor processes, such as CMOS technology, allowing easy fabrication of the biochip.
Further improvement of the properties of the biochip and/or simplification of the fabrication process can be achieved by doping hafnium oxide, for example, if the hafnium oxide with ferroelectric properties is doped with silicon. Alternatively, the hafnium oxide may be doped with any of the following materials: Aluminum (Al), Germanium (Ge), Yttrium (Y), Gadolinium (Gd), Lanthanum (La) or Strontium (Sr).
For example, the hafnium oxide with ferroelectric properties may also be doped with zirconium (Zr). That is, the layer comprises or consists of a material of the class Hf1-xZrxO2.
Preferably, the material is Hf0.5Zr0.5O2. This material has a high remanent polarization Pr compared to other dopants with zirconium, making the additional contribution to electrical stimulation of biological material described above particularly pronounced.
It may also be provided that the layer comprises or consists of zirconium oxide (ZrO2) having ferroelectric properties.
Furthermore, it is also possible that the layer comprises aluminum scandium nitride with ferroelectric properties or consists of aluminum scandium nitride. Aluminum scandium nitride refers to materials of the class Al1-xScxN. On the one hand, this class of material is compatible with common manufacturing processes, which are also used to produce CMOS circuits, and on the other hand, it exhibits a particularly high remanent polarization of over 100 μC/cm2.
It is also possible that the layer comprises or consists of a ferroelectric perovskite and/or ferroelectric polymer.
The applicability of the technical teaching described here is not limited to materials with purely ferroelectric properties. It is also possible that the layer has multiferroic properties. Thus, the layer may comprise or may consist of a multiferroic material. The multiferroic material may, for example, be bismuth ferrite (BiFeO3).
It shall be understood that any material systems mentioned in the prior art, such as barium titanate (BaTiO3) or PZT (lead zirconate titanate, Pb(ZrxTi1-x)O3), do not by default have ferroelectric properties. In some publications, this is presented in an abbreviated and inaccurately simplified way. While material systems such as barium titanate and PZT can be configured such that they exhibit ferroelectric properties. However, this is by no means always the case (see for example D. J. McClure and J. R. Crowe; “Characterization of amorphous barium titanate films prepared by rf sputtering,” Journal of Vacuum Science and Technology 16, 311 1979 for barium titanate without ferroelectric properties; and Hu et al, “EXAFS study of PZT ferroelectric thin films of different crystallinities,” Journal of Physics: Conference Series 430 (2013), 15th International Conference on X-ray Absorption Fine Structure (XAFS15), 2013 for PZT without ferroelectric properties). In particular, for layers such as thin dielectric films with amorphous (possibly metallic) materials, it is not necessarily the case that these layers are configured such that they necessarily exhibit ferroelectric properties. If a material that may have ferroelectric properties as a “bulk” material (e.g., PZT or barium titanate) is fabricated as a layer or thin film, it is not necessarily the case that the fabricated layer or thin film will also have ferroelectric properties. However, it is possible to also provide a layer or thin film such that the layer or thin film has ferroelectric properties. The ferroelectric properties can be detected by measurement. Optionally, the layer with ferroelectric properties does not consist of barium titanate and/or the layer with ferroelectric properties does not consist of PZT. Optionally, the layer with ferroelectric properties does not comprise barium titanate and/or the layer with ferroelectric properties does not comprise PZT.
In particular in the case of electrical stimulation of the biological material, a thickness of the layer can be greater than 200 nm and in this case can preferably lie in the range between 200 nm and 1500 nm, in particular between 500 nm and 1500 nm or between 200 nm and 800 nm. Unlike known biochips, which exhibit exclusively capacitive coupling and thus rely on the lowest possible layer thickness to achieve the greatest possible coupling capacity, in the biochip described herein the layer thickness can be selected to be relatively high and still achieve good stimulation efficiency. The high layer thickness ensures good electrical insulation between the biochip and the biological material, i.e., low leakage currents. Furthermore, a biochip with a comparatively large layer thickness provides better long-term stability.
If the support structure comprises or consists of a substrate of a semiconductor material, the biochip can be easily fabricated using fabrication processes known from semiconductor technology. It may also be provided that the support structure comprises or consists of at least one of the following materials: polyimide, epoxy resin, parylene. These materials are biocompatible and therefore particularly suitable for manufacturing the biochip. However, other biocompatible and/or dielectric materials may also be used.
In particular, if the biochip is (also) adapted for electrical measurements on the biological material, the layer may form part of a ferroelectric field effect transistor (FeFET) of the biochip. Herein, the FeFET may form part of an input stage of a respective measurement circuitry. It is also possible that the FeFET belongs to an artificial neuron. This may, for example, be coupled to a biological neuron which is present in the biological material.
Hereby, it is possible that the coupling surface comprises or forms a gate electrode of the ferroelectric field effect transistor. Hereby, the layer can correspond to a ferroelectrically acting insulating layer of the FeFET. Alternatively, a multilayer structure of the gate region of the FeFET is also conceivable, wherein the gate region comprises the ferroelectric layer and a further layer, which may be an insulating layer.
The biochip can be adapted such that it has memresistive or memristive properties. In particular, the layer can be adapted such that a ferroelectric tunnel contact is formed. The biochip may be configured as a memristor. In particular, if the layer with ferroelectric properties is particularly thin, the memristive properties can occur in particular by forming a so-called ferroelectric tunnel contact. Memristive properties can then occur due to the ferroelectric properties of the layer between the electrodes: For example, because a ferroelectric tunnel contact is formed. Thus, the biochip may be adapted for a ferroelectric tunnel contact to form. A thickness of the layer with ferroelectric properties is, for example, less than or equal to 10 nm, in particular less than or equal to 7.5 nm, in particular less than or equal to 5 nm. A biochip adapted as a memristor can be used as an artificial synapse.
The biochip may be adapted to be used as part of an arrangement that couples at least one artificial neural network to a biological neural network. The biochip may be adapted to couple an artificial neuron to a biological neuron.
The biochip can comprise a plurality of coupling surfaces of different coupling arrangements of the biochip, which are separated from each other. Hereby, a coupling surface can be respectively assigned to each coupling arrangement. In this way, a multi-channel biochip can be provided. The coupling surfaces (coupling areas) can for example be arranged along a line or in a grid. Such a biochip can have several layers with ferroelectric properties separated from each other.
According to a further embodiment, a method of fabricating a biochip comprising at least one coupling arrangement for electrical stimulation of biological material or for electrical measurements on the biological material is provided, the method comprising: arranging a support structure at and/or in the coupling arrangement; and fabricating a layer such that its one layer surface is arranged at the coupling arrangement and its opposite layer surface forms a coupling surface for electrical stimulation of the biological material and/or for electrical measurements on the biological material, wherein the layer is fabricated as a layer with ferroelectric properties. With such a method, the advantages described above in connection with the biochip can be realized. The features of the biochip can be provided accordingly in the method.
Another embodiment comprises an electrically active implant comprising the biochip described herein.
The implant may, for example, be a retinal implant, a cochlear implant, an implant for deep brain stimulation, and/or an implant for providing a brain-machine interface. In general, implants may be provided for stimulating neurons and/or providing measurements on neurons, wherein such implants comprise at least one biochip described herein.
In yet another embodiment, an in vitro assembly comprising a biochip described herein and an electrolyte receptacle, that is, an arrangement for receiving an electrolyte, is disclosed, wherein the electrolyte receptacle is adapted to dispose the electrolyte on at least one coupling surface of the biochip for electrical stimulation of the biological material and/or electrical measurement of the biological material.
Hereby, an in vitro assembly comprising at least one biological neuron and at least one artificial neuron may be provided. For example, the biological neuron may be formed by a neuron of the biological material present in the electrolyte. The artificial neuron may comprise an FeFET, which may be part of the biochip and may be embodied as described above.
The implant or in vitro device may comprise a semiconductor chip separate from the biochip, wherein a terminal of the semiconductor chip is electrically connected via a conductor track to an electrode layer adjacent to the layer surface and the conductor track and the biochip are arranged on a common substrate.
Further features and advantages may be apparent from the following description. Herein:
The arrangement 11 may for example be an electrically active implant such as a neuroprosthesis. The arrangement may be a cochlear or retinal implant. Further, the arrangement 11 may be an implant for deep brain stimulation for treating neurological conditions such as Parkinson's disease. In such neuroprostheses 11, it may be provided that all coupling surfaces 15 of the at least one biochip 13 are adapted for stimulation of neurons (nerve cells).
Alternatively, the arrangement may be an in vitro arrangement comprising a microelectrode array (MEA) comprising microelectrodes corresponding to coupling surfaces 15. Such an in vitro arrangement may comprise at least one biological neuron formed by a neuron located in the biological tissue and/or at least one artificial neuron belonging to the biochip 13. Such an arrangement may be applied, for example, to the study of neural networks or neural tissue. The biological material can be arranged in an electrolyte that can be brought into contact with the biochip 13, in particular its coupling surfaces 15, via a suitable electrolyte receptacle of the arrangement 11, such as an electrolyte container 16.
Known devices 11 (for example neuroprostheses and not purely capacitive MEAs) feature electrically conductive (metallic) electrodes. Such electrodes allow a high charge transfer per unit area (stimulation efficiency) of electrical charge between the biological material and the biochip 11. The high stimulation efficiency allows the area of the individual electrodes to be kept small, which in turn allows a high area density of electrodes. However, it should be noted that a threshold of charge density to be transferred to the nerve tissue required for successful stimulation of nerve cells depends on the size of the electrodes or coupling surfaces 15.
A disadvantage of conductive electrodes is that irreversible electrochemical processes in the form of a Faraday current can occur at the electrode/electrolyte interface, which can lead to degradation of the electrode or lead to cell damage in the biological material. Faraday currents at the electrodes can be avoided, at least to a large extent, if a biochip with pure capacitive coupling is used. Such a biochip usually has conductive regions (for example, p-doped regions in silicon) covered with a dielectric layer that prevents Faraday currents. However, the stimulation efficiency of these biochips is relatively low and is determined in particular by the relative dielectric constant of the dielectric layer and its thickness. Thus, efforts are made to use materials with the highest possible relative dielectric constant and to keep the thickness of the layer low. However, a low layer thickness can lead to increased leakage currents, which counteracts the goal of reducing irreversible processes.
In the arrangement 11 described herein, the biochip 13 comprises at least one layer 17 with ferroelectric properties confined by the coupling surface 15.
The basic structure of the biochip 13 is shown in detail in
The coupling surface 15 of the layer 17 delimits the biochip to an area 25 where the biological material is arranged. The biological material may be in an electrolyte 24. The biochip 13 and the region 25 comprising the biological material are components of the biochip arrangement or assembly 11. The biological material may include at least one neuron that may form a biological neuron.
In the shown example, the coupling surface 15 provides an electrode with a substantially smooth surface. In an example not shown, the coupling surface 15 is machined to have an increased surface area. This can increase an actively effective surface area to further increase charge transfer. The coupling surface 15 can overall be circular with a diameter of 5 μm to 200 μm, in particular 5 μm to 100 μm, in particular 30 μm. The coupling surface 15 may also have another shape, for example a rectangular or square shape or the shape of any other polygon (preferably with the same area as the circular coupling area). If several coupling areas 15 are provided per biochip 13, they may have a smallest distance of 5 μm to 500 μm from each other.
If the biological material (e.g. a nerve cell) in the electrolyte 24 is to be stimulated, an electrical voltage is applied to the electrode layer 27 and the counter electrode. U(t) is applied to the electrode layer 27 acting as an electrode and the counter electrode. Unlike devices with only electrically conductive electrodes, the electrolyte 24 is electrically insulated from the electrode layer 27 so that no direct current can flow that would lead to electrochemical charge transport.
As shown in
The displacement current density is given as the time derivative
For a material with ferroelectric properties is D(E)=ε0εrE+P(FE)(E) where ε0 denotes the permittivity of the vacuum.
In the case of a ferroelectric layer, the displacement current density
in electrolyte 24 is therefore composed of two components. One component is caused by a temporal change in the dielectric polarization P(DE) which, in turn, is influenced by the electric field E(t) within the layer 17 corresponding to the voltage U(t) electric field. This purely dielectric displacement current density is proportional to the dielectric constant ∈r of layer 17 and forms the only contribution in purely capacitive stimulation of biological material. In the case of a layer with ferroelectric properties, however, a further contribution occurs, which is caused by the temporal change in the ferroelectric polarization P(FE) which in turn is also influenced by the electric field E(t) within the layer 17 corresponding to the voltage. U(t). For a layer 17 of thickness d (see
From the understanding of the nonlinear and hysteretic relationship D(E) shown in
When the polarity of a ferroelectric material is reversed, which, for example, has the hysteresis curve D(E) shown in
ρstim=Cs(Umax−Umin)+2Pr
Wherein Cs is the capacitance per unit area (measured e.g. in μF/cm2) of a plate capacitor formed by the two layer surfaces 15, 19 and Pr corresponds to the amount of the remanent polarization of the ferroelectric material of the layer 17.
The contribution resulting from the ferroelectric properties 2Pr of the transferred charge density ρstim results from the fact that the voltage U(t) produced by the voltage source 31 causes a polarity reversal of the remanent polarization Pr in the layer 17. For driving the biochip 13, the amplitude of the voltage signal U(t) can be selected in such a way that the corresponding field strength E in layer 17 is in terms of its magnitude at least as large as the coercive field strength EC.
The layer 17 may consist of or at least comprise hafnium oxide (HfO2) with ferroelectric properties or doped hafnium oxide with ferroelectric properties.
For example, the layer 17 can consist of or at least comprise hafnium oxide doped with zirconium (Hf1-xZrxO2). For x=0.5 follows Hf0.5Zr0.5O2, which allows to produce the layer 17 with a thickness of d=9.5 nm. Such a layer 17 has the following properties at Umin=0V and Umax=1V:
∈r=40, CS=3.7 μF/cm2, EC=100 or 1000 kV/cm, Pr=16 μC/cm2, ρstim=35.7 μC/cm2
It can be seen that the contribution 2Pr in this example is already 32 μC/cm2 thus far exceeds the contribution achieved by purely capacitive stimulation.
The material which the layer 17 may also consist of or comprise aluminum scandium nitride (Al1-xScxN) with ferroelectric properties. This material is compatible with semiconductor fabrication processes that are also used for fabrication of CMOS circuits. Because of its relatively high remanent polarization of over 100 μC/cm2 transmittable charge densities of more than 200 μC/cm2 result.
Furthermore, the material that the layer 17 consists of or that the layer 17 comprises can also be an antiferroelectric. For example, the material may be silicon (Si) doped hafnium oxide (HfO2). Antiferroelectrics have a characteristic D(E) shown qualitatively in
Finally, the material that the layer 17 comprises or that the layer consists of may also have multiferroic properties, i.e., be both ferroelectric and ferromagnetic. For example, this may be bismuth ferrite (BiFeO3).
Since the stimulation efficiency is largely determined by the ferroelectric properties, the thickness d of the layer 17 can be chosen comparatively large. Instead of the above-mentioned value of d=9.5 nm mentioned above, significantly larger values are also possible, e.g. more than 200 nm, 200 nm to 1500 nm, 200 nm to 800 nm or 500 nm to 1500 nm.
However, another effect can also be used. If the layer with ferroelectric properties is particularly thin, the memristive properties can occur in particular by forming a so-called ferroelectric tunnel contact. The biochip may thus be adapted for a ferroelectric tunnel contact to be formed. A thickness of the layer with ferroelectric properties is, for example, less than or equal to 100 nm, in particular less than or equal to 50 nm, in particular less than or equal to 20 nm, in particular less than or equal to 10 nm, in particular less than or equal to 7.5 nm, in particular less than or equal to 5 nm. in particular less than or equal to 4 nm in particular less than or equal to 2.5 nm.
It shall be understood that the ferroelectric layer 17 may be arranged not only exclusively in a planar (2D) plate capacitor design, but also in other arrangements such as a 3D capacitor structure such as a so-called deep-trench capacitor.
The substrate layer 29, the drain region 35 and the layer 17 form a ferroelectric field effect transistor (FeFET). The coupling surface 15 of the layer 17 corresponds to a gate contact of the FeFET 39, which is electrically connected to the electrolyte 24. The layer 17 forms an insulating layer of the FeFET 39, which is comparable to a gate oxide of a classical MOSFET. The drain region 35, the source region 37, and the substrate layer 29 are electrically connected to respective terminals UD, US, and UB of the FeFET 39, which form a drain contact, a source contact, and a bulk contact of the FeFET 39, respectively. The electrolyte 24 may be brought to a reference potential, for example a ground potential GND, with a reference electrode. Here, it may be provided that the bulk terminal UB of the FeFET is at the same electrical potential as the electrolyte 24 and/or that the reference electrode is integrated into the substrate layer 29.
The FeFET 39 may form a part of an input stage of the biochip arrangement 11, which is adapted for electrical measurements on biological material, in particular on neurons arranged therein. Furthermore, the FeFET 39 may further form a part of an artificial neuron. Overall, the biochip arrangement 11 can be used to perform studies on neural tissue. The biochip arrangement 11 may be used for neuromorphic computing. Furthermore, the biochip arrangement 11 may be a brain-machine interface, in particular a brain-computer interface.
A measuring device of the biochip 11 can also be implemented as shown in
Another example of a measuring device is the arrangement 11 shown in
In the measuring arrangement, the elements 43, 27 and 17 may be provided a plurality of times and arranged side by side, for example in a direction at least substantially orthogonal to the drawing plane of
The arrangement 11 in
In conclusion, a biochip 13 is described herein that exhibits the nonlinear and hysteretic pattern D(E) shown in
Number | Date | Country | Kind |
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10 2020 126 759.2 | Oct 2020 | DE | national |
10 2020 132 756.0 | Dec 2020 | DE | national |
This application is a Continuation of International Patent Application PCT/EP2021/084639, filed Dec. 7, 2021 and designating the United States, which was published in German as WO 2022/122756 A1, and claims priority to German patent application DE 10 2020 132 756.0, filed Dec. 9, 2020. This application is also at Continuation-in-Part of U.S. patent application Ser. No. 18/133,100 filed Apr. 11, 2023, which is a Continuation application of International Patent Application PCT/EP2021/077671, filed Oct. 7, 2021 and designating the United States, which was published in German as WO 2022/078864 A1, and claims priority to German patent application DE 10 2020 126 759.2, filed Oct. 12, 2020, each of which are incorporated herein by reference in their entirety.
Number | Date | Country | |
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Parent | PCT/EP2021/084639 | Dec 2021 | US |
Child | 18205755 | US | |
Parent | PCT/EP2021/077671 | Oct 2021 | US |
Child | 18133100 | US |
Number | Date | Country | |
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Parent | 18133100 | Apr 2023 | US |
Child | PCT/EP2021/084639 | US |