Method for preparing layered metal oxide field effect material

A method for preparing a layered metal oxide field effect material includes depositing a first metal oxide, a core-layer metal, and a second metal oxide sequentially on the substrate by vacuum vapor deposition, the first metal oxide and the core-layer metal undergoing a redox reaction to form a first surface layer and a core-layer precursor on the substrate, and the core-layer precursor and the second metal oxide undergoing a redox reaction to form a core layer and a second surface layer; and the band gap of the metal oxide in the core layer is ≥3 eV, the band gaps of the metal oxide in the first surface layer and the second surface layer are independently ≤3 eV, and the difference between the band gap of the metal oxide in the core layer and the band gap of the metal oxide in the first surface layer is ≥1 eV. The present preparation method has advantages of simple operation, a low production cost, a good film forming property, and the high carrier mobility of the product.

This application claims priority to Chinese patent application number 201810695671.2, filed on Jun. 29, 2018, entitled “METHOD FOR PREPARING LAYERED METAL OXIDE FIELD EFFECT MATERIAL”, which is incorporated herein by reference in its entirety.

TECHNICAL FIELD

The present invention relates to the field of semiconductor integrated circuit technology, and in particular to a method for preparing a layered metal oxide (LMO) field effect material.

BACKGROUND

The development level of integrated circuits has become a hallmark of a country's industrial development level. At present, the widely used semiconductor material for integrated circuits is a hydrogenated amorphous silicon material (a-Si:H), but it has low field effect mobility (about 0.5-1.0 cm2/V·s), poor light transmission, low carrier density and mechanical flexibility that is less than ideal, and it is not easy to be used to prepare a high-performance and flexible active matrix liquid crystal display (AMLCD), an active matrix organic light-emitting diode (AMOLED) and the like mainstream displays and flexible integrated circuits.

With the rapid development of integrated circuits, the metal oxide field effect material is widely used in the electronic industry since it has advantages such as having a simpler preparation process and a cheaper cost as compared with other materials, having uniform film formation, being capable of enabling high performance and high integration, and being capable of preparing transparent integrated circuits and flexible integrated circuits. However, the current carrier mobility of the metal oxide field effect material is still low, and less than 10 cm2/V·s; and in order to improve the carrier mobility of the metal oxide field effect material, it is required to fabricate the metal oxide field effect material into a crystal phase structure with a relatively high cost, and even a substrate thereof with a crystalline structure is required.

The metal oxide field effect material, as a thin-film material, is obtained in a microelectronic process through a preparation method which mainly includes physical vapor deposition (PVD), chemical vapor deposition (CVD), epitaxy, electrochemistry deposition (ECD) and so on. Among them, the physical vapor deposition becomes the most commonly used method for preparing the thin film because of its advantages such as an easily-controlled thickness, a simple reaction mechanism, a fast film forming speed and high efficiency. The physical vapor deposition method mainly includes several methods such as sputter coating, ion plating, vacuum evaporation, and so on. The sputter coating is the use of a certain amount of energy particles (ionic or neutral atoms, molecules) that generated by gas discharge plasma to bombard a surface of a solid at a low pressure, so that atoms or molecules near the surface of the solid get large enough energy to finally escape from the surface of the solid, which can be used to prepare a variety of thin-film materials such as metals, semiconductors, and insulators, etc.; and however, for the sputter coating, the equipment is complex and requires a high-voltage device or a magnetic control unit, and a target material needs to be refined, has a low utilization rate, and is susceptible to impurities. The ion plating is the use of gas discharge to ionize a gas or an evaporated substance under a vacuum condition, and further to vapor-deposit the evaporated substance or its reactant onto a substrate while ions of the gas or evaporated substance exert a bombardment effect; and however, for the ion plating, it is necessary to introduce gas discharge, and the devices and operations are complicated.

SUMMARY

An object of the present invention provides a method for preparing a layered metal oxide field effect material. The preparation method provided by the present invention has advantages of simple operation, a low production cost, a good film forming property, and the high carrier mobility of the prepared layered metal oxide field effect material.

In order to achieve the above object, the present invention provides the following technical solutions:

The present invention provides a method for preparing a layered metal oxide field effect material, including the following steps:

depositing a first metal oxide, a core-layer metal, and a second metal oxide sequentially on a substrate by vacuum vapor deposition, the first metal oxide and the core-layer metal undergoing a redox reaction to form a first surface layer and a core-layer precursor on the substrate, and the core-layer precursor and the second metal oxide undergoing a redox reaction to form a core layer and a second surface layer;

where the band gap of the metal oxide in the core layer is ≥3 eV, the band gaps of the metal oxides in the first surface layer and the second surface layer are independently ≤3 eV, and the difference between the band gap of the metal oxide in the core layer and the band gap of the metal oxide in the first surface layer is ≥1 eV.

Preferably, the first metal oxide and the second metal oxide are MoO3.

Preferably, the first metal oxide and the second metal oxide are used in the form of a thin film, and the thicknesses of the first metal oxide and the second metal oxide are independently from 1 to 10 nm.

Preferably, the core-layer metal is Al.

Preferably, the core-layer metal is used in the form of a thin film, and the thickness of the core-layer metal is from 1 to 10 nm.

Preferably, the substrate includes a silicon substrate or a glass substrate.

The present invention provides a method for preparing a layered metal oxide field effect material, including the following steps: depositing a first metal oxide, a core-layer metal, and a second metal oxide sequentially on a substrate by vacuum vapor deposition, the first metal oxide and the core-layer metal undergoing a redox reaction to form a first surface layer and a core-layer precursor on the substrate, and the core-layer precursor and the second metal oxide undergoing a redox reaction to form a core layer and a second surface layer; where the band gap of the metal oxide in the core layer is ≥3 eV, the band gaps of the metal oxides in the first surface layer and the second surface layer are independently ≤3 eV, and the difference between the band gap of the metal oxide in the core layer and the band gap of the metal oxide in the first surface layer is ≥1 eV. The preparation method provided by the present invention has the advantages of simple operation, a low production cost and a good film forming property. The layered metal oxide field effect material prepared using the method provided by the present invention forms a heterojunction from metal oxides with different band gaps, and defines a band gap difference (ΔE)≥1 eV. Band bending is generated at the interface of the heterojunction, such that a potential barrier is formed on the side with the larger band gap and a triangular potential well is formed on the side with the smaller band gap, and under the induction of a gate electric field, a polarized charge is generated at the interface of the heterojunction, and a large number of carriers are accumulated. Therefore, the layered metal oxide field effect material provided by the present invention has high carrier mobility higher than 103cm2/V·s, and overcomes the problem that the carrier mobility of a conventional metal oxide field effect material is low, it is required to fabricate the metal oxide field effect material into a crystal phase structure with a relatively high cost, and even that a substrate thereof with a crystal phase structure is required, which can be widely used in the fields of field effect transistors, field effect transparent electrodes, driving organic light-emitting diodes, logic circuits, memories or flexible semiconductor integrated circuits.

Furthermore, the layered metal oxide field effect material prepared using the method provided by the present invention has a thickness not more than 30 nm and thus has good light transmittance.

DETAILED DESCRIPTION

The present invention provides a method for preparing a layered metal oxide field effect material, including the following steps: depositing a first metal oxide, a core-layer metal, and a second metal oxide sequentially on a substrate by vacuum vapor deposition, the first metal oxide and the core-layer metal undergoing a redox reaction to form a first surface layer and a core-layer precursor on the substrate, and the core-layer precursor and the second metal oxide undergoing a redox reaction to form a core layer and a second surface layer; where the band gap of the metal oxide in the core layer is ≥3 eV, the band gaps of the metal oxides in the first surface layer and the second surface layer are independently ≤3 eV, and the difference between the band gap of the metal oxide in the core layer and the band gap of the metal oxide in the first surface layer is ≥1 eV.

In the present invention, the first metal oxide and the second metal oxide preferably independently include AgO, Bi2O5, CeO2, Co2O3, CuO, Fe2O3, Mn2O7, MoO3, PbO2, V2O5or WO3, and more preferably MoO3.

In the present invention, the first metal oxide and the second metal oxide are preferably used in the form of a thin film, and the thicknesses of the first metal oxide and the second metal oxide are independently from 1 to 10 nm, more preferably from 2 to 7 nm, and most preferably from 3 to 5 nm.

In the present invention, the core-layer metal is preferably used in the form of a thin film, and the thickness of the core-layer metal is preferably from 1 to 10 nm, more preferably from 2 to 7 nm, and most preferably from 3 to 5 nm.

In the present invention, the degree of vacuum in the vacuum vapor deposition method is preferably 10−4to 10−5Pa, and the vapor-deposition distance is preferably 20 to 30 cm.

In the present invention, in the vacuum vapor deposition method the core-layer metal has the evaporation temperature which is specifically determined according to the evaporation temperature of an actual metal and is preferably 200-1000° C., and more preferably 500-750° C.; the evaporation current which is preferably 160-180 A; and the evaporation rate which is preferably 1-2 Å/s. In the present invention, accumulation of the evaporation material on the substrate will be caused if the evaporation rate of the core-layer metal is too small, and a large gap of the evaporation material on the substrate will be caused if the evaporation rate is too large.

In the present invention, in the vacuum vapor deposition method the first metal oxide and the second metal oxide have evaporation temperatures which are specifically determined according to the evaporation temperatures of actual metal oxides, and are preferably 500-1500° C., and more preferably 570˜700° C. independently; the evaporation currents which are preferably 4 to 5 A independently; and the evaporation rates which are preferably 0.1 to 0.5 Å/s independently. In the present invention, accumulation of the evaporation material on the substrate will be caused if the evaporation rates of the first metal oxide and the second metal oxide are too small, and a large gap of the evaporation material on the substrate will be caused if the evaporation rates are too large.

The present invention has no special limitation on the substrate, and a substrate well known to those skilled in the art may be used, particularly such as a silicon substrate or a glass substrate.

In the present invention, the purities of the first metal oxide and the second metal oxide are preferably ≥99.95% independently, and the purity of the core-layer metal is preferably ≥99.99%.

In the present invention, by using the vacuum vapor deposition method, firstly the first metal oxide is deposited on the substrate, and then during the deposition of the core-layer metal, the first metal oxide and the core-layer metal undergo a redox reaction to form the first surface layer and the core-layer precursor on the substrate, and finally during the deposition of the second metal oxide, the core-layer precursor and the second metal oxide undergo a redox reaction to form the core layer and the second surface layer.

The layered metal oxide field effect material prepared by the preparation method of the above technical solution of the present invention has a sandwich structure, which sequentially includes the first surface layer, the core layer and the second surface layer, the core layer being a metal oxide layer with a wide band gap, and the first surface layer and the second surface layer being metal oxide layers with narrow band gaps; where, the band gap of the metal oxide in the core layer is ≥3 eV, the band gaps of the metal oxides in the first surface layer and the second surface layer are independently ≤3 eV, and the difference between the band gap of the metal oxide in the core layer and the band gap of the metal oxide in the first surface layer is ≥1 eV.

In the present invention, the thickness of the layered metal oxide field effect material is preferably ≤30 nm, more preferably 10 to 25 nm, and most preferably 10 to 15 nm.

In the present invention, the thicknesses of the first surface layer, the second surface layer and the core layer are preferably ≤10 nm, more preferably 3 to 8 nm, and most preferably 5 to 6 nm independently.

In the present invention, the core layer is a metal oxide layer with a wide band gap, and the band gap of the metal oxide in the core layer is ≥3 eV, preferably 3.5 to 7 eV, and more preferably 4 to 5 eV. In the present invention, the metal oxide in the core layer preferably includes a binary metal oxide or a ternary metal oxide; the binary metal oxide in the core layer preferably includes Al2O3, Cr2O3, CaO, Ga2O3, La2O3, MnO, Nb2O5, Nd2O3, NiO, Pr2O3, Sb2O3, Sm2O3, SnO, SnO2, Ta2O5, Tb2O3, TiO2, ZnO or ZrO2; and the ternary metal oxide in the core layer preferably includes AlTiO3, BaTiO3, KNbO3, KTaO3, LaTi2O7, LiTaO3, LiNbO3, MgTiO3, MnTiO3, SrTiO3or ZnTiO3.

In the present invention, the metal oxide in the core layer and its corresponding conduction band, valence band energy level and band gap are as shown in the table below:

The type of the metal oxide in the core layer and its correspondingconduction band, valence band energy level and band gapConductionValence BandBandMetalBandEnergy LevelGapOxide(Ec)(Ev)(Eg)Al2O35.412.47Cr2O3−0.572.933.5CaO−1.093.915 eVGa2O3−1.553.254.8La2O3−1.973.535.5MnO−1.012.593.6Nb2O50.093.493.4Nd2O3−1.633.074.7NiO−0.53.03.5Pr2O3−1.262.643.9Sb2O30.323.323Sm2O3−1.432.974.4SnO−0.913.294.2SnO203.53.5Ta2O5−0.173.834Tb2O3−1.062.743.8TiO2−0.292.913.2ZnO−0.312.893.2ZrO2−1.093.915SrTiO3−1.262.143.4AlTiO3−0.862.743.6BaTiO30.083.383.3KNbO3−0.862.443.3KTaO3−0.932.573.5LaTi2O7−0.63.44LiTaO3−0.953.054LiNbO3−0.732.773.5MgTiO3−0.752.953.7MnTiO3−0.462.643.1ZnTiO3−0.232.833.06

In the present invention, the first surface layer and the second surface layer are metal oxide layers with narrow band gaps; and the band gaps of the metal oxides in the first surface layer and the second surface layer are independently ≤3 eV, preferably 0-2.5 eV, and more preferably 1-2 eV. In the present invention, the metal oxides in the first surface layer and the second surface layer are preferably binary metal oxides independently, and the binary metal oxides in the first surface layer and the second surface layer preferably include Ag2O, Bi2O3, Ce2O3, CoO, Cu2O, FeO, Fe3O4, MnO2, MoO2, PbO, VO, VO2, WO or WO2independently.

In the present invention, the partial binary metal oxides in the first surface layer and the second surface layer and their corresponding conduction bands, valence band energy levels and band gaps are as shown in the table below:

partial binary metal oxides in the first surface layer andthe second surface layer and their corresponding conductionbands, valence band energy levels and band gapsConductionValence BandBandMetalBandEnergy LevelGapOxide(Ec)(Ev)(Eg)Ag2O0.191.391.2Bi2O30.333.132.8Ce2O3−0.51.92.4CoO−0.112.492.6Cu2O−0.281.922.2FeO−0.172.232.4Fe3O41.231.330.1MnO21.331.580.25MoO20PbO−0.482.322.8

In the present invention, the difference between the band gap of the metal oxide in the core layer and the band gap of the metal oxide in the first surface layer is ≥1 eV, preferably 1.5 to 7 eV, and more preferably 2.0 to 4.0 eV.

In the embodiments of the present invention, particularly a thin MoO3film (with the thickness of 2 nm), a thin Al film (with the thickness of 2 nm), and a MoO3film (with the thickness of 3 nm) are sequentially deposited on the substrate by vacuum vapor deposition, to form a layered metal oxide field effect material on the substrate. The layered metal oxide field effect material includes a first surface layer of MoO2, a core layer of Al2O3, and a second surface layer of MoO2. The following reaction will occur at the interface of two different materials:
2Al(s)+3MoO3(s)→Al2O3(s)±3MoO2(s)

where, a redox reaction occurs at the interface between the thin MoO3film at the bottom layer and the thin Al film at the interlayer, and MoO3loses an oxygen atom to become MoO2, where the valence state of molybdenum changes from +6 to +4, and the thin Al film at the interlayer is oxidized to Al2O3; and similarly, the interface between the thin MoO3film at the top layer and the thin Al film at the interlayer also undergoes a redox reaction, in which MoO3loses an oxygen atom to become MoO2, where the valence state of molybdenum changes from +6 to +4, and the thin Al film at the interlayer is oxidized to Al2O3.

In chemical thermodynamics, a thermodynamic function G, called Gibbs free energy or free enthalpy, is introduced to judge the direction of the reaction. In the isothermal-isobaric reaction, if the Gibbs free energy G is negative, the positive reaction is spontaneous, otherwise the reverse reaction is spontaneous; and if it is 0, the reaction is in equilibrium. The amount of change in Gibbs free energy of the redox reaction involved in the present invention is as follows:

The standard Gibbs free energy in the redox reaction equation can be calculated from the redox reaction equation below:
2Al(s)+3MoO3(s)→Al2O3(s)+3MoO2(s)
ΔG=−281.39 kcal/since

the Gibbs free energy G of the redox reaction is changed to −281.39 kcal/mol, the redox reaction proceeds spontaneously toward the positive reaction direction.

In the present invention, the layered metal oxide field effect material of the above technical solution can be applied in the fields of field effect transistors, field effect transparent electrodes, driving organic light-emitting diodes, logic circuits, memories or flexible semiconductor integrated circuits. In the present invention, the field effect transistor preferably includes an organic field effect transistor, an inorganic field effect transistor, a thin film transistor, an insulated gate field effect transistor or a junction field effect transistor, more preferably an organic field effect transistor, and most preferably a flexible organic field effect transistor.

In the present invention, the flexible organic field effect transistor preferably includes a source/drain electrode10, a layered metal oxide field effect material11disposed on the source/drain electrode, a gate insulation layer12disposed on the layered metal oxide field effect material, and a gate electrode13disposed on the gate insulation layer, as shown inFIG. 1.

In the present invention, the flexible organic field effect transistor preferably includes the source/drain electrode10; the source/drain electrode10preferably includes a source electrode101and a drain electrode102. In the present invention, the electrode material for forming the source electrode and the drain electrode preferably includes a metal conductive material or a metal oxide conductive material independently; the metal conductive material preferably includes Ag, Cu, Au, Al, W, Ni, Ti, Zn, Cr or Mo; and the metal oxide conductive material preferably includes indium tin oxide (ITO), indium zinc oxide (IZO) or SnO. In the embodiments of the present invention, particularly Al is used as the electrode material for forming the source electrode and the drain electrode.

In the present invention, the flexible organic field effect transistor preferably includes the layered metal oxide field effect material11disposed on the source/drain electrode. In the present invention, it is only required that the surface layer of the layered metal oxide field effect material is in contact with the source/drain electrodes, and for example the first surface layer or the second surface layer of the layered metal oxide field effect material is in contact with the source/drain electrode. In the embodiments of the present invention, the layered metal oxide field effect material11particularly includes a first surface layer111, a core layer112, and a second surface layer113, where the first surface layer111is in contact with the source/drain electrodes. In the present invention, the layered metal oxide field effect material is used as a P-channel material in the flexible organic field effect transistor; and in the embodiments of the present invention, the channel has a length of particularly 6 mm, and a width of particularly 16 mm.

In the present invention, the flexible organic field effect transistor preferably includes the gate insulation layer12disposed on the layered metal oxide field effect material. In the present invention, the gate insulation layer preferably includes an organic light-emitting layer121and a hole transport layer122disposed on the organic light-emitting layer. In the present invention, the thickness of the organic light-emitting layer is preferably 50 to 60 nm, and the thickness of the hole transport layer is preferably 40 to 45 nm. The present invention has no special limitation on the organic light-emitting material used for forming the organic light-emitting layer and the hole transport material used for forming the hole transport layer, and the organic light-emitting material and the hole transport material well known to those skilled in the art may be used. In the embodiments of the present invention, particularly tris (8-hydroxyquinolinato) aluminum (Alq3) is used as the organic light-emitting material, and N,N′-bis(1-naphthyl)-N,N′-diphenyl-1,1′-biphenyl-4-4′-diamine (NPB) is used as the hole transport material.

In the present invention, it is only required that the gate insulation layer is in contact with the surface layer of the layered metal oxide field effect material, and for example the gate insulation layer is in contact with the first surface layer or the second surface layer of the layered metal oxide field effect material. In the embodiments of the present invention, particularly the organic light-emitting layer121of the gate insulation layer is in contact with the second surface layer113of the layered metal oxide field effect material.

In the present invention, the flexible organic field effect transistor preferably includes a gate electrode13disposed on the gate insulation layer. The present invention has no special limitation on the gate material used to form the gate electrode, and an electrode material well known to those skilled in the art may be used. In the embodiments of the present invention, particularly Al is used as the electrode material for forming the gate electrode.

The technical solutions in the present invention will be clearly and completely described below in connection with the Examples of the present invention. Obviously, the described Examples are only part of the Examples of the present invention, not all of the embodiments. Based on the embodiments of the present invention, all other Examples obtained by those of ordinary skill in the art on the premise of not paying creative labor belong to the claimed scope of the present invention.

A thin MoO3film (with a purity of 99.95%, and a thickness of 2 nm), a thin Al film (with a purity of 99.99%, and a thickness of 2 nm), and a thin MoO3film (with a purity of 99.95%, and a thickness of 3 nm) were sequentially deposited on a silicon substrate by vacuum vapor deposition, so as to form a layered metal oxide field effect material on the silicon substrate. The layered metal oxide field effect material included a first surface layer111of MoO2(with a thickness of 2 nm, being in contact with the silicon substrate), a core layer112of Al2O3(with a thickness of 2 nm), and a second surface layer113of MoO2(with a thickness of 3 nm), where the operating parameters for depositing the thin Al film were: a vacuum degree of 10−5Pa, a vapor-deposition distance of 30 cm, a evaporation temperature of 750° C., an evaporation current of 180 A, and an evaporation rate of 1 Å/s; and the operating parameters for depositing the MoO3film were: a vacuum degree of 10−5Pa, a vapor-deposition distance of 30 cm, an evaporation temperature of 570° C., an evaporation current of 4.5 A, and an evaporation rate of 0.5 Å/s.

In order to demonstrate the valence structures of respective substances in the layered metal oxide field effect material, X-ray photoelectron spectroscopy analysis was performed on the layered metal oxide field effect material, and the result was as shown inFIG. 2.FIG. 2was a Mo 3d and Al 2p core X-ray photoelectron spectroscopy of samples at different stages of the layered metal oxide field effect material deposited on the silicon substrate (the deposited raw materials were the thin MoO3film (2 nm), the thin MoO3film (2 nm)/the thin Al film (2 nm), the thin MoO3film (2 nm)/the thin Al film (2 nm)/the thin MoO3film (3 nm) respectively. It could be seen fromFIG. 2, the result of the spontaneous redox chemical reaction at the interface was that a structure of Mo4+/Al3+/Mo4+was formed in the layered metal oxide field effect material.

In order to compare topographic characteristics of a single thin film and the layered metal oxide field effect material, the thin MoO3film and the thin Al film were deposited on formvar stabilized with carbon support films under the same conditions to form a flat thin film with an amorphous structure, and the result was as shown inFIG. 3.FIG. 3was the transmission electron micrographs of the layered metal oxide field effect material (the raw materials are the thin MoO3film (2 nm)/the thin Al film (2 nm)/the thin MoO3film (3 nm)) prepared in Example 1, a single thin MoO3film (the raw material was the thin MoO3film (2 nm)) and the thin Al film (the raw material was the thin Al film (2 nm)), and the transmission electron microscope diffraction pattern of the layered metal oxide field effect material. As can be seen fromFIG. 3, the single thin Al film and the thin MoO3film were uniformly deposited on the formvar stabilized with carbon support films, and the layered metal oxide field effect material also had a uniform and flat surface structure, and one layer of an amorphous thin film structure was formed because the substrate was not heated.

In order to verify the interface stacking characteristics of the layered metal oxide field effect material provided by the present invention, a multilayer layered metal oxide field effect material MoO2(2 nm)/Al2O3(2 nm)/MoO2(4 nm)/Al2O3(2 nm)/MoO2(4 nm)/Al2O3(2 nm)/MoO2(4 nm) was prepared according to the method of Example 1.FIG. 4was a cross-sectional STEM image of the multilayer layered metal oxide field effect material prepared in this example. It could be seen fromFIG. 4, the interface between the thin MoO2film and the thin Al2O3film exhibited a distinct interface (white represented MoO2film, and gray black represented the thin Al2O3film).

The layered metal oxide field effect material prepared in Example 1 was used as a P-channel material (with a channel length set as 6 mm, and a width set as 16 mm) to prepare a flexible organic field effect transistor. In particular, the source electrode101and the drain electrode102were disposed under the first surface layer111of MoO2(the source electrode and the drain electrode were formed of Al), the organic light-emitting layer121(formed by Alq3and having a thickness of 60 nm) was disposed over the second surface layer113of MoO2, the hole transport layer122(formed by NPB and having a thickness of 45 nm) was disposed on the organic light-emitting layer121, and the gate electrode13(formed of Al) was disposed on the hole transport layer122.

The flexible organic field effect transistor prepared in Example 3 was tested for its performance, the test was particularly as follows:

A HP-4140B picoammeter/DC voltage power was used to output a constant voltage to the gate of the flexible organic field effect transistor, and another HP-4140B picoammeter/DC voltage power was used to output voltage to the source electrode and the drain electrode of the flexible organic field effect transistor. Under different constant gate voltage outputs, through software control, the voltage output to the source electrode and the drain electrode of the organic field effect transistor was enabled to rise stepwise, and meanwhile the values of the current passing through the source and drain electrodes were measured synchronously, to output real-time voltage-current values on a computer.

FIG. 5is a diagram showing the output characteristics of the flexible organic field effect transistor. It can be seen fromFIG. 5that when the gate voltage is zero, the source/drain voltage VDSis 0.2 V, and the source/drain current IDSis saturated at about 1 mA, which is very small. When a positive voltage is applied to the gate, the source/drain current IDSquickly becomes 0, indicating that the layered metal oxide field effect material is a P-type semiconductor material for transporting holes, and the flexible organic field effect transistor has a P-type unipolar conductance characteristic. When a negative voltage is applied to the gate, the carrier concentration at the interface between the layered metal oxide field effect material and the organic light-emitting layer increases, the source/drain current IDSincreases, and as the gate voltage increases, a significant field effect transistor characteristic relationship appears between the source/drain voltage VDSand the source/drain current IDS. The source/drain voltage VDSis in a range of less than 0.6 V, the IDSincreases along with the increase of VDS, and the IDS-VDShas a linear relationship, which indicates that the layered metal oxide field effect material provided by the present invention forms a good ohmic contact with the source/drain aluminum electrodes.

FIG. 6is a transfer characteristic diagram of the flexible organic field effect transistor. It can be seen fromFIG. 6that, in absence of the gate voltage, the layered metal oxide field effect material has a large sheet resistance of approximately 104Ω/□ as tested by a surface resistance tester (model: RTS-9), and thus can be regarded as an insulator. When the gate voltage VGis increased, the top and bottom surfaces of the layered metal oxide field effect material generate an induced charge, and the core layer is a oxide material with a wide band gap, such that the carriers in the layered metal oxide field effect material are confined in the narrow-band-gap oxide of the top and bottom surfaces, forming a two-dimensional hole gas. When an external electric field is applied between the source and drain electrodes, the channel current IDcan be detected. The carrier concentration can be controlled by changing the gate voltage VG.

The carrier mobility is calculated as follows:

where, μ is the carrier mobility, h is the thickness of the gate insulation layer, Lchis the channel length, d is the channel width, εris the relative dielectric constant of the gate insulation layer (in NPB), ε0is the vacuum dielectric constant, and gmis the transconductance.

As calculated by the above equation, μ is about 105cm2/V·s.

It can be seen from the above embodiments that the layered metal oxide field effect material provided by the present invention has high carrier mobility higher than 103cm2/V·s, and thus overcomes the problem that the conventional metal oxide field effect material has low carrier mobility, and thus it is required to fabricate it into a crystal phase structure having a relatively high cost, and even that a substrate having a crystal phase structure is required.

PARTS LIST

10source/drain electrode11layered metal oxide field effect material12gate insulation layer13gate electrode101source electrode102drain electrode111first surface layer of layered metal oxide field effect material112core layer of layered metal oxide field effect material113second surface layer of layered metal oxide field effect material121organic light-emitting layer of the gate insulation layer122hole transport layer

Listing of Acronyms and Abbreviations

The above description is only preferred embodiments of the present invention, and it should be noted that several improvements and modifications can also be made by those skilled in the art without departing from the principles of the present invention, these improvements and modifications should also be regarded as in the claimed scope of the present invention.