阅读说明：本技术 超低功耗的薄膜晶体管及其制备方法 (Ultra-low power consumption thin film transistor and preparation method thereof ) 是由 程为军 梁仁荣 任天令 李宇星 于 2020-04-20 设计创作，主要内容包括：本发明提出了超低功耗的薄膜晶体管及其制备方法。该超低功耗的薄膜晶体管包括层叠设置的衬底、隔离层、栅极、栅堆叠结构、沟道薄膜、源漏电极和钝化层,其中,栅堆叠结构设置在栅极与沟道薄膜之间；并且,栅堆叠结构包括层叠设置的至少一层铁电介质薄膜和至少一层金属层。本发明所提出的超低功耗薄膜晶体管,其栅堆叠结构包含至少一层铁电介质薄膜,由于铁电材料的极化反转,引入了负电容效应,栅堆叠结构出现负的微分电容值,从而使薄膜晶体管在室温下能够实现亚阈值摆幅小于60mV/decade,且还具有关态电流小和开态电流大的优势。(The invention provides a thin film transistor with ultra-low power consumption and a preparation method thereof. The ultra-low power consumption thin film transistor comprises a substrate, an isolation layer, a grid electrode, a grid stacking structure, a channel thin film, a source electrode, a drain electrode and a passivation layer which are arranged in a stacked mode, wherein the grid stacking structure is arranged between the grid electrode and the channel thin film; and the gate stack structure comprises at least one ferroelectric dielectric thin film and at least one metal layer which are arranged in a stacked mode. The gate stack structure of the ultra-low power consumption thin film transistor provided by the invention comprises at least one layer of ferroelectric dielectric film, and due to polarization reversal of ferroelectric materials, a negative capacitance effect is introduced, and a negative differential capacitance value appears in the gate stack structure, so that the thin film transistor can realize that the sub-threshold swing amplitude is less than 60mV/decade at room temperature, and has the advantages of small off-state current and large on-state current.)

1. The ultra-low power consumption thin film transistor is characterized by comprising a substrate, an isolation layer, a grid electrode, a grid stacking structure, a channel thin film, a source drain electrode and a passivation layer which are arranged in a stacking mode, wherein the grid stacking structure is arranged between the grid electrode and the channel thin film; and the gate stack structure comprises at least one ferroelectric dielectric thin film and at least one metal layer which are arranged in a stacked mode.

2. The thin film transistor of claim 1, wherein the gate stack structure comprises a plurality of the ferroelectric dielectric thin films and a metal layer in a stacked arrangement.

3. The thin film transistor of claim 1, wherein the gate stack structure comprises a plurality of the ferroelectric thin films and a plurality of the metal layers alternately stacked, and one of the metal layers is disposed between two adjacent ferroelectric thin films.

4. The thin film transistor of claim 1, wherein the gate stack structure comprises:

the metal layer is arranged on the surface of the grid electrode;

the ferroelectric dielectric film is arranged on the surface of the metal layer close to the channel film;

an insulating dielectric thin film disposed between the ferroelectric dielectric thin film and the channel thin film.

5. The thin film transistor according to claim 1, wherein the ferroelectric material forming each of the ferroelectric thin films is different in kind, and the total equivalent capacitance of the plurality of ferroelectric thin films is substantially equal to that of the MOS structure.

6. The thin film transistor of claim 1, wherein the material forming the ferroelectric dielectric thin film is doped hafnium oxide, wherein the doped element comprises at least one of zirconium, silicon, aluminum, yttrium, lanthanum, and gadolinium; the material forming the metal layer includes at least one of titanium nitride, titanium, tantalum nitride, tantalum, tungsten, platinum, palladium, and ruthenium.

7. The thin film transistor of claim 1, wherein the ferroelectric thin film has a thickness of 0.5 to 20nm, and the metal layer has a thickness of 0.5 to 20 nm.

8. A method of fabricating an ultra-low power thin film transistor, comprising:

forming an isolation layer on the surface of the substrate;

forming a grid electrode;

forming a gate stack structure, wherein the gate stack structure comprises at least one ferroelectric dielectric thin film and at least one metal layer which are arranged in a stacked mode;

forming a channel film;

forming a source drain electrode;

and forming a passivation layer.

9. The method of claim 8, wherein the step of forming a gate stack structure comprises:

depositing a first metal layer on the surface of the grid electrode far away from the isolation layer;

and growing a first ferroelectric dielectric film on the surface of the first metal layer far away from the grid.

10. The method of claim 9, wherein the step of forming the gate stack structure further comprises:

depositing a second metal layer on the surface of the first ferroelectric dielectric film far away from the first metal layer;

and growing a second ferroelectric dielectric film on the surface of the second metal layer far away from the grid.

Technical Field

The invention relates to the technical field of semiconductor manufacturing, in particular to a thin film transistor with ultra-low power consumption and a preparation method thereof.

Background

Thin Film Transistors (TFT) are a special type of metal-oxide-semiconductor field effect transistor (MOSFET) and are widely used in displays. Unlike MOSFET devices of monocrystalline channel materials, such as silicon, germanium, III-V compounds, etc., the channel material is formed by a layer of semiconductor thin film deposited on a substrate (panel) and is thus called a thin film transistor. For a TFT device, typical channel materials are amorphous silicon (a-Si), amorphous silicon germanium (a-SiGe), polysilicon (poly-Si), polycrystalline silicon germanium (poly-SiGe), zinc oxide (ZnO), amorphous indium zinc oxide (a-InZnO), amorphous indium gallium zinc oxide (a-InGaZnO), and various organics (e.g., pentacene), among others. In recent years, with the vigorous development of two-dimensional materials (such as graphene, molybdenum disulfide, molybdenum ditelluride, tungsten diselenide, and the like), the two-dimensional materials are expected to be applied to commercial thin film transistors as novel channel materials due to the advantages of ultrathin thickness (which is beneficial to enhancing the control capability of a gate on a channel), good carrier transport property, large-area low-cost preparation process, and the like.

With the development of computers, mobile phones and the internet, a man-machine interaction mode taking a flat panel display as a core has penetrated into every corner of life of people and becomes a window for intelligent extension and sharing of human beings. Recall history that display technologies have undergone a change from the world to the earth, and have only been able to display low-resolution numbers in the past, and have progressed to the playing of today's high-definition gorgeous animations; from the past, bulky and heavy displays, to today's small and light display panels; from the planar structure with single function in the past, the curved surface display capable of interacting today is developed. One of the core devices of flat panel display technology is the thin film transistor, and each of its improvements does not depart from the innovation of the thin film transistor in material, device structure and process. Currently, the development of thin film transistors mainly focuses on improving the device performance, including optimizing the channel material components and the forming process conditions thereof, so as to reduce the defects of the channel material and improve the carrier mobility thereof; the interface state of the semiconductor channel material and the gate dielectric is improved, the voltage hysteresis of the device is reduced, the service life of the device is prolonged, and the like. In the future, the development in the fields of mobile intelligence, flexible wearable, internet of things, flexible display and the like will certainly put forward higher requirements on electronic components, especially thin film transistor devices, that is, the power consumption of the devices is also very urgent to be reduced while the performance of the devices is improved.

However, at present, the materials, device structures, and manufacturing methods of thin film transistor devices, especially the power consumption and performance of the devices, are still to be improved.

Disclosure of Invention

The present invention has been completed based on the following findings of the inventors:

in the research process, the inventor finds that a Thin Film Transistor (TFT) is one of the core devices for implementing systems such as on-board integration, three-dimensional monolithic integration, flat panel display, etc., and a typical device structure thereof is shown in fig. 1. With the increasing application demands, these new integration techniques are demanding higher performance TFT devices. However, due to various defects in the TFT channel and multiple limitations of low thermal budget and low cost in application scenarios, the fabrication of high performance, low power consumption TFT devices faces a number of technical challenges.

The inventor finds out through intensive research and a large number of experiments that on one hand, the driving current of a main flow device such as a-Si, poly-Si and amorphous indium zinc oxide (a-InZnO) TFT is mainly improved, and the reliability of the device is improved; on the other hand, in order to suppress off-state leakage, the current measures are to reduce the doping concentration of the channel, reduce the thickness of the channel, and improve the gate control capability by adopting a high-dielectric-constant gate dielectric. However, these methods do not make the TFT device break the limit of the thermodynamic limit of boltzmann, i.e. the Subthreshold Swing (SS) of most current TFT devices at room temperature is still larger than 60 mV/decade. Therefore, it is difficult to achieve the requirement of ultra-low power consumption.

The present invention is directed to solving, at least to some extent, one of the technical problems in the related art. Therefore, the invention provides a novel ultra-low power consumption thin film transistor and a preparation method thereof, wherein the gate stack structure of the ultra-low power consumption thin film transistor comprises one layer, two layers or multiple layers of ferroelectric dielectric films; because the Gibbs free energy of the ferroelectric film has a region with negative curvature between two polarization states, and the capacitance value of the ferroelectric film in the region is negative, a negative capacitance effect is introduced into the gate stack by the ferroelectric film, so that the capacitance of the gate stack containing the ferroelectric film is higher than that of the capacitor without the gate stack, the gate control capability of the transistor is improved, the transistor can break through the Boltzmann thermodynamic limit, and due to the mutual regulation effect among the multiple layers of ferroelectric media, the whole gate oxygen capacitor is matched with the channel capacitor of the device in an effective capacitance range, the subthreshold voltage swing SS is less than 60mV/decade at a wide leakage current voltage range, and the advantages of small off-state current, large on-state current, large driving and the like are achieved; and the material system and the preparation process of the transistor are compatible with the mainstream thin film transistor preparation process.

Additional aspects and advantages of the invention will be set forth in part in the description which follows and, in part, will be obvious from the description, or may be learned by practice of the invention.

Drawings

The foregoing aspects of the invention are explained in the description of the embodiments with reference to the following drawings, in which:

FIG. 1 is a schematic cross-sectional view of a typical TFT;

FIG. 2 is a schematic cross-sectional view of an ultra-low power thin film transistor according to an embodiment of the present invention;

FIG. 3 is Q of SBT ferroelectric material at room temperature_f-V_fA curve;

FIG. 4 shows different thicknesses t_fThe variation curve of the surface potential of the channel of the ultra-low power consumption thin film transistor device along with the grid voltage is shown;

FIG. 5 different thicknesses t_fThe variation curve of the charge density of the channel surface of the ultra-low power consumption thin film transistor device along with the grid voltage is shown;

FIG. 6 is a schematic cross-sectional view of an ultra-low power consumption thin film transistor according to another embodiment of the present invention;

FIG. 7 is a schematic diagram of an equivalent circuit from the gate to the channel of a gate stack structure containing two thin films of ferroelectric dielectric in accordance with one embodiment of the present invention;

FIG. 8 is a schematic diagram of an equivalent circuit from the gate to the channel of a gate stack structure having three or more ferroelectric thin films according to one embodiment of the present invention;

FIG. 9 shows a gate stack structure with more than two ferroelectric thin films with a total capacitance C according to one embodiment of the present invention_fe,effAnd C_MOSSchematic diagram of the variation relationship with the grid charge;

FIG. 10 is a schematic cross-sectional structural view of the product at each step in the course of a manufacturing process according to one embodiment of the invention;

FIG. 11 is a photograph of a sample low power thin film transistor TFT device according to one embodiment of the present invention;

FIG. 12 is a life microscope photograph of a low power thin film transistor TFT device according to one embodiment of the invention;

figure 13 is a graph of the sub-threshold swing of an ultra-low power thin film transistor device and a comparative device at different drain-source voltages extracted from a measured transfer characteristic according to one embodiment of the present invention.

Reference numerals

100 substrate

200 isolation layer

300 grid

401 ferroelectric dielectric thin film 1

410 metal layer

420 ferroelectric dielectric thin film 2

430 insulating dielectric film

500 channel film

600 source drain electrode

700 passivation layer

Detailed Description

The following examples of the present invention are described in detail, and it will be understood by those skilled in the art that the following examples are intended to illustrate the present invention, but should not be construed as limiting the present invention. Unless otherwise indicated, specific techniques or conditions are not explicitly described in the following examples, and those skilled in the art may follow techniques or conditions commonly employed in the art or in accordance with the product specifications.

In one aspect of the invention, an ultra-low power thin film transistor is presented.

According to an embodiment of the present invention, referring to fig. 2, the ultra-low power consumption thin film transistor includes a substrate 100, an isolation layer 200, a gate 300, a gate stack structure, a channel film 500, a source/drain electrode 600, and a passivation layer 700, which are stacked, wherein the gate stack structure is disposed between the gate 300 and the channel film 500; also, the gate stack structure includes at least one ferroelectric dielectric thin film 420 and at least one metal layer 410 which are stacked. In addition, "ultra low power consumption" specifically means that the subthreshold swing SS of the thin film transistor at room temperature is less than 60mV/decade, and "stacked arrangement" specifically means that the thin film transistors are sequentially stacked in the direction from the channel thin film 500 to the gate 300.

According to the embodiment of the present invention, the thin film transistor may be a bottom gate type (for example, as shown in fig. 2), a top gate type or a double gate type TFT, and the specific kind of the thin film transistor may be selected by those skilled in the art according to the actual use requirement of the thin film transistor. According to embodiments of the present invention, the substrate 100 may be, but is not limited to, silicon, germanium, gallium nitride, diamond, silicon carbide, quartz, glass, mica, polyimide, and the like. According to an embodiment of the present invention, the channel thin film 500 may include, but is not limited to, amorphous silicon (a-Si), amorphous silicon germanium (a-SiGe), polycrystalline silicon (poly-Si), polycrystalline silicon germanium (poly-SiGe), zinc oxide (ZnO), amorphous indium zinc oxide (a-InZnO), amorphous indium gallium zinc oxide (a-InGaZnO), various organic substances (e.g., pentacene), and two-dimensional materials (e.g., graphene, molybdenum disulfide, tungsten diselenide, black phosphorus, etc.).

In some embodiments of the present invention, for a bottom gate type TFT, referring to fig. 2, the gate stack structure 400 may include a metal layer 410, a ferroelectric dielectric film 420 and an insulating dielectric film 430, wherein the metal layer 410 may be disposed on a surface of the gate electrode 300, the ferroelectric dielectric film 420 is disposed on a surface of the metal layer 410 adjacent to the channel film 500, and the insulating dielectric film 430 is disposed between the ferroelectric dielectric film 420 and the channel film 500. Thus, a layer of metal is deposited on the upper surface of the gate 300, which is beneficial to improving the ferroelectric property of the ferroelectric medium grown on the gate, especially improving the crystal structure and improving the remanent polarization; while the insulating dielectric thin film 430 is advantageous for improving the interface characteristics between the ferroelectric dielectric thin film 420 of hafnium oxide material and the channel thin film 500 of semiconductor material.

Specifically, according to the operating principle of a Thin Film Transistor (TFT), the device generally needs to go through a subthreshold region (depletion state), a weak accumulation region, and a strong accumulation region from an off state to an on state. However, as shown in FIG. 2, due to the capacitance C of the ferroelectric medium_feAnd a capacitance C of a metal-oxide-semiconductor (MOS) transistor over the gate stack structure_MOSIt has strong non-linear variation with the change of the grid voltage or the grid charge. It is noted that when an insulating dielectric layer is present between the ferroelectric dielectric and the semiconductor channel, C is generally used_inAnd C_SRespectively represent a common insulating dielectric layer and a semiconductor channel capacitor, in which case C_MOSBeing the total capacitance of the MOS structure, i.e. C_inAnd C_SIn series, C_MOS ^-1＝C_in ^-1+C_S ^-1(ii) a And C_eqIs the total gate dielectric layer equivalent capacitance, i.e. C_feAnd C_inIn series, C_eq ^-1＝C_fe ^-1+C_in ^-1(ii) a When there is no insulating dielectric layer between the ferroelectric medium and the semiconductor channel, C_eqIs the total equivalent capacitance of the ferroelectric gate dielectric layer, i.e. C_eq＝C_fe. As such, the sub-threshold swing (SS) of the novel ultra-low power thin film transistor device can be written as:

in the formula (1), k_BBoltzmann constant, T is temperature, q is electron charge amount; gamma is a short channel factor, a specific value of which can be extracted experimentally, and is generally equal to 1 for long channel devices.

Wherein the ferroelectric material has a capacitance (C)_fe) Is differential capacitance, defined as dQ_f/dV_fThe method can be obtained from the Landau-Khalatnikov equation which is the physical state equation of the ferroelectric material:

in the formulae (2) and (3), a₀、b₀And c₀Is a parameter dependent on the specific ferroelectric material, can be determined by experimental measurements, and has a relationship with Landau coefficients α, β and gamma as follows₀＝2αt_f、b₀＝4βt_fAnd c₀＝6γt_fWherein t is_fIs the thickness of the ferroelectric material, and the Landau coefficient of the common ferroelectric material, namely Strontium Bismuth Tantalate (SBT), is α ═ 1.3 × 10 at room temperature⁸m/F、β＝1.3×10¹⁰m⁵/F/coul²And γ is 0m⁹/F/coul⁴。

Further, the calculated Q of the SBT ferroelectric material at room temperature according to equation (2)_f-V_fThe curve, with reference to fig. 3, exhibits an "S" shape. It can be observed that for the dotted line of the "S" type in the figure, there are two stable states and one metastable state. Both steady states often lead to a hysteresis loop in the experiment, as shown by the black dot lines in the figure. For ferroelectric capacitors in isolation, the intermediate metastable state (e.g., AC segment) is unstable when C is present_fe< 0 when it satisfiesnamely-C_fe＜C_inAccording to equation (1), the sub-threshold swing SS is less thanI.e., SS value less than 60mV/decade at room temperature.

However, by placing a conventional positive capacitor, such as an insulating layer dielectric capacitor or/and a semiconductor channel capacitor, in series with the ferroelectric capacitorTransistor grid total capacitance C_GSatisfy the requirement ofIf C_GNegative values, i.e. C, during the variation of the grid voltage_MOS＞-C_feThen, similar to the ferroelectric capacitor, there exist two polarization states, and the transfer characteristic of the transistor will have a hysteresis window; if C_GAlways positive during the variation of the grid voltage, i.e. C_MOS＜-C_feThe Gibbs free energy of the whole system is a concave function in the metastable state region, and the metastable state becomes a steady state, so that the transfer characteristic curve does not have a hysteresis window.

In summary, for a new ultra-low power thin film transistor including only one ferroelectric thin film, the capacitance matching condition of the transistor having a subthreshold swing less than 60mV/decade and no hysteresis window is C_MOS＜-C_fe＜C_in. Therefore, for a new ultra-low power thin film transistor including only one ferroelectric thin film, in order to allow the negative capacitance effect introduced in the gate stack thereof to effectively act on the sub-threshold region, C_fePreferably with C_MOSMatching, i.e., both exhibit the same trend with gate charge or gate charge and are approximately equal in value.

For different ferroelectric material thicknesses t_fWhen the drain voltage is zero, the variation curve of the surface potential of the channel of the N-type novel ultra-low power consumption thin film transistor device along with the grid voltage is shown in fig. 4; for different ferroelectric material thicknesses t_fThe variation curve of the channel surface charge density (Q) with the gate voltage corresponding to the same novel ultra-low power consumption thin film transistor device is shown in fig. 5. When the grid voltage is below the flat band voltage (V)_gs＜V_FB) Channel surface potential (phi) when the device is operated in a depletion region (Depleted region)_s) With t_fIs decreased, that is, the negative capacitance effect of the ferroelectric material acts to suppress the surface potential. In the depletion region, referring to FIG. 5, the channel charge density follows t_fIs increased because the channel charge Q is an ionized charge (qN)_dt_si/2) and movable electron charge density (Q)_m，Q_m< 0), so | Q_mI with t_fIs increased and decreased. The channel current of the device can be described by a Pao-Sah current double integral equation:

in the formula (4), V_chquasi-Fermi potential for channel electrons as a function of channel position and having values of 0V and V at source and drain terminals, respectively_ds。

From equation (4), it can also be seen that the channel current Id_sFollowing | Q_mI is reduced, i.e. in the depletion region, I_dsWith t_fIs increased and decreased. When the grid voltage exceeds the flat band voltage (V)_gs＞V_FB) The device begins to operate in the accumulation region (accumulation region) when the channel surface potential (phi) is present_S) With t_fIs increased and the surface potential is amplified (G ═ d phi-_s/dV_gs> 1). In the weak accumulation region and the strong accumulation region, referring to FIG. 5, the channel charge density Q follows t_fDecreases (but the absolute value | Q | increases). That is, movable electron charge density (| Q)_mL) with t_fIs increased. Then according to equation (4), the channel current I of the accumulation region_dsWith t_fIs increased, and thus, the current switching ratio (I) of the device is increased_on/I_off) And also with ferroelectric material thickness with t_fIs increased.

In other embodiments of the present invention, referring to fig. 6, the gate stack 400 may also include a plurality of ferroelectric dielectric thin films 420 and a plurality of metal layers 410 alternately stacked, such as 2 ferroelectric thin films 420 and 2 metal layers 410 alternately stacked as shown in fig. 6, and one metal layer 410 is disposed between two adjacent ferroelectric thin films 420. Therefore, the problems that the transfer characteristic curve (Ids-Vgs) voltage hysteresis and the small capacitance matching grid voltage range of the thin film transistor device are easily caused when the CMOS works in a strong accumulation region can be solved, and the performance of the device and the circuit characteristics of the device are optimized. The "alternately stacked arrangement" specifically means an arrangement alternately stacked in the direction from the channel film 500 to the gate electrode 300.

In particular, the use of two or more layers of ferroelectric materials in the gate stack allows for more efficient control of C_feWith the shape of the gate voltage or gate charge. Referring to fig. 7, C when the gate stack contains two layers of different ferroelectric dielectric materials_fe，eff＝C_fe1||C_fe2In other words, the invention further proposes to move from the subthreshold region to the weak accumulation region and even to the strong accumulation region, C_fe，effAnd C_MOSAre matched in a homogeneous way. It is noted that in order to make the two better match, C should be satisfied_MOS＜-C_fe，eff＜C_inStrictly speaking, C_fe，effThe closer to C_MOSThe better. Wherein, refer to FIG. 8, C_fe，effRepresenting the ferroelectric dielectric material of each layer (assuming each layer is named fe₁，fe₂，……，fe_n) Of a total capacitance equal to the series connection of the respective single layers of ferroelectric material, i.e. C_fe，eff＝C_fe1||C_fe2.....||C_fen. In fact, due to the physical parameters of the ferroelectric materials of the layers and the process tolerance during the process preparation, the capacitance may not satisfy the matching condition C_MOS＜-C_fe，eff＜C_in，C_feIs not strictly equal to C_MOSTherefore, the present invention proposes C_feIs preferably greater than C_MOSThe variation of both with gate charge is shown in fig. 9.

Therefore, in some specific examples, the ferroelectric material type forming each ferroelectric dielectric thin film 420 may be different, and the total equivalent capacitance C of the multilayered ferroelectric dielectric thin film 420_fe，effCapacitor C capable of being connected with MOS structure_MOSSubstantially equal, i.e. C_fe，effAnd C_MOSIs not more than C_fe，effOr C_MOS25% of the total. Thus, the above condition is satisfied, C_fe，effAnd C_MOSThe same trend appears with gate charge or gate charge.

According to an embodiment of the present invention, the material forming the ferroelectric dielectric thin film 420 is doped hafnium oxide (HfZrO), wherein the doped element includes at least one of zirconium (Zr), silicon (Si), aluminum (Al), yttrium (Y), lanthanum (La), and gadolinium (Gd), which can be selected or adjusted by one skilled in the art according to the performance of the actual thin film transistor. In some embodiments of the present invention, the thickness of the ferroelectric thin film 420 may be 0.5-20 nm, so that the additional gate stack structure does not significantly increase the total thickness of the thin film transistor, and the subthreshold swing of the thin film transistor is smaller.

According to an embodiment of the present invention, a material forming the metal layer 410 includes at least one of titanium nitride (TiN), titanium (Ti), tantalum nitride (TaN), tantalum (Ta), tungsten (W), platinum (Pt), palladium (Pd), and ruthenium (Ru), and those skilled in the art may select accordingly according to the performance of an actual thin film transistor. In some embodiments of the present invention, the thickness of the metal layer 410 may be 0.5 to 20nm, so that the additional gate stack structure does not significantly increase the total thickness of the thin film transistor, and the subthreshold swing of the thin film transistor is smaller.

In summary, according to the embodiments of the present invention, the gate stack structure of the ultra-low power consumption thin film transistor includes one, two, or more layers of ferroelectric dielectric thin films, and due to polarization reversal of the ferroelectric material, a negative capacitance effect is introduced, and a negative differential capacitance value appears in the gate stack structure, so that the thin film transistor can realize a subthreshold swing smaller than 60mV/decade at room temperature, and has the advantages of small off-state current, large on-state current, and the like.

In another aspect of the invention, a method of fabricating an ultra-low power thin film transistor is presented. According to an embodiment of the present invention, the preparation method comprises:

s100: and forming a grid electrode.

In this step, for a Thin Film Transistor (TFT) of a bottom gate structure, the patterned gate electrode 300 may be directly sputter formed on the surface of the isolation layer 200 away from the substrate 100. The schematic cross-sectional structure of the product obtained in this step can be referred to fig. 10 (b).

In some embodiments of the present invention, the prepared substrate 100 may be cleaned, and then the isolation layer 200 may be deposited by using an Atomic Layer Deposition (ALD) system, so that the gate material layer is formed on the upper surface of the isolation layer 200 by sputtering, and the gate 300 is patterned by photolithography for the first time.

S200: and forming a gate stack structure.

In this step, a gate stack structure is formed, and the gate stack structure includes at least one ferroelectric dielectric thin film 420 and at least one metal layer 410, which are stacked. In some embodiments of the present invention, for the bottom-gate TFT, the deposition of the metal layer 410 and the growth of the ferroelectric thin film 420 may be continued alternately on the upper surface of the gate electrode 300 fabricated in step S100.

In some specific examples, a metal layer 410 may be formed on the upper surface of the gate 300 formed in step S100 by sputtering, and then a ferroelectric thin film 420 (the material of which may be a doped hafnium oxide) may be grown by ALD, specifically, tetrakis (methylethylamino) hafnium and tetrakis (methylethylamino) zirconium may be used as the precursor sources of hafnium and zirconium elements, respectively, and deionized water or ozone (O) may be used₃) As an oxidant source and grown by HfO₂And ZrO₂The films are alternately grown and subjected to a rapid annealing process, and then ALD is used to grow the insulating dielectric film 430. Thus, the metal layer 410 is beneficial to improving the ferroelectric property of the surface of the ferroelectric medium grown thereon subsequently, in particular improving the crystal structure and the residual polarization strength; while the insulating dielectric film 430 is beneficial for improving the interface between the hafnium oxide ferroelectric dielectric film 420 and the semiconductor channel film 500. And, the schematic view of the cross-sectional structure of the product obtained in this step can refer to (d) of fig. 10.

In other specific examples, a first metal layer may be formed on the upper surface of the gate 300 formed in step S100 by sputtering, and then a first thin ferroelectric dielectric film is grown by using ALD, and a second metal layer is formed by continuing sputtering, and then a second thin ferroelectric dielectric film is grown by using ALD, … …. In this manner, by alternately forming the metal layer 410 and growing the ferroelectric thin film 420 repeatedly, a gate stack structure including two or more ferroelectric thin films 420 can be obtained.

According to an embodiment of the invention, ironThe electric grid medium is not limited to the ferroelectric hafnium oxide system, and can be SrBi₂Ta₂O₉、 Pb(Zrx,Ti_1-x)O₃And ferroelectric materials such as PVDF (TrFE), and the like, and the preparation method comprises the methods of sol-gel method (sol-gel), magnetron sputtering (Magnetic sputtering), metal oxide vapor deposition (MOCVD), Pulse Laser Deposition (PLD), and the like. And, HfO₂And ZrO₂In the method of thin film alternating growth, HfO₂And ZrO₂The deposition cycle ratio can be set to 5:5, the element ratio of hafnium and zirconium in the HfZrO ferroelectric dielectric film obtained in the way is about 1:1, and the growth temperature is 200-350 ℃; in addition, HfO may be varied₂And ZrO₂And (3) adjusting the ferroelectric properties of the HfZrO ferroelectric dielectric film by changing the deposition cycling ratio, namely changing the element ratio of hafnium and zirconium, such as changing the cycling ratio to 3:7, 6:4, 7:3, 8:2 and the like. The impurities doped in the hafnium oxide thin film include, but are not limited to, elements such as zirconium (Zr), silicon (Si), aluminum (Al), lanthanum (La), and gadolinium (Gd).

According to the embodiment of the invention, the insulating medium film can be selected from Al with the thickness of 6nm₂O₃The growth temperature is 200 ℃, and the precursor of the Al element and the oxidant are respectively trimethylaluminum (Al (CH)₃)₃TMA) and deionized water, and Al is used₂O₃The interface formed by the dielectric and the InGaZnO channel is better. In special cases, the dielectric layer may be 0.1nm thick Al₂O₃An interfacial layer.

S300: a channel film is formed.

In this step, for the bottom-gate TFT, the sputtering of the channel film 500 may be continued on the upper surface of the gate stack structure. In some embodiments of the present invention, a magnetron sputtering apparatus may be used to sputter at room temperature to form a semiconductor thin film, and then a second photolithography may be performed to form the channel thin film 500 and form a contact hole communicating with the gate electrode 300. And, the schematic view of the cross-sectional structure of the product obtained in this step can refer to (e) of fig. 10.

S400: and forming a source drain electrode.

In this step, for the bottom-gate TFT, the source-drain electrode 600 may be continuously formed on the upper surface of the channel film 500 by sputtering. In some embodiments of the present invention, the source/drain electrode material layer may be formed by sputtering, and then the pattern of the source/drain electrode 600 may be formed by performing the third photolithography.

S500: and forming a passivation layer.

In this step, for the bottom-gate TFT, the passivation layer 700 may be continuously formed on the upper surfaces of the channel film 500 and the source and drain electrodes 600. And, the schematic view of the cross-sectional structure of the product obtained in this step can refer to (f) of fig. 10.

In summary, according to the embodiments of the present invention, the present invention provides a method for manufacturing an ultra-low power consumption thin film transistor, which can not only manufacture an ultra-low power consumption thin film transistor with a subthreshold swing smaller than 60mV/decade, but also does not need a high temperature annealing process, and has good compatibility with the conventional manufacturing process of the thin film transistor.

The invention will now be described with reference to specific examples, which are intended to be illustrative only and not to be limiting in any way.