Many modern electronic devices include non-volatile memory. Non-volatile memory is electronic memory that is able to store data both when powered and also in the absence of power. A promising candidate for next-generation non-volatile memory is ferroelectric random-access memory (FeRAM). FeRAM has a relatively simple structure and is compatible with complementary metal-oxide-semiconductor (CMOS) logic fabrication processes.
Aspects of the present disclosure are best understood from the following detailed description when read with the accompanying figures. It is noted that, in accordance with the standard practice in the industry, various features are not drawn to scale. In fact, the dimensions of the various features may be arbitrarily increased or reduced for clarity of discussion.
The following disclosure provides many different embodiments, or examples, for implementing different features of the provided subject matter. Specific examples of elements and arrangements are described below to simplify the present disclosure. These are, of course, merely examples and are not intended to be limiting. For example, the formation of a first feature over or on a second feature in the description that follows may include embodiments in which the first and second features are formed in direct contact, and may also include embodiments in which additional features may be formed between the first and second features, such that the first and second features may not be in direct contact. In addition, the present disclosure may repeat reference numerals and/or letters in the various examples. This repetition is for the purpose of simplicity and clarity and does not in itself dictate a relationship between the various embodiments and/or configurations discussed.
Further, spatially relative terms, such as “beneath,” “below,” “lower,” “above,” “upper,” “on” and the like, may be used herein for ease of description to describe one element or feature's relationship to another element(s) or feature(s) as illustrated in the figures. The spatially relative terms are intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the figures. The apparatus may be otherwise oriented (rotated 90 degrees or at other orientations) and the spatially relative descriptors used herein may likewise be interpreted accordingly.
As used herein, although the terms such as “first,” “second” and “third” describe various elements, components, regions, layers and/or sections, these elements, components, regions, layers and/or sections should not be limited by these terms. These terms may be only used to distinguish one element, component, region, layer or section from another. The terms such as “first,” “second” and “third” when used herein do not imply a sequence or order unless clearly indicated by the context.
Notwithstanding that the numerical ranges and parameters setting forth the broad scope of the disclosure are approximations, the numerical values set forth in the specific examples are reported as precisely as possible. Any numerical value, however, inherently contains certain errors necessarily resulting from the standard deviation found in the respective testing measurements. Also, as used herein, the terms “substantially,” “approximately” or “about” generally mean within a value or range that can be contemplated by people having ordinary skill in the art. Alternatively, the terms “substantially,” “approximately” or “about” mean within an acceptable standard error of the mean when considered by one of ordinary skill in the art. People having ordinary skill in the art can understand that the acceptable standard error may vary according to different technologies. Other than in the operating/working examples, or unless otherwise expressly specified, all of the numerical ranges, amounts, values and percentages such as those for quantities of materials, durations of times, temperatures, operating conditions, ratios of amounts, and the likes thereof disclosed herein should be understood as modified in all instances by the terms “substantially,” “approximately” or “about.” Accordingly, unless indicated to the contrary, the numerical parameters set forth in the present disclosure and attached claims are approximations that can vary as desired. At the very least, each numerical parameter should be construed in light of the number of reported significant digits and by applying ordinary rounding techniques. Ranges can be expressed herein as from one endpoint to another endpoint or between two endpoints. All ranges disclosed herein are inclusive of the endpoints, unless specified otherwise.
A ferroelectric field-effect transistor (FeFET) device is a type of ferroelectric random access-memory (FeRAM) device including a ferroelectric material arranged between a conductive gate structure and a channel region disposed between a source region and a drain region. During operation of a FeFET device, an application of a gate voltage to the gate structure will generate an electric field that causes a dipole moment to form within the ferroelectric material. Depending on a value of the gate voltage, a direction of the dipole moment (i.e., a polarization) may be one of two opposing directions. Since a threshold voltage (e.g., a minimum gate-to-source voltage that forms a conductive path between the source region and the drain region) of a FeFET device is dependent upon the polarization within the ferroelectric material, the different polarizations effectively split the threshold voltage of the FeFET device into two distinct values corresponding to different data states.
For example, in an n-type FeFET (e.g., a FeFET device having a channel region with an n-type doping), a positive gate voltage will form an electric field that gives a ferroelectric material a first polarization pointing towards the channel region and that causes electrons to accumulate within the channel region. The electrons will reinforce the first polarization within the ferroelectric material and give the FeFET device a first threshold voltage corresponding to a first data state (e.g., a logical “1”). Alternatively, a negative gate voltage will form an electric field that gives the ferroelectric material a second polarization pointing towards the gate structure and that causes holes to accumulate within the channel region. The holes will reinforce the second polarization within the ferroelectric material and give the FeFET device a second threshold voltage corresponding to a second data state (e.g., a logical “0”). The difference between the first threshold value and the second threshold value defines a memory window of the FeFET device (e.g., corresponding to a difference of threshold voltages of the first and second data states).
The channel region of a FeFET device may include a semiconductor material (e.g., silicon, germanium, etc.). However, it has been appreciated that using an oxide semiconductor for a channel region of a FeFET device allows the FeFET device to achieve a good performance (e.g., a high endurance, low access times, etc.). It has also been appreciated that a memory window of a FeFET device using an oxide semiconductor is relatively small. This is because the oxide semiconductor is not able to accumulate large numbers of different types of charge carriers (e.g., holes and electrons). For example, while a channel region using an n-type oxide semiconductor can accumulate electrons to reinforce a polarization within a ferroelectric material when a positive gate voltage is applied to a gate structure, the n-type oxide semiconductor cannot also accumulate holes to reinforce the polarization within the ferroelectric material when a negative gate voltage is applied to the gate structure. Therefore, a negative gate voltage applied to the gate structure will cause the ferroelectric material to polarize; however, when the negative gate voltage is removed, the ferroelectric material will revert to a remnant polarization. The remnant polarization will reduce the memory window of the FeFET device (e.g., to about half that of a FeFET device having a channel region that is a semiconductor material) and also reduce the endurance of the FeFET device.
The present disclosure therefore provides a semiconductor memory structure and a method for forming the same. In some embodiments, the semiconductor memory structure provides an ultra-thin structure between the channel layer and the ferroelectric layer. The ultra-thin structure helps reduce charge trapping and provides interface engineering such that device performance and endurance are improved. In some embodiments, the semiconductor memory structure may be a memory structure disposed in a front-end-of-line (FEOL) structure or a back-end-of-line (BEOL) interconnect structure. Functionality of the FeFET memory structure is thus further improved.
In some embodiments, the substrate, though not shown, may be any type of semiconductor body (e.g., silicon (Si), silicon germanium (SiGe), silicon-on-insulator (SOI), etc.), such as a semiconductor wafer and/or one or more dies on a wafer, as well as any other type of semiconductor and/or epitaxial layers, associated therewith. In some embodiments, a dielectric structure may be formed over the substrate, though not shown, and the gate structure 110 may be formed in the dielectric structure over the substrate.
In some embodiments, the gate structure 110 may include a conductive material. In some embodiments, the conductive material of the gate structure 110 may have a metal work function that is configured to increase a threshold voltage of the semiconductor memory structure 100, thereby further mitigating a current flowing through the channel layer 130. In some embodiments, the gate structure 110 may include platinum (Pt), titanium (Ti), titanium nitride (TiN), tantalum (Ta), tantalum nitride (TaN), tungsten (W), tungsten nitride (WN), copper (Cu), gold (Au), zinc (Zn), aluminum (Al), iron (Fe), nickel (Ni), beryllium (Bc), chromium (Cr), cobalt (Co), antimony (Sb), iridium (Ir), molybdenum (Mo), osmium (Os), thorium (Th), vanadium (V), or a combination thereof. In some embodiments, the gate structure 110 may include a buried gate structure, but the disclosure is not limited thereto. In such embodiments, a top surface of the gate structure 110 may be aligned with (i.e., coplanar with) a top surface of the substrate or a top surface of the dielectric structure, but the disclosure is not limited thereto.
The ferroelectric layer 120 includes a material having dielectric crystals which exhibit an electric polarization having a direction that can be controlled by an electric field. For example, in some embodiments, the ferroelectric layer 1120 may include hafnium-oxide (HfO2), hafnium zinc oxide (HfZnO2), zinc oxide (ZnO), or the like. In some embodiments, a thickness of the ferroelectric layer 120 may be between approximately 5 nanometers and approximately 20 nanometers, but the disclosure is not limited thereto. In some embodiments, the ferroelectric layer 120 may be in contact with the gate structure 110. In other embodiments, one or more other layer, such as a buffer layer or a barrier layer, may be disposed between the ferroelectric layer 120 and the gate structure 110, though not shown.
The channel layer 130 includes oxide semiconductor materials. In some embodiments, the oxide semiconductor material may include indium gallium zinc oxide (IGZO), indium gallium zinc tin oxide (IGZTO), indium tungsten oxide (IWO), indium tungsten zinc oxide (IWZO), indium zinc oxide (IZO), zinc oxide (ZnO), or the like. In some embodiments, a thickness of the channel layer 130 may be between approximately 3 nanometers and 20 nanometers, but the disclosure is not limited thereto.
The source structure 140S and the drain structure 140D are disposed over the channel layer 130. The source structure 140S and the drain structure 140D respectively include conductive materials. In some embodiments, the conductive materials includes metals such as TiN and molybdenum (Mo), but the disclosure is not limited thereto. In some embodiments, the source structure 140S and the drain structure 140D include a conductive material same as that of the gate structure 110. In other alternative embodiments, the source structure 140S and the drain structure 140D include a conductive material different from that of the gate structure 110.
In some embodiments, a thickness of the intervening structure 150 is less than the thickness of the ferroelectric layer 120, and less than the thickness of the channel layer 130. In some embodiments, the thickness of the intervening structure 150 is less than 5 angstroms. Both the thickness of the ferroelectric layer 120 and the thickness of the channel layer 130 are greater than approximately 3 nanometers while the thickness of the intervening structure 150 is less than 0.5 nanometer; therefore, the thickness of the intervening structure 150 is much less than the thickness of the ferroelectric layer 120 and the thickness of the channel layer 130. In some embodiments, the intervening structure 150 may be referred to as an ultra-thin structure disposed between the ferroelectric layer 120 and the channel layer 130. In some embodiments, the intervening structure 150 may be referred to as an interface between the ferroelectric layer 120 and the channel layer 130 due to its relatively ultra-thin configuration.
In some embodiments, the intervening structure 150 and the channel layer 130 include different materials. In some embodiments, the material of the intervening structure 150 is further different from that of the ferroelectric layer 120. The materials used to form the intervening structure 150 are described below.
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In some embodiments, the intervening structure 150 (i.e., the first layer 152, the second layer 154 and the third layer 156) includes oxide materials. In some embodiments, for example but not limited thereto, the intervening structure 150 includes indium oxide (In2O3), gallium oxide (Ga2O3), zinc oxide (ZnO), hafnium oxide (HfO2), zirconium dioxide (ZrO2), aluminum oxide (Al2O3), silicon oxide (SiO2), tin oxide (SnO2), tungsten oxide (WO3), lanthanum oxide (La2O3), strontium oxide (SrO), ceric oxide (CeO2), yttrium oxide (Y2O3), or tantalum oxide (Ta2O5). Therefore, the first layer 152, the second layer 154 and the third layer 156 are respectively referred to as a first oxide layer 152, a second oxide layer 154 and a third oxide layer 156. In some embodiments, the first oxide layer 152 and the second oxide layer 154 include a same oxide material, while the third oxide layer 156 includes an oxide material different from that of the first oxide layer 152 and the second oxide layer 154. For example but not limited thereto, the first oxide layer 152 and the second oxide layer 154 may include In2O3, and the third oxide layer 156 includes Ga2O3. In such embodiments, an In2O3/Ga2O3/In2O3 tri-layered intervening structure 150 is provided between the ferroelectric layer 120 and the channel layer 130.
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When the tri-layered intervening structure 150 is disposed between the ferroelectric layer 120 and the channel layer 130, such arrangement helps reduce charge trapping. As mentioned above, because the thickness of the tri-layered intervening structure 150 is much less than the thickness of the ferroelectric layer 120 and much less than the thickness of the channel layer 130, the tri-layered intervening structure 150 may serve as an interface between the ferroelectric layer 120 and the channel layer 130. Further, influence on the ferroelectric layer 120 and the channel layer 130 by the tri-layered intervening structure 150 is negligible due to its ultra-thin configuration.
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When the bi-layered intervening structure 150 is disposed between the ferroelectric layer 120 and the channel layer 130, it helps reducing charge trapping. As mentioned above, because the thickness of the bi-layered intervening structure 150 is much less than the thickness of the ferroelectric layer 120 and much less than the thickness of the channel layer 130, the bi-layered intervening structure 150 may serve as an interface between the ferroelectric layer 120 and the channel layer 130. Further, influence on the ferroelectric layer 120 and the channel layer 130 by the bi-layered intervening structure 150 is negligible due to its ultra-thin configuration.
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When the single-layered intervening structure 150 is disposed between the ferroelectric layer 120 and the channel layer 130, such arrangement helps reduce charge trapping. As mentioned above, because a thickness of the single-layered intervening structure 150 is much less than the thickness of the ferroelectric layer 120 and much less than the thickness of the channel layer 130, the single-layered intervening structure 150 may serve as an interface between the ferroelectric layer 120 and the channel layer 130. Further, influence on the ferroelectric layer 120 and the channel layer 130 by the single-layered intervening structure 150 is negligible due to its ultra-thin configuration.
Accordingly, the intervening structure 150 disposed between the ferroelectric layer 120 and the channel layer 130 may be a single-layered, a bi-layered, or a tri-layered structure. The thickness of the intervening structure 150 is less than 5 angstroms, and the influence on the ferroelectric layer 120 and the channel layer 130 is therefore negligible. Further, the intervening structure 150 may serve as an interface between the ferroelectric layer 120 and the channel layer 130. Such interface helps reduce charge trapping in the channel layer 130. Further, the interface helps filling of vacancies in the ferroelectric layer 120 and/or the channel layer 130 and suppression of inter-diffusion of oxygen, hydrogen and vacancies such that the intrinsic fatigue performance and endurance of the ferroelectric layer 120 are improved. The intervening structure 150 further helps tuning band diagram between the ferroelectric layer 120 and the channel layer 130. Accordingly, breakdown strength, memory window and performance of the semiconductor memory structure 100 having the intervening structure 150 between the ferroelectric layer 120 and the channel layer 130 are all improved.
As shown in the cross-sectional view of the semiconductor memory structure 300 of
As shown in the cross-sectional view of the semiconductor memory structure 400 of
As shown in the cross-sectional view of the semiconductor memory structure 500 of
As shown in the cross-sectional view of the semiconductor memory structure 600 of
As shown in the cross-sectional view of the semiconductor memory structure 700 of
As shown in the cross-sectional view of the semiconductor memory structure 800a in
As shown in the cross-sectional view of the semiconductor memory structure 900a of
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In some embodiments, an interlayer dielectric (ILD) structure (not shown) may be formed over a semiconductor memory structure after formation of a source structure 140S and a drain structure 140D when the semiconductor memory structure is formed by FEOL manufacturing. In such embodiments, connecting structures such as contact plugs or vias may be formed in the ILD structure. The ILD structure may include one or more dielectric layers, and the dielectric layer may include silicon dioxide, silicon nitride, carbon-doped silicon dioxide, silicon oxynitride, borosilicate glass (BSG), phosphorus silicate glass (PSG), borophosphosilicate glass (BPSG), fluorosilicate glass (FSG), undoped silicate glass (USG), a porous dielectric material, or the like.
In other embodiments, an inter-metal dielectric (IMD) structure (not shown) may be formed over the semiconductor memory structure after the forming of the source structure 140S and the drain structure 140D when the semiconductor memory structure is formed by BEOL manufacturing. The IMD structure may include one or more dielectric layers, and the dielectric layer may include silicon oxide, silicon nitride, carbon doped silicon dioxide, BSG, PSG, BPSG, FSG, USG, a porous dielectric material, or the like. In various embodiments, one or more etch stop layers may be formed in the IMD structure, wherein the etch stop layer includes a carbide (e.g., silicon carbide, silicon oxycarbide, or the like), a nitride (e.g., silicon nitride, silicon oxynitride, or the like), or the like. In such embodiments, metal layers may be formed in the IMD structure and may be connected by vias. Thus, a BEOL interconnect structure is obtained with the semiconductor memory structure buried or embedded therein.
While the disclosed method 10 is illustrated and described herein as a series of acts or operations, it will be appreciated that an order of the illustrated acts or operations is not to be interpreted in a limiting sense. For example, some operations may occur in different orders and/or concurrently with other acts or operations apart from those illustrated and/or described herein. In addition, not all illustrated operations may be required to implement one or more aspects or embodiments of the description herein. Further, one or more of the operations depicted herein may be carried out in one or more separate operations and/or phases.
In operation 11, a ferroelectric layer is formed on a gate structure.
In operation 12, an intervening structure is formed over the ferroelectric layer.
In operation 13, a channel layer is formed over the intervening structure.
In operation 14, a source structure and a drain structure are formed over the channel layer.
Accordingly, the present disclosure provides a semiconductor memory structure and a method for forming the same. In some embodiments, the semiconductor memory structure provides an ultra-thin layer between a channel layer and a ferroelectric layer. The ultra-thin layer helps reduce charge trapping and provides interface engineering such that device performance and endurance are improved. In some embodiments, the semiconductor memory structure may be a memory structure disposed in a front-end-of-line (FEOL) structure or a back-end-of-line (BEOL) interconnect structure. Thus, functionalality of a FeFET memory structure is further improved.
In some embodiments, a semiconductor memory structure is provided. The semiconductor memory structure includes a gate structure, a ferroelectric layer over the gate structure, a channel layer over the ferroelectric layer, a first oxide layer and a second oxide layer between the channel layer and the ferroelectric layer, a third oxide layer between the first oxide layer and the second oxide layer, and a source structure and a drain structure over the channel layer. The first oxide layer includes a first oxide material different from a material of the channel layer. A sum of a thickness of the first oxide layer, a thickness of the second oxide layer and a thickness of the third oxide layer is less than a thickness of the channel layer.
In some embodiments, a semiconductor memory structure is provided. The semiconductor memory structure includes a gate structure, a ferroelectric layer over the gate structure, a channel layer over the ferroelectric layer, an intervening structure between the ferroelectric layer and the channel layer, and a source structure and a drain structure separated from each other over the channel layer. A thickness of the intervening structure is less than a thickness of the channel layer and less than a thickness of the ferroelectric layer. The channel layer and the intervening structure include different materials.
In some embodiments, a method for forming a semiconductor memory structure is provided. The method includes following operations. A gate structure is formed over the substrate. A ferroelectric layer is formed over the gate structure. An intervening structure is formed over the ferroelectric layer. A channel layer is formed over the intervening structure. A source structure and a drain structure are formed over the channel layer. A thickness of the intervening structure is less than a thickness of the ferroelectric layer and less than a thickness of the channel layer.
The foregoing outlines features of several embodiments so that those skilled in the art may better understand the aspects of the present disclosure. Those skilled in the art should appreciate that they may readily use the present disclosure as a basis for designing or modifying other processes and structures for carrying out the same purposes and/or achieving the same advantages of the embodiments introduced herein. Those skilled in the art should also realize that such equivalent constructions do not depart from the spirit and scope of the present disclosure, and that they may make various changes, substitutions, and alterations herein without departing from the spirit and scope of the present disclosure.