|Número de publicación||US20050145957 A1|
|Tipo de publicación||Solicitud|
|Número de solicitud||US 11/059,594|
|Fecha de publicación||7 Jul 2005|
|Fecha de presentación||16 Feb 2005|
|Fecha de prioridad||20 Feb 2002|
|También publicado como||US6893984, US20030157764|
|Número de publicación||059594, 11059594, US 2005/0145957 A1, US 2005/145957 A1, US 20050145957 A1, US 20050145957A1, US 2005145957 A1, US 2005145957A1, US-A1-20050145957, US-A1-2005145957, US2005/0145957A1, US2005/145957A1, US20050145957 A1, US20050145957A1, US2005145957 A1, US2005145957A1|
|Inventores||Kie Ahn, Leonard Forbes|
|Cesionario original||Micron Technology, Inc.|
|Exportar cita||BiBTeX, EndNote, RefMan|
|Citas de patentes (99), Citada por (60), Clasificaciones (21)|
|Enlaces externos: USPTO, Cesión de USPTO, Espacenet|
The invention relates to semiconductor devices and device fabrication. Specifically, the invention relates to gate dielectric layers of transistor devices and their method of fabrication.
The semiconductor device industry has a market driven need to improve speed performance, improve its low static (off-state) power requirements, and adapt to a wide range of power supply and output voltage requirements for it silicon based microelectronic products. In particular, in the fabrication of transistors, there is continuous pressure to reduce the size of devices such as transistors. The ultimate goal is to fabricate increasingly smaller and more reliable integrated circuits (ICs) for use in products such as processor chips, mobile telephones, or memory devices such as DRAMs. The smaller devices are frequently powered by batteries, where there is also pressure to reduce the size of the batteries, and to extend the time between battery charges. This forces the industry to not only design smaller transistors, but to design them to operate reliably with lower power supplies.
Currently, the semiconductor industry relies on the ability to reduce or scale the dimensions of its basic devices, primarily, the silicon based metal-oxide-semiconductor field effect transistor (MOSFET). A common configuration of such a transistor is shown in
In fabricating transistors to be smaller in size and reliably operating on lower power supplies, one important design criteria is the gate dielectric 140. The mainstay for forming the gate dielectric has been silicon dioxide, SiO2. Thermally grown amorphous SiO2 provides a electrically and thermodynamically stable material, where the interface of a SiO2 layer with an underlying Si provides a high quality interface as well as superior electrical isolation properties. In typical processing, use of SiO2 on Si has provided defect charge densities on the order of 1010/cm2, midgap interface state densities of approximately 1010/cm2 eV, and breakdown voltages in the range of 15 MV/cm. With such qualities, there would be no apparent need to use a material other than SiO2, but with increased scaling, other requirements for gate dielectrics create the need to find other dielectric materials to be used for a gate dielectric.
A gate dielectric 140, when operating in a transistor, has both a physical gate dielectric thickness and an equivalent oxide thickness (teq) The equivalent oxide thickness quantifies the electrical properties, such as capacitance, of a gate dielectric 140 in terms of a representative physical thickness. teq is defined as the thickness of a theoretical SiO2 layer that would be required to have the same capacitance density as a given dielectric, ignoring leakage current and reliability considerations. A SiO2 layer of thickness, t, deposited on a Si surface as a gate dielectric will also have a teq larger than its thickness, t. This teq results from the capacitance in the surface channel on which the SiO2 is deposited due to the formation of a depletion/inversion region. This depletion/inversion region can result in teq being from 3 to 6 Angstroms (Å) larger than the SiO2 thickness, t. Thus, with the semiconductor industry driving to someday scale the gate dielectric equivalent oxide thickness, teq, to under 10 Å, the physical thickness requirement for a SiO2 layer used for a gate dielectric would be need to be approximately 4 to 7 Å. Additional requirements on a SiO2 layer would depend on the gate electrode used in conjunction with the SiO2 gate dielectric. Using a conventional polysilicon gate would result in an additional increase in teq for the SiO2 layer. This additional thickness could be eliminated by using a metal gate electrode, though metal gates are not currently used in complementary metal-oxide-semiconductor field effect transistor (CMOS) technology. Thus, future devices would be designed towards a physical SiO2 gate dielectric layer of about 5 Å or less. Such a small thickness requirement for a SiO2 oxide layer creates additional problems.
Silicon dioxide is used as a gate dielectric, in part, due to its electrical isolation properties in a SiO2—Si based structure. This electrical isolation is due to the relatively large band gap of SiO2 (8.9 eV) making it a good insulator from electrical conduction. Signification reductions in its band gap would eliminate it as a material for a gate dielectric. As the thickness of a SiO2 layer decreases, the number of atomic layers, or monolayers of the material in the thickness decreases. At a certain thickness, the number of monolayers will be sufficiently small that the SiO2 layer will not have a complete arrangement of atoms as in a larger or bulk layer. As a result of incomplete formation relative to a bulk structure, a thin SiO2 layer of only one or two monolayers will not form a full band gap. The lack of a full band gap in a SiO2 gate dielectric would cause an effective short between an underlying Si channel and an overlying polysilicon gate. This undesirable property sets a limit on the physical thickness to which a SiO2 layer can be scaled. The minimum thickness due to this monolayer effect is thought to be about 7-8 Å. Therefore, for future devices to have a teq less than about 10 Å, other dielectrics than SiO2 need to be considered for use as a gate dielectric.
For a typical dielectric layer used as a gate dielectric, the capacitance is determined as one for a parallel plate capacitance: C=κε0A/t, where κ is the dielectric constant, ε0 is the permittivity of free space, A is the area of the capacitor, and t is the thickness of the dielectric. The thickness, t, of a material is related to teq for a given capacitance with the dielectric constant of SiO2, κox32 3.9, associated with teq, as
t=(κ/κox)t eq=(κ/3.9)t eq.
Thus, materials with a dielectric constant greater than that of SiO2, 3.9, will have a physical thickness that can be considerably larger than a desired teq, while providing the desired equivalent oxide thickness. For example, an alternate dielectric material with a dielectric constant of 10 could have a thickness of about 25.6 Å to provide a teq of 10 Å, not including any depletion/inversion layer effects. Thus, the reduced equivalent oxide thickness of transistors can be realized by using dielectric materials With higher dielectric constants than SiO2.
The thinner equivalent oxide thickness, teq, required for lower transistor operating voltages and smaller transistor dimensions may be realized by a significant number of materials, but additional fabricating requirements makes determining a suitable replacement for SiO2 difficult. The current view for the microelectronics industry is still for Si based devices. This requires that the gate dielectric employed be grown on a silicon substrate or silicon layer, which places significant restraints on the substitute dielectric material. During the formation of the dielectric on the silicon layer, there exists the possibility that a small layer of SiO2 could be formed in addition to the desired dielectric. The result would effectively be a dielectric layer consisting of two sublayers in parallel with each other and the silicon layer on which the dielectric is formed. In such a case, the resulting capacitance would be that of two dielectrics in series. As a result, the teq of the dielectric layer would be the sum of the SiO2 thickness and a multiplicative factor of the thickness of the dielectric being formed. Thus, if a SiO2 layer is formed in the process, the teq is again limited by a SiO2 layer. In the event, that a barrier layer is formed between the silicon layer and the desired dielectric in which the barrier layer prevents the formation of a SiO2 layer, the teq would be limited by the layer with the lowest dielectric constant. However, whether a single dielectric layer with a high dielectric constant or a barrier layer with a higher dielectric constant than SiO2 is employed, the layer interfacing with the silicon layer must provide a high quality interface to maintain a high channel carrier mobility.
What is needed is an alternate dielectric material for forming a gate dielectric that has a high dielectric constant relative to SiO2, and is thermodynamically stable with respect to silicon such that forming the dielectric on a silicon layer will not result in SiO2 formation, or diffusion of material, such as dopants, into the gate dielectric from the underlying silicon layer.
A solution to the problems as discussed above is addressed in the present invention. In accordance with the present invention, a method of forming a gate dielectric on a transistor body region includes evaporating Al2O3 at a given rate, evaporating La2O3 at another rate, and controlling the first rate and the second rate to provide an amorphous film containing LaAlO3 on the transistor body region. The evaporation deposition of the LaAlO3 film is performed using two electron guns to evaporate dry pellets of Al2O3 and La2O3. The two rates for evaporating the materials are selectively chosen to provide a dielectric film composition having a predetermined dielectric constant ranging from the dielectric constant of an Al2O3 film to the dielectric constant of a La2O3 film.
A transistor is fabricated by forming two source/drain regions separated by a body region, evaporating Al2O3 using an electron gun at one rate, evaporating La2O3 using a second electron gun at a second rate, controlling the two evaporation rates to provide a film containing LaAlO3 on the body region, and forming a conductive gate on the film containing LaAlO3. Dry pellets of Al2O3 and La2O3 are used for evaporating Al2O3 and La2O3. Controlling the two rates provides the capability to form a film composition having a predetermined dielectric constant.
Advantageously, these methods can be used to further form a memory array where the process of forming the memory is adapted to form the gate dielectric in accordance with the present invention. Additionally, an information handling system can be formed using the methods of the present invention, wherein a memory array formed in conjunction with forming a processor is formed to include transistors having gate dielectrics containing LaAlO3. These gate dielectrics are formed by evaporating Al2O3 using an electron gun at one rate, evaporating La2O3 using a second electron gun at a second rate, and controlling the two evaporation rates to provide a film containing LaAlO3 for use as the gate dielectric.
In accordance with the present invention, a transistor having two source/drain regions separated by a body region includes an amorphous gate dielectric containing LaAlO3 located above the body region between the two source/drain regions. The gate dielectric may be essentially composed of LaAlO3 or it may also contain Al2O3, and La2O3. Depending on its composition, the dielectric constant of the gate dielectric can range from about 9 to about 30. Depending on its composition, the gate dielectric can have a thickness corresponding to an equivalent oxide thickness (teq) in the range from about 1.5 Angstroms to about 5 Angstroms, in addition to larger teq values.
Advantageously, a memory array includes a number of transistors having two source/drain regions separated by a body region with an amorphous gate dielectric containing LaAlO3 located above the body region between the two source/drain regions. These transistors provide the memory array with an array of transistors having gate dielectrics with equivalent oxide thickness (teq) in the range from about 1.5 Angstroms to about 5 Angstroms, providing transistors operable at reduced voltage levels. Additionally, an information handling device, such as a computer, includes a processor and a memory array having a number of transistors having two source/drain regions separated by a body region that includes an amorphous gate dielectric containing LaAlO3 located above the body region between the two source/drain regions.
These and other embodiments, aspects, advantages, and features of the present invention will be set forth in part in the description which follows, and in part will become apparent to those skilled in the art by reference to the following description of the invention and referenced drawings or by practice of the invention. The aspects, advantages, and features of the invention are realized and attained by means of the instrumentalities, procedures, and combinations particularly pointed out in the appended claims.
In the following detailed description of the invention, reference is made to the accompanying drawings which form a part hereof, and in which is shown, by way of illustration, specific embodiments in which the invention may be practiced. In the drawings, like numerals describe substantially similar components throughout the several views. These embodiments are described in sufficient detail to enable those skilled in the art to practice the invention. Other embodiments may be utilized and structural, logical, and electrical changes may be made without departing from the scope of the present invention.
The terms wafer and substrate used in the following description include any structure having an exposed surface with which to form the integrated circuit (IC) structure of the invention. The term substrate is understood to include semiconductor wafers. The term substrate is also used to refer to semiconductor structures during processing, and may include other layers that have been fabricated thereupon. Both wafer and substrate include doped and undoped semiconductors, epitaxial semiconductor layers supported by a base semiconductor or insulator, as well as other semiconductor structures well known to one skilled in the art. The term conductor is understood to include semiconductors, and the term insulator or dielectric is defined to include any material that is less electrically conductive than the materials referred to as conductors.
The term “horizontal” as used in this application is defined as a plane parallel to the conventional plane or surface of a wafer or substrate, regardless of the orientation of the wafer or substrate. The term “vertical” refers to a direction perpendicular to the horizontal as defined above. Prepositions, such as “on”, “side” (as in “sidewall”), “higher”, “lower”, “over” and “under” are defined with respect to the conventional plane or surface being on the top surface of the wafer or substrate, regardless of the orientation of the wafer or substrate. The following detailed description is, therefore, not to be taken in a limiting sense, and the scope of the present invention is defined only by the appended claims, along with the full scope of equivalents to which such claims are entitled.
In a recent article by G. D. Wilk et al., Journal of Applied Physics, vol. 89: no. 10, pp. 5243-5275 (2001), material properties of high dielectric materials for gate dielectrics were discussed. Among the information disclosed was the viability of Al2O3 as a substitute for SiO2. Al2O3 was disclosed has having favourable properties for use as a gate dielectric such as high band gap, thermodynamic stability on Si up to high temperatures, and an amorphous structure. In addition, Wilk disclosed that forming a layer of Al2O3 on silicon does not result in a SiO2 interfacial layer. However, the dielectric constant of Al2O3 is only 9, where thin layers may have a dielectric constant of about 8 to about 10. Though the dielectric constant of Al2O3 is in an improvement over SiO2, a higher dielectric constant for a gate dielectric is desirable. Other dielectrics and heir properties discussed by Wilk include
Dielectric Constant Band gap Material (κ) Eg (eV) Crystal Structure(s) SiO2 3.9 8.9 Amorphous Si3N4 7 5.1 Amorphous Al2O3 9 8.7 Amorphous Y2O3 15 5.6 Cubic La2O3 30 4.3 Hexagonal, Cubic Ta2O3 26 4.5 Orthorhombic TiO2 80 3.5 Tetrag. (rutile, anatase) HfO2 25 5.7 Mono., Tetrag., Cubic ZrO2 25 7.8 Mono., Tetrag., Cubic
One of the advantages using SiO2 as a gate dielectric has been that the formation of the SiO2 layer results is an amorphous gate dielectric. Having an amorphous structure for a gate dielectric is advantageous because grain boundaries in polycrystalline gate dielectrics provide high leakage paths. Additionally, grain size and orientation changes throughout a polycrystalline gate dielectric can cause variations in the film's dielectric constant. The abovementioned material properties including structure are for the materials in a bulk form. The materials having the advantage of a high dielectric constants relative to SiO2 also have the disadvantage of a crystalline form, at least in a bulk configuration. The best candidates for replacing SiO2 as a gate dielectric are those with high dielectric constant, which can be fabricated as a thin layer with an amorphous form.
Reportedly, a physical thickness of about 21 Å of Al2O3, grown by thermal oxidation following thermal evaporation of an Al layer, could be obtained providing a teq of 9.6 Å with an interface state density greater than or equal to 3×1010 eV−1 cm−2. Higher physical thicknesses of about 48 Å of Al2O3 provided films with teq of 21 Å with leakage current of approximately 10−8 A/cm2 at 1 V gate bias, which is good when compared to a leakage current of 10−1 A/cm2 at 1 V gate bias for a physical thickness of 21 Å for a pure SiO2 layer.
Another abovementioned material, La2O3, reportedly provided good results when fabricating thin films on silicon. A physical thickness of 33 Å was obtained for a layer of La2O3, grown by thermal oxidation following thermal evaporation of a La layer, providing a teq of 4.8 Å, a leakage current of 10−1 A/cm2 at 1 V gate bias, and an interface state density of approximately 3×1010 eV−1 cm2. Other studies on La2O3 showed reduced leakage current but an interfacial SiOx layer.
Though both Al2O3 and La2O3 demonstrated good qualities as a substitute for SiO2, better dielectrics are needed. In a recent article by B. Park et al., Applied Physics Letters, vol. 79: no. 6, pp. 806-808 (2001), use of LaAlO3 on silicon as a buffer layer between the silicon surface and a ferroelectric film was reported. A LaAlO3 film was deposited on a silicon substrate by heating single crystal pellets of LaAlO3 using an electron gun with the substrate maintained at room temperature. The LaAlO3 film was annealed ex situ in an electric furnace at 700° C. for 10 minutes in N2 ambience. Films having thickness from 18 nm to 80 nm were grown. The resultant films were determined to have a leakage current density decreased by about three orders of magnitude after annealing. This reported experimentation providing a LaAlO3 buffer layer between silicon and a ferroelectric film demonstrated that a LaAlO3 film could be obtained on silicon providing an amorphous dielectric layer with a dielectric constant between 21 and 24. Other reports indicate that LaAlO3 film can be grown by metal-organic chemical-vapor-deposition method, pulsed-laser depositions method, and rf magnetron sputtering method.
In accordance with the present invention, layers of LaAlO3 can be deposited on silicon using low cost starting materials and resulting in dielectric layers whose dielectric constant can be chosen to range from the dielectric constant of Al2O3 to the dielectric constant of La2O3. Advantageously, a layer of LaAlO3 is grown using dry pellets of Al2O3 and La2O3. The gate dielectric is formed on a silicon substrate or silicon layer by electron beam evaporation of the dry pellets of using two electron guns controlled by two rate monitors. Controlling the rates for evaporating the dry pellets Al2O3 and La2O3 allows for the formation of a gate dielectric having a composition with a predetermined dielectric constant. The predetermined dielectric constant will range from the dielectric constant of Al2O3 to the dielectric constant of La2O3, depending on the composition of the film. The composition of the film can be shifted more towards an Al2O3 film or more towards a La2O3 film, depending upon the choice of the dielectric constant.
During the evaporation process, the electron guns 263, 265 generate electron beams 264, 266. Beginning the evaporation process using electron gun 265 is performed substantially concurrent with beginning the evaporation process using electron gun 265. The electron beam 264 hits target 261 containing dry pellets of Al2O3, and heats a portion of target 261 enough to cause the dry pellets of Al2O3 on the surface of the target 261 to evaporate. The evaporated material 268 is then distributed throughout the chamber 260. The electron beam 266 hits target 262 containing dry pellets of La2O3, and heats a portion of target 262 enough to cause the dry pellets of La2O3 the surface of the target 262 to evaporate. The evaporated material 269 is then distributed throughout the chamber 260. Evaporate material 268 and evaporate material 269 are intermingled throughout the chamber forming a film 240 containing LaAlO3 on the surface of the exposed body region 233 that it contacts.
The evaporation process can be performed in chamber 260 using a base pressure lower than about 5×10−7 Torr and a deposition pressure less than about 2×10−6 Torr. Performing the evaporation under these conditions should allow a growth rate in the range from about 0.5 to about 50 nm/min. After deposition, the wafer or substrate 210 containing the film is annealed ex situ in an electric furnace at about 700° C. for about 10 minutes in N2 ambience. Alternately, the wafer or substrate 210 can be annealed by RTA for about 10 to about 15 seconds in N2 ambience.
The LaAlO3 dielectric film should have a dielectric constant in the range of about 21 to about 25. However, by controlling the evaporation rates of the first electron gun 263 and the second electron gun 265, the composition of the film can vary from be a film of essentially Al2O3 to a film that is essentially La2O3. Correspondingly, the dielectric constant of the formed film will range from about 9 to about 30, with a dielectric constant in the range of about 21 to about 25 corresponding to a layer that is essentially LaAlO3. Thus, choosing a predetermined dielectric constant in the range of about 9 to about 30, the two electron guns will be controlled to formed a film containing Al2O3, La2O3, and LaAlO3 in varying amounts depending on the setting for controlling the evaporation rates.
A range of equivalent oxide thickness, teq, attainable in accordance with the present invention is associated with the capability to provide a composition having a dielectric constant in the range form about 9 to about 30, and the capability to attain growth rates in the range of from about 0.5 to about 50 nm/min. The teq range in accordance with the present invention are shown in the following
Physical Thickness Physical Thickness Physical Thickness t = 0.5 nm (5 Å) t = 1.0 nm (10 Å) t = 50 nm (500 Å) κ teq (Å) teq (Å) teq (Å) 9 2.17 4.33 216.67 21 .93 1.86 92.86 25 .78 1.56 78 30 .65 1.3 65
LaAlO3 in a bulk form at room temperature has a nearly cubic perovskite crystal structure with a lattice constant of 0.536 nm. Fortunately, the films grown by electron gun evaporation have an amorphous form, though it is expected that a dimension for a monolayer of LaAlO3 is related to its lattice constant in bulk form. At a physical thickness about 0.5 nm, teq would be expected to range from about 2.2 Å to about 0.65 Å for the dielectric constant ranging from 9 to 30. For a layer of essentially LaAlO3, teq would be expected to range from about 0.93 Å to about 0.78 Å for a physical layer of 0.5 nm. The lower limit on the scaling of a layer containing LaAlO3 would depend on the monolayers of the film necessary to develop a full band gap such that good insulation is maintained between an underlying silicon layer and an overlying conductive layer to the LaAlO3 film. This requirement is necessary to avoid possible short circuit effects between the underlying silicon layer and the overlying conductive layer. For a substantially LaAlO3 film having a thickness of approximately 2 nm, teq would range from about 3 Å to about 3.7 Å. From above, it is apparent that a film containing LaAlO3 can be attained with a teq ranging from 1.5 Å to 5 Å. Further, such a film can provide a teq significantly less than 2 or 3 Å, even less than 1.5 Å.
The novel process described above provides significant advantages by evaporating dry pellets of Al2O3 and La2O3. Dry pellets of Al2O3 and La2O3 are less expensive than single crystal pellets of LaAlO3. Further, using two electron guns allows the formation of a gate dielectric with a chosen dielectric constant. Additionally, the novel process can be implemented to form transistors, memory devices, and information handling devices.
A transistor 100 as depicted in
The method of evaporating LaAlO3 films for a gate dielectric in accordance with the present invention can be applied to other transistor structures having dielectric layers. For example, the structure of
Transistors created by the methods described above may be implemented into memory devices and information handling devices as shown in
A personal computer, as shown in
Microprocessor 506 produces control and address signals to control the exchange of data between memory bus circuit 508 and microprocessor 506 and between memory bus circuit 508 and peripheral circuitry 510. This exchange of data is accomplished over high speed memory bus 520 and over high speed I/O bus 522.
Coupled to memory bus 520 are a plurality of memory slots 512(a-n) which receive memory devices well known to those skilled in the art. For example, single in-line memory modules (SIMMs) and dual in-line memory modules (DIMMs) may be used in the implementation of the present invention.
These memory devices can be produced in a variety of designs which provide different methods of reading from and writing to the dynamic memory cells of memory slots 512. One such method is the page mode operation. Page mode operations in a DRAM are defined by the method of accessing a row of a memory cell arrays and randomly accessing different columns of the array. Data stored at the row and column intersection can be read and output while that column is accessed. Page mode DRAMs require access steps which limit the communication speed of memory circuit 508. A typical communication speed for a DRAM device using page mode is approximately 33 MHZ.
An alternate type of device is the extended data output (EDO) memory which allows data stored at a memory array address to be available as output after the addressed column has been closed. This memory can increase some communication speeds by allowing shorter access signals without reducing the time in which memory output data is available on memory bus 520. Other alternative types of devices include SDRAM, DDR SDRAM, SLDRAM and Direct RDRAM as well as others such as SRAM or Flash memories.
Control, address and data information provided over memory bus 520 is further represented by individual inputs to DRAM 600, as shown in
As is well known in the art, DRAM 600 includes memory array 610 which in turn comprises rows and columns of addressable memory cells. Each memory cell in a row is coupled to a common wordline. The wordline is coupled to gates of individual transistors, where at least one transistor has a gate coupled to a gate dielectric containing LaAlO3 in accordance with the method and structure previously described above. Additionally, each memory cell in a column is coupled to a common bitline. Each cell in memory array 610 includes a storage capacitor and an access transistor as is conventional in the art.
DRAM 600 interfaces with, for example, microprocessor 606 through address lines 604 and data lines 602. Alternatively, DRAM 600 may interface with a DRAM controller, a micro-controller, a chip set or other electronic system. Microprocessor 506 also provides a number of control signals to DRAM 600, including but not limited to, row and column address strobe signals RAS and CAS, write enable signal WE, an output enable signal OE and other conventional control signals.
Row address buffer 612 and row decoder 614 receive and decode row addresses from row address signals provided on address lines 604 by microprocessor 506. Each unique row address corresponds to a row of cells in memory array 610. Row decoder 614 includes a wordline driver, an address decoder tree, and circuitry which translates a given row address received from row address buffers 612 and selectively activates the appropriate wordline of memory array 610 via the wordline drivers.
Column address buffer 616 and column decoder 618 receive and decode column address signals provided on address lines 604. Column decoder 618 also determines when a column is defective and the address of a replacement column. Column decoder 618 is coupled to sense amplifiers 620. Sense amplifiers 620 are coupled to complementary pairs of bitlines of memory array 610.
Sense amplifiers 620 are coupled to data-in buffer 622 and data-out buffer 624. Data-in buffers 622 and data-out buffers 624 are coupled to data lines 602. During a write operation, data lines 602 provide data to data-in buffer 622. Sense amplifier 620 receives data from data-in buffer 622 and stores the data in memory array 610 as a charge on a capacitor of a cell at an address specified on address lines 604.
During a read operation, DRAM 600 transfers data to microprocessor 506 from memory array 610. Complementary bitlines for the accessed cell are equilibrated during a precharge operation to a reference voltage provided by an equilibration circuit and a reference voltage supply. The charge stored in the accessed cell is then shared with the associated bitlines. A sense amplifier of sense amplifiers 620 detects and amplifies a difference in voltage between the complementary bitlines. The sense amplifier passes the amplified voltage to data-out buffer 624.
Control logic 606 is used to control the many available functions of DRAM 600. In addition, various control circuits and signals not detailed herein initiate and synchronize DRAM 600 operation as known to those skilled in the art. As stated above, the description of DRAM 600 has been simplified for purposes of illustrating the present invention and is not intended to be a complete description of all the features of a DRAM. Those skilled in the art will recognize that a wide variety of memory devices, including but not limited to, SDRAMs, SLDRAMs, RDRAMs and other DRAMs and SRAMs, VRAMs and EEPROMs, may be used in the implementation of the present invention. The DRAM implementation described herein is illustrative only and not intended to be exclusive or limiting.
A gate dielectric containing LaAlO3 and method of fabricating a gate dielectric contained LaAlO3 are provided that produces a reliable gate dielectric having a thinner equivalent oxide thickness than attainable using SiO2. LaAlO3 gate dielectrics formed using the methods described herein are thermodynamically stable such that the gate dielectrics formed will have minimal reactions with a silicon substrate or other structures during processing.
Transistors and higher level ICs or devices are provided utilizing the novel gate dielectric and process of formation. Gate dielectric layers containing LaAl3 are formed having a high dielectric constant (κ) capable of a teq thinner than 5 Å, thinner than the expected limit for SiO2 gate dielectrics. At the same time, the physical thickness of the LaAlO3 layer is much larger than the SiO2 thickness associated with the teq limit of SiO2. Forming the larger thickness provides advantages in processing the gate dielectric. In addition forming a dielectric containing LaAlO3, Al2O3, and La2O3 through controlling the evaporation of Al2O3 and La2O3 sources allows the selection of a dielectric constant ranging from that of Al2O3 to the dielectric constant of La2O3.
Although specific embodiments have been illustrated and described herein, it will be appreciated by those of ordinary skill in the art that any arrangement which is calculated to achieve the same purpose may be substituted for the specific embodiment shown. This application is intended to cover any adaptations or variations of the present invention. It is to be understood that the above description is intended to be illustrative, and not restrictive. Combinations of the above embodiments, and other embodiments will be apparent to those of skill in the art upon reviewing the above description. The scope of the invention includes any other applications in which the above structures and fabrication methods are used. The scope of the invention should be determined with reference to the appended claims, along with the full scope of equivalents to which such claims are entitled.
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|Clasificación de EE.UU.||257/410, 438/261, 438/216, 257/411, 438/591|
|Clasificación internacional||H01L21/28, H01L29/51|
|Clasificación cooperativa||H01L21/02192, H01L29/517, H01L21/02194, H01L21/02178, H01L21/02269, H01L21/28185, H01L21/28194|
|Clasificación europea||H01L21/02K2C1M3A, H01L21/02K2C1M3U, H01L21/02K2C1M3R, H01L21/02K2E3B4, H01L29/51M, H01L21/28E2C2C, H01L21/28E2C2D|