阅读说明：本技术 半导体非易失性存储器的抹除方法 (Erasing method of semiconductor nonvolatile memory ) 是由 王立中 于 2019-10-15 设计创作，主要内容包括：本发明揭露一种半导体非易失性存储器的抹除方法。为抹除四端点的半导体非易失性存储器装置,施加一高的正电压偏压至控制栅,且源极、基底及漏极电极连接至接地电压,以将电荷储存物质中的储存电荷移至控制栅。通过降低施加电压偏压及降低施加电压期间以改善抹除效率及半导体NVM装置的耐久性寿命,本发明在接近介电层介面设计控制栅的侧面杂质分布剖面,使电荷储存物质至控制栅的穿隧效应发生于介电层介面的控制栅的小侧面区。本发明亦利用半导体非易失性存储器装置电荷储存物质及控制栅之间的耦合介电层的厚度不均匀,导致进行抹除操作的穿隧效应发生于小的薄耦合介电层区。其中,小的薄耦合介电层区内的电场强度最强以进行穿隧抹除操作。(The invention discloses an erasing method of a semiconductor nonvolatile memory. To erase a four-terminal semiconductor non-volatile memory device, a high positive voltage bias is applied to the control gate, and the source, substrate and drain electrodes are connected to a ground voltage to move the stored charge in the charge storing substance to the control gate. By reducing the applied voltage bias and reducing the applied voltage period to improve erase efficiency and endurance life of the semiconductor NVM device, the present invention designs the lateral impurity profile of the control gate near the dielectric interface such that tunneling of charge storage material to the control gate occurs at the small lateral area of the control gate at the dielectric interface. The present invention also takes advantage of the non-uniform thickness of the coupling dielectric between the charge storage material and the control gate of a semiconductor nonvolatile memory device, resulting in tunneling for erase operations occurring in small thin coupling dielectric regions. Wherein the electric field strength in the small thin coupling dielectric layer region is strongest for tunneling erase operation.)

1. A method of erasing a semiconductor nonvolatile memory device on a substrate, the semiconductor nonvolatile memory device comprising a source electrode, a drain electrode, a charge storage material, and a control gate, the method comprising:

applying a first voltage to the source electrode, the drain electrode and the substrate electrode; and

applying a second voltage to the electrode of the control gate such that electrons tunnel from the charge storage material into the control gate;

wherein the first voltage is less than or equal to 0V and the second voltage is greater than or equal to 0V.

2. The method of claim 1, wherein a voltage difference between a control gate and the charge storage material is maximized if a capacitance of the control gate to the charge storage material is minimized.

3. The method of claim 1, wherein the control gate has a first surface and a second surface and includes a first impurity region and N second impurity regions overlapping the charge storage material, wherein a tunnel dielectric film is between the charge storage material and the control gate, and wherein the N second impurity regions have a higher impurity concentration than the first impurity region and N > 1.

4. The method of claim 3, wherein the step of applying the second voltage to the electrode of the control gate comprises:

applying the second voltage to the electrode of the control gate on the second surface causes the plurality of electrons to tunnel from the charge storage material through a portion of the tunnel dielectric film into the N second impurity regions, and forming a charge-depleted region from the first surface in the first impurity region, wherein the first surface is in contact with the tunnel dielectric film.

5. The method of claim 4, wherein a depth of the charge-depleted region extending from the first surface to the control gate is determined by an impurity concentration of the first impurity region and a magnitude of the second voltage.

6. The method of claim 5 wherein a capacitance of a control gate to charge storage material decreases as a depth of the charge-depleted region in the control gate increases.

7. The method of claim 4, wherein said charge-depleted region is not formed within said N second impurity regions.

8. The method of claim 4, wherein the maximum value of the second voltage is a breakdown voltage of a junction between the control gate and the substrate if the control gate is embedded in the substrate.

9. The method of claim 4, wherein if condition C is met_cg＝C_cgm+N×C_cge≈N×C_cge<<C_S+C_sub+C_DA voltage difference between the control gate and the charge storage material is maximized, where C_cgA capacitance value, C, representing a control gate to the charge storage material_cgmA capacitance value C representing a first impurity region to the charge storage material_cgeA capacitance value C representing a second impurity region to the charge storage material_SRepresenting a source to charge storage material capacitance value, C_DRepresents a drain to charge storage material capacitance and C_subRepresenting the capacitance from a substrate to the charge storage material.

10. The method of claim 9, wherein C is_cgAnd C_cgmIs a function of the second voltage.

11. The method of claim 1, wherein the semiconductor nonvolatile memory device further comprises: a tunnel dielectric film between the charge storage material and the control gate, wherein the tunnel dielectric film comprises a first dielectric region and a second dielectric region, and the first dielectric region is thicker than the second dielectric region, and wherein the step of applying the second voltage to the electrode of the control gate comprises:

applying the second voltage to the electrode of the control gate causes the plurality of electrons to tunnel from the charge storage material, through the second dielectric region, and into the control gate.

12. The method of claim 11, wherein if the condition is met: c_cg＝C_cg1+C_cg2<<C_S+C_sub+C_DA voltage difference between the control gate and the charge storage material is maximized, where C_cgRepresenting the capacitance from a control gate to the charge storage material、C_cg1A first capacitance value, C, representing the first dielectric region of the tunneling dielectric film between the control gate and the charge storage material_cg2A second capacitance value, C, representing the second dielectric region of the tunneling dielectric film between the control gate and the charge storage material_SRepresenting a source to charge storage material capacitance value, C_DRepresents a drain to charge storage material capacitance and C_subRepresenting the capacitance from a substrate to the charge storage material.

13. The method of claim 12, wherein C is C when the thickness of the first dielectric region increases_cgWith a consequent reduction.

14. The method of claim 12, wherein C is C when the area ratio of the first dielectric region to the second dielectric region is increased_cgWith a consequent reduction.

15. The method of claim 11, wherein the first dielectric region has an area greater than an area of the second dielectric region.

16. The method of claim 11, wherein a magnitude of a first electric field from the control gate through the first dielectric region to the charge storage material is less than a magnitude of a second electric field from the control gate through the second dielectric region to the charge storage material.

17. The method of claim 11, wherein the second dielectric region has an oxide layer thickness in a range of

18. The method of claim 1, wherein the charge storage material is one of a conductive floating gate, a charge trapping dielectric film, and a nanocrystal.

Technical Field

The present invention relates to a method of erasing a semiconductor non-volatile memory (NVM), and more particularly to a method of erasing a NVM using capacitive coupling between a charge storage material and a control gate to generate a strong electric field at a desired location to move charge away from the charge storage material.

Background

An electrically-erasable-programmable-read-only memory (EEPROM) is a semiconductor NVM device that can be electrically programmed and erased. The non-volatile nature allows the memory device to continue to retain the stored digital information, which is representative of the amount of charge stored in the charge storing material, such as conductive floating gates, charge trapping dielectric films, or nanocrystals. The isolating dielectric material permanently surrounds the charge storage material to retain the charge representing the stored non-volatile information for a long period of time, typically over ten years. Nonvolatile data is stored in binary format (binary format) in NVM cells by setting each NVM cell to a programmed state and resetting (reset) the NVM cell to an erased state. Programming of NVM cells is typically accomplished by storing electrons in the charge storage material by electron tunneling (tunneling) through an isolation dielectric (dielectric) or by injecting high kinetic energy electrons through an isolation dielectric. Erasing an EEPROM cell is typically accomplished by either tunneling electrons through the isolation dielectric or injecting high kinetic energy holes through the isolation dielectric to remove electrons from the charge storage material.

In the enclosed isolation dielectric, there must be a strong enough electric field to tunnel electrons into/out of the charge storage material. For example, the Fowler-Nordheim tunneling (Fowler-Nordheim tunneling) current in an oxide layer (dielectric layer) is expressed by the following equation:and Frankel-Pool emission (Frankel-Pool emission) in the charge trapping dielectric layer is expressed by the following equation:where E represents the electric field and constants a and b are independent of the electric field. Due to the exponential terms in the above equation, the electric field generated by applying different voltage biases to the semiconductor NVM device terminals (terminals) must be strong enough to generate a large enough moving current in the isolation dielectric. FIG. 1 shows a conventional semiconductor NVThe Fowler-Nordheim tunneling erase operation is performed in the tunnel oxide of the M device by applying ground voltage to the control gate 101 and coupling a high positive voltage V_hTo the other terminals (source electrode 102/drain electrode 103/substrate electrode 104). According to the rule of thumb (rule of thumb), the electric field strength of Fowler-Nordheim tunneling in the oxide layer is about 10⁷V/cm, which is equivalent to applying a voltage difference of 10V to a thickness ofOxide layer of (2). When the strong electric field is generated in the tunnel oxide layer between the floating gate 105 and the substrate 104 of the semiconductor NVM device: (>10⁷V/cm) a large number of electrons stored in the floating gate 105 tunnel out of the floating gate 105 and into the source region 102/drain region 103/substrate region 104.

Therefore, the prior art erase efficiency is low and the endurance life of the semiconductor NVM device is short.

Disclosure of Invention

Embodiments of the present invention provide a method of erasing a semiconductor non-volatile memory device to improve erase efficiency and endurance life of the semiconductor NVM device.

The embodiment of the invention provides a method for erasing a semiconductor nonvolatile memory, wherein a semiconductor nonvolatile memory device on a substrate comprises a source electrode, a drain electrode, a charge storage substance and a control gate, and the method comprises the following steps:

applying a first voltage to the source electrode, the drain electrode and the substrate electrode; and

applying a second voltage to the electrode of the control gate such that electrons tunnel from the charge storage material into the control gate;

wherein the first voltage is less than or equal to 0V and the second voltage is greater than or equal to 0V.

In one embodiment, a voltage difference between a control gate and a charge storage material is maximized if the capacitance of the control gate to the charge storage material is minimized.

In one embodiment, the control gate has a first surface and a second surface and includes a first impurity region and N second impurity regions overlapping the charge storage material, wherein a tunnel dielectric film is interposed between the charge storage material and the control gate, and wherein the N second impurity regions have an impurity concentration higher than the first impurity region and N > 1.

In one embodiment, the step of applying the second voltage to the electrode of the control gate comprises:

applying the second voltage to the electrode of the control gate on the second surface causes the plurality of electrons to tunnel from the charge storage material through a portion of the tunnel dielectric film into the N second impurity regions, and forming a charge-depleted region from the first surface in the first impurity region, wherein the first surface is in contact with the tunnel dielectric film.

In one embodiment, the depth of the charge-depleted region extending from the first surface to the control gate depends on the impurity concentration of the first impurity region and the magnitude of the second voltage.

In one embodiment, the capacitance of a control gate to charge storage material is reduced as the depth of the charge depletion region in the control gate is increased.

In one embodiment, the charge-depleted region is not formed in the N second impurity regions.

In one embodiment, if the control gate is embedded in the substrate, the maximum value of the second voltage is a breakdown voltage of a junction between the control gate and the substrate.

In one embodiment, if condition C is met_cg＝C_cgm+N×C_cge≈N×C_cge<<C_S+C_sub+C_DA voltage difference between the control gate and the charge storage material is maximized, where C_cgA capacitance value, C, representing a control gate to the charge storage material_cgmA capacitance value C representing a first impurity region to the charge storage material_cgeA capacitance value C representing a second impurity region to the charge storage material_SRepresenting a source to charge storage material capacitance value, C_DRepresents a drain to charge storage materialAnd C_subRepresenting the capacitance from a substrate to the charge storage material.

In one embodiment, C_cgAnd C_cgmIs a function of the second voltage.

In one embodiment, the semiconductor nonvolatile memory device further comprises: a tunnel dielectric film between the charge storage material and the control gate, wherein the tunnel dielectric film comprises a first dielectric region and a second dielectric region, and the first dielectric region is thicker than the second dielectric region, and wherein the step of applying the second voltage to the electrode of the control gate comprises:

applying the second voltage to the electrode of the control gate on the second surface causes the plurality of electrons to tunnel from the charge storage material, through the second dielectric region, and into the control gate.

In one embodiment, if the condition is met: c_cg＝C_cg1+C_cg2<<C_S+C_sub+C_DA voltage difference between the control gate and the charge storage material is maximized, where C_cgA capacitance value, C, representing a control gate to the charge storage material_cg1A first capacitance value, C, representing the first dielectric region of the tunneling dielectric film between the control gate and the charge storage material_cg2A second capacitance value, C, representing the second dielectric region of the tunneling dielectric film between the control gate and the charge storage material_SRepresenting a source to charge storage material capacitance value, C_DRepresents a drain to charge storage material capacitance and C_subRepresenting the capacitance from a substrate to the charge storage material.

In one embodiment, C is added when the thickness of the first dielectric region is increased_cgWith a consequent reduction.

In one embodiment, C is increased when the area ratio of the first dielectric region to the second dielectric region is increased_cgWith a consequent reduction.

In one embodiment, the area of the first dielectric region is larger than the area of the second dielectric region.

In one embodiment, a magnitude of a first electric field from the control gate through the first dielectric region to the charge storage material is less than a magnitude of a second electric field from the control gate through the second dielectric region to the charge storage material.

In one embodiment, the second dielectric region has an oxide layer thickness in a range

In one embodiment, the charge storage material is one of a conductive floating gate, a charge trapping dielectric film, and a nanocrystal.

With the present invention, erase efficiency and endurance life of the semiconductor NVM device can be improved.

Drawings

In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below, it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to the drawings without creative efforts.

FIG. 1 shows a schematic diagram of a Fowler-Nordheim tunneling erase operation performed in a tunnel oxide layer of a conventional semiconductor NVM device.

Fig. 2 shows the fowler-nordheim tunneling occurring at two corners of a control gate having a non-uniform lateral impurity profile, wherein a high impurity concentration is located at two corner regions of the control gate and a low impurity concentration is located in a middle region of the control gate, according to an embodiment of the present invention.

Fig. 3 is a circuit diagram of the semiconductor NVM device of fig. 2.

Fig. 4 shows the reduction of the electric field in the tunneling dielectric layer of the control gate with a low uniform impurity concentration.

FIG. 5 is a schematic diagram of a floating gate NVM device with two dielectric layer thicknesses between the control gate and the floating gate according to another embodiment of the present invention.

Fig. 6a and 6b show the concept of converting an existing floating gate (stacked double gate) NVM device into an SGLNVM device.

Fig. 7a shows a top view of the SGLNVM apparatus.

Fig. 7b shows a cross-sectional view of an impurity profile of the N-type control gate (word line AA') in the SGLNVM device of fig. 7 a.

Fig. 8 is a graph showing electrical characteristics of a programmed SGLNVM device and an erased SGLNVM device according to an embodiment of the present invention by using the erasing method of the present invention.

Fig. 9a shows a top view of a conventional floating gate flash memory device with thick and thin tunneling dielectric layers between the floating gate and the control gate.

FIG. 9b shows a cross-sectional view of the control gate along a word line AA' in FIG. 9 a.

Reference numerals:

101. 201a, 301, 401a, 501, 601a, 601b control gate electrode

102. 202, 302, 402, 502, 602a, 602b source electrode

103. 203, 303, 403, 503, 603a, 603b drain electrode

104. 204, 304, 404, 504, 604a, 604b substrate electrodes

201. 401, 930 control gate

201c dielectric layer interface

201d, 401d charge depletion region

205. 305, 505, 605a, 605b, 710, 960 floating gate

60a conventional floating gate NVM device

Model 60b N SGLNVM device

606a, 606b coupling dielectric layers

607a, 607b tunnel oxide layer

712 high impurity concentration extended tip

910 thin tunnel oxide layer

920 common source

940 bit line

Detailed Description

The following detailed description is merely exemplary in nature and is not intended to be limiting. It is to be understood that other embodiments may be utilized and structural changes and modifications may be made without departing from the scope of the claimed invention. Also, it is to be understood that the phraseology and terminology used herein is for the purpose of description and should not be regarded as limiting. The use of the word "comprise" or variations such as "comprises" or "comprising" is used herein to encompass the items listed thereafter and equivalents thereof as well as additional items.

By reducing the applied terminal voltage bias and reducing the applied voltage duration to improve erase efficiency and endurance life (endrandom life) of the semiconductor NVM device, applicants designed a fine capacitive coupling between the charge storage material and the control gate of the semiconductor NVM device.

In order to achieve high efficiency of the tunneling erase operation from the charge storage material to the control gate, the present invention designs a lateral impurity profile (lateral erase profile) in the control gate near the dielectric layer interface, as shown in fig. 2, with a low impurity concentration in the middle region and a high impurity concentration in the two small corner regions (edge regions). When a high positive voltage V is applied_h(>0) to the control gate electrode 201a and the other terminals (source electrode 202/drain electrode 203/substrate electrode 204) are connected to a ground voltage (or a voltage less than 0V), a charge depletion region 201d is formed in the control gate 201 from the dielectric layer interface 201c toward the control gate electrode 201a due to the low impurity concentration, as shown in fig. 2. The depletion depth d in the middle region of the control gate 201 depends on the depth profile (depth profile) of the low impurity concentration from the dielectric layer interface 201c of the control gate 201 and the voltage bias V applied to the control gate electrode 201a_cgThe size of (2). The lower the impurity concentration of the intermediate region and the applied control gate voltage V_cgThe higher the depletion depth d, the deeper the depletion depth d can penetrate from the dielectric interface 201c to the control gate electrode 201 a. Because of the increased depletion depth d, the control gate-to-floating gate capacitance between control gate 201 and floating gate 205 decreases.

For convenience in further explanation of the principles of the present invention, reference is made to the schematic diagram of a floating gate semiconductor NVM device of FIG. 3. The floating gate semiconductor NVM device has four terminalsThe dotted MOSFET device has a control gate electrode 301, a source electrode 302, a drain electrode 303 and a substrate electrode 304 for applying a voltage bias. A floating gate 305 electrically isolates the control gate electrode 301, the source electrode 302, the drain electrode 303 and the substrate electrode 304 to form a control gate to floating gate total capacitance C, respectively_cg(V_cg)＝C_cgm(V_cg)+2C_cgeA source-to-floating gate capacitance Cs, a drain-to-floating gate capacitance C_DAnd a substrate-to-floating gate capacitance C_sub. Wherein the control gate voltage V is applied by increasing_cgTo increase the depletion depth of the low impurity concentration depth profile region and further reduce the middle depletion capacitance value C_cgm(V_cg) And C_cgeRepresents the angular capacitance (edge capacitance) of two non-depleted regions with high impurity concentration. Wherein, C_cg(V_cg) Is represented by C_cgIs V_cgA function of, and C_cgm(V_cg) Is represented by C_cgmIs V_cgAs a function of (c). Thus, the voltage V of the floating gate 305_fCan be expressed by the following equation:

wherein, V_S、V_sub、V_DAnd V_cgAre voltage biases applied to the source electrode 302, the substrate electrode 304, the drain electrode 303 and the control gate electrode 301. When a high voltage V is applied_h(>0) to the control gate electrode 301 of the semiconductor NVM device and the other terminal is connected to a ground voltage (i.e., V)_S＝V_sub＝V_D0V) (or a voltage less than 0V), the floating gate voltage can be further simplified as:

wherein, C_cg(V_h) Is represented by C_cgIs V_hAs a function of (c). On floating gate 305 and control gateAn electric field E generated between the electrodes 301_cgIs represented as follows:

for a given control gate voltage V_hThe condition for maximizing the voltage difference across the control gate electrode 301 and floating gate 305 is C_s+C_sub+C_D>>C_cg(V_h) This case also indicates the total applied voltage difference V_hAlmost straddling the control gate electrode 301 and floating gate 305. However, although the total control gate to floating gate capacitance C is reduced by increasing the depletion depth_cg(V_h) The voltage difference across the control gate electrode 301 and floating gate 305 is maximized, but the tunneling capability in the tunneling dielectric layer is also reduced for a uniform low impurity concentration control gate, as shown in fig. 4. This is because the control gate-to-floating gate capacitance C of a control gate of uniform low impurity concentration_cg(V_cg) Equivalent to a dielectric layer thickness of t_oxDielectric layer capacitance value C_oxAnd the control gate has a hollow depletion thickness of t_dDepletion capacitance value C_dBy the depletion capacitance value C_dThe electric field generated in the tunneling process in the dielectric layer is greatly reduced The method aims to solve the following two problems that: to reduce the total control gate-to-floating gate capacitance to maximize the voltage difference across the control gate electrode 301 and floating gate 305 while maintaining tunneling in the dielectric layer, the present invention designs the impurity profile of the control gate such that a small portion of the high impurity concentration in the control gate (e.g., the corner portion of the control gate of fig. 2) is not affected by the applied control gate voltage V_hAnd deplete (deplete into) the control gate, which has a major portion with a low surface impurity concentration(e.g., the middle portion of the control gate of fig. 2) depletes the control gate, resulting in a reduction in the total capacitance to meet the following condition: c_cg(V_h)＝C_cgm(V_h)+2C_cge≈2C_cge<<C_S+C_sub+C_D. Because the dielectric layer under the non-depleted portion of the control gate receives the full electric field strength to achieve the maximum voltage difference V in the dielectric layer_hThe tunneling effect of the erase operation occurs in the two non-depleted portions of FIG. 2.

It is noted that the two portions of the control gate 201 of fig. 2 having high interface impurity concentrations are merely exemplary and not limiting. In practice, other numbers of portions of control gate 201 of fig. 2 may have high interface impurity concentrations and are within the scope of the present invention.

Another way to minimize the control gate to floating gate capacitance in order to have the maximum voltage difference across the control gate electrode 301 and floating gate 305 without depleting the control gate is to increase the dielectric thickness of the main portion of the control gate. Fig. 5 shows a schematic diagram of a floating gate NVM device with two dielectric layer thicknesses between the control gate 501 and the floating gate 505. Control gate to floating gate total capacitance C_cg＝C_cg1+C_cg2Wherein, C_cg1Indicating the thickness t₁C of the thick tunneling dielectric layer_cg2Indicating the thickness t₂The capacitance of the thin tunneling dielectric layer. At C_s+C_sub+C_D>>C_cgIn order to maximize the voltage difference V across the control gate electrode 501 and floating gate 505_hBy increasing the thickness t of the thick tunneling dielectric layer₁And increasing the area ratio of the thick to thin tunneling dielectric A1/A2 under the overlapping control gate surface region to reduce C_cgWherein A1 and A2 represent the areas of the thick tunneling dielectric layer region and the thin tunneling dielectric layer region, respectively, and A1>A2. Therefore, in the thickness t of the dielectric layer₁And t₂The electric fields in (a) and (b) are respectively represented as follows:

and

because of t₁>t₂When E is greater_cg2>E_cg1And a thickness t in an overlapping region between the control gate and the floating gate₂Tunneling occurs in the thin dielectric layer of (2), as shown in fig. 5.

In one embodiment, the applicant applies the erase method to a Scalable Gate Logic NVM (SGLNVM) device of chinese patent publication No. CN104303310B (the contents of the above patent are incorporated herein by reference in their entirety as part of the present specification). The SGLNVM device is similar to the conventional floating gate NVM device, having a single poly-gate (SGLNVM) structure such as a floating gate with a control gate embedded in a silicon substrate, and is fabricated by conventional CMOS logic process technology. Fig. 6b shows the concept of capacitive coupling for SGLNVM devices with the control gate of the existing floating gate NVM device (fig. 6a) folded into the silicon substrate. Referring to fig. 6b, an N-type SGLNVM device 60b includes a control gate 601b, a source electrode 602b, a base electrode 604b, a floating gate 605b, a drain electrode 603b, a coupling dielectric layer 606b, and a tunnel oxide layer 607 b. In the N-type SGLNVM device 60b, an N-type semiconductor control gate 601b is embedded (embedded) in a P-type semiconductor substrate 604 b. Referring to fig. 6a, a conventional floating gate NVM device 60a includes a control gate 601a, a source electrode 602a, a base electrode 604a, a floating gate 605a, a drain electrode 603a, a coupling dielectric layer 606a, and a tunnel oxide layer 607 a. In contrast to the conventional floating gate NVM device 60a in which a negative voltage (═ 0V) is applied to the control gate 601a and a positive voltage (> ═ 0V) is applied to the source electrode 602a, the base electrode 604a and the drain electrode 603a, applying a negative high voltage to the control gate 601b of the N-type SGLNVM device 60b and connecting a positive voltage (> ═ 0V) to the source electrode 602b, the base electrode 604b and the drain electrode 603b is not allowed because of the forward bias at the junction between the embedded N-type control gate 601b and the P-type semiconductor base 604 b. The only option to apply a bias to the control gate 601b of the N-type SGLNVM device 60b is to apply a high positive voltage (> ═ 0V) to the control gate 601b of the N-type SGLNVM device 60b and connect a negative voltage or ground to the other terminals (source/base/drain) to create a reverse biased junction. For erasing, the maximum value of the bias voltage applied to the control gate is the breakdown voltage of the junction between the embedded N-type control gate 601b and the P-type semiconductor substrate 604 b. For the Fowler-Nordheim tunneling erase, it is necessary to apply a positive voltage lower than the junction breakdown voltage to the embedded N-type control gate to generate a low junction leakage current, which is maintained by the load of the charge pumping circuit. It is desirable to apply a lower control gate voltage to produce a very low junction leakage current between the embedded N-type control gate 601b and the P-type semiconductor substrate 604b to achieve the erase operation. In order to enable a lower control gate voltage, a large portion of the applied voltage difference must be generated in the coupling dielectric 606b between the floating gate 605b and the control gate 601 b. To achieve this, the applicants have designed the profile of the impurity profile of the embedded N-type control gate under the two corners of the floating gate 710 by adding an additional high impurity concentration extension tip (tip)712 near the substrate surface, as shown in fig. 7 b.

Fig. 7a shows a top view of the SGLNVM apparatus. Fig. 7b shows a cross-sectional view of an impurity profile of the N-type control gate (word line AA') in the SGLNVM device of fig. 7 a. Without adding new process, the N-type impurity profile of the control gate with the high impurity concentration extension tip 712 in FIG. 7b is formed by the same process as the highly doped N-type extension (high doped N-type extension) of the conventional N-type metal Oxide Semiconductor Field Effect Transistor (NMOSFET) device in the deep sub-micron (deep sub-micron) CMOS logic process technology. The process of highly doped N-type extensions of conventional NMOSFET devices in deep sub-micron CMOS logic process technology is typically accomplished using a low energy and high dose arsenic implant (inductive implant) prior to forming the device spacers. FIG. 8 shows electrical characteristics of a programmed SGLNVM device and an erased SGLNVM device fabricated in a 40nm CMOS logic process technology of a foundry, where the Fowler-Nordheim tunneling operation can only be accomplished with the erase method of the present invention.

In another embodiment, the dielectric thickness is increased over the main area of the control gate of a floating gate (stacked double gate) semiconductor NVM cell to reduce the control gate to floating gate total capacitance C_cgAnd then to C_S+C_sub+C_D>>C_cg. Figure 9a shows a top view of a conventional floating gate NOR type flash memory array. FIG. 9b shows a cross-sectional view of the control gate along a word line AA' in FIG. 9 a. In a conventional floating gate NVM process, a first dielectric film is deposited over the floating gate 960 to form a coupling dielectric layer before depositing a second polysilicon film (poly-silicon film). In this embodiment, the first dielectric film of the dotted inner region of the highlight tone mask (clear tone mask) is removed as shown in fig. 9 a. Thereafter, an oxide layer is grown or deposited to a thickness rangeOn the removed region of the first dielectric film to form a thin tunnel oxide layer of tunnel oxide region 910. When a high positive voltage is applied to a row (row) of control gates and the common source 920, bit line(s) 940 and substrate are connected to ground (0V), tunneling erase occurs in the thin tunnel oxide 910 between the floating gate 960 and the control gate 930.

Although the embodiments and examples described above illustrate the charge storage material as a floating gate, it should be understood that the invention is not limited thereto, and the invention can be applied to any type of charge storage material, such as: charge trapping dielectric films and nanocrystals.

The preferred embodiments provided above are merely illustrative of the present invention and are not intended to limit the invention to a specific type or exemplary embodiment. The description is thus to be regarded as illustrative instead of limiting. Obviously, various modifications and alterations will become apparent to those skilled in the art. The foregoing description of the preferred embodiments is provided to best explain the principles of the invention and its best mode for practical application, to thereby enable others skilled in the art to understand the invention for various embodiments and with the various modifications as are suited to the particular use or use contemplated. The scope of the invention is defined by the claims and their equivalents, in which all names (term) are meant in their broadest reasonable sense unless otherwise specifically indicated. Thus, the terms "present invention" and the like do not limit the scope of the claimed subject matter to a particular embodiment, and any reference to a particular preferred embodiment of the invention is not intended to limit the invention, and no such limitation is to be inferred. The invention is to be defined only by the scope and spirit of the appended claims. The abstract of the invention is provided in accordance with the statutory requirements so that a searcher can quickly ascertain the subject matter of the technical disclosure (subject matter) from any patent approved by the specification, and is not intended to interpret or limit the scope or meaning of the claims. Any advantages and benefits may not apply to all embodiments of the invention. It should be understood that various changes and modifications can be made by one skilled in the art without departing from the scope of the invention as defined by the appended claims. Further, all elements and components (components) in the present specification are not intended to be popular regardless of whether they are listed in the claims.