Method of forming ono stacked films and DCS tungsten silicide gate to improve polycide gate performance for flash memory devices

Information

  • Patent Grant
  • 6380029
  • Patent Number
    6,380,029
  • Date Filed
    Friday, December 4, 1998
    25 years ago
  • Date Issued
    Tuesday, April 30, 2002
    22 years ago
Abstract
In one embodiment, the present invention relates to a method of forming a flash memory cell, involving the steps of forming a tunnel oxide on a substrate; forming a first polysilicon layer over the tunnel oxide; forming an insulating layer over the first polysilicon layer, the insulating layer comprising a first oxide layer over the first polysilicon layer, a nitride layer over the first oxide layer, and a second oxide layer over the nitride layer; forming a second polysilicon layer over the insulating layer; forming a tungsten silicide layer over the second polysilicon layer by chemical vapor deposition using WF6 and SiH2Cl2; etching at least the first polysilicon layer, the second polysilicon layer, the insulating layer, and the tungsten silicide layer thereby defining at least one stacked gate structure; and forming a source region and a drain region in the substrate, thereby forming at least one memory cell.
Description




TECHNICAL FIELD




The present invention generally relates to flash memory devices such as EEPROMs. More particularly, the present invention relates to flash memory devices exhibiting increased charge coupling ratio, reduced thickness of the multilayer insulator and increased gate oxide reliability.




BACKGROUND ART




Nonvolatile memory devices include flash EEPROMs (electrical erasable programmable read only memory devices).

FIG. 1

represents the relevant portion of a typical flash memory cell


10


. The memory cell


10


typically includes a source region


12


, a drain region


14


and a channel region


16


in a substrate


18


; and a stacked gate structure


20


overlying the channel region


16


. The stacked gate


20


includes a thin gate dielectric layer


22


(commonly referred to as the tunnel oxide) formed on the surface of the substrate


18


. The stacked gate


20


also includes a polysilicon floating gate


24


which overlies the tunnel oxide


22


and an interpoly dielectric layer


26


which overlies the floating gate


24


. The interpoly dielectric layer


26


is often a multilayer insulator such as an oxide-nitride-oxide (ONO) layer having two oxide layers


26




a


and


26




b


sandwiching a nitride layer


26




c.


A polysilicon control gate


28


overlies the interpoly dielectric layer


26


and a conductive layer


30


, such as a tungsten silicide layer, overlies the polysilicon control gate


28


. The conductive layer


30


may constitute, in part, a word line. The channel region


16


of the memory cell


10


conducts current between the source region


12


and the drain region


14


in accordance with an electric field developed in the channel region


16


by the stacked gate structure


20


.




Generally speaking, a flash memory cell is programmed by inducing hot electron injection from a portion of the substrate, such as the channel section near the drain region, to the floating gate. Electron injection carries negative charge into the floating gate. The injection mechanism can be induced by grounding the source region and a bulk portion of the substrate and applying a relatively high positive voltage to the control electrode to create an electron attracting field and applying a positive voltage of moderate magnitude to the drain region in order to generate “hot” (high energy) electrons. After sufficient negative charge accumulates on the floating gate, the negative potential of the floating gate raises the threshold voltage (V


th


) of its field effect transistor (FET) and inhibits current flow through the channel region through a subsequent “read” mode. The magnitude of the read current is used to determine whether or not a flash memory cell is programmed. The act of discharging the floating gate of a flash memory cell is called the erase function. The erase function is typically carried out by a Fowler-Nordheim tunneling mechanism between the floating gate and the source region of the transistor (source erase or negative gate erase) or between the floating gate and the substrate (channel erase). A source erase operation is induced by applying a high positive voltage to the source region and a 0 V to the control gate and the substrate while floating the drain of the respective memory cell.




Referring still to

FIG. 1

, conventional source erase operations for the flash memory cell


10


operate in the following manner. The memory cell


10


is programmed by applying a relatively high voltage V


G


(e.g., approximately 12 volts) to the control gate


28


and a moderately high voltage V


D


(e.g., approximately 9 volts) to the drain region


14


in order to produce “hot” electrons in the channel region


16


near the drain region


14


. The hot electrons accelerate across the tunnel oxide


22


and into the floating gate


24


and become trapped in the floating gate


24


since the floating gate


24


is surrounded by insulators (the interpoly dielectric


26


and the tunnel oxide


22


). As a result of the trapped electrons, the threshold voltage of the memory cell


10


increases by about 3 to 5 volts. This change in the threshold voltage (and thereby the channel conductance) of the memory cell


10


created by the trapped electrons causes the cell to be programmed.




To read the flash memory cell


10


, a predetermined voltage V


G


that is greater than the threshold voltage of an unprogrammed cell, but less than the threshold voltage of a programmed cell, is applied to the control gate


28


. If the memory cell


10


conducts, then the memory cell


10


has not been programmed (the cell


10


is therefore at a first logic state, e.g., a zero “0”). Likewise, if the memory cell


10


does not conduct, then the memory cell


10


has been programmed (the cell


10


is therefore at a second logic state, e.g., a one “1”). Consequently, it is possible to read each cell


10


to determine whether or not it has been programmed (and therefore identify its logic state).




In order to erase the flash memory cell


10


, a relatively high voltage V


S


(e.g., approximately 12 volts) is applied to the source region


12


and the control gate


28


is held at a ground potential (V


G


=0), while the drain region


14


is allowed to float. Under these conditions, a strong electric field is developed across the tunnel oxide


22


between the floating gate


24


and the source region


12


. The electrons that are trapped in the floating gate


24


flow toward and cluster at the portion of the floating gate


24


overlying the source region


22


and are extracted from the floating gate


24


and into the source region


12


by way of Fowler-Nordheim tunneling through the tunnel oxide


22


. Consequently, as the electrons are removed from the floating gate


24


, the memory cell


10


is erased.




The ONO interpoly dielectric layer has a number of important functions including insulating the control gate from the floating gate. Accordingly, it is desirable to form a high quality, relatively thin ONO interpoly dielectric layer. When forming an ONO interpoly dielectric layer, there are a number of concerns. For example, if the top oxide layer is too thick, the required programming voltage increases undesirably. Precisely controlling the thickness of the top oxide layer is a notable concern.




When forming a conductive layer made of tungsten silicide over the polysilicon control gate, tungsten hexafluoride is typically employed. The fluorine content of a tungsten silicide layer made in a conventional manner is typically above about 2×10


20


atoms/cm


3


. However, when forming tungsten silicide from tungsten hexafluoride, fluorine undesirably diffuses into the top oxide of the ONO interpoly dielectric layer. The undesirable fluorine diffusion causes the top oxide to swell, often by at least about 10%, and even by at least about 20% in thickness. As stated above, an increase in the top oxide thickness requires an undesirable increase in the required programming voltage thus lowering the coupling ratio.




In this connection, there are a number of concerns when forming the conductive layer over the polysilicon control gate. For example, the conductive layer should adequately adhere to the polysilicon control gate. The inability of the conductive layer to adequately adhere to the polysilicon control gate is typically due to delamination of the conductive layer. The conductive layer should also effectively conduct an electrical current. However, current methods of forming a tungsten silicide conductive layer over the polysilicon control gate of a flash memory device result in deleterious microcracking within the tungsten silicide. This is sometimes due to poor step coverage when forming a tungsten silicide conductive layer. Microcracking leads often to undesirably increased word line resistance and poor polysilicon control gate performance.




In view of the aforementioned concerns and problems, there is a need for flash memory cells of improved quality and more efficient methods of making such memory cells.




SUMMARY OF THE INVENTION




As a result of the present invention, a flash memory cell having improved reliability is obtainable by providing an improved ONO interlayer dielectric layer and an improved tungsten silicide conductive layer. By forming a tungsten silicide conductive layer in accordance with the present invention, swelling of the top oxide of the ONO interlayer dielectric layer is minimized and/or eliminated. The present invention also makes it possible to control more precisely the thickness of the top oxide layer. Moreover, by forming a tungsten silicide conductive layer in accordance with the present invention, the occurrence of microcracking in the tungsten silicide conductive layer is minimized and/or eliminated thus improving the electrical properties of the tungsten silicide conductive layer.




In one embodiment, the present invention relates to a method of forming a flash memory cell, involving the steps of forming a tunnel oxide on a substrate; forming a first polysilicon layer over the tunnel oxide; forming an insulating layer over the first polysilicon layer, the insulating layer comprising a first oxide layer over the first polysilicon layer, a nitride layer over the first oxide layer, and a second oxide layer over the nitride layer; forming a second polysilicon layer over the insulating layer; forming a tungsten silicide layer over the second polysilicon layer by chemical vapor deposition using WF


6


and SiH


2


Cl


2


; etching at least the first polysilicon layer, the second polysilicon layer, the insulating layer, and the tungsten silicide layer thereby defining at least one stacked gate structure; and forming a source region and a drain region in the substrate, thereby forming at least one memory cell.




In another embodiment, the present invention relates to a method of forming a tungsten silicide layer for a flash memory cell without substantially increasing multilayer dielectric thickness, involving depositing the tungsten silicide layer over the multilayer dielectric by chemical vapor deposition using WF


6


and SiH


2


Cl


2


at a temperature from about 450° C. to about 650° C. under a pressure from about 70 Pa to about 120 Pa to a thickness from about 1,000 Å to about 1,800 Å.




In yet another embodiment, the present invention relates to a method of decreasing fluorine diffusion from a tungsten silicide layer to an ONO multilayer dielectric in a flash memory cell comprising a substrate, a tunnel oxide over the substrate, a floating gate over the tunnel oxide, an ONO multilayer dielectric over the floating gate, a control gate over the ONO insulating layer, and the tungsten silicide layer over the control gate, involving the steps of depositing the tungsten silicide layer over the control gate by chemical vapor deposition using WF


6


and SiH


2


Cl


2


at a temperature from about 450° C. to about 650° C. under a pressure from about 70 Pa to about 120 Pa; and annealing the chemical vapor deposited tungsten silicide layer, wherein the tungsten silicide layer comprises less than about 1×10


18


atoms/cm


3


of fluorine.











BRIEF DESCRIPTION OF DRAWINGS





FIG. 1

is a cross-sectional view of relevant portions of a conventional memory cell in a flash memory cell.





FIGS. 2A

to


2


H are cross-sectional views illustrating a flash memory cell fabrication method according to one embodiment of the present invention.











DISCLOSURE OF INVENTION




By forming a tungsten silicide layer having a lower stress value and thus less microcracks, the reliability of the interpoly dielectric layer can be increased in flash memory cells. While not wishing to be bound to any theory, it is believed that by forming a tungsten silicide layer according to the present invention, it is consequently possible to prevent the occurrence of microcracks due to good step coverage of the tungsten silicide layer and minimize fluorine diffusion to the multilayer dielectric layer. By minimizing fluorine diffusion to the multilayer dielectric layer, the ONO dielectric thickness is reduced (compared with forming a silane based tungsten silicide layer) thus improving the coupling ratio. By preventing microcracks in the tungsten silicide layer, word line resistance is decreased thus improving the performance of resultant flash memory devices.




According to the present invention, the tungsten silicide layer of a flash memory cell, typically formed over a second polysilicon layer (control gate), is formed using dichlorosilane. The flash memory cells according to the invention contain a silicon substrate, a tunnel oxide layer over the silicon substrate, a first polysilicon layer (floating gate) over the tunnel oxide layer, an ONO dielectric layer (an oxide/nitride/oxide multilayer dielectric layer) over the first polysilicon layer, a second polysilicon layer (control gate) and the tungsten silicide layer as described herein. The process conditions involve forming the tungsten silicide layer using a dichlorosilane process in a manner to minimize fluorine diffusion and microcracking optionally followed by an annealing step.




Depositing the tungsten silicide is conducted at a temperature from about 450° C. to about 650° C. and a pressure from about 70 Pa to about 120 Pa. In a preferred embodiment, the temperature is from about 500° C. to about 600° C. and the pressure is from about 80 Pa to about 110 Pa. The gas flow includes SiH


2


Cl


2


and WF


6


. In one embodiment, the gas flow does not contain silane. Although not required, the gas flow may optionally include an inert or carrier gas such as a noble gas or nitrogen. Nobles gases include He, Ne, Ar, Kr, and Xe.




The gas flow generally contains a sufficient amount of SiH


2


Cl


2


and WF


6


to form a tungsten silicide layer (a WSi


2


layer). During formation of the tungsten silicide layer, it is believed that the following chemical reaction takes place.






10SiH


2


Cl


2


+2WF


6


→2WSi


2


+3SiF


4


+3SiCl


4


+8HCl+6H


2








In one embodiment, the gas flow contains from about 50 standard cubic centimeters per minute (sccm) to about 250 sccm SiH


2


Cl


2


and from about 2 sccm to about 10 sccm WF


6


. In another embodiment, the gas flow contains from about 100 sccm to about 200 sccm SiH


2


Cl


2


and from about 3 sccm to about 9 sccm WF


6


. In embodiments where an inert gas is employed, the gas flow further contains from about 100 sccm to about 250 sccm of an inert gas. In other embodiments where an inert gas is employed, the gas flow further contains from about 150 sccm to about 200 sccm of an inert gas, such as Ar.




Depositing the tungsten silicide is conducted for a time sufficient to form a tungsten silicide layer of desired thickness. The thickness of the tungsten silicide layer is sufficient to provide a resultant tungsten silicide layer having a thickness from about 1,000 Å to about 1,800 Å, after optional anneal if performed. In one embodiment, the resultant tungsten silicide layer has a thickness from about 1,100 Å to about 1,700 Å. In another embodiment, the resultant tungsten silicide layer has a thickness from about 1,200 Å to about 1,600 Å.




The tungsten silicide deposition according to the present invention forms a tungsten silicide layer having a low or no occurrence of microcracking. As a result, the tungsten silicide layer made in accordance with the present invention has low resistance compared to tungsten silicide layers made using silane.




The tungsten silicide deposition according to the present invention prevents or minimizes fluorine diffusion (emanating from the tungsten hexafluoride) into the ONO If multilayer dielectric, and particularly into the top oxide layer of the ONO multilayer dielectric, compared to tungsten silicide layers made using silane. Although not wishing to be bound by any theory, it is believed that fluorine diffusion causes an undesirable increase in ONO multilayer dielectric thickness. Thus, the tungsten silicide deposition according to the present invention also minimizes the thickness of the ONO multilayer dielectric. In one embodiment, compared to the thickness of an ONO multilayer dielectric over which a tungsten silicide deposition technique using silane is performed, the thickness of the ONO multilayer dielectric over which a tungsten silicide deposition according to the present invention is performed is at least about 8 Å less. In another embodiment, compared to the thickness of an ONO multilayer dielectric over which a tungsten silicide deposition technique using silane is performed, the thickness of the ONO multilayer dielectric over which a tungsten silicide deposition according to the present invention is performed is at least about 10 Å less. In other words, the thickness of the ONO multilayer dielectric over which a tungsten silicide deposition according to the present invention is performed does not increase or does not substantially increase (less than about 2 Å in a 40 Å thick multilayer dielectric) due to fluorine diffusion.




The fluorine content of the tungsten silicide layer made in accordance with the present invention is relatively low compared with the fluorine content of conventionally made tungsten silicide layers, such as those made using silane. In one embodiment, the fluorine content of the tungsten silicide layer made in accordance with the present invention is below about 1×10


18


atoms/cm


3


. In another embodiment, the fluorine content of the tungsten silicide layer made in accordance with the present invention is below about 1×10


17


atoms/cm


3


. In yet another embodiment, the fluorine content of the tungsten silicide layer made in accordance with the present invention is below about 1×10


16


atoms/cm


3


.




After the tungsten silicide deposition, an optional anneal step is performed. Although not required, annealing the tungsten silicide layer can, in some instances, further contribute to the ability of the tungsten silicide layer to resist microcracking and minimize fluorine diffusion. In a preferred embodiment, a rapid thermal anneal (RTA) is performed. Annealing of the tungsten silicide layer is preferably conducted in an ambient atmosphere, such as a nitrogen (N


2


) atmosphere. In one embodiment, annealing is conducted at a temperature from about 850° C. to about 950° C. In a preferred embodiment, annealing is conducted at a temperature from about 875° C. to about 925° C.




In one embodiment, annealing is conducted for a time from about 10 seconds to about 30 seconds. In a preferred embodiment, annealing is conducted for a time from about 15 seconds to about 25 seconds. The annealing primarily serves to further decrease the occurrence of microcracking in the tungsten silicide layer.




Flash memory cells made in accordance with the present invention (containing a dichlorosilane based tungsten silicide film) are characterized by a high charge to breakdown (Qbd) compared to flash memory cells made with a silane based tungsten silicide film. To measure Qbd of a dielectric layer, a current is forced through a specified path until the dielectric layer is rendered conductive. A high Qbd is desirable. For example, Qbd for an oxide layer having a thickness of about 85 Å under a dichlorosilane based tungsten silicide film having a thickness of about 1,200 Å (made in accordance with the present invention) and over a doped amorphous polysilicon layer having a thickness of about 1,200 Å (mimicking a control gate) is about 7.5 C/cm


2


compared to a Qbd of 3.5 C/cm


2


for an oxide layer having a thickness of about 85 Å under a silane (monosilane, SiH


4


) based tungsten silicide film having a thickness of about 1,500 Å (not made in accordance with the present invention) and over a doped amorphous polysilicon layer having a thickness of about 1,200 Å (mimicking a control gate). In another example, Qbd for an oxide layer having a thickness of about 150 Å under a dichlorosilane based tungsten silicide film having a thickness of about 1,200 Å (made in accordance with the present invention) and over a doped amorphous polysilicon layer having a thickness of about 1,200 Å is about 20 C/cm


2


compared to a Qbd of 10 C/cm


2


for an oxide layer having a thickness of about 150 Å under a silane based tungsten silicide film having a thickness of about 1,500 Å (not made in accordance with the present invention) and over a doped amorphous polysilicon layer having a thickness of about 1,200 Å.




Moreover, flash memory cells made in accordance with the present invention (containing a dichlorosilane based tungsten silicide film) have high current densities, especially when compared with flash memory cells made with a silane based tungsten silicide film. Since less charge trapping is associated with high current densities, flash memory cells made in accordance with the present invention have less charge trapping compared with flash memory cells made with a silane based tungsten silicide film.




Referring to

FIGS. 2A

to


2


H, the fabrication of a single flash memory cell is described. A plurality of flash memory cells can be formed on a semiconductor substrate, such as a silicon die, each with an N-type source region and N-type drain region formed within a P portion of the substrate and a P-type channel region interposed between the source and drain regions in accordance with the present invention. Although fabrication of one flash memory cell is described below, it will be understood by those skilled in the art that the methods described herein are applicable to mass production methods wherein two or more cells are formed.




Specifically referring to

FIG. 2A

, a P-type substrate


40


is provided. Thereafter, a thin tunnel oxide layer


42


is formed over the substrate


40


having a thickness of, for example, about 50 Å to about 150 Å using a thermal growth process in a dry oxidation furnace. For instance, the tunnel oxide layer


42


can be formed via dry oxidation at a temperature of about 1050° C., under an atmosphere of oxygen at about 1.33 l, HCl at about 70 cc and argon at about 12.6l. Alternatively, the tunnel oxide can be formed from oxynitride.




Referring to

FIG. 2B

, a first polysilicon layer


44


is formed in any suitable manner over the tunnel oxide layer


42


. For example, a phosphorus doped polysilicon layer is deposited via CVD to form a doped polysilicon layer


44


at 530° C., 400 mTorr, SiH


4


at 2000 sccm, and a mixture of 1% by weight PH


3


in helium at about 22 sccm. Doping lowers the resistivity of the polysilicon rendering it conductive.




A multi-layer interpoly dielectric


46


is then formed in any suitable manner over the surface of the substrate


40


, as illustrated in FIG.


2


C. This layer


46


is often called the interpoly dielectric since (as will be seen shortly) it is sandwiched between the phosphorus doped polysilicon layer (first polysilicon layer constituting the floating gate for a flash memory cell) and a second polysilicon layer which forms the control gate for the cell. The interpoly dielectric


46


is preferably a three layer region of oxide/nitride/oxide (the so called “ONO” layer) and typically has a total thickness of about 120 Å to about 400 Å. Generally speaking, the ONO layer


46


is formed by repetitive depositions of oxide, nitride and oxide to form a dielectric layer in which the nitride is sandwiched between a bottom oxide layer and top oxide layer.




Specifically referring to

FIG. 2C

, a first or bottom oxide layer


46




a


is deposited using CVD techniques. For example, a bottom oxide layer


46




a


is deposited at a temperature of about 750° C. under SiH


4


at 20 sccm, N


2


O at 1.2 l, and a carrier gas and a pressure of 600 mTorr via LPCVD oxide on the first polysilicon layer. The bottom oxide layer may have a suitable thickness, for example, from about 40 Å to about 60 Å, but typically the thickness is about 50 Å. A nitride layer


46




b


is next deposited also using CVD techniques. For example, nitride is deposited at a temperature of about 760° C. under NH


3


at 600 sccm, SiH


2


Cl


2


at 100 sccm and a pressure of 330 mTorr to form a nitride layer


46




b.


The nitride layer


46




b


may have a suitable thickness, for example, from about 60 Å to about 100 Å, preferably from about 70 Å to about 90 Å, but typically the thickness is about 80 Å.




The second or top oxide layer


46




c


is formed in a similar manner as the first oxide layer or by wet oxidation at about 950° C. for about 40 minutes using oxygen (about 5 l) and hydrogen (about 9 l) to provide an oxide layer. The top oxide layer may have a thickness from about 20 Å to about 80 Å, but in this embodiment the thickness is about 40 Å.




Referring to

FIG. 2D

, a second polysilicon layer is deposited in any suitable manner. Specifically, a phosphorus doped amorphous polysilicon layer is deposited via CVD to form a doped polysilicon layer


48


at about 530° C., 400 mTorr, SiH


4


at 2,000 sccm, and a mixture of 1% by weight PH


3


in helium at about 75 sccm. Alternatively, the second polysilicon layer can be deposited by LPCVD followed by ion implantation of a dopant such as phosphorus. Doping lowers the resistivity of the polysilicon rendering it conductive.




Referring to

FIG. 2E

, a tungsten silicide layer


50


is deposited via CVD. The tungsten silicide layer


50


provides a lower resistance contact for improved flash memory cell performance. Specifically, the tungsten silicide is deposited at a temperature of about 565° C. and a pressure of about 93 Pa. The gas flow includes SiH


2


Cl


2


and WF


6


. The gas flow contains about 150 sccm SiH


2


Cl


2


and about 5 sccm WF


6


. The gas flow may further contain about 150 sccm to about 200 sccm of an inert gas, such as Ar. The thickness of the tungsten silicide layer is about 1,400 Å. After the tungsten silicide deposition, an optional RTA is performed in a nitrogen atmosphere. RTA is conducted at about 900° C. for about 20 seconds.




The tungsten silicide deposition according to the present invention forms a tungsten silicide layer having no detectable microcracking. As a result, the tungsten silicide layer made in accordance with the present invention has low resistance compared to tungsten silicide layers made using silane.




The tungsten silicide deposition according to the present invention prevents or minimizes fluorine diffusion into the ONO multilayer dielectric, and particularly into the top oxide layer of the ONO multilayer dielectric, compared to tungsten silicide layers made using silane. Compared to the thickness of an ONO multilayer dielectric over which a tungsten silicide deposition technique using silane is performed wherein the thickness may increase as much as about 8 Å to about 10 Å, the thickness of the ONO multilayer dielectric over which a tungsten silicide deposition according to the present invention is performed does not increase.




The remaining steps are generally well known in the art and may be varied. For instance, poly-cap layer


52


is deposited over the tungsten silicide layer


50


. The poly-cap layer


52


is about 500 Å thick, and is formed via, for example, LPCVD. The poly-cap layer


52


can be used to prevent any potential peeling or cracking of the underlying tungsten silicide


50


. A capping layer


54


, for example, of SiON is deposited over the poly-cap layer


52


. The capping silicon oxynitride layer


54


provides an anti-reflective coating at masking and also acts as a masking layer for subsequent etching.




Referring to

FIGS. 2F

, suitable lithography and etching procedures are used to remove various portions of the device. After the second polysilicon layer


48


, the tungsten silicide layer


50


, the poly-cap layer


52


and the capping layer


54


have been formed (a plurality of word lines for the memory cells can be defined in this manner) etching is performed to define one or more pre-stack structures. The etching may be achieved by depositing and defining a photoresist masking layer over the entire surface of the substrate using standard lithography procedures. This is generally termed the gate mask and gate etch. Subsequently, a number of successive etching steps, such as the gate etch and the self aligned etch, are performed to define one or more stack structures


56


. This is generally termed the self aligned mask and self aligned etch.




The gate mask and gate etch are performed as follows. First, a resist (not shown) is applied, selectively exposed to radiation and developed whereby various portions removed (either the exposed or unexposed portions). Next, in one embodiment, the etching steps take place in a multi-chamber etch tool wherein a silicon oxynitride capping layer is selectively etched with a fluorinated chemistry such as CHF


3


—O


2


in an oxide chamber. The exposed poly-cap layer and the tungsten silicide layer are then etched with SF


6


/HBr (or alternatively, SF


6


/Cl


2


or Cl


2


—O


2


) and the exposed second polysilicon layer is etched with HBr—O


2


in a poly chamber. Etching steps are preferably formed in an integrated process in which the wafers are not exposed to atmosphere when transferring the wafers from one chamber to another.




Once the second polysilicon layer


48


, the tungsten silicide layer


50


, the poly-cap layer


52


and the capping layer


54


have been removed, a self aligned etch (“SAE”) is performed to remove the ONO layer


46


and the phosphorus doped polysilicon layer (first polysilicon layer)


44


in the regions that are not covered by the pre-stack structure (constituted by the unremoved second polysilicon layer, tungsten silicide layer, poly-cap layer and capping layer). The SAE etch is a two step etch process in which the ONO layer


46


is first removed using, for example, a CF


4


—O


2


RIE etch. The second phase of the SAE etch is the removal of the exposed first polysilicon layer


44


to thereby further define the floating gate structures for each respective word line. The polysilicon etch includes, for example, an HBr—O


2


or a HBr—Cl


2


—O


2


RIE etch chemistry. The gate etch and SAE serve to define the stack structure


56


.




The fabrication of the flash memory cells is then completed by forming the source and drain regions by, for example, ion implantation. During the formation of the source and drain regions, the stacked gate structure


56


serves as a self-aligning mechanism. Specifically referring to

FIG. 2G

, resist


62


is applied and selectively stripped followed by performing a first ion implantation using phosphorus (1×10


14


ions/cm


2


at 60 KeV) to form an N-type source region


64


(double diffused implant). Referring to

FIG. 2H

, resist


62


is removed followed by performing a second ion implantation using arsenic (5×10


14


ions/cm


2


at 40 KeV) to form deep N-type source region


66


, shallow N-type source region


68


and N-type drain region


70


(modified drain diffusion). Annealing completes the formation of the source and drain regions. In the above manner, an easy method for forming flash memory cells is provided. Although a flash memory cell with a double-diffused source region is described, the present invention is also applicable to flash memory cells with a single-diffused source region.




During programming, the source regions


66


and


68


and the substrate


40


of the memory cell may be tied to a ground via a terminal (not shown), respectively, the drain region


70


is coupled to a relatively high voltage (for example, between about +5 V to about +9 V) via a terminal (not shown) and the control gate


48


is connected to a relatively high voltage level (for example, above about +10 V) via a terminal (not shown). Electrons are accelerated from the source regions


66


and


68


to the drain region


70


and so-called “hot-electrons” are generated near the drain region


70


. Some of the hot electrons are injected through the relatively thin tunnel oxide layer


42


and become trapped in the floating gate


44


thereby providing the floating gate


44


with a negative potential.




During erasure, a high positive voltage (such as above about +12 V) is applied to the source regions


66


and


68


via a source terminal (not shown). A ground potential (V


g


equals 0 V) is applied to the control gate


48


via the control terminal (not shown). A similar ground potential (V


sub


equals 0 V) is applied to the substrate


40


via a substrate terminal (not shown). The voltage V


D


of the drain region


70


is permitted to float. In this mode, electrons previously stored during programming in the floating gate


44


pass through tunnel oxide layer


42


by way of Fowler-Nordheim tunneling and travel into the source regions


66


and


68


as a result of the electric field established between the control gate


48


and the source regions


66


and


68


(V


GS


equals about 12 V). Since the top oxide layer is characterized by reduced charge trapping, Fowler-Nordheim tunneling and travel of electrons from the floating gate


44


to the source regions


66


and


68


are facilitated.




Although the invention has been shown and described with respect to a certain preferred embodiment or embodiments, it is obvious that equivalent alterations and modifications will occur to others skilled in the art upon the reading and understanding of this specification and the annexed drawings. In particular regard to the various functions performed by the above described components (assemblies, devices, circuits, etc.), the terms (including a reference to a “means”) used to describe such components are intended to correspond, unless otherwise indicated, to any component which performs the specified function of the described component (i.e., that is functionally equivalent), even though not structurally equivalent to the disclosed structure which performs the function in the herein illustrated exemplary embodiments of the invention. In addition, while a particular feature of the invention may have been disclosed with respect to only one of several embodiments, such feature may be combined with one or more other features of the other embodiments as may be desired and advantageous for any given or particular application.



Claims
  • 1. A method of forming a flash memory cell, comprising:forming a tunnel oxide on a substrate; forming a first polysilicon layer over the tunnel oxide; forming an insulating layer over the first polysilicon layer, the insulating layer comprising a first oxide layer over the first polysilicon layer, a nitride layer over the first oxide layer, and a second oxide layer over the nitride layer; forming a second polysilicon layer over the insulating layer; forming a tungsten silicide layer over the second polysilicon layer by chemical vapor deposition using WF6 and SiH2Cl2; etching at least the first polysilicon layer, the second polysilicon layer, the insulating layer, and the tungsten silicide layer thereby defining at least one stacked gate structure; and forming a source region and a drain region in the substrate, thereby forming at least one memory cell.
  • 2. The method of claim 1, wherein the tungsten silicide layer comprises less than about 1×1018 atoms/cm3 of fluorine.
  • 3. The method of claim 1, wherein the chemical vapor deposition of the tungsten silicide layer is conducted under a pressure from about 70 Pa to about 120 Pa.
  • 4. The method of claim 1, wherein the chemical vapor deposition of the tungsten silicide layer is conducted at a temperature from about 450° C. to about 650° C.
  • 5. The method of claim 1, further comprising annealing the tungsten silicide layer before etching.
  • 6. The method of claim 1, wherein the chemical vapor deposition of the tungsten silicide layer is conducted using a gas flow comprising from about 2 sccm to about 10 sccm of WF6 and from about 50 sccm to about 250 sccm SiH2Cl2.
  • 7. The method of claim 1, wherein the insulating layer has a first thickness after formation and a second thickness after the tungsten silicide layer formation, and the second thickness is substantially the same as the first thickness.
  • 8. A method of forming a tungsten silicide layer for a flash memory cell without substantially increasing multilayer dielectric thickness, comprising:depositing the tungsten silicide layer over the multilayer dielectric by chemical vapor deposition using WF6 and SiH2Cl2 at a temperature from about 450° C. to about 650° C. under a pressure from about 70 Pa to about 120 Pa to a thickness from about 1,000 Å to about 1,800 Å.
  • 9. The method of claim 8, wherein a polysilicon layer is positioned over the multilayer dielectric, and the tungsten silicide layer is deposited on the polysilicon layer.
  • 10. The method of claim 8, wherein the chemical vapor deposition is conducted using a gas flow comprising from about 2 sccm to about 10 sccm of WF6, from about 50 sccm to about 250 sccm SiH2Cl2 and from about 100 sccm to about 250 sccm of an inert gas.
  • 11. The method of claim 10, wherein the inert gas comprises at least one of N2, He, Ne, Ar, Kr, and Xe.
  • 12. The method of claim 8, wherein the chemical vapor deposition using WF6 and SiH2Cl2 is conducted at a temperature from about 500° C. to about 600° C. and a pressure from about 80 Pa to about 110 Pa.
  • 13. The method of claim 8, further comprising annealing the chemical vapor deposited tungsten silicide layer at a temperature from about 875° C. to about 925° C.
  • 14. A method of decreasing fluorine diffusion from a tungsten silicide layer to an ONO multilayer dielectric in a flash memory cell comprising a substrate, a tunnel oxide over the substrate, a floating gate over the tunnel oxide, an ONO multilayer dielectric over the floating gate, a control gate over the ONO insulating layer, and the tungsten silicide layer over the control gate, comprising:depositing the tungsten silicide layer over the control gate by chemical vapor deposition using WF6 and SiH2Cl2 at a temperature from about 450° C. to about 650° C. under a pressure from about 70 Pa to about 120 Pa; and annealing the chemical vapor deposited tungsten silicide layer, wherein the tungsten silicide layer comprises less than about 1×1018 atoms/cm3 of fluorine.
  • 15. The method of claim 14, wherein the tungsten silicide layer comprises less than about 1×1017 atoms/cm3 of fluorine.
  • 16. The method of claim 14, wherein the chemical vapor deposition is conducted using a gas flow comprising from about 3 sccm to about 9 sccm of WF6 and from about 100 sccm to about 200 sccm SiH2Cl2.
  • 17. The method of claim 14, wherein the chemical vapor deposition is conducted using a gas flow comprising from about 2 sccm to about 10 sccm of WF6, from about 50 sccm to about 250 sccm SiH2Cl2 and from about 100 sccm to about 250 sccm of an inert gas.
  • 18. The method of claim 14, wherein the inert gas comprises Ar.
  • 19. The method of claim 14, wherein the chemical vapor deposition using WF6 and SiH2Cl2 is conducted at a temperature from about 500° C. to about 600° C. and a pressure from about 80 Pa to about 110 Pa.
  • 20. The method of claim 14, wherein the tungsten silicide layer has a thickness from about 1,100 Å to about 1,700 Å.
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