The present invention relates to nonvolatile memories, and more particularly to memories with charge trapping regions containing silicon nitride.
Tunnel dielectric 150 is formed between charge trapping region 130 and substrate 122 to reduce charge leakage from the charge trapping region to the substrate. Blocking dielectric 170 is formed between charge trapping region 130 and gate 140 to reduce charge leakage from the charge trapping region to the gate. Charge trapping region 130 can be formed of silicon nitride (Si3N4). Dielectric layer 150 can be silicon dioxide, and dielectric 170 can be silicon dioxide or aluminum oxide. See e.g. U.S. patent application published as no. 2006/0261401 A1 on Nov. 23, 2006, filed by A. Bhattacharyya on May 17, 2005, incorporated herein by reference.
When gate 140 is at a positive voltage relative to channel 110 or a source/drain region 124, some electrons in channel 110 or source/drain region 124 gain enough energy to tunnel through dielectric 150 into charge trapping region 130. The electrons become trapped in the charge trapping region, increasing the threshold voltage of the memory cell. The threshold voltage can be sensed by sensing the current between source/drain regions 124 when suitable voltages are applied to control gate 140, substrate 122, and source/drain regions 124. When a negative voltage is applied to gate 140 relative to channel 110 or a source/drain region or regions 124, the cell's threshold voltage returns to its original state.
Charge trapping region 130 can be provided with silicon, germanium, or metal nanocrystals 180. Each nanocrystal contains a few hundred atoms. The nanocrystals serve as additional trapping sites for electron trapping. Higher trapping site density is therefore achieved to provide a more reliable threshold voltage differentiation and to counteract leakage of trapped charges from the charge trapping layer.
Germanium enhancement of silicon nitride is also described in an article by Chun-Hao Tu et al. entitled “Formation of silicon germanium nitride layer with distributed charge storage elements, published in Applied Physics Letters, vol. 88, issue 11, March 2006. See
Alternative techniques for increasing the charge trapping density are desirable.
This section summarizes some features of the invention. Other features are described in the subsequent sections. The invention is defined by the appended claims, which are incorporated into this section by reference.
Providing uniform, dense, reproducible distribution of nanocrystals 180 (
Some embodiments of the present invention increase the charge trapping density by doping silicon nitride with germanium and/or phosphorus without requiring nanocrystal formation. In the germanium case, the germanium concentration can be less than 10% (atomic) relative to silicon. Alternatively, or in addition, chlorine can be used to form Ge—Cl bonds in the charge trapping layer. These bonds are typically more stable than Ge—H bonds (perhaps because chlorine atoms are heavier than hydrogen).
The invention is not limited to the features or advantages described above. Other features are described below. The invention is defined by the appended claims.
The embodiments described in this section illustrate but do not limit the invention. The invention is defined by the appended claims.
Charge trapping layer 130 is formed of silicon nitride SixNy doped with germanium or phosphorus atoms 210. At least 95% percent of these atoms do not form crystals with each other, and in fact may have no bonds with each other. Germanium or phosphorus atoms may bind with silicon or nitrogen. We will call this material SixDzNy where D is germanium (Ge) or phosphorus (P). In some embodiments, the ratio (x+z):y is greater than 3:4. In some embodiments, the D atoms that do not form crystals with each other are uniformly distributed through the charge trapping layer 130.
In some germanium embodiments, the germanium concentration is under 10% (atomic) relative to the silicon concentration. This concentration can be achieved by reducing the flow rate of the germanium precursor (which can be GeH4). In some phosphorus embodiments, the phosphorus concentration is under 10% (atomic) relative to the silicon concentration.
In some germanium embodiments, the germanium concentration may be under 10% or may be 10% or higher, but chlorine is also present in the charge trapping layer 130. The charge trapping layer thus may have Ge—Cl bonds.
The memory cell can be operated using prior art techniques, but the invention is not limited to such techniques. Suitable operation includes the techniques described above in connection with
In some embodiments, the memory is fabricated as follows. Dielectric 150 is formed on monocrystalline silicon substrate 122 using conventional techniques (e.g. thermal oxidation if dielectric 150 is silicon dioxide). Charge trapping layer 130 is formed on dielectric 150, for example, as follows. Silicon nitride is deposited by LPCVD (low pressure chemical vapor deposition) from ammonia (NH3) and either tetrachlorosilane (TCS, SiCl4) or dichlorosilane (DCS, SiH2Cl2). See e.g. U.S. Pat. No. 6,906,390 B2 issued Jun. 14, 2005 to Nomoto et al. and incorporated herein by reference. The TCS or DCS flow rate and the ammonia flow rate can be adjusted to provide the desired ratio x:y in the resulting SixNy compound. In some embodiments, x=3 and y=4. In other embodiments, silicon-rich silicon nitride is formed (x:y>3:4) to increase the number of silicon dangling bonds. Additional silicon dangling bonds may provide additional charge trapping sites. The silicon nitride layer may contain chlorine residue, and additional chlorine containing reagents can be provided to increase chlorine concentration in the charge trapping layer. An exemplary chlorine concentration range is 0.1˜5% (atomic) relative to silicon, and other concentrations are possible. Chlorine is optional however.
Silicon nitride 130 is doped with germanium or phosphorus during or after deposition. In some embodiments, the doping is performed after the deposition as follows. A few monolayers of germanium are deposited by atomic layer deposition (from GeH4 for example, or from a liquid source), or by epitaxial deposition (to reduce the hydrogen content), and then driven in by rapid thermal anneal (RTA). An exemplary anneal temperature is 900° C. or higher, and the exemplary anneal time is 30 seconds. The anneal can be combined with forming blocking layer 170 if suitable temperatures are used for the blocking layer, e.g. if the blocking layer is silicon dioxide obtained by high temperature oxidation of a silicon layer. In some embodiments, however, the blocking layer is aluminum oxide deposited at 400° C., or some other material deposited at relatively low temperatures, so RTA is used as a separate step for the germanium or phosphorus drive in. If chlorine is present in layer 170, some of germanium may bond with chlorine during the anneal to form Ge—Cl bonds. Germanium can also be introduced by ion implantation followed by RTA.
Alternatively, phosphorus doping is performed using liquid POCl3. Phosphorus can be deposited and then driven in by thermal anneal, or can be introduced by ion implantation. In some embodiments, the phosphorus concentration is under 10% (atomic) relative to silicon, but other concentrations are also possible.
In still other embodiments, the phosphorus or germanium doping is performed during the silicon nitride deposition. An exemplary technique is atomic layer deposition (ALD).
Dielectric layer 170 is deposited on charge trapping layer 130, possibly by known techniques (e.g. CVD of silicon dioxide, or CVD of polysilicon or amorphous silicon followed by oxidation of the silicon, or deposition of aluminum oxide, or by some other techniques).
Doped polysilicon, tantalum, or some other conductive material or materials are deposited on dielectric 170 to form the gate layer 140. Then the layers 150, 130, 210, 170, 140 are patterned as desired, possibly using a single mask. Then N+ dopant is implanted to form source/drain regions 124.
This fabrication process is not limiting. For example, any one or more of layers 150, 130, 210, 170, 140 can be patterned using a separate mask, and the layers other than 140 can be patterned before the layer 140 deposition. The P and N conductivity types can be reversed. The charge trapping region may include multiple layers, e.g. layers 130.1, 130.2 in