Patent Document

RELATED APPLICATION 
   This application is a divisional of U.S. application Ser. No. 11/044,511, filed Jan. 27, 2005, now U.S. Pat. No. 7,375,393, issued May 20, 2008, which is hereby incorporated by reference herein in its entirety. 

   TECHNICAL FIELD 
   The present invention relates to a methodology for improving the retention properties of a non-volatile memory (NVM) cell by utilizing an electrical shield to protect against charge redistribution in the layers surrounding the cell&#39;s floating gate. 

   
     DESCRIPTION OF THE DRAWINGS 
       FIG. 1  is a partial cross section drawing illustrating a conventional electrically programmable read only memory (EPROM) cell structure. 
       FIG. 2  is a partial cross section drawing illustrating a conventional electrically erasable programmable read only memory (EEPROM) cell structure. 
       FIGS. 3   a  and  3   b  are, respectively, a plan view and a partial cross section drawing illustrating an alternate embodiment of a conventional EEPROM cell. 
       FIG. 4  is a partial cross sectioning drawing illustrating a conventional Frohmann-Bentchkowsky EPROM cell. 
       FIG. 5  is a plot presenting typical dependence of VT vs. time for a programmed non-volatile memory (NVM) cell. 
       FIG. 6  is a partial cross-section drawing illustrating a NVM cell and corresponding electrical model, in accordance with the concepts of the present invention. 
       FIG. 7  is a partial cross section drawing illustrating an embodiment of an NVM cell utilizing an electrical shield for the cell&#39;s floating gate in accordance with the concepts of the present invention. 
   

   DESCRIPTION OF THE INVENTION 
   U.S. Pat. No. 4,698,787, issued on Oct. 6, 1987, discloses as prior art the conventional electrically programmable read only memory (EPROM) device structure shown in  FIG. 1 . The  FIG. 1  EPROM transistor device includes a source  10  and drain  12  formed in a substrate  14 . The source  10  and the drain  12  define a channel  16  in the substrate  14 . Positioned above the channel  16  is a layer of insulating material that forms a gate dielectric layer  18 . A floating gate  20  of semiconductor material is formed over the gate dielectric layer  18 . A second layer  22  of insulating material is formed over the floating gate  20 . Finally, a layer of semiconductor material is formed over the second layer of insulating material  22  to form a control gate  24 . Field oxide  26  isolates the transistor structure from periphery devices. Electrical connections  27 ,  28  and  30  are provided for applying voltages to the drain  12 , control gate  24 , and source  10 , respectively. 
   Programming of the  FIG. 1  EPROM cell is accomplished by raising the potential of the drain  12  (e.g., 8-12V), holding the source  10  at ground and applying a programming pulse (e.g., approximately 13-21V) to the control gate  24  for a preselected period of time (e.g., 1-10milliseconds). The result of these conditions is that a conductive region is established in the channel  16  across which electrons  32  are accelerated. The conductive region is designated by the dashed line  34  in  FIG. 1 . The magnitude and polarity of the voltages applied to the drain  12 , the source  10  and the control gate  24  are such that this conductive region is “pinched off ”in the region adjacent to the drain  12 . This causes electrons  32  to be raised sufficiently in potential so that they become “hot.” These “hot ”electrons create additional electron/hole pairs by impact ionization. In this condition, these electrons are elevated to an energy level that permits them to overcome the insulating properties of the gate dielectric  18 . The hot electrons can thus “jump ” the potential barrier of the gate dielectric  18 . Due to the electric field created by the control gate  24 , the hot electrons are attracted to the floating gate  20  where they are stored, thereby programming the cell. 
   The above-cited &#39;787 patent also discloses a programming mechanism for an electrically erasable programmable read only memory (FEPROM), shown in  FIG. 2 . The EEPROM cell structure shown in  FIG. 2  utilizes a different programming mechanism than does the EPROM cell described above. As with the EPROM structure, the EEPROM structure includes a drain  36 , a source  38 , a floating gate  42  separated from the substrate by a gate oxide layer  43 , a gate  40  separated from the floating gate  42  by another layer of oxide  45 , all of which are deposited or thermally grown. However, the EEPROM structure differs from the EPRO structure in that it provides a thin tunnel dielectric  46  between the drain  36  and the floating gate  42 . As shown in  FIG. 2 , the portion of the floating gate  42  that is positioned above the tunnel dielectric  46  is positioned on the drain region  36 . Further, the portion of the gate  40  that is aligned with the tunnel dielectric  46  is also positioned on the drain  36 . Programming (and erasing) of this structure is achieved by inducing potential differences between the gate  40  and drain  36  that are on the order of 20V. The thin dielectric region coupled with the high voltage between the gate  40  and the drain  36  induces “Fowler-Nordheim tunneling. ” 
   To program the  FIG. 2  cell, i.e. to place electrons on the floating gate  42 , the drain  36  is held at ground potential while the gate  40  is pulsed for approximately 10 milliseconds at a potential of approximately 20V. During this programming operation, the source  38  is allowed to float. Under these conditions, electrons tunnel through the tunnel dielectric  46  to the floating gate  42 . 
   The &#39;787 patent also discloses another EEPROM cell structure, shown in  FIGS. 3   a and  3   b . In this structure, a relatively shallow drain  54  and a deeper source  56  are formed in a silicon substrate  52 . A channel  58  is defined between the source  56  and the drain  54 . A gate dielectric  60  is formed over the channel  58  and extends over the channel  58  and to extend between the drain  54  and to overlap a portion of the source  56 . The gate dielectric  60  has a relatively uniform thickness over its entire cross section. A floating gate  64  is formed over the gate dielectric  60 . A second layer of dielectric material  66  is formed over the floating gate  64 . A control gate  68  is formed over the second layer dielectric material  66 . 
   Programming the cell shown in  FIGS. 3   a  and  3   b  is achieved by raising the drain  54  and the control gate  68  to predetermined potentials above that of the source  56 . For example, in one programming scheme, the drain  54  is raised to between 4-6V, while the control gate  68  is pulsed at about 10-12V for approximately 0.5-5 msec. Under these conditions, “hot ”electrons are generated and accelerated across the gate dielectric  60  and onto the floating gate  64 . Thus, the programming operation for this cell is similar to that of a conventional EPROM cell. 
   U.S. Pat. No. 6,137,723, issued on Oct. 24, 2000, discloses a so-called “Frohmann-Bentchkowsky ”memory transistor, shown in  FIG. 4 . The  FIG. 4  device includes spaced-apart p-type source  70  and drain  72  formed in an n-well  74 , which in turn is formed in a p-type silicon substrate. A channel is defined between the source  70  and the drain  72  and a layer of gate oxide  80  is formed over the channel  78 . A gate  82  is formed over the gate oxide layer  80 . A layer of dielectric material  84  along with gate oxide  80  encapsulates the gate  82 . 
   The  FIG. 4  cell is programmed by applying biasing voltages to the n-well and to the drain  72  that are sufficient to induce avalanche breakdown. For example, avalanche breakdown is induced by applying ground to the n-well  74  and a negative breakdown voltage to drain  72 , while either grounding or floating the source  70 , while floating or applying the positive breakdown voltage to the source  70 . The biasing voltages that are sufficient to induce avalanche breakdown establish a strong electric field across the drain-to-well junction depletion region. The strong electric field accelerates electrons in the junction depletion region into substrate hot electrons. A number of these substrate hot electrons penetrate the gate oxide layer  80  and accumulate on the gate  82 , thereby programming the cell. 
   Each of the cells described above is exemplary of a programming scheme for a non-volatile memory (NVM) cell. One of the basic properties of NVM cells is the ability to maintain charge on the floating gate within a required period of time (retention). The method to control retention is to monitor the threshold voltage VT of the cell over time. A typical dependence of VT versus time is presented in  FIG. 5 . The  FIG. 5  plot shows two mechanisms in effect with different characteristics that are commonly attributed to two leakage mechanisms: an initial leakage mechanism that leads to a significant VT shift within a short time (seconds or minutes) followed by a more gradual decrease in VT over a much longer period of time (e.g. 10 years). 
   The present invention is based upon the concept that the initial radical VT shift is not related to leakage from the floating gate, as is commonly believed, but rather may be attributed to charge redistribution in the dielectric layers/interfaces that surround the floating gate that effect the floating gate voltage due to capacitive coupling, as shown in  FIG. 6 . That is, after programming, the floating gate has a negative voltage that results in an electric field directed to the floating gate. This electric field forces positive charges to move toward the floating gate where they can be trapped at some of the interfaces. This process stops when the amount of trapped charge is sufficient to reduce the electric field outside the interface to zero. 
   In  FIG. 6 , the polysilicon floating gate electrode is formed on gate oxide, which, in turn, is formed on the composite. Additional gate oxide and plasma enhanced TEOS (PETEOS) insulates the floating gate, as does sacrificial SION and PETEOS. 
   This, a new control gate design is proposed that utilizes a protective shield. The shield can be made from the commonly employed second polysilicon layer or from other conductive material deposited over the floating gate. The second poly shield is similar to the well-known stacked gate design, but has a new function—to prevent the floating gate from being influenced by surrounding charges resulting from a programming operation. In the new design, the coupling between the control gate and the floating gate has low components due to the capacitance to the well and to the shield. 
     FIG. 7  shows a cross section of the new shielded NVM cell. The transistor (Transistor) is formed in the substrate in an active region defined by shallow trench isolation (STI). Gate oxide (Gate Oxide) separates the polysilicon floating gate (FG) from the substrate. In the  FIG. 7  embodiment, a control gate diffusion region (CG Cap) is formed in the substrate and is overlapped by the floating gate (FG), with intervening gate oxide (Gate Oxide) therebetween. A protective polysilicon cap (Poly Cap) is formed over the floating gate (FG) with intervening cap oxide (Cap Ox) therebetween. A layer of cobalt silicide (CoSi) is formed on the polysilicon cap (Poly Cap) and a layer of silicon oxinitride (SION) is formed on the CoSi layer. As stated above, the poly cap (Poly Cap) may be grounded. The  FIG. 7  embodiment shows the poly cap (Poly Cap) electrically connected to the substrate control gate via a metal interconnect structure (Metal). Isolation is provided by an overlapping layer of PETEOS.

Technology Category: 5