Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
2002-07-08
2004-12-07
Cao, Phat X. (Department: 2814)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S326000, C257S315000
Reexamination Certificate
active
06828625
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to the manufacture of semiconductor products in general, and particularly to protection against damage to semiconductor circuits from effects of electromagnetic wave energy generated during an etch process.
BACKGROUND OF THE INVENTION
During the manufacture of semiconductor products, layers of material are laid down or grown. Some layers are then etched, to produce the desired shapes of transistors, metal lines, and other microelectronics devices. When the processing has finished, a functioning chip is produced. If the chip contains a memory array, it typically has a plurality of memory transistors that may be programmed or erased. For example, the memory transistors may be floating gate transistors, nitride read only memory (NROM) transistors, silicon oxide-nitride oxide-silicon (SONOS) transistors, and any other non-volatile memory metal oxide semiconductor (MOS) devices capable of storing charge. Unfortunately, the manufacturing process may have some undesirable side effects. For example, in MOS technology, the charging of active elements during the manufacturing process may alter the device's characteristics or even damage them.
Reference is now made to
FIG. 1
, which illustrates a typical cross-section of an MOS or complementary MOS (CMOS) transistor wafer. It is typically formed of a gate oxide
10
over which is a polysilicon element
12
. On either side of the gate oxide
10
are field oxide
14
which are much thicker than the gate oxide
10
. Typically, the polysilicon element
12
also spreads over the field oxides
14
. A more advanced process may have trench isolation instead of field oxides, but the effects discussed hereinbelow are the same in such a case.
During manufacture, the field oxides
14
are first produced on a substrate
8
, after which the gate oxides
10
are grown. A layer of polysilicon is laid over the oxides
10
and
14
, and then etched to the desired shapes, such as by employing a shaped photoresist layer
15
. The etching process typically involves placing a plasma
16
, as is now explained.
The etching process may be carried out by many methods, however, plasma based processes such as plasma enhanced chemical vapor deposition (CVD) and reactive ion etching (RIE) are very common. Typically, energy for etching is generated by coupling radio frequency (RF) electromagnetic energy to a plasma
16
. The RF energy may be supplied by an RF generator coupled to a power supply. In
FIG. 1
, the etching process involves placing plasma
16
between the transistor and a electrified plate
18
connected to a high voltage source, and electrically connecting a second electrified plate
20
to the substrate
8
.
Plasma may generate ultraviolet (UV) photons. UV photons may also be generated during deposition of metal layers, such as in sputtering techniques. High energy electrons associated with the UV photons may charge the transistor. More specifically, since polysilicon is a conductive material, the polysilicon element
12
may become charged by the high energy photons. This is known as the “charging effect”. The charging effect is not generally a problem in conventional floating gate transistors because the excess charge may be erased. However, it may degrade the gate oxide as is now explained.
The more charge the polysilicon element
12
attracts, the greater the voltage drop between the polysilicon element
12
and the substrate
8
. If the voltage drop is high enough, it induces Fowler-Nordheim (F-N) tunneling of charge from the substrate
8
to the polysilicon element
12
, via the gate oxide
10
, as indicated by arrows
24
. Since the field oxides
14
are quite thick, no F-N tunneling generally occurs through them. Unfortunately, F-N tunneling may cause breakdown of the gate oxide
10
, especially if the gate oxide
10
is quite thin. It is appreciated that, once the gate oxide
10
has broken down, the transistor will not function.
Solutions are known for handling the gate oxide degradation problem of CMOS and floating gate transistors. The extent of the F-N tunneling is a function of the size of the polysilicon element
12
, the area of the gate oxide
10
and its thickness. As long as the area of polysilicon over the field oxides
14
is no larger than K times the area over the thin gate oxides
10
(where K, called the “antenna ratio”, varies according to the specific manufacturing process), the F-N tunneling will not occur. Alternatively, the total charge passing through the oxide will be small enough not to cause breakdown of the oxide. Accordingly, the amount of F-N tunneling may be reduced by reducing the area of the field oxide relative to the area of the gate.
In NROM devices, similar to the CMOS and floating gate memory devices, the abovementioned charging effect may be reduced by various techniques, such as the reduction of the antenna ratio K and adding discharge devices along the poly lines. Such techniques are discussed in applicant/assignee's U.S. patent application Ser. No. 09/336,666, filed Jun. 18, 1999 and entitled “Method and Circuit for Minimizing the Charging Effect During Manufacture of Semiconductor Devices”, now U.S. Pat. No. 6,337,502, issued Jan. 8, 2002.
However, in NROM devices, yet another problem may occur, wherein excess charge may accumulate along the edges of word lines. The excess charge is not uniform, and increases the threshold voltage V
t
of the cell. The increase in threshold voltage being non-uniform across the device width, may degrade the reliability and endurance of the cell. In NROM cells, programmed bits in the charge-trapping nitride layer are generally erased by hot hole injection. However, hot hole injection may only erase charge next to the source/drain junctions. The charge along the word line edge, far from the source/drain junctions, may not generally be erased. It would therefore be desirable to prevent UV photon-induced charge effect in the word-line edges of NROM devices.
SUMMARY OF THE INVENTION
The present invention seeks to provide methods and apparatus for protecting against plasma-induced damage to semiconductor circuits. The invention may be used in any non-volatile memory device, particularly a memory device with a non-conducting charge layer. The invention will be described with reference to an NROM device, although it is understood that the invention is not limited to NROM devices.
In accordance with a preferred embodiment of the present invention, a protective layer is formed in the NROM device over a polycide structure (e.g., a word line). The protective layer may comprise an ultraviolet absorber, e.g., a nitride layer. Nitride is a good absorber of UV energy, and accordingly may prevent UV photons from the plasma etching from inducing stress in the polysilicon layer or gate stress in an oxide-nitride-oxide (ONO) layer. One preferred nitride comprises a thick silicon-rich silicon nitride alloy. Additionally or alternatively, the protective layer may comprise a layer of highly resistive undoped polysilicon.
There is thus provided in accordance with a preferred embodiment of the present invention a method for protecting a non-volatile memory device, the method including forming a non-volatile memory device including a polycide structure formed over a non-conducting charge trapping layer, and forming a protective layer over at least a portion of the polycide structure, the protective layer being adapted to absorb electromagnetic wave energy having a wavelength shorter than visible light.
There is also provided in accordance with a preferred embodiment of the present invention a non-volatile memory device including a polycide structure formed over a non-conducting charge trapping layer, and a protective layer formed over at least a portion of the polycide structure, the protective layer being adapted to absorb electromagnetic wave energy having a wavelength shorter than visible light.
In accordance with a preferred embodiment of the present invention the protective layer includes an ultraviolet absorber.
Further in acco
Bloom Iian
Eitan Boaz
Cao Phat X.
Doan Theresa T.
Eitan, Pearl, Latzer & Cohen Zedek LLP
Saifun Semiconductors Ltd.
LandOfFree
Protective layer in memory device and method therefor does not yet have a rating. At this time, there are no reviews or comments for this patent.
If you have personal experience with Protective layer in memory device and method therefor, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Protective layer in memory device and method therefor will most certainly appreciate the feedback.
Profile ID: LFUS-PAI-O-3311476