A Nonvolatile Memory Overview

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					A Nonvolatile Memory Overview
By Jitu J. Makwana, Dr. Dieter K. Schroder*

A Nonvolatile Memory Overview
Jitu J. Makwana, Dr. Dieter K. Schroder*

This paper presents a basic nonvolatile memory (NVM) overview. Section I begins
with the introduction including a brief background of NVM's and the common
terms used in the memory industry. The description and explanation of how an
NVM is programmed (adding electrons) using hot-carrier injection is covered in
section II. Section III covers the erasing or removing of electrons from floating gates
of NVM's. A brief mechanism of Fowler-Nordheim tunneling is covered. Section IV
introduces the model that can be used to predict the NVM programming
characteristics. The hot-carrier injection model addressed is the "Lucky Electron"
model. Section V covers the reliability aspects of NVM's. The common reliability
issues an NVM encounters are the data retention, endurance, and disturbs.

Memory can be split into two main categories: volatile and nonvolatile. Volatile memory
loses any data as soon as the system is turned off; it requires constant power to remain
viable. Most types of random access memory (RAM) fall into this category. Nonvolatile
memory does not lose its data when the system or device is turned off. A nonvolatile
memory (NVM) device is a MOS transistor that has a source, a drain, an access or a
control gate, and a floating gate. It is structurally different from a standard MOSFET in
its floating gate, which is electrically isolated, or "floating". Nonvolatile memories are
subdivided into two main classes: floating gate and charge-trapping. Kahng and Sze
proposed the first floating gate device in 1967 [1]. In this memory, electrons were
transferred from the floating gate to the substrate by tunneling through a 3 nm thin silicon
dioxide (SiO2) layer. Tunneling is the process by which an NVM can be either erased or
programmed and is usually dominant in thin oxides of thicknesses less than 12 nm.
Storage of the charge on the floating gate allows the threshold voltage (VT) to be
electrically altered between a low and a high value to represent logic 0 and 1,

In floating gate memory devices, charge or data is stored in the floating gate and is
retained when the power is removed. All floating gate memories have the same generic
cell structure. They consist of a stacked gate MOS transistor as shown in figure 1. The
first gate is the floating gate that is buried within the gate oxide and the inter-polysilicon
dielectric (IPD) beneath the control gate. The IPD isolates the floating gate and can be
oxide or oxide-nitride-oxide, ONO. The SiO2 dielectric surrounding the transistor serves
as a protective layer from scratches and defects. The second gate is the control gate which
is the external gate of the memory transistor. Floating gate devices are typically used in
EPROM (Electrically Programmable Read Only Memory) and EEPROM's (Electrically
Erasable and Programmable Read Only Memory).

                   Figure 1. A typical floating gate memory structure.

Charge-trapping devices were invented in 1967 [2] and were the first electrically alterable
semiconductor devices. In charge-trapping memory devices, charge or data is stored in
the discrete nitride traps and is also retained when the power is removed. Charge-trapping
devices are typically used in MNOS (Metal Nitride Oxide Silicon) [3], [4], SNOS
(Silicon Nitride Oxide Semiconductor) [5], and SONOS (Silicon Oxide Nitride Oxide
Semiconductor) [6]. Figure 2 shows a typical MNOS charge-trapping memory structure.

                       Figure 2. An MNOS memory cell structure.

The charges in MNOS memories are injected from the channel region into the nitride by
quantum mechanical tunneling through an ultra-thin oxide (UTO) which is typically 1.5
to 3 nm.

The first EPROM, a floating gate device, was developed using a heavily doped
polysilicon (poly-Si) as the floating gate material known as the floating gate avalanche-
injection MOS memory (FAMOS) [7]. The gate oxide thickness was of the order of 100
nm to prevent weak spot or shorting path between the floating gate and the substrate.
Charging of the EPROM was achieved by biasing the drain junction to avalanche
breakdown where the electrons in the avalanche plasma were injected from the drain
region into the floating gate. The FAMOS could only be erased by ultraviolet (UV) or x-
ray. The EPROM was perceived as a tool for system prototyping before a design was
committed to Read Only Memory (ROM). Today, one can obtain EPROM's in either a
ceramic package with a quartz window that allows for UV exposure or a plastic package
without a quartz window. These memories are known as one-time-programmable (OTP)
EPROM's. OTP's are inexpensive, however, additional testing after assembly is not
possible. EPROM's in ceramic packages with a quartz window are expensive but do
allow additional testing since the memory can be erased using UV light.
Although the 1970's saw the UV-erasable, electrically programmable memories become
commercially successful, there was an ever-present attraction toward making the
EPROM's electrically erasable, EEPROM. H. Iizuka et. al [8], proposed the first
electrical erasing NVM known as the stacked gate avalanche-injection MOS (SAMOS)
memory. SAMOS memory consisted of double poly-Si gates with an external control
gate. The external control gate made electrical erasability possible and as a result
improved the erasing efficiency. The EEPROM's basic approach with electrical means of
restoring the charged floating gate to its original uncharged status replaced UV emission
approach. Cheaper packaging and a greater ease of use were the first advantages of
EEPROM's over their UV-erasable counterparts. The disadvantage of EEPROM's was the
cell size that was two to three times the size of an EPROM cell that resulted in a larger
die size. EEPROM cells consist of two transistors, one, a floating gate transistor and the
other, a select gate transistor, as shown in figure 3. The select gate transistor is used to
select or deselect floating gate transistors for programming or erasing. Die size was
further increased to incorporate error correction circuitry or redundancy circuits.

                    Figure 3. An EEPROM with select gate transistor.

During the 1980's, a novel nonvolatile memory product was introduced, referred to as
Flash EEPROM [9]. The first products were merely the result of adapting EPROM's in
such a way that the cell could be erased electrically as well. These devices used hot-
electron injection for programming and tunneling for erasing. This new genre of Flash
EEPROM's could not be erased by bytes but could only be erased by the entire chip or
large sections of the chip. Since the need to erase by bytes as in EEPROM's was no
longer needed in Flash EEPROM's, the select transistor was removed from the cell
structure. Thus the Flash EEPROM's were two to three times smaller than earlier
EEPROM cells. The generic cell structure of a Flash EEPROM is similar to a generic cell
structure shown in figure 1.

Below is a nomenclature or a list of memory terms (not exhaustive) used in the literature,
industry, and education fields:

      Bit - The basic unit of memory, "1" or "0".
      Byte - A group of 8 bits.
      Cell - The physical semiconductor structure that stores one bit of data.
      Array - Repetition of memory cell in a two-dimensional matrix.
      RAM - Random access memory is fast, temporary storage for your computer
      ROM - Read-only memory is fast, permanent storage for your computer.
      Program - The operation of adding or removing electrons from the storage
       medium** of a memory cell. Sometimes called "Write". Charge is altered in the
       storage medium and thus the threshold voltage.
      Erase - The operation of adding or removing electrons from the storage
       medium** of a memory cell. Charge is altered in the storage medium and thus the
       threshold voltage.
       ** Floating gate (1st Polysilicon) or discrete nitride traps.
      Read - The process of determining the state of the bit cell.
      Endurance - Write/erase cycles a memory can endure before failure, typical
       guarantee is 10 K cycles.
      Injection - Common terms HCI: Hot-carrier Injection, HEI: Hot-electron
       Injection, CHEI: Channel Hot-electron Injection. Process of adding charge using
       high fields.
      Tunneling - Process of adding/removing charge but does not require high fields.
       Gate oxides are thin < 12 nm.
      Data Retention - Typically a time value pertaining to a memory cell's ability to
       retain data.
      Disturb - Charge gain or loss in a memory cell, gate disturb, read disturb,
       program disturb, etc.
      EPROM - Electrically programmable read-only memory.
      EEPROM - Electrically programmable and erasable read-only memory.
      Flash - Term used to describe erasing of a memory in large sections.

In both the floating gate and charge-trapping memories, the charge needed to program the
device has to be injected into the floating gate or into the nitride layer respectively. In
order to change the charge or data content of NVM';s, two major mechanisms have been
shown to be viable: FN tunneling (F-N) through thin oxides (< 12 nm) [10] and channel
hot-electron injection (CHE) [11].

IIa. Fowler-Nordheim (FN) Tunneling
One of the most important injection mechanisms used in NVM's is FN tunneling. When a
large voltage Vcg is applied at the control gate during programming, its energy band
structure will be influenced as shown in figure 4.

  Figure 4. Energy band diagram of a floating gate memory during programming by FN

In the figure, ec and ev are the conduction and valence bands respectively, Eg is the
energy band gap (1.1 eV for silicon), fb is the Si-SiO2 energy barrier (fb is 3.2 eV for
electrons and 4.7 eV for holes). The applied Vcg creates the electric field resulting in a
potential barrier. This barrier provides a path for the electrons in the substrate to tunnel
through the thin gate oxide (typically less than 12 nm) and eventually be collected in the
n+ poly-Si floating gate. The bending of the energy bands of the IPD and the gate oxide
are different due to the thickness differences between them. The IPD ranges from 25 nm
to 45 nm while the gate oxide ranges from 5 nm to 12 nm. The electrons collected at the
floating gate leads to a tunneling current density and is given by [12].



h = Planck's constant
  = Energy barrier at the injecting surface (3.2 eV for Si-SiO2)
q = Charge of a single electron (1.6x10-19 C)
m = Mass of a free electron (9.1x10-31 kg)
m* = Effective mass of an electron in the band gap of SiO2 (0.42 m)
 = h/2

?inj = Electric field at the injecting surface =   (V/cm)
Vapp = Voltage applied across the tunnel oxide (V)
Vfb = Flat band voltage (V)
tox = Tunnel oxide thickness (cm)

Equation 1 shows that tunneling current density is exponentially dependent on the applied
voltage, Vapp, which influences the electric field, ?inj, across the gate oxide.
Figure 5 shows a cross-section of an NVM with electrons tunneling uniformly with Vcg at
positive potential while the source (Vs), the drain (Vd), and the substrate (Vsub) are at
ground potential.

                Figure 5. Uniform tunneling to program Flash EEPROM.

An optional method that can be used to program Flash EEPROM's is given in figure 6
which is called drain-side tunneling. Drain-side tunneling is sometimes preferred over the
uniform tunneling due to the programming speed as a result of higher tunneling current
density due to smaller injecting area.

               Figure 6. Drain-side tunneling to program Flash EEPROM.

IIb. Hot-carrier Injection (HCI)
NVM's can also be programmed by hot-carrier injection. The method of programming is
by hot-electron injection for n-type NVM's built on p-substrates and by hot hole injection
for p-type NVM's built on n-substrates. Hot-hole injection is very slow due to the hole
mass as well as the Si-SiO2 energy barrier of 4.7 eV for holes, which is why all NVM's
manufactured today are n-type on p-substrates.
The memory cell is programmed by charging the floating gate via the injection of hot-
electrons from the drains pinch-off region. The hot-electrons get their energy from the
voltage applied to the drain (Vd) of the memory cell. They are accelerated by the lateral
electric field (Elat) along the channel into even higher fields surrounding the drain
depletion region. Once these electrons gain sufficient energy they surmount the energy
barrier of 3.2 eV between the silicon substrate and the silicon dielectric layer or gate
With positive Vd and channel voltages, electrons injected into the oxide of an n-channel
memory cells return to the substrate unless a high positive Vcg is applied to pull the
electrons toward the floating gate. The energy band structure for NVM programming by
hot-electron injection is shown in figure 7.

 Figure 7. Energy band diagram of a floating gate memory during programming by hot-
                                  electron injection.

As the floating gate becomes fully charged, the gate current (Ig) is reduced to almost zero
because the oxide electric field (Eox) (in the beginning of the injection process Eox was
attractive to the electrons) is now repulsive to the electrons. In general, to the first order,
Vcg increases the charge on the floating gate while Vd affects the programming speed.
Figure 8 shows a cross-section of an NVM with hot-electron injection programming. Vcg
and Vd are at positive potential of 15 V and 10 V respectively while Vs and Vsub are at
ground potential. The p-well is also shown, as it is the process needed to separate n-
channel and p-channel MOS transistors from NVM's devices.
        Figure 8. Hot-electron injection mechanism for programming in NVM's.

Section II covered the two programming schemes, namely, FN tunneling and hot-electron
injection. In order to reprogram an NVM, it first has to be erased. This section will cover
the erasing schemes commonly employed in the industry.
The electrons that are injected into the floating gate are trapped by the high gate to oxide
energy barrier of 3.2 eV. Since the potential-energy barrier at the oxide-silicon interface
is greater than 3.0 eV, the rate of spontaneous emission of electrons from the oxide over
this barrier is negligibly small. The net negative charge which remains on the floating
gate shifts the VT to a positive value.
There are two methods of erasing or removing charge:

   1. UV emission.
   2. FN tunneling.

IIIa. UV Emission
Referring to figure 9, electrons gain enough energy acquired from the UV radiation to
surmount the energy barrier from the floating gate to either the control gate or to the
substrate, which reduces the VT. The typical time it takes to change the VT from
programmed state to neutral or erased state is 10 minutes.

                 Figure 9. Energy band diagram of UV erase of an NVM.
IIIb. FN Tunneling
FN tunneling can also be used to erase an NVM. One of the methods is by applying a
large negative voltage at the control gate. The energy band structure will be influenced as
in figure 10. The applied Vcg creates the electric field resulting in a potential barrier. This
barrier provides a path for the electrons to tunnel from the floating gate to the substrate
through the thin gate oxide.

    Figure 10. Energy band diagram of a floating gate memory during erasing by FN

Figure 11a and 11b shows two choices to erase a Flash EEPROM. For uniform tunneling,
a large negative Vcg is applied while for drain-side tunneling method, both a negative Vcg
and a positive Vd are applied.

                 Figure 11a. Uniform tunneling to erase Flash EEPROM.
                Figure 11b. Drain-side tunneling to erase Flash EEPROM.

In general, uniform tunneling is slower that drain-side tunneling, but, drain-side tunneling
tends to cause reliability issues. The reliability issue is the gate oxide damage that occurs
near the drain since a small area is bombarded by electrons and that the tunneling current
density as a result of small area is higher.
One of the methods of programming an EPROM or a Flash EEPROM is by channel hot-
electron injection (CHE) where hot-electrons are generated in the high field region
between the pinched-off channel and drain. Electrons with sufficient energy are injected
across the oxide to the floating gate, thereby programming the device (increasing the
threshold voltage to positive value, VT). This process of programming is slow due to the
injection efficiency, which is dependent on three probability events. The hot-carrier
injection mechanism gives rise to impact ionization at the drain, by which both minority
(electrons) and majority (holes) carriers are generated. The highly energetic holes are
normally collected at the substrate contact and form the substrate current (Isub) while the
minority carriers are collected at the drain and forms the drain current (Ids). If the oxide
electric field (Eox) favors injection, these carriers are injected over the energy barrier (fb)
of the gate oxide and gives rise to hot-carrier injection gate current (Ig). In the case of
floating gate memories, these electrons change the charge content of the floating gate.
There are two models that can be used to describe the gate current due to hot-electron
injection. The two models are the lucky-electron model [13] and the effective electron
temperature model [14].
     IVa. Lucky-electron Model and Threshold Programmed VT
     The lucky-electron approach of modeling the hot-electron distribution was originated by
     Shockley [15]. Conceptually, the lucky-electron model can be described as follows. In
     order for hot-electrons to reach the gate, the hot-electrons must gain sufficient kinetic
     energy from the lateral channel field (Elat) and have its momentum redirected towards the
     Si-SiO2 interface in order to surmount the SiO2 energy barrier (fb). Figure 12 shows the
     concepts involved in the lucky-electron model. The three events involved in the lucky-
     electron model are:

           A - B Event: A channel electron has to gain energy from the Elat and become
            "hot". The hot-electron momentum has to be re-directed towards the Si-SiO2
            interface. The probability associated with this process is and is defined as the
            probability of an electron having enough normal momentum to surmount the Si-
            SiO2 potential barrier height.

                Figure 12. The three processes in the lucky-electron injection model.

I.           B - C Event: Once the hot-electron is re-directed, it must not suffer any energy
     robbing collisions. The probability associated with this event is PSEMI. PSEMI is defined as
     the probability of an electron traveling to the Si-SiO2 interface without suffering any
       II.   C - D Event: While in transit from the Si-SiO2 interface to the floating gate, the
             electron must not suffer any collisions in the oxide image potential well. The
             probability associated with this event is Pinsul and is defined as the probability of
             an electron suffering no collision in the oxide image potential well.

     Since these three probabilities are statistically independent, the resultant probability is the
     product of the probability for each individual event. The gate current is given by
lr = Momentum re-direction scattering mean free path = 92 nm
Leff = Effective channel length of the floating gate transistor (cm)
Ids = Drain-source current (A)

The charge on the floating gate changes the threshold voltage (VT) of the floating gate
transistor by

DVT = VT (Programmed) - VT (Initial)
DQfg = Qfg (Programmed) - Qfg (Initial) = Change in floating gate charge.
The floating gate charge changes according to

Dt is the programming time (s)

The change in floating gate charge shifts VT from the initial or natural threshold voltage
VTi by

Cfg = Floating gate to control gate capacitance (F)

Figure 13 shows a typical transfer characteristic for the programmed and initial or erased
states. The figure shows that the Ids-Vcg curves are parallel to each other. The shift of the
Ids-Vcg curve from initial or erased state to programmed state is equal to DQfg/ Cfg.

Figure 13. Ids-Vcg transfer characteristics.
Nonvolatile memory cells have some important functional characteristics, which are used
to evaluate the performance of the cell. These characteristics are divided into two main
classes, namely endurance and retention. In order to understand endurance and retention
characteristics, it is imperative to know some of the fundamentals associated with gate
oxide and interpolysilicon dielectric, IPD, integrity. Although traps are the storage sites
in MNOS, SNOS, and SONOS memories, they constitute the very means that lead to
reliability failures in EPROM's, EEPROM's, and Flash EEPROM's. The gate oxide and
IPD quality can affect endurance and retention.

The primary failure mechanism of the gate oxide pertains to oxide breakdown and trap-
up due to high injection electric field stressing during hot-electron injection or FN
tunneling. It was suggested that oxide defects and broken Si-O bonds serve as trapping
centers [16] for positive (holes) charge. Oxide breakdown occurs after a fixed amount of
charge per unit area (Qbd) has been injected and has been shown to be a function of
applied electric field [17]. Qbd is an industry standard electrical test used to measure the
quality of the oxide with higher Qbd (good oxide quality) as the desired goal. Trap-up is
defined as the trapping of electrons in the oxide during programming/writing operations.
These trapped charges change the injection fields and thus, the amount of charge
transferred to and from the floating gate during programming.

As described earlier, one of the components of a nonvolatile memory cell structure is the
IPD. In nonvolatile memories, IPD is used to isolate the floating gate from other
electrodes (control gate, source, drain, and the substrate) and hence, should be defect-free
to prevent charge leakage from the floating gate. Since the floating gate is a poly-Si layer,
it is commonly oxidized during the IPD growth process. The oxidation of poly-Si layer
modifies the surface topology due to enhanced oxidation at the grain boundaries of the
poly-Si, forming interface protuberances and inclusions [18]. The surface
nonuniformities causes electric field enhancement resulting in higher leakage currents,
which is a drawback for an insulating IPD. Figure 14 shows a circuit diagram of the
effects of nonuniformities with respect to electric field enhancement. Other factors that
influences the IPD quality are the doping of the floating gate poly-Si layer and the
temperature of both the poly-Si deposition and the oxidation [19]. Multiple dielectric
stacks such as the oxide-nitride-oxide (ONO) are now commonly used as IPD's for lower
leakage due to lower defect densities and higher electric field properties [20]. The lower
leakage currents are achieved due to the fact that the electrons that have leaked from the
floating gate gets trapped in the oxide-nitride interface which builds an electric field that
opposes further charge loss [21]. Typical thicknesses of the ONO stack are 5 - 10 nm, 20
nm, and 3 nm for the bottom oxide, nitride, and the top oxide respectively. The bottom
oxide is the oxide above the floating gate while the top oxide is the oxide beneath the
control gate.
                  Figure 14. IPD leakage current due to nonuniformities.

Va. Endurance Characteristics
The endurance characteristics give the memory threshold voltage window, which is the
difference between the threshold voltages in the programmed/written state and the erased
states, as a function of the number of programming cycles, as shown in figure 15.
Nonvolatile memories can be programmed and erased frequently at the expense of
introducing permanent gate oxide damage such as oxide breakdown and trap-up. This
implies that the total number of program operations is limited; for example, most
commercially available EEPROM products are guaranteed to withstand 106 programming
cycles. The damaging of the memory cell during cycling is normally referred to as
"degradation" and the number of cycles the memory can withstand is called "endurance".
Threshold voltage window closure occurs when the threshold voltage difference between
the programmed and erased states cannot be distinguished. The phenomenon of window
closure has been attributed to trapping of injected electrons in the gate oxide due to pre-
existing electron traps. There is also evidence of trap generation during programming and
erasing due to high electric field stress (Einj). It is thus important to have high quality gate
oxides that can endure constant electron stress during hot-electron injection or FN

      Figure 15. Typical EEPROM cell threshold voltage window versus log cycles.
Vb. Retention Characteristics

When a nonvolatile memory cell can no longer hold the charge in the floating gate, it is
said to have affected its retention capability. Retention is a measure of the time that a
nonvolatile memory cell can retain the charge whether it is powered or unpowered. In
floating gate memories, the stored charge can leak away from the floating gate through
the gate oxide or through the IPD. This leakage caused by mobile ions and oxide defects,
result in a shift of the threshold voltage of the memory cell. Different charge loss
mechanisms have been described [22], [23], namely, charge loss due to thermionic
emission, charge loss due to electron detrapping, and charge loss due to contamination
such as positive mobile ions. To improve the retention characteristics of the memory cell,
various improvements to the quality of the gate oxide and IPD becomes very important.
Retention can be quantified by measuring or estimating the time it takes for the floating
gate to discharge when it is intended to keep the information stored. When charge loss
occurs, a shift in the VT of the memory cell occurs according to equation 8.
where dQFG, CFG, and dVT are the floating gate charge loss, floating gate capacitance, and
the floating gate VT shift respectively. Equation 9 shows the evaluation of the number of
electrons lost and equation 10 shows how the number of electrons lost is related to
leakage current, ILeakage and retention time, dt.
For a typical CFG of 30 fF and a VT shift of 3 V, the # of electrons lost from the floating
gate to control gate is 5.6x105. Table 1 shows the retention time, dt, for various ILeakage
associated with a loss of 5.6x105 electrons or 3 V VT shift.

  Leakage Current,       Retention Time, dt
    ILeakage (A)              (Years)
      1x10-20                   0.28
       5x10-21                   0.56
       1x10-21                   2.84
       5x10-22                   5.68
      2.85x10-22                  10

                      Table 1. Retention time as function of ILeakage.

Table 1 shows that it would take 10 years for an NVM to loose charge equivalent to 3 V
shift for a leakage current of 2.85x10-22 A.
Vc. Memory Disturbs
Widespread use of nonvolatile memories in production systems requires data retention
for ten years or more. A typical memory array undergoes stresses that arise during
programming and erasing commonly referred to as disturbs. The four principal memory
cell disturbs that can occur in an array are dc erase, dc program, program disturb, and
read disturb [24]. The two common disturbs that can impact memory cells during
programming are dc program and program disturb. Memory cell disturbs can also occur
during erasing and is called dc erase. Finally, during "read" operation when the memory
is read to determine the state (logic 0 or 1), memory cell disturb can also occur and is
called read disturb. Figure 16 shows the schematic description of a memory array and
will be used to describe the memory cell disturbs.

            Figure 16. Schematic description of a memory array with disturbs.

In figure 16, the memory array has columns connected to the drain of each memory cell
(COL 1, COL 2, and COL 3) that represent the "bitline" and are used to select or deselect
the memory cell for programming or erasing. The memory array also has rows that are
connected to the control gate of each memory cell (ROW 0 and ROW 1) that represent
the "wordline" and are also used to select or deselect the memory cell for programming or
erasing. From previous discussions on hot-carrier injection, both the bitline and the
wordline have to have voltages applied in order for the memory cell to program. If either
the bitline or the wordline is not connected to a high potential, then hot-carrier injection
will not occur.
The four types of memory disturbs are:
1) DC Erase: This type of disturb occurs on cells that are already programmed (Cell A).
These programmed cells are on the same wordline (ROW 1) as the cell being
programmed (COL 2 and ROW 1). During the programming operation ROW 1 is brought
to a high voltage of 15 V. The electric field due to the high voltage appears across the
IPD, which may be high enough to cause conduction of electrons across it from the
floating gate (also known as poly-Si to poly-Si erase mode mechanism) to the control
gate. The result, loss of charge and consequent reduction of the programmed threshold
voltage, which in severe cases causes complete loss of data.
2) DC Program: Also known as gate-disturb, occurs on cells that are unprogrammed or in
erased state (Cell B). These unprogrammed cells are on the same wordline (ROW 1) as
the cell being programmed (COL 2 and ROW 1). These unprogrammed cells have a few
electrons on their floating gates and thus low threshold voltages, VT. When ROW 1 is
raised to 15 V, the electric field across the tunneling gate dielectric may be high enough
to cause electron tunneling into the floating gate from the substrate and increase the VT.
In severe cases, the cell is programmed unintentionally and is called soft-write.
3) Program Disturb: Also known as drain-disturb occurs on programmed cells. A
programmed cell (Cell C) sharing a column (COL 2) with the cell being programmed
(COL 2 and ROW 1) will also experience high electric fields between the floating gate
and the drain. This may cause electrons to tunnel from the floating gate to the drain, and
lead to a reduced VT.
4) Read Disturb: This disturb mechanism occurs on erased bits that share a wordline with
a bit that is being read. The common wordline places the control gate of the erased cells
at 5 V. The selected device's drain is driven to about 1 V. The unselected bits have their
source, drain, and substrate at 0 V.
An NVM overview was given which began with a brief background of nonvolatile
memories and the terminology's used in the NVM industry. The two common methods of
programming are the hot-carrier injection and FN tunneling. In FN tunneling, gate oxides
thicknesses have to be less than 12 nm whereas in the case of hot-carrier injection, the
thickness of the gate oxide is not critical. The two common methods employed for
erasing are by UV emission and FN tunneling. UV emission is commonly used for UV
EPROM's while FN tunneling is commonly employed in EEPROM's and Flash
EEPROM's, provided the thicknesses are less than 12 nm. UV emission takes a long time
to erase relative to FN tunneling. Typical UV emission erase time is 10 minutes while the
FN tunneling takes anywhere from 1 ms to 10 ms depending on the applied potentials at
the control gate and the drain. The fastest method of programming is via hot-carrier
injection that can typically take up to 100 ms. To understand the physics of hot-carrier
injection, a "lucky-electron" model was covered. The model shows how the gate current
is evaluated based on various probability events. Although the injection efficiency is low,
the process of adding electrons onto the floating gate is fast due to high electric fields. As
for every device, reliability issues are encountered. Endurance and data retention are the
two common reliability issues an NVM undergoes. In addition to endurance and data
retention, memory disturbs also occur due to memory stressing during programming and
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