Alternate timing wafer burn-in method

Electricity: measuring and testing – Fault detecting in electric circuits and of electric components – Of individual circuit component or element

Reexamination Certificate

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C324S1540PB, C365S201000, C365S149000

Reexamination Certificate

active

06388460

ABSTRACT:

CROSS-REFERENCE TO RELATED APPLICATION
This application claims the priority benefit of Taiwan application serial no. 89121546, filed Oct. 16, 2000.
BACKGROUND OF THE INVENTION
1. Field of Invention
The present invention relates to a wafer burn-in method. More particularly, the present invention relates to a wafer burn-in method that uses alternate timing.
2. Description of Related Art
In the manufacturing of semiconductor chips, various integrated circuits are formed on a wafer. The wafer is then cut out and sealed to form integrated circuit packages to be sold in the market.
Because each integrated circuit has its own characteristic properties, internal circuitry has to be checked to decide the quality of the chip. Conventionally, testing is conducted after the silicon chip is sealed. To test the package, voltages are applied to various exposed leads and measured. This process is commonly referred to as package burn-in. However, information regarding the quality of the chip is only obtained after packaging. Hence, packaging material and many processing steps are wasted whenever a sub-quality chip is found. To prevent the above problem, wafer burn-in is conducted in the wafer stage where probes are attached to the bonding pads of a wafer to carry out electrical testing. Any problem on a wafer can be found and tagged before packaging.
To develop memory cell stress during wafer burn-in, considerable time is required. Hence, DC timing must be used to prolong bit line conductance.
FIG. 1
is a timing diagram showing voltage variation of various input terminals. As shown in
FIG. 1
, voltage source VCC, word line voltage VW, word line conduct timing WL are at a high potential state. Because of the use of DC timing and the need for stressing the bit-line and the bit-line bar, the state of bit line voltage VBL and lower electrode voltage VEQ can be arranged into four types of combinations.
The effects of each of the four combinations are further explained below using the capacitor of a DRAM as an illustration.
FIGS. 2A through 2D
show the four combinations of states for the bit-line and the bit-line bar.
First, in the first combination
10
shown in
FIG. 1
, the bit line voltage VBL and the lower electrode voltage VEQ are at logic level ‘1’ and ‘0’ respectively. Hence, in
FIG. 2A
, since the upper electrode of the capacitor
18
is connected to the bit line voltage VBL, the upper electrode is at a potential level of ‘1’ potential (a high voltage state). On the other hand, since the lower electrode of the capacitor
18
is connected to the lower electrode voltage VEQ, the lower electrode is at a potential level of ‘0’ (a low voltage state). Thus, a stress from the upper electrode to the lower electrode (up/down direction) is created. Similarly, since the upper electrode of the capacitor
20
is connected to the bit line bar voltage VBLB, the upper electrode is at a potential level of ‘0’ (a low voltage state). Since the lower electrode is connected to the lower electrode voltage VEQ, the lower electrode is at a potential of ‘0’ (a low voltage state). Consequently, the capacitor
20
is in an idle state without any stress.
In the second combination
12
shown in
FIG. 1
, both the bit line voltage VBL and the lower electrode voltage VEQ are at logic level ‘0’. Hence, in
FIG. 2B
, since the upper electrode of the capacitor
22
is connected to the bit line voltage VBL, the upper electrode is at a potential level of ‘0’ potential (a low voltage state). Since the lower electrode of the capacitor
22
is connected to the lower electrode voltage VEQ, the lower electrode is at a potential level of ‘0’ (a low voltage state). Thus, the capacitor
22
is in an idle state without any stress. Similarly, since the upper electrode of the capacitor
24
is connected to the bit line bar voltage VBLB, the upper electrode is at a potential level of ‘1’ (a high voltage state). Since the lower electrode is connected to the lower electrode voltage VEQ, the lower electrode is at a potential of ‘0’ (a low voltage state). Consequently, a stress from the upper electrode to the lower electrode (up/down direction) is created.
In the third combination
14
shown in
FIG. 1
, both the bit line voltage VBL and the lower electrode voltage VEQ are at logic level ‘1’. Hence, in
FIG. 2C
, since the upper electrode of the capacitor
26
is connected to the bit line voltage VBL, the upper electrode is at a potential level of ‘1’ potential (a high voltage state). Since the lower electrode of the capacitor
26
is connected to the lower electrode voltage VEQ, the lower electrode is at a potential level of ‘1’ (a high voltage state). Thus, the capacitor
26
is in an idle state without any stress. Similarly, since the upper electrode of the capacitor
28
is connected to the bit line bar voltage VBLB, the upper electrode is at a potential level of ‘0’ (a low voltage state). Since the lower electrode is connected to the lower electrode voltage VEQ, the lower electrode is at a potential of ‘1’ (a high voltage state). Consequently, a stress from the lower electrode to the upper electrode (down/up direction) is created.
In the fourth combination
16
shown in
FIG. 1
, the bit line voltage VBL and the lower electrode voltage VEQ are at a logic level ‘0’ and a logic level ‘1’ respectively. Hence, in
FIG. 2D
, since the upper electrode of the capacitor
30
is connected to the bit line voltage VBL, the upper electrode is at a potential level of ‘0’ potential (a low voltage state). Since the lower electrode of the capacitor
30
is connected to the lower electrode voltage VEQ, the lower electrode is at a potential level of ‘1’ (a high voltage state). Thus, a stress from the lower electrode to the upper electrode (down/up direction) is created. Similarly, since the upper electrode of the capacitor
32
is connected to the bit line bar voltage VBLB, the upper electrode is at a potential level of ‘1’ (a high voltage state). Since the lower electrode is connected to the lower electrode voltage VEQ, the lower electrode is also at a potential of ‘1’ (a high voltage state). Consequently, the capacitor
32
is in an idle state without any stress.
Following from the aforementioned description, if both the bit-line and the bit-line bar are subjected to a stress, idle state occurs half of the time. Ultimately, burn-in test efficiency is cut in half.
SUMMARY OF THE INVENTION
Accordingly, one object purpose of the present invention is to provide a wafer burn-in method that uses alternate timing to prevent idling state and increase operating efficiency.
To achieve these and other advantages and in accordance with the purpose of the invention, as embodied and broadly described herein, the invention provides an alternate timing burn-in method suitable for testing a memory unit on a wafer. First, a first bit line voltage clocking signal is generated and sent to one end of the memory unit. A second bit line voltage clocking signal is generated and sent to the other end of the memory unit. The edge of the second bit line voltage clocking signal corresponds to the mid-point of the first bit line voltage clocking signal. The clocking rate of the first bit line voltage clocking signal and the second bit line voltage clocking signal is at the highest frequency of a station. The memory unit can be a capacitor with the first bit line voltage clocking signal sent to the upper electrode of the capacitor while the second bit line voltage clocking signal sent to the lower electrode of the capacitor.
It is to be understood that both the foregoing general description and the following detailed description are exemplary, and are intended to provide further explanation of the invention as claimed.


REFERENCES:
patent: RE37072 (2001-02-01), Gillingham
patent: 6188622 (2001-02-01), Beigel et al.

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