Method for testing leakage current caused self-aligned silicide

Information

  • Patent Grant
  • 6249138
  • Patent Number
    6,249,138
  • Date Filed
    Tuesday, November 23, 1999
    24 years ago
  • Date Issued
    Tuesday, June 19, 2001
    23 years ago
Abstract
A method of testing a leakage current caused by a self-aligned silicide process is described. The invention uses different test structure to monitor degree of and reason for a leakage current caused by a self-aligned silicide process. While monitoring a self-aligned silicide process performed on a metal-oxide semiconductor transistor without a LDD region, in addition to considering a leakage current occurring from the metal silicide layer to the junction and occurring at edge of the metal silicide layer, the invention further considers a leakage current at comer of the metal silicide layer. For a metal-oxide semiconductor transistor having a LDD region, the invention further considers a leakage current from the metal silicide layer to the LDD region. The invention monitors a leakage current at comer of the metal silicide layer.
Description




BACKGROUND OF THE INVENTION




1. Field of Invention




The present invention relates to a method for testing reliability of a self-aligned silicide process. More particularly, the present invention relates to a method for testing a leakage current caused by self-aligned silicide, using different test structures after a self-aligned silicide process.




2. Description of Related Art




In a conventional method for testing reliability of a self-aligned silicide process, test structures, as shown in FIG.


1


and

FIG. 2

, are commonly deposited on wafer scribe lines. These test structures include a big diffusion region


102


(FIG.


1


), or multiple bars of diffusion regions


102


on the wafer


100


(FIG.


2


), and a metal silicide layer


104


thereon. These test structures and a metal-oxide semiconductor (MOS) transistor in a chip are simultaneously formed, therefore, the test structures can monitor reliability of the self-aligned silicide layer on a source/drain region of the MOS transistor to avoid malfunction of the MOS transistor. The two test structures (shown in FIG.


1


and

FIG. 2

) are designed according to a leakage current occurring from the metal silicide layer to the junction, and a leakage current occurring at the edge of the metal silicide layer. Therefore, design parameters of the two test structures in

FIGS. 1 and 2

include area and perimeter of the metal silicide layer.




Accordingly, the conventional method for testing reliability of a self-aligned silicide process is to measure a current of the test structure shown in

FIG. 1

or

FIG. 2

, and then calculate current density from the metal silicide to the junction region and current density of the edge of the metal silicide. According to these two current densities, the leakage current caused by the metal silicide layer can be monitored. If the leakage current is not in an allowable range, the self-aligned silicide process has to be immediately rectified so as to reduce wafer nullity probability.




However, when the test structures shown in

FIG. 1 and 2

are employed in 0.25 μm semiconductor processes, some problems arise. The device malfunction probability is still large when testing for device electricity after the whole semiconductor processes, even though the test result of the self-aligned process is favorable. In other words, the conventional test structure cannot accurately monitor the reliability of the self-aligned process. This leads to an increase of the wafer malfunction probability and capital expenditure.




SUMMARY OF THE INVENTION




Accordingly, the invention provides a method for testing reliability of a self-aligned silicide process. The method can be employed in a 0.25 μm or lower than 0.25 μm semiconductor process.




The invention provides a method for testing reliability of a self-aligned silicide process. The invention uses different test structures to monitor degree of and reason for a current leakage caused by a self-aligned silicide process so as to immediately discover problems, and then immediately resolve the problems.




The invention provides a method for testing reliability of a self-aligned silicide process. In addition to considering a leakage current occurring from a metal silicide layer to the junction and a leakage current occurring at edge of the metal silicide layer, the invention further considers a leakage current occurring from the metal silicide layer to a LDD region and a leakage current occurring at comer of the metal silicide layer adjacent to a shallow trench isolation structure.




Accordingly, the invention provides a method of testing a leakage current caused by a self-aligned silicide process, which is suitable for monitoring the self-aligned silicide process performed on a metal-oxide semiconductor transistor having no lightly doped drain (LDD) structure. At first, parameters for monitoring the self-aligned silicide process are considered. The parameters include an area current density (J


A


) an edge current density (J


E


), and a comer current density (J


C


) A total current (J) of the metal silicide layer is calculated as follows:






J=J


A


×A+J


E


×L+J


C


×C,






wherein A is an area of the metal silicide layer, L is an edge perimeter of the metal silicide layer, and C is comer number of the metal silicide layer. At least three test structures including a first test structure, a second test structure, and a third test structure are deposited on a wafer. The first test structure, the second test structure and the third test structure respectively comprises a first, a second and a third diffusion regions and a first, a second, and a third metal silicide layer on the first, the second, the third diffusion regions. The first, the second and the third diffusion regions are respectively surrounded by a first, a second, and a third isolation structures, wherein an area of the first metal silicide layer of the first test structure is A


1


, its edge perimeter is L


1


, its comer number is C


1


, an area of the second metal silicide layer of the second test structure is A


2


, its edge perimeter is L


2


, its corner number is C


2


, and an area of the third metal silicide layer of the third test structure is A


3


, its edge perimeter is L


3


, and its corner number is C


3


. Electricity of the first test structure, the second test structure, and the third test structure is measured to respectively obtain total currents J


1


, J


2


, and J


3


; J


1


, J


2


, and J


3


are then substituted into a total current equation to obtain three linear equations:






J


1


=J


A


×A


1


+J


E


×L


1


+J


C


×C


1


,








J


2


=J


A


×A


2


+J


E


×L


2


+J


C


×C


2


, and








J


3


=J


A


×A


3


+J


E


×L


3


+J


C


×C


3


.






The three linear equations are calculated to obtain a set of values for J


A


, J


E


, and J


C


. The self-aligned silicide process is monitored according to the set of values for J


A


, J


E


, and J


C


.




The invention provides another method of testing a leakage current caused by a self-aligned silicide process, which is suitable for monitoring the self-aligned silicide process performed on a metal-oxide semiconductor transistor having a lightly doped drain (LDD) structure. At first, parameters for monitoring the self-aligned silicide process are considered. The parameters comprises an area current density (J


A


), an interface current density (J


isolation,L


) between the metal silicide layer and a device isolation structure, and a current density (J


LDD,L


) from the metal silicide layer to the LDD region. A total current (J) of the metal silicide layer is calculated as follows:






J=J


A


×A+J


isolation,L


×L


isolation


+J


LDD,L


×L


LDD


,






wherein A is an area of the metal silicide layer, L


isolation


is an interface perimeter between the metal silicide layer and the device isolation structure, and L


LDD


is a path of the LDD region. At least three test structures including a first test structure, a second test structure, and a third test structure are deposited on a wafer. The first test structure, the second test structure and the third test structure respectively comprises a first, a second and a third diffusion regions and a first, a second, and a third metal silicide layers respectively on the first, the second, and the third diffusion regions. The first, the second and the third diffusion regions are electrically isolated by a first, a second, and a third isolation structures. At least one of the first, the second, the third diffusion regions has the LDD region, such that an area of the first metal silicide layer of the first test structure is A


1


, an interface perimeter between the first metal silicide layer and the first device isolation structure is L


isolation1


, a length of the LDD region is L


LDD1


, an area of the second metal silicide layer of the second test structure is A


2


, an interface perimeter between the second metal silicide layer and the second device isolation structure is L


isolation2


, a length of the LDD region is L


LDD2


, an area of the third metal silicide layer of the third test structure is A


3


, an interface perimeter between the third metal silicide layer and the third device isolation structure is L


isolation3


, and a length of the LDD region is L


LDD3


. Electricity of the first test structure, the second test structure, and the third test structure are measured to respectively obtain total currents J


1


, J


2


, and J


3


; J


1


, J


2


, and J


3


are substituted into a total current equation to obtain three linear equations:






J


1


=J


A


×A


1


+J


isolation,L


×L


isolation1


+J


LDD,L


×L


LDD1


,








J


2


=J


A


×A


2


+J


isolation,L


×L


isolation2


+J


LDD,L


×L


LDD2


, and








J


3


=J


A


×A


3


+J


isolation,L


×L


isolation3


+J


LDD,L


×L


LDD3


,






The three linear equations are calculated to obtain a set of values for J


A


, J


isolation,L


, and J


LDD,L


. The self-aligned silicide process is monitored according to the set of values for J


A


, J


isolation,L


, and J


LDD,L


.




In addition, the invention further comprises depositing a fourth test structure on the wafer. The fourth test structure comprises a fourth diffusion region and a fourth metal silicide layer on the fourth diffusion region, and the fourth diffusion region has a LDD structure. The fourth diffusion region is electrically isolated by a fourth isolation structure, wherein area of the fourth metal silicide layer of the fourth test structure is A


4


, an interface perimeter between the fourth metal silicide layer and the fourth device isolation structure is L


isolation4


, and a length of the LDD region is L


LDD4


. The fourth test structure mainly increases the corner number of the fourth metal silicide layer adjacent to the fourth isolation structure. A


4


, L


isolation4


, L


LDD4


, and the set of values for J


A


, J


isolation,L


, and J


LDD,L


are substituted into an equation for the total current to obtain an ideal total current J


ideal


. Electricity of the fourth test structure is measured to obtain an actual total current J


4


. The self-aligned silicide process is monitored by comparing the actual total current J


4


with the ideal total current J


ideal


.




Therefore, while monitoring a self-aligned silicide process performed on a metal-oxide semiconductor transistor without a LDD structure, in addition to considering a leakage current occurring from the metal silicide layer to the junction and a leakage current occurring at edge of the metal silicide layer, the invention further takes a leakage current occurring at comer of the metal silicide layer into consideration. While monitoring a self-aligned silicide process performed on a metal-oxide semiconductor transistor having a LDD structure, the invention further takes a leakage current occurring from the metal silicide layer to the LDD region into consideration. Additionally, in order to avoid a situation where a leakage current occurring at comer of the metal silicide layer adjacent to a shallow trench isolation structure is not immediately monitored, another test structure is added as a check. Thus, reliability of the self-aligned silicide process is more accurately controlled. The self-aligned silicide process can be immediately rectified to reduce probability of useless wafers, and further to enhance device reliability.




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.











BRIEF DESCRIPTION OF THE DRAWINGS




The accompanying drawings are included to provide a further understanding of the invention, and are incorporated in and constitute a part of this specification. The drawings illustrate embodiments of the invention and, together with the description, serve to explain the principles of the invention. In the drawings,




FIG.


1


and

FIG. 2

are top views showing two conventional test structures for monitoring a current leakage caused by a self-aligned silicide process;





FIG. 3

is a schematic, cross-sectional view of a metal-oxide semiconductor (MOS) transistor without a LDD structure;





FIG. 4

,

FIG. 5

, and

FIG. 6

are top views showing three different test structures which are deposited in scribe lines of a wafer to monitor a self-aligned silicide process according to one preferred embodiment of this invention wherein the test structures are suitable for monitoring a metal silicide on a metal-oxide semiconductor transistor without a LDD region;





FIG. 7

is a schematic, cross-sectional view of a metal-oxide semiconductor transistor having a lightly doped drain (LDD) structure; and





FIG. 8

,

FIG. 9

, FIG.


10


and

FIG. 11

respectively show four different test structures which are deposited in scribe lines of a wafer to monitor a self-aligned silicide process, wherein the test structures are suitable for monitoring a metal silicide on a metal-oxide semiconductor transistor having a LDD region.











DESCRIPTION OF THE PREFERRED EMBODIMENTS




When design rule is reduced to 0.25 μm or less, required quality for a self-aligned process is thus increased. Leakage current caused by metal silicide not only occurs from the metal silicide to the junction and the edge of the metal silicide, but also occurs from the metal silicide to a lightly doped drain (LDD) region and comer of the metal silicide adjacent to a shallow trench isolation (STI) structure. However, the conventional test structures cannot monitor these two mechanisms of leakage current. Therefore, the invention provides a test structure and a test method which can monitor the above-mentioned two mechanisms. The first embodiment illustrates a test structure for monitoring a leakage current caused by a self-aligned silicide layer on a metal-oxide semiconductor (MOS) transistor without a LDD region. The second embodiment illustrates a test structure for monitoring a leakage current caused by a self-aligned silicide on a metal-oxide semiconductor (MOS) transistor having a LDD region.




First Embodiment





FIG. 3

is a schematic, cross-sectional view of a metal-oxide semiconductor (MOS) transistor without a LDD structure. A device isolation structure


316


such as a shallow trench isolation structure is formed on a wafer


300


to define an active region. A well region is formed in the active region of the wafer


300


. A gate oxide layer


306


and a gate


308


are formed in the active region. With the gate


308


serving as a mask of an ion implantation, a diffusion region


302


is formed in the well region beside the gate


308


. The diffusion region


302


is also called a source/drain region. A self-aligned process is performed to form a metal silicide layer


304


on the diffusion region


302


. A portion of silicon in the diffusion region


302


is consumed because of the formation of the metal silicide layer


304


. Therefore, if the self-aligned process is not carefully controlled, the electrical quality of the diffusion region


302


is affected so as to easily generate a leakage current. A MOS transistor may fail due to serious leakage current.




This embodiment not only considers a leakage current (J


A


×A) occurring from the metal silicide layer to the junction and a leakage current (J


E


×L) occurring at the edge of the metal silicide layer, but also considers a leakage current (J


C


×C) occurring at the corner of the metal silicide layer adjacent to a shallow trench isolation structure. Thus, reliability of a self-aligned process can be more accurately controlled. Accordingly, a total current (J) is expressed as:






J=J


A


×A+J


E


×L+J


C


×C.






J


A


is an area current density, A is an area of the metal silicide layer, J


E


is an edge current density, L is an edge perimeter of the metal silicide layer, J


C


is a corner current density, and C is comer number of the metal silicide layer adjacent to the shallow trench isolation structure. When the condition of a self-aligned silicide process is fixed, then J


A


, J


E


, and J


C


are fixed. Therefore, different total currents J can be obtained through changing conditions A, L, and C so that three liner equations are obtained to obtain a set of values for J


A


, J


E


, and J


C


. Reliability of a self-aligned process can be rectified by J


A


, J


E


, and J


C


.





FIG. 4

,

FIG. 5

, and

FIG. 6

respectively show three different test structures which are deposited in scribe lines of a wafer to monitor a self-aligned silicide process. The test structure includes a diffusion region


302


and a metal silicide layer


304


thereon. the diffusion region


302


is electrically isolated by a device isolation structure


316


such is a shallow trench isolation structure. A, L, and C of the test structures in

FIG. 4

, FIG.


5


and

FIG. 6

can be obtained through calculation. In the test structure in

FIG. 4

, the area of a metal silicide layer A


1


, the edge perimeter L


1


, and the comer number C


1


, are obtained through calculation, and then the total current J


1


is obtained through an electricity measurement. In the test structure in

FIG. 5

, the area of a metal silicide layer A


2


, the edge perimeter L


2


, and the comer number C


2


are obtained through calculation, then the total current J


2


is obtained through an electricity measurement. In the test structure in

FIG. 6

, the area of a metal silicide layer A


3


, the edge perimeter L


3


, and the comer number C


3


are obtained through calculation, and then the total current J


3


is obtained through electricity measurement. Accordingly, three linear equations are expressed as follows:






J


1


=J


A


×A


1


+J


E


×L


1


+J


C


×C


1










J


2


=J


A


×A


2


+J


E


×L


2


+J


C


×C


2










J


3


=J


A


×A


3


+J


E


×L


3


+J


C


×C


3








Thus, one set of values for J


A


, J


E


and J


C


can be obtained. The degree of and the reason for a leakage current can be judged according to J


A


, J


E


, and J


C


. Thus, problems can be immediately discovered, and then immediately resolved.




In the above-mentioned test structure, the area of the metal silicide layer (A


1


, A


2


, or A


3


) is generally larger than the edge perimeter (L


1


, L


2


, or L


3


) and the comer number (C


1


, C


2


, or C


3


). Moreover, the orders of J


A


, J


E


, and J


C


are commonly closed. Therefore, for the total current, contribution of the leakage current (J


A


×A


1


, J


A


×A


2


, or J


A


×A


3


) occurring from the metal silicide layer to the junction is larger than that of the leakage current (J


E


×L


1


, J


E


×L


2


, or J


E


×L


3


) occurring at the edge of the metal silicide layer and that of the leakage current (J


C×C




1


, J


C


×C


2


, or J


C


×C


3


) occurring at the comer of the metal silicide layer. For the consideration of electricity measurement, the area of the metal silicide layer in

FIG. 4

, FIG.


5


and

FIG. 6

is commonly fixed to lower error when measuring the leakage current occurring at the edge of the metal silicide layer and the leakage current occurring at the corner of the metal silicide layer. Thus, accuracy of test results can be enhanced.




Second Embodiment





FIG. 7

is a schematic, cross-sectional view of a metal-oxide semiconductor transistor having a lightly doped drain (LDD) structure. A device isolation structure


716


such as a shallow trench isolation structure is formed on a wafer


700


to define an active region. A well region is formed in the active region of the wafer


700


. A gate oxide layer


706


and a gate


708


are formed in the active region. With the gate


708


serving as a mask, a first lightly doped ion implantation is performed. A spacer


712


is formed on a sidewall of the gate


708


. With the gate


708


and the spacer


712


serving as a mask, a second ion implantation is performed to form a diffusion region


702


in the well region of the wafer


700


. The diffusion region


702


is so-called a source/drain region having a LDD structure. A self-aligned process is performed to form a metal silicide layer


704


on the diffusion region


702


and a metal silicide layer


710


on the gate


708


. A portion of silicon of the diffusion region


702


is consumed because of the formation of the metal silicide


704


. Therefore, if the self-aligned process is not well controlled, electricity quality of the diffusion region


702


is affected so as to easily lead to a leakage current. A MOS transistor may fail due to a serious leakage current.




This embodiment not only considers a leakage current (J


A


×A) occurring from the metal silicide layer to the junction and a leakage current (J


isolation,L


×L


isolation


) occurring at the edge of the metal silicide layer, but also considers a leakage current (J


LDD,L


×L


LDD


) occurring from the metal silicide layer to the LDD region, that is, the region denoted as


720


in FIG.


7


. Accordingly, a total current (J) is expressed as:






J=J


A


×A+J


isolation,L


×L


isolation


+J


LDD,L


×L


LDD








where J


A


is an area current density, A is an area of the metal silicide layer, J


isolation,L


is an interface current density between the metal silicide layer and the device isolation structure, L


isolation


is the interface perimeter between the metal silicide layer and the device isolation structure, J


LDD,L


is a current density from the metal silicide layer to the LDD region, and L


LDD


is the length of the LDD region. When the condition of a self-aligned silicide process is fixed, then J


A


, J


isolation,L


, and J


LDD,L


are fixed. Therefore, different total currents J can be obtained through changing conditions A, L


isolation


, and L


LDD


so that three liner equations are obtained to obtain a set of values for J


A


, J


isolation,L


, and J


LDD,L


. Reliability of a self-aligned process can be judged by judging J


A


, J


isolation,L


, and J


LDD,L


.





FIG. 8

,

FIG. 9

, and

FIG. 10

respectively show three different test structures which are deposited in scribe lines of a wafer to monitor a self-aligned silicide process. The test structure includes a diffusion region


702


and a metal silicide layer


704


thereon wherein at least one of the three test structures has a diffusion region


702


with a LDD structure, as shown in FIG.


10


. The diffusion region


716


is electrically isolated by a device isolation structure


316


such as a shallow trench isolation structure. A, L


isolation


, and L


LDD


of the test structures in

FIG. 8

, FIG.


9


and

FIG. 10

can be obtained through calculation. In the test structure in

FIG. 8

, the area of a metal silicide layer A


1


, the interface perimeter between the metal silicide layer and the device isolation structure L


isolation1


, and the length of the LDD region L


LDD1


are obtained by calculation, then the total current J


1


is obtained through electricity measurement. In the test structure in

FIG. 9

, the area of a metal silicide layer A


2


, the interface perimeter between the metal silicide layer and the device isolation structure L


isolation2


, and the length of the LDD region L


LDD 2


are obtained by calculation, and then the total current J


2


is obtained through electricity measurement. In the test structure in

FIG. 10

, the area of a metal silicide layer A


3


, the interface perimeter between the metal silicide layer and the device isolation structure L


isolation3


, and the length of the LDD region L


LDD3


are obtained by calculation, and then the total current J


3


is obtained through electricity measurement. Accordingly, three linear equations are expressed as follows:






J


1


=J


A


×A


1


+J


isolation,L


×L


isolation1


+J


LDD,L


×L


LDD 1










J


2


=J


A


×A


2


+J


isolation,L


×L


isolation2


+J


LDD,L


×L


LDD 2










J


3


=J


A


×A


3


+J


isolation,L


×L


isolation3


+J


LDD,L


×L


LDD 3








Thus, one set of J


A


, J


isolation,L


, and J


LDD,L


values can be obtained. The degree of and the reason for a leakage current are judged according to J


A


, J


isolation,L


, and J


LDD,L


. Thus, problems can be immediately discovered, and then immediately resolved.




In the above-mentioned test structure, for the total current, the contribution of the leakage current (J


A


×A


1


, J


A


×A


2


, or J


A


×A


3


) occurring from the metal silicide layer to the junction is larger than that of the leakage current (J


isolation,L


×L


isolation1


, J


isolation,L


×L


isolation2


, or J


isolalion,L


×L


isolation3


) occurring at the interface between the metal and that of the leakage current (J


LDD,L


×L


LDD1


, J


LDD,L


×L


LDD2


, or J


LDD,L


×L


LDD3


) occurring from the metal silicide layer to the LDD region. For the consideration of electricity measurement, the area of the metal silicide layer in

FIG. 8

, FIG.


9


and

FIG. 10

is commonly fixed to lower error of measuring the leakage current occurring at the interface between the metal silicide layer and the device isolation structure. Thus, accuracy of test results can be enhanced.




In addition to the test structures in

FIG. 8

, FIG.


9


and

FIG. 10

, another test structure can be deposited in the scribe line, as shown in FIG.


11


. The test structure in

FIG. 11

mainly increases the comer number of the metal silicide layer adjacent to the shallow trench isolation structure. In

FIG. 11

, through calculation, the area of the metal silicide layer, A


4


, the perimeter of the interface between the metal silicide layer and the device isolation structure, L


isolation4


, and length of the LDD region, L


LDD4


can be obtained. J


A


, J


isolation,L


, and J


LDD,L


obtained from the test structures in

FIG. 8

,

FIG. 9

, and

FIG. 10

are substituted into the equation for the total current, then an ideal total current J


ideal


is obtained as followed:






J


ideal


=J


A


×A


4


+J


isolation,L


×L


isolation4


+J


LDD,L


×L


LDD,4








In addition, the actual total current is J


4


through electricity measurement. Compared with the actual total current J


4


and the ideal total current J


ideal


, in the case where the difference between J


4


and J


ideal


is in an allowable range, the leakage current occurring at the comer of the metal silicide layer is in an allowable range, or no leakage current occurs. In the case that the difference between J


4


and J


ideal


is too large, the self-aligned silicide process has to be adjusted.




In general, the area of the metal silicide layer in

FIG. 11

is the same as the areas in

FIG. 8

, FIG.


9


and

FIG. 10

to enhance accuracy of the test result.




Accordingly, advantages of the invention are as followed:




(1) While monitoring a self-aligned silicide process of a metal-oxide semiconductor transistor without a LDD structure, in addition to considering a leakage current occurring from a metal silicide layer to the junction and a leakage current occurring at the edge of the metal silicide layer in a conventional method, the invention further takes a leakage current occurring at a corner of a metal silicide layer into consideration. Thus, reliability of a self-aligned silicide process can be accurately controlled. The self-aligned silicide process can be immediately rectified to reduce probability of nullified wafers, further enhancing device reliability.




(2) While monitoring a self-aligned silicide process of a metal-oxide semiconductor transistor having a LDD structure, in addition to considering a leakage current occurring from a metal silicide layer to the junction and a leakage current occurring at the edge of the metal silicide layer in a conventional method, the invention further takes a leakage current occurring from a metal silicide layer to the LDD region into consideration. Thus, reliability of a self-aligned silicide process can be accurately controlled. The self-aligned silicide process can be immediately rectified to reduce probability of nullified wafers, further enhancing device reliability.




(3) While monitoring a self-aligned silicide process of a metal-oxide semiconductor transistor having a LDD structure, the invention further takes a leakage current occurring from a metal silicide layer to the LDD region into consideration. In order to avoid a failure to detect a serious leakage current occurring at corner of the metal silicide adjacent to a shallow trench isolation structure, another test structure is added as a check. The feature of the test structure is to increase the comer number of a metal silicide layer adjacent to a shallow trench isolation structure.




It will be apparent to those skilled in the art that various modifications and variations can be made to the structure of the present invention without departing from the scope or spirit of the invention. In view of the foregoing, it is intended that the present invention cover modifications and variations of this invention provided they fall within the scope of the following claims and their equivalents.



Claims
  • 1. A method of testing a leakage current caused by a self-aligned silicide process, suitable for monitoring the self-aligned silicide process performed on a metal-oxide semiconductor transistor having no lightly doped drain (LDD) structure, the method comprising:considering parameters for monitoring the self-aligned silicide process, the parameters comprising an area current density (JA), an edge current density (JE), and a corner current density (JC), a total current (J) of the metal silicide layer being calculated from an equation as follows: J=JA×A+JE×L+JC×C,  wherein A is an area of the metal silicide layer, L is an edge perimeter of the metal silicide layer, and C is a corner number for the metal silicide layer; depositing at least three test structures comprising a first test structure, a second test structure, and a third test structure on a wafer, the first test structure, the second test structure and the third test structure respectively comprising a first, a second and a third diffusion regions and a first, a second, and a third metal silicide layer on the first, the second, the third diffusion regions, the first, the second and the third diffusion regions being respectively surrounded by a first, a second, and a third isolation structures, wherein an area of the first metal silicide layer of the first test structure is A1, its edge perimeter is L1, its corner number is C1, an area of the second metal silicide layer of the second test structure is A2, its edge perimeter is L2, its corner number is C2, and an area of the third metal silicide layer of the third test structure is A3, its edge perimeter is L3, its corner number is C3; measuring electricity of the first test structure, the second test structure, and the third test structure to respectively obtain total currents J1, J2, and J3, and then substituting these values into a total current equation to obtain three linear equations: J1=JA×A1+JE×L1+JC×C1, J2=JA×A2+JE×L2+JC×C2, and J3=JA×A3+JE×L3+JC×C3,  which three linear equations are then used to obtain a set of values for JA, JE, and JC; and monitoring the self-aligned silicide process according to the set of values for JA, JE, and JC.
  • 2. The method according to claim 1, wherein the first test structure, the second test structure, the third test structure are deposited in a scribe line.
  • 3. The method according to claim 1, wherein the first isolation structure, the second isolation structure, and the third isolation structure include shallow trench isolation structures.
  • 4. The method according to claim 1, the method further including fixing the area of the first metal silicide layer A1, the area of the second metal silicide layer A2, and the area of the third metal silicide layer A3.
  • 5. A method of testing a leakage current caused by a self-aligned silicide process, suitable for monitoring the self-aligned silicide process performed on a metal-oxide semiconductor transistor having a lightly doped drain (LDD) structure, the method comprising:considering parameters for monitoring the self-aligned silicide process, the parameters comprising an area current density (JA), an interface current density (Jisolation,L) between the metal silicide layer and a device isolation structure, and a current density (JLDD,L) from the metal silicide layer to the LDD region, a total current (J) of the metal silicide layer being calculated from an equation as follows: J=JA×A+Jisolation,L×Lisolation+JLDD,L×LLDD,  wherein A is an area of the metal silicide layer, Lisolation is an interface perimeter between the metal silicide layer and the device isolation structure, and LLDD is a length of the LDD region; depositing at least three test structures comprising a first test structure, a second test structure, and a third test structure on a wafer, the first test structure, the second test structure and the third test structure respectively comprising a first, a second and a third diffusion regions and a first, a second, and a third metal silicide layers respectively on the first, the second, and the third diffusion regions, the first, the second and the third diffusion regions being electrically isolated by a first, a second, and a third isolation structures, at least one of the first, the second, the third diffusion regions having the LDD region, wherein an area of the first metal silicide layer of the first test structure is A1, an interface perimeter between the first metal silicide layer and the first device isolation structure is Lisolation1, a length of the LDD region is LLDD1, an area of the second metal silicide layer of the second test structure is A2, an interface perimeter between the second metal silicide layer and the second device isolation structure is Lisolation2, a length of the LDD region is LLDD2, an area of the third metal silicide layer of the third test structure is A3, an interface perimeter between the third metal silicide layer and the third device isolation structure is Lisolation3, and a path of the LDD region is LLDD3; measuring electricity of the first test structure, the second test structure, and the third test structure to respectively obtain total currents J1, J2, and J3, and substituting these into a total current equation to obtain three linear equations: J1=JA×A1+Jisolation,L×Lisolation1+JLDD,L×LLDD1, J2=JA×A2+Jisolation,L×Lisolation2+JLDD,L×LLDD2, and J3=JA×A3+Jisolation,L×Lisolation3+JLDD,L×LLDD3,  which three linear equations are then used to obtain a set of values for JA, Jisolation,L, and JLDD,L; and monitoring the self-aligned silicide process according to the set of values for JA, JisolationL,, and JLDD,L.
  • 6. The method according to claim 5, wherein the first test structure, the second test structure, the third test structure are deposited in a scribe line.
  • 7. The method according to claim 5, wherein the first isolation structure, the second isolation structure, and the third isolation structure include shallow trench isolation structures.
  • 8. The method according to claim 5, the method further comprising fixing the area of the first metal silicide layer A1, the area of the second metal silicide layer A2, and the area of the third metal silicide layer A3.
  • 9. The method according to claim 5, the method further comprising:depositing a fourth test structure on the wafer, the fourth test structure comprising a fourth diffusion region and a fourth metal silicide layer on the fourth diffusion region, the fourth diffusion region having the LDD structure, the fourth diffusion region being electrically isolated by a fourth isolation structure, wherein area of the fourth metal silicide layer of the fourth test structure is A4, an interface perimeter between the fourth metal silicide layer and the fourth device isolation structure is Lisolation4, a length of the LDD region is LLDD4, wherein the fourth test structure mainly increases a corner number of the fourth metal silicide layer adjacent to the fourth isolation structure; substituting A4, Lisolation4, LLDD4, and the set of values for JA, Jisolation,L, and JLDD,L into an equation for the total current to obtain an ideal total current Jideal; and measuring electricity of the fourth test structure to obtain an actual total current J4; and monitoring the self-aligned silicide process by comparing the actual total current J4 with the ideal total current Jideal.
  • 10. The method according to claim 9, wherein the first test structure, the second test structure, the third test structure, and the fourth test structure are deposited in a scribe line.
  • 11. The method according to claim 9, wherein the first isolation structure, the second isolation structure, the third isolation structure, and the fourth isolation structure include shallow trench isolation structures.
  • 12. The method according to claim 9, the method further including fixing the area of the first metal silicide layer A1, the area of the second metal silicide layer A2, the area of the third metal silicide layer A3, and the area of the fourth metal silicide layer A4.
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Number Name Date Kind
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4588946 Lin May 1986
5420520 Anschel et al. May 1995
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6043102 Fang et al. Mar 2000