The disclosure of Japanese Patent Application No. 2011-6699 filed on Jan. 17, 2011 including the specification, drawings and abstract is incorporated herein by reference in its entirety.
The present invention relates to a method of manufacturing a semiconductor device and a semiconductor device.
In a semiconductor device, an insulation performance required for an insulating film may disappear due to time degradation of the insulating film. The characteristics of a semiconductor device regarding such degradation of insulation performance are called TDDB (Time Dependent Dielectric Breakdown) characteristics.
On the other hand, Japanese Unexamined Patent Application Publication No. 2009-10135 discloses TEG for measuring an influence of the distance between a contact of source/drain of a transistor and the gate electrode of the transistor, which affects DC characteristics of the transistor.
In recent years, miniaturization of semiconductor devices advances, and the distance between a contact of source/drain of a transistor and the gate electrode of the transistor becomes small. Therefore, it becomes necessary to evaluate the TDDB characteristics of an insulating film located between the contact and the gate electrode. The TDDB characteristics are largely affected by the distance between the contact and the gate electrode. However, the distance between the contact and the gate electrode could not be measured efficiently so far.
According to one aspect of the present invention, there is provided a method of manufacturing a semiconductor device, which includes the steps of preparing a semiconductor device including a first contact and a first gate electrode located adjacent to the first contact, measuring a first leakage current generated between the first contact and the first gate electrode, obtaining conversion data indicating a correlation between a distance between a contact coupled to an impurity layer that is a source or a drain of a transistor and a gate electrode of the transistor and a magnitude of a leakage current generated between the contact and the gate electrode, and calculating a distance between the first contact and the first gate electrode by using the first leakage current and the conversion data.
The inventors found that a magnitude of leakage current generated between the contact and the gate electrode has a correlation with the distance between the contact and the gate electrode, so that the inventors invented the above-described invention. In the present invention, a measurement result of the first leakage current is converted into the distance between the first contact and the first gate electrode by using the conversion data. Therefore, the measurement efficiency can be higher than that in a case in which the actual distance between the first contact and the first gate electrode is measured.
According to another aspect of the present invention, there is provided a method of manufacturing a semiconductor device, which includes the steps of preparing a semiconductor device including a TEG having a first contact, a first gate electrode located adjacent to the first contact, and a transistor, measuring a first leakage current generated between the first contact and the first gate electrode, obtaining conversion data indicating a correlation between a TDDB life between a contact coupled to an impurity layer that is a source or a drain of a transistor and a gate electrode of the transistor and a magnitude of a leakage current generated between the contact and the gate electrode, and calculating the TDDB life between the contact and the gate electrode of the transistor by using the first leakage current and the conversion data.
According to still another aspect of the present invention, there is provided a semiconductor device, which includes a substrate, an insulating film formed over a surface of the substrate, and a TEG formed over the insulating film, and in which the TEG includes first gate electrode located over the insulating film, a first contact which is located over the insulating film and located adjacent to the first gate electrode, a first electrode pad coupled to the first contact, and a second electrode pad coupled to the first gate electrode.
According to the aspects of the present invention, the distance between the contact and the gate electrode can be measured efficiently.
Hereinafter, embodiments of the present invention will be described. In all the drawings, the same constituent elements are given the same reference numerals and the description thereof will be appropriately omitted.
In the present embodiment, the first gate electrode 310 and the first contact 320 form a TEG 300. The TEG 300 is a TEG for measuring a positional shift between the first gate electrode 310 and the first contact 320 (mask superposition error).
Specifically, conversion data indicating a correlation between the distance between the first gate electrode 310 and the first contact 320 and a magnitude of a leakage current amount is prepared in advance. The leakage current amount between the first gate electrode 310 and the first contact 320 is measured, and the measured leakage current amount is converted into the distance between the first gate electrode 310 and the first contact 320 by using the conversion data. Then, a superposition error between an exposure process for forming the first gate electrode 310 and an exposure process for forming the first contact 320 can be measured from a difference between the measured value of the distance between the first gate electrode 310 and the first contact 320 and a design value of the distance. Hereinafter, the details will be described.
First, the configuration of the semiconductor device will be described. In the semiconductor device, the TEG 300 is disposed in a scribe area 20. The scribe area 20 is located between multiple chip areas 10, which will be semiconductor chips. A dicing blade 50 (see
In the present embodiment, the TEG 300 is located on the element separating film 102. Thereby, a current flowing between the first gate electrode 310 and the first contact 320 can be assumed to be a leakage current generated between the first gate electrode 310 and the first contact 320. However, the TEG 300 may not have to be located on an insulating film such as the element separating film 102 depending on a correction method. The first contact 320 is buried in an interlayer insulating film 200 formed on the substrate 100.
A gate insulating film 312 is formed between the first gate electrode 310 of the TEG 300 and the element separating film 102. A side wall 330 is formed on a side surface of the first gate electrode 310.
In the chip area 10, a transistor 110 (not shown in
As shown in
However, as shown in
The relationship between the distance between the first gate electrode 310 and the first contact 320 and the magnitude of leakage current generated between the first gate electrode 310 and the first contact 320 varies depending on the configuration of the semiconductor device, such as material of the first gate electrode 310, material of the first contact 320, shape of the first gate electrode 310, shape of the first contact 320, structure of the side wall 330, and material of the interlayer insulating film 200. Therefore, actually, the conversion data shown in
The formula (1) described below which represents Schottky emission or Poole-Frenkel current can be applied to the magnitude of the leakage current generated between the first gate electrode 310 and the first contact 320.
The phenomenon shown in
Here, β is a geometry parameter of the Weibull distribution and η is a scale parameter (characteristic life) of the Weibull distribution. When the distance between the contact and the gate electrode varies due to the superposition error and an applied electric field intensity E varies, cumulative failure probability varies through electric field acceleration of the scale parameter η=η(E). The cumulative failure probability in actual use is estimated by the formula (2). For the TDDB of a silicon oxide film and the TDDB of a low-k film, a power-law model represented by the formula (3) and a √E model represented by the formula (4) are proposed as an electric field acceleration model. ([Related Art Document 1] E. Wu, et al., IEEE Tran. Electron Devices, vol. 49, p. 2244 (2002), [Related Art Document 2] F. Chen, et al., IRPS 2006, p. 46)
Here, V is an applied voltage and s is the distance between the contact and the gate. Further, n is an exponent of an electric field acceleration term in the power law model and γ is an electric field acceleration coefficient in the √E model. If these models are applied, it is possible to estimate variation of a life distribution when the distance s varies due to the superposition error.
Next, a first example of a method of manufacturing the semiconductor device will be described with reference to a flowchart in
Specifically, first, the element separating film 102 is formed on the substrate 100. Next, the gate insulating film 111 and the gate insulating film 312 are formed, and further, the gate electrode 112 and the first gate electrode 310 are formed. At this time, the gate insulating film 111 and the gate insulating film 312 are formed in the same process, and the gate electrode 112 and the first gate electrode 310 are formed in the same process. In other words, the gate insulating film 111 and the gate insulating film 312 are formed to the same thickness by the same material, and the gate electrode 112 and the first gate electrode 310 are formed to the same thickness by the same material.
Next, impurities are injected into the substrate 100 by using the element separating film 102 as a mask. Thereby, the extension area 116 of the transistor 110 is formed. Next, the side wall 114 and the side wall 330 are formed. The side wall 114 and the side wall 330 are also formed in the same process. Next, impurities are injected into the substrate 100 by using the element separating film 102 and the side wall 114 as a mask. Thereby, the impurity layer 116 is formed.
In this way, the transistor 110 and the first gate electrode 310 of the TEG 300 are formed. Next, the interlayer insulating film 200 is formed on the transistor 110 and the first gate electrode 310, and the second contact 210 and the first contact 320 are buried into the interlayer insulating film 200. The second contact 210 and the first contact 320 are formed in the same process and have at least the same shape of upper ends.
Thereafter, a required number of wiring layers are formed on the interlayer insulating film 200, the second contact 210, and the first contact 320. At this time, the electrode pads 12, 332, and 334 are formed on the uppermost wiring layer. Next, a protective insulating layer is formed on the multiple wiring layers. The protective insulating layer has openings for exposing the electrode pads.
In this way, semiconductor devices before being separated into individual chips are formed. Next, inspection of the semiconductor device is performed (steps S20 to S60).
Specifically, first, the inspection apparatus reads the conversion data corresponding to the semiconductor device to be inspected and sets the conversion data (step S20). Next, the inspection apparatus causes probe needles to come into contact with the first electrode pad 332 and the second electrode pad 334, applies a predetermined voltage between the electrode pads, and measures a current (leakage current) flowing between the first electrode pad 332 and the second electrode pad 334 (step S30).
Next, the inspection apparatus calculates the distance between the first gate electrode 310 and the first contact 320 by using the conversion data read in step S20 and the leakage current measured in step S30. Next, the inspection apparatus calculates the superposition error between the first gate electrode 310 and the first contact 320 on the basis of the calculated distance. Next, the inspection apparatus calculates the distance between the gate electrode 112 and the second contact 210 by using the superposition error (step S40). If the design value of the distance between the first gate electrode 310 and the first contact 320 is the same as the design value of the distance between the gate electrode 112 and the second contact 210, the distance between the first gate electrode 310 and the first contact 320 can be assumes to be the distance between the gate electrode 112 and the second contact 210 without change.
Next, the inspection apparatus calculates the electric field intensity between the gate electrode 112 and the second contact 210 by using the distance between the gate electrode 112 and the second contact 210 and a design value of the voltage applied between the gate electrode 112 and the second contact 210 (step S50). Next, the inspection apparatus calculates the TDDB life of the semiconductor device by using the electric field intensity between the gate electrode 112 and the second contact 210 and the data shown in
Thereafter, the semiconductor devices are diced into individual chips.
Next, the functions and effects of the present embodiment will be described. According to the present embodiment, the leakage current amount between the first gate electrode 310 and the first contact 320 is measured. The leakage current amount is converted into the distance between the first gate electrode 310 and the first contact 320 by using the conversion data. Therefore, the efficiency of the measurement of the distance between the first gate electrode 310 and the first contact 320 can be improved.
Thereby, the TDDB life between the gate electrode 112 and the second contact 210 of the semiconductor device can be efficiently calculated. Therefore, a defective semiconductor device can be efficiently detected.
In the semiconductor device according to the present embodiment, the process shown in
In the semiconductor device according to the present embodiment, the process shown in
In the semiconductor device according to the present embodiment, the process shown in
In the semiconductor device according to the present embodiment, the process shown in
In the present embodiment, the process shown in
A superposition error (dx, dy) at a point where the TEG group 303 is provided can be calculated. It is possible to calculate an in-plane distribution of superposition errors (for example, distribution in the chip area 10) by applying the superposition error to a linear interpolation model formula representing positional dependence of the superposition error. An example of such a model formula is the formula (5) (W. H. Arnold, SPIE 1988) described below.
dX=−(θs+θskew)Y+MXX+∈X
dY=θ
s
X+M
Y
Y+∈
Y (5)
Here, θs is a coefficient of rotation direction error, MX is a coefficient of magnification error in the horizontal direction, MY is a coefficient of magnification error in the vertical direction, and θskew is a coefficient of orthogonality error. The terms ∈X and ∈Y represent effects of residual nonlinear errors that cannot be represented by linear models in the horizontal and vertical directions.
In the present embodiment, the TEG 300 shown in
Also in the present embodiment, the same effects as those of the present embodiment can be obtained. In the method described with reference to
Specifically, multiple first contacts 320 included in one TEG 300 are located on the same side with respect to the first gate electrode 310, and the distances between the first contacts 320 and the first gate electrode 310 are the same. The first contacts 320 included in one TEG 300 are coupled to the same first electrode pad 332.
Also in the present embodiment, the same effects as those of the second embodiment can be obtained. The summation of leakage currents flowing between the first contacts 320 and the first gate electrode 310 flows between the first electrode pad 332 and the second electrode pad 334. Therefore, even when the leakage current amount per the first contact 320 is very small, it is possible to calculate the magnitude of the superposition error and the TDDB life at a high degree of accuracy.
Specifically, the first contacts 320 included in one TEG 300 are located on the same side with respect to the first gate electrode 310, and the distances between the first contacts 320 and the first gate electrode 310 are different from each other. The first contacts 320 included in one TEG 300 are respectively coupled to different first electrode pads 332.
Also in the present embodiment, the same effects as those of the second embodiment can be obtained. As described above, in the method described with reference to
Although the embodiments of the present invention have been described with reference to the drawings, these are examples of the present invention and a variety of configurations other than the above can be employed.
Number | Date | Country | Kind |
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2011-006699 | Jan 2011 | JP | national |