Using localized ionizer to reduce electrostatic charge from...

Electricity: electrical systems and devices – Electric charge generating or conducting means

Reexamination Certificate

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C361S225000, C361S220000, C361S212000

Reexamination Certificate

active

06507474

ABSTRACT:

TECHNICAL FIELD
The present invention generally relates to improved lithography processing by using a feedback system to screen and treat structures with electrostatic charges. In particular, the present invention relates to determining if electrostatic charges on developed photoresists and masks exist, and if so, reducing electrostatic charges on developed photoresists and masks using an ionizer.
BACKGROUND ART
Microlithography processes for making miniaturized electronic components, such as in the fabrication of computer chips and integrated circuits, involve using photoresists and masks. Generally, a coating or film of a photoresist is applied to a substrate material, such as a silicon wafer used for making integrated circuits. The substrate may contain any number of layers or devices thereon.
The photoresist coated substrate is baked to evaporate any solvent in the photoresist composition and to fix the photoresist coating onto the substrate. The baked coated surface of the substrate is next subjected to selective radiation; that is, an image-wise exposure to radiation. This radiation exposure causes a chemical transformation in the exposed areas of the photoresist coated surface. After selective exposure, the photoresist coated substrate is treated with a developer solution to dissolve and remove either the radiation-exposed or the unexposed areas of the photoresist (depending upon whether a positive photoresist or a negative photoresist is utilized) resulting in a patterned or developed photoresist. Many developer solutions contain water and a base, such as water and a hydroxide compound.
Treating a selectively exposed photoresist with a developer conventionally involves depositing the liquid developer solution over the photoresist clad substrate and spinning the substrate whereby the liquid developer solution and dissolved areas of the photoresist are removed from the substrate by centrifugal forces. A rinsing solution, typically water, is then deposited over the photoresist clad substrate and the substrate is spun again to remove the water and any debris solubilized by the water. Spinning the substrate is a convenient and inexpensive method of removing materials from substrate. However, electrostatic charges build up on the developed photoresist during the development and water rinse cycles.
Negative charges are particularly encountered on developed photoresists, notwithstanding whether the photoresist is patterned over a wafer or a mask. While the causes of this phenomenon are not completely understood, it is believed that electrostatic charges and/or resist developer and/or deionized water rinse contribute to charge accumulation. Charge accumulation on developed photoresists can be as high as 300-400 volts, and it is typically negative. Electrostatic charges also build up on the developed photoresist that are evaluated using a scanning electron microscope (SEM) or an atomic force microscope (AFM).
Negative charge accumulation on a developed photoresist presents a number of problems. One notable problem is that measurement of various resist features, such as linewidth and profiling, is rendered inaccurate. Especially when using a SEM or an AFM, it is difficult to obtain accurate data. This is because SEMs and AFMs use an electron beam for generating images (both in projection and detection). The electron beam from the SEM or AFM may be repulsed by the negative charge accumulated on the photoresist or mask. The degree of repulsion or deviation from an ideal direction is dependent upon the magnitude of the accumulated negative charge.
Another aspect of this problem is that secondary electrons emitted from the surface of the features under measurement (such as the patterned photoresist) are reduced due to negative charge accumulation. As a result, the secondary electron signal received at the detector does not represent the correct signal (as in instances where electrostatic charges do not exist on the patterned photoresist). Hence, in the case of a linewidth measurement having a developed photoresist with negative charge accumulation thereon, the SEM does not accurately measure the width because the secondary electron signal is reduced.
This phenomenon is shown in
FIGS. 1 and 2
. Referring to
FIG. 1
, SEM
10
emits an electron beam (represented by the arrow(s)) from tip
11
towards a developed photoresist structure
12
on semiconductor substrate
14
. The developed photoresist structure
12
has an accumulation of negative charge
16
as a result of the lithography process. Due to repulsion between the electron beam and the negative charge
16
of the developed photoresist structure
12
, the electron beam path is altered away from the developed photoresist structure
12
without having reflected off or contacting the developed photoresist structure
12
. Since the electron beam does not reflect off of the developed photoresist structure
12
, an accurate measure/profile of the structure cannot be obtained. Detection of the altered electron beams by detector
18
of SEM
10
provides data indicating at least one of inaccurate linewidth, fuzzy corner definition, and otherwise non-focused images. Assessment of the quality and parameters of a lithography process is consequently difficult or inaccurate and often impossible.
Referring to
FIG. 2
, SEM
10
emits an electron beam (represented by the arrow(s)) from tip
11
towards a developed photoresist structure
12
on semiconductor substrate
14
. The developed photoresist structure
12
has an accumulation of negative charge
16
as a result of the lithography process and/or repeated use as a standard. Due to the negative charge
16
of the developed photoresist structure
12
, the secondary electron signal is reduced; that is, the accumulation of negative charges
16
interferes with the ability of the electron beam to neatly reflect off of and be received by detector
18
of SEM
10
.
This is especially true with regard to measuring linewidth and with using photoresists sensitive to small wavelengths of light. Photoresists sensitive to relatively small wavelengths of light are typically formed or developed into finer patterns (e.g., smaller linewidths) compared to photoresists sensitive to relatively large wavelengths of light. Linewidth measurements taken on undesirably charged photoresists often yield parameters in error, sometimes by an order of magnitude. For example, an SEM scanning an undesirably charged photoresist having a linewidth of 0.20 &mgr;m may incorrectly indicate that the linewidth is 0.24 &mgr;m. This is primarily due to charge induced deviation of the electron beam used to measure the linewidth. Such errors cannot be tolerated because they lead to fatal construction errors in subsequent processing.
Referring to
FIG. 3
, the critical dimension data graph of the developed photoresist of
FIG. 1
using an SEM is shown by the solid line. An accurate measurement of the developed photoresist of
FIG. 1
should yield the dashed line of
FIG. 3
, but due to undesirable charge accumulation, the apparent critical dimension is inaccurately wide. Accurate critical dimension measurements are desired.
SUMMARY OF THE INVENTION
The present invention provides improved methods and systems for evaluating a lithography process using an ionizer. The present invention also provides methods for minimizing charge accumulation and/or dissipating charge accumulation on a patterned photoresist, whether or not the photoresist is patterned over a wafer or a mask, using a feedback system wherein charge accumulation is addressed if detected. As a result of the present invention, evaluation of a patterned photoresist, such as linewidth measurement, profile data, corner sharpness, critical dimension determinations, and image inspection, is substantially improved. Subsequent processing of semiconductor substrates after lithography is accordingly improved.
One aspect of the present invention relates to a method of reducing electrostatic charges on a patterned photoresist to improve evaluation of the developed photoresist, invol

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