Source: http://www.patentgenius.com/patent/7705973.html
Timestamp: 2018-11-12 22:00:17
Document Index: 268974721

Matched Legal Cases: ['Application No. 10', 'art 310', 'art 320', 'art 310', 'art 320', 'art 310', 'art 320', 'art 310', 'art 320', 'art 310', 'art 320', 'art 320', 'art 310', 'art 310', 'art 320']

Methods and systems for monitoring state of plasma chamber - Patent # 7705973 - PatentGenius
7705973 Methods and systems for monitoring state of plasma chamber
Application: 12/151,516
Inventors: Bai; Keun-Hee (Suwon-si, KR)
Kim; Yong-Jin (Suwon-si, KR)
Attorney Or Agent: Milles & Onello, LLP
U.S. Class: 356/72; 356/316
Field Of Search: 356/72; 356/316
International Class: G01J 3/443; H05H 1/00
Foreign Patent Documents: 2002-168774; 2003-0073327; 10-2006-0009359; 10-2006-0123098; 10-2007-0028204; WO 2004/105101
Abstract: Provided are methods and systems for monitoring a state of a plasma chamber. In the method, an optical characteristic of plasma generated in a plasma chamber including a window is measured in a predetermined measurement wavelength band. A process status index (PSI) is extracted from the measured optical characteristic. A state of the plasma chamber is evaluated by analyzing the extracted PSI. The optical characteristic of the plasma is measured in the predetermined measurement wavelength band in which a transmittance of light passing through the window is substantially independent of a wavelength of the light.
1. A method of monitoring a plasma chamber, comprising: measuring an optical characteristic of plasma in a predetermined measurement wavelength band, the plasma beinggenerated in the plasma chamber including a window; extracting a process status index (PSI) from the measured optical characteristic; and evaluating a state of the plasma chamber by analyzing the extracted PSI, wherein the optical characteristic of theplasma is measured in the predetermined measurement wavelength band in which a transmittance of light passing through the window is substantially independent of a wavelength of the light.
2. The method of claim 1, wherein the optical characteristic of the plasma is measured in the predetermined measurement wavelength band in which a transmittance of light passing through the window varies in a range from about 1% to about 20%according to a wavelength of the light.
5. The method of claim 1, wherein the predetermined measurement wavelength band is a band in which a transmittance variation of light passing through the window is substantially independent of a thickness of a by-product deposited on thewindow.
6. The method of claim 1, wherein the extracting of the PSI comprises performing an inner product of data of the optical characteristic and wavelength-weight data, wherein the wavelength-weight data are obtained by principal component analysis(PCA) or multi-way principal component analysis (MPCA).
7. The method of claim 6, wherein the extracting of the PSI further comprises normalizing intensity values of light measured in the predetermined measurement wavelength band based on an intensity value of light measured at a predeterminedreference wavelength, prior to the performing of the inner product.
9. The method of claim 8, wherein the evaluating of the state of the plasma chamber further comprises transmitting a signal to an operator to inform the operator of a process error when a difference between the PSI and the PSI trend data isequal to or greater than a predetermined critical value.
10. The method of claim 9, wherein the evaluating of the state of the plasma chamber comprises disregarding a variation of the PSI caused by an intended process condition change by evaluating the variation of the PSI using condition-result dataproviding information about a relationship between process condition changes and variations of the PSI.
11. A system for monitoring a plasma chamber, comprising: a measurement unit configured to measure light emitted from the plasma chamber through a window of the plasma chamber in a predetermined measurement wavelength band; a process statusindex (PSI) extraction part configured to extract a PSI from an optical characteristic of the light; and a status decision part configured to evaluate a state of the plasma chamber by analyzing the extracted PSI, wherein the predetermined measurementwavelength band is a band in which a transmittance of light passing through the window is substantially independent of a wavelength of the light.
15. The system of claim 11, wherein the predetermined measurement wavelength band is a band in which a transmittance variation of light passing through the window is substantially independent of a thickness of a by-product deposited on thewindow.
16. The system of claim 11, wherein the PSI extraction part comprises a first processing part configured to convert intensity values of light measured in the predetermined measurement wavelength band into ratios to an intensity value of lightmeasured at a predetermined reference wavelength.
17. The system of claim 16, wherein the PSI extraction part further comprises a second processing unit configured to calculate an inner product of wavelength-weight data and intensity values of light measured in the measurement wavelength band,wherein the wavelength-weight data are data obtained by principal component analysis (PCA) or multi-way principal component analysis (MPCA) for assigning different weights to the measured intensity values according to wavelength.
19. The system of claim 18, further comprising a user interface configured to transmit a signal to an operator to inform the operator of a process error when a difference between the PSI and the PSI trend data is equal to or greater than apredetermined critical value.
20. The system of claim 19, wherein the status decision part is configured to disregard a variation of the PSI caused by an intended process condition change by evaluating the variation of the PSI using condition-result data providinginformation about a relationship between process condition changes and variations of the PSI.
This U.S. non-provisional patent application claims priority under 35 U.S.C. .sctn. 119 of Korean Patent Application No. 10-2007-0045570, filed on May 10, 2007, the entire contents of which are hereby incorporated by reference.
The present invention disclosed herein relates to plasma chamber systems and methods of operating the plasma chamber systems, and more particularly, to methods and systems for monitoring a state of a plasma chamber.
Plasma is used in etching, deposition, and sputtering processes for manufacturing semiconductors and liquid crystal displays (LCDs). More specifically, plasma is formed in a vacuum chamber (i.e., a plasma chamber) using electricity supplied inthe form of a high-frequency voltage or current, and the above-mentioned processes are performed using the physical or chemical characteristics of ions of the plasma.
To satisfy certain technical demands related to integration level and performance, highly advanced techniques have been applied to the processes, resulting in changes to process conditions. However, the repeatability of the processes or productperformance can be largely affected by even a small variation in process condition, and therefore, it may be necessary to monitor variations of process conditions.
However, it can be difficult to evaluate the repeatability of a process by monitoring process conditions since various process conditions can affect the repeatability of the process. For example, process conditions, such as gas flow,unintentional fluctuation, chamber memory effect, arching, and plasma instability, can affect the repeatability of the process and product performance. It can be difficult to precisely measure all of such various process conditions. In addition, it canalso be difficult to predict changes of process outputs from the measurement results.
The state of a process in which plasma is used can be monitored based on the fact that the state of the process is sensitive to the state of the plasma. For example, an etch stop point can be determined by measuring variations in opticalcharacteristics of plasma. More specifically, when a lower layer disposed beneath an etch target layer is exposed while etching the etch target layer, gas ratios and pressure of a chamber vary, and thus the intensity of light emitted from plasma canvary at a specific wavelength. The etch stop point can be determined by monitoring variations of the intensity in the light emitted from the plasma. However, this method can be used to determine only the etch stop point since the method uses lighthaving a specific wavelength. That is, the repeatability of a process may not be properly evaluated by the method.
Embodiments of the present invention provide reliable methods of evaluating process conditions.
Embodiments of the present invention provide methods of monitoring a plasma chamber by measuring light in a wavelength band in which a transmittance of the light is substantially independent of a wavelength of the light. The methods includemeasuring an optical characteristic of plasma in a predetermined measurement wavelength band, the plasma being generated in a plasma chamber including a window; extracting a process status index (PSI) from the measured optical characteristic; andevaluating a state of the plasma chamber by analyzing the extracted PSI. The optical characteristic of the plasma may be measured in the predetermined measurement wavelength band in which a transmittance of light passing through the window issubstantially independent of a wavelength of the light.
In some embodiments, the optical characteristic of the plasma is measured in the predetermined measurement wavelength band in which a transmittance of light passing through the window varies in a range from about 1% to about 20% according to awavelength of the light. For example, the measuring of the optical characteristic includes measuring light emitted from the plasma chamber and having a wavelength in a range from about 900 nm to about 1700 nm.
In even other embodiments, the extracting of the PSI includes performing an inner product of data of the optical characteristic and wavelength-weight data. The wavelength-weight data may be obtained by principal component analysis (PCA) ormulti-way principal component analysis (MPCA). Prior to the performing of the inner product, the extracting of the PSI may further include normalizing intensity values of light measured in the predetermined measurement wavelength band based on anintensity value of light measured at a predetermined reference wavelength.
In yet other embodiments, the evaluating of the state of the plasma chamber includes comparing the PSI with PSI trend data providing information about a variation trend of the PSI with respect to time. The evaluating of the state of the plasmachamber may further include transmitting a signal to an operator to inform the operator of a process error when a difference between the PSI and the PSI trend data is equal to or greater than a predetermined critical value.
In further embodiments, the evaluating of the state of the plasma chamber includes disregarding a variation of the PSI caused by an intended process condition change by evaluating the variation of the PSI using condition-result data providinginformation about a relationship between process condition changes and variations of the PSI.
In other embodiments of the present invention, there are provided systems for monitoring a plasma chamber by analyzing light in a wavelength band in which a transmittance of the light is substantially independent of a wavelength of the light. The systems include: a measurement unit configured to measure light emitted from a plasma chamber through a window of the plasma chamber in a predetermined measurement wavelength band; a PSI extraction part configured to extract a PSI from an opticalcharacteristic of the light; and a status decision part configured to evaluate a state of the plasma chamber by analyzing the extracted PSI. The predetermined measurement wavelength band may be a band in which a transmittance of light passing throughthe window is substantially independent of a wavelength of the light.
In some embodiments, the predetermined measurement wavelength band is a band in which a transmittance of light passing through the window varies in a range from about 1% to about 20% according to a wavelength of the light. For example, thepredetermined measurement wavelength band may range from about 900 nm to about 1700 nm. Alternatively, the predetermined measurement wavelength band can range from about 600 nm to about 3000 nm.
In still other embodiments, the PSI extraction part includes a first processing part configured to convert intensity values of light measured in the predetermined measurement wavelength band into ratios to an intensity value of light measured ata predetermined reference wavelength. The PSI extraction part may further include a second processing unit configured to calculate an inner product of wavelength-weight data and intensity values of light measured in the measurement wavelength band,wherein the wavelength-weight data are data obtained by PCA or MPCA for assigning different weights to the measured intensity values according to wavelength.
In yet other embodiments, the system may further include a user interface configured to transmit a signal to an operator to inform the operator of a process error when a difference between the PSI and the PSI trend data is equal to or greaterthan a predetermined critical value.
In further embodiments, the status decision part is configured to disregard a variation of the PSI caused by an intended process condition change by evaluating the variation of the PSI using condition-result data providing information about arelationship between process condition changes and variations of the PSI.
Referring to FIG. 1, the monitoring system for monitoring a state of a plasma chamber includes a plasma chamber 100 in which plasma 99 is generated, a measurement unit 200 configured to measure optical characteristics of light PL emitted from theplasma chamber 100, and an analysis unit 300 detecting a state of the plasma chamber 100 using the measured optical characteristics of the light PL. The plasma 99 forms above a wafer chuck 110 on which a semiconductor substrate 120 is loaded. Themeasurement unit 200 receives light PL emitted from the plasma 99 through a window 130 formed in a sidewall of the plasma chamber 100. The window 130 can be formed of a transparent material such as quartz and sapphire.
As shown, the plasma chamber 100 can be used as an etching chamber for etching the semiconductor substrate 120, however, the present invention is not limited thereto. For example, the plasma chamber 100 can be used as a deposition or sputteringchamber. The use of the plasma chamber 100 is not limited to semiconductor manufacturing. The plasma chamber 100 can be used in various industrial fields such as in the liquid crystal display (LCD) manufacturing industry.
The analysis unit 300 may include a process status index (PSI) extraction part 310 and a status decision part 320. The PSI extraction part 310 extracts a PSI using optical characteristics of light measured by the measurement unit 200. Thestatus decision part 320 analyzes the PSI to detect a process state of the plasma chamber 100. The analysis unit 300 may further include a memory device 30. The memory device 30 stores PSI data and other various data used to detect the process state ofthe plasma chamber 100. The PSI extraction part 310 and the status decision part 320 can be hardware parts formed of electric circuits or software loaded in a computer. The PSI extraction part 310, the status decision part 320, and the memory device 30are electrically connected to each other for data transmission. A method of extracting PSI data using the PSI extraction part 310, and a method of detecting a process state of the plasma chamber 100 using the status decision part 320 will be describedin detail with reference to FIG. 2.
The monitoring system may further include a user interface 400 for alarming an operator when the status decision part 320 detects an error in the plasma chamber 100. The measurement unit 200 further includes an optical sensor that can detectlight transmitted through the window 130 in a specific wavelength band where the transmittance of the light is independent of its wavelength. Hereinafter, the specific wavelength band will be referred to as a measurement wavelength band.
In the measurement wavelength band, the transmittance of light PL passing through the window 130 may be independent of the wavelength of the light PL. For example, in the measurement wavelength band, the transmittance of the light PL passingthrough the window 130 may vary within a narrow range from about 1% to about 20% according to the wavelength of the light PL. Since the intensity of the light PL after passing through the window 130 is proportional to the transmittance of the light PLthrough the window 130, the intensity variation of the light PL and the transmittance variation of the light PL will be interchangeably used.
In operation S20, the spectrum data D10 are processed to obtain normalized spectrum data D20. Through the normalization, the spectrum data D10 are expressed as ratios to an intensity value of the light PL measured at a reference wavelength. Thenormalized spectrum data D20 can be stored in the memory device 30. Referring to FIG. 8, exemplary normalized spectrum data are shown. The PSI extraction part 310 can perform operation S20.
In operation S30, PSI data D30 corresponding to the measured optical characteristics are prepared by extracting a PSI from the normalized spectrum data D20. The PSI data D30 can be obtained by the inner product of the normalized spectrum dataD20 and predetermined weight data D25. The weight data D25 are data for assigning different weights to measured intensity values of the light PL according to the wavelength of the light PL. The weight data D25 can be prepared using a predeterminedstatistical method in operation S40. For example, the weight data D25 are prepared in a manner such that relatively large weights can be assigned to intensity values of the light PL measured at specific wavelengths that dominantly influence a process inthe plasma chamber 100. For this, the weight data D25 can be obtained by an analysis method such as principal component analysis (PCA) and multi-way principal component analysis (MPCA). The PSI extraction part 310 can perform operation S30.
In operation S50, the state of the plasma chamber 100 is analyzed using the PSI data D30. In operation S50, predetermined PSI trend data D40 and predetermined condition-result data D50 can be used to determine whether the state of the plasmachamber 100 deviates from a PSI trend. For example, if a variation between the PSI data D30 and the PSI trend data D40 is equal to or larger than a critical value, it can be determined that the process performed in the plasma chamber 100 is underconditions not guaranteeing process repeatability. In this case, in operation S60, a predetermined alarming signal can be generated using a predetermined user interface such as the user interface 400 to report generation of a process error.
The PSI trend data D40 can be obtained by accumulating sets of PSI data D30 derived from different measurement results. The condition-result data D50 can be empirical or theoretical data indicating a relationship between process conditionvariations and the PSI data D30. The condition-result data D50 are used to determine whether a difference between the PSI data D30 and the PSI trend data D40 is a result of a process condition variation.
More specifically, in operation S50, when it is analyzed and determined, using the condition-result data D50, that a difference between the PSI data D30 and the PSI trend data D40 is a result of a process condition variation, it is consideredthat the PSI data D30 has not deviated from a PSI trend. For example, in an etch process using oxygen, the condition-result data D50 can be empirical data indicating a relationship between oxygen flowrate variation and pattern width variation. If a PSIdata variation is a result of an intended oxygen flowrate variation in the etch process, the PSI data variation is not due to faults of the etch process. Therefore, in this example, it is considered that the PSI data has not deviated from a PSI trend.
As explained above, when the condition-result data D50 are used to evaluate the state of the plasma chamber 100, a process can be smoothly performed in the plasma chamber 100 without unintended interruptions caused by false alarms. The statusdecision part 320 can perform operations S50 and S60.
FIGS. 3A and 3B are experimental graphs showing transmittance characteristics of visible light. In detail, referring to FIGS. 3A and 3B, the transmittance of the visible light decreases with time, and the decrease is dependent on wavelength. Initial spectral characteristics of the visible light shown in FIG. 3A vary with time as shown in FIG. 3B. In FIGS. 3A and 3B, the horizontal axis denotes wavelength of visible light, and the vertical axis denotes measured intensity of the visiblelight.
Referring to FIGS. 3A and 3B, the intensity of light PL measured after the light PL passes through the window 130 (refer to FIG. 1) has peak values at several wavelengths. However, the peak values decrease with time. It can be believed that thedecrease of the intensity in the light PL is a result of process by-products such as polymer particles attached to the window 130.
Referring to FIG. 3B, the decreased amounts of the peak values are different according to the wavelength of the light PL. For example, at an initial time (t=0), intensity peak values of the light PL are I.sub.1(0) and I.sub.2(0) at wavelengths.lamda..sub.1 and .lamda..sub.2, respectively. However, at a time t=t, the intensity peak values I.sub.1(0) and I.sub.2(0) of the light PL at wavelengths .lamda..sub.1 and .lamda..sub.2 are reduced to I.sub.1(t) and I.sub.2(t), respectively. Here, adecrease rate at the shorter wavelength
.lamda..times..function..function..function. ##EQU00001## is greater than a decrease rate at the longer wavelength
.lamda..times..function..function..function. ##EQU00002##
That is, when visible light PL passes through the window 130, the transmittance of the visible light PL varies according to the wavelength of the visible light PL.
FIG. 4 is another experimental graph showing transmittance characteristics of visible light. In detail, referring to FIG. 4, the transmittance of light decreases with time, and the decrease is dependent on wavelength. In the experimentssummarized in FIG. 4, the transmittance of 263-nm light and the transmittance of 387-nm light were measured over a predetermined period of days. In FIG. 4, the horizontal axis denotes date, and the vertical axis denotes intensity of light.
Referring to FIG. 4, the intensity value of the 263-nm light measured on October 23rd is less than the intensity value of the 263-nm light measured on October 13th by about 50%. The intensity value of the 387-nm light measured on October 23rd isless than the intensity value of the 387-nm light measured on October 13th by about 30%. These experimental results show that the time-dependent decrease in the intensity of the 387-nm light is less than that time-dependent decrease in the intensity ofthe 263-nm light. The transmittance of visible light is wavelength-dependent and can decrease with time by about 30% to about 50%.
The relationship between wavelength and transmittance variation of light can be explained by the Cauchy equation, which is known to be useful for at least visible light. According to the Cauchy equation, a relationship between index ofrefraction and wavelength can be expressed as follows:
.function..lamda. ##EQU00003## where n denotes an index of refraction, A denotes a coefficient of refraction, B denotes a coefficient of dispersion, and .lamda. denotes a wavelength.
dd.lamda..times..lamda. ##EQU00004##
Since the transmittance of light passing through the window 130 can be expressed as a function of refractive index, it follows that the variation rate of transmittance decreases as wavelength increases, from the equation showing that thevariation rate of the refractive index decreases as wavelength increases. This conclusion may be helpful to understand the experimental results shown in FIGS. 3A, 3B, and 4.
FIG. 5 is an experimental graph showing a relationship between transmittance and wavelength of light passing through a window 130. The experiment was performed while varying the thickness of by-products deposited on the window. In FIG. 5, acurve C1 was obtained when substantially no by-product was deposited on the window 130, and a curve C2 was obtained when by-products were deposited on the window approximately to an allowable thickness limit level. In FIG. 5, the horizontal axis denoteswavelength of light, and the vertical axis denotes transmittance of the light.
It can be understood from the experimental results shown in FIG. 5 that a wavelength band from about 900 nm to about 1700 nm can be the above-described measurement wavelength band where the transmittance of light passing through a window isindependent of the wavelength of the light. That is, the measurement wavelength band can range from about 900 nm to about 1700 nm.
In addition, other wavelength bands can be used as the measurement wavelength band. The measurement wavelength band is not limited to the range of about 900 nm to 1700 nm or the range of about 600 nm to about 3000 nm. In other words, althoughthe experimental results shown in FIGS. 3A, 3B, 4, and 5 indicate that the wavelength range of about 200 nm to about 500 nm is not included in the measurement wavelength band, other wavelength bands such as ultraviolet band, far-infrared band, andinfrared band can be fully or partially used as the measurement wavelength band if the transmittance of light passing through a window is wavelength-independent in those bands. That is, such wavelength bands can also be used as the measurementwavelength band if they satisfy certain conditions.
FIG. 6 is an experimental graph showing transmittance characteristics of light in a measurement wavelength band of an embodiment of the present invention. More specifically, FIG. 6 is an experimental graph showing how the transmittance of lightvaries with time in a measurement wavelength band. In the experiment summarized in FIG. 6, 966-nm light, 1066-nm light, 1099-nm light, 1505-nm light, and 1679-nm light are used. In FIG. 6, the horizontal axis denotes date, and the vertical axis denotesrelative intensity of light.
Referring to FIG. 6, the intensity of light decreases with time regardless of wavelength. However, the decrease of the light intensity for thirteen days is small at about 15%. The intensity decrease rate of the light in the measurementwavelength band is much smaller than the intensity decrease rates of the 263-nm light and the 387-nm light shown in FIG. 4 (about 30% to 50% for ten days).
In addition, the intensity decrease rate of light is substantially wavelength-independent in the measurement wavelength band. For example, the intensity of the 966-nm light decreases with time at substantially the same rate as the intensity ofthe 1673-nm light. Meanwhile, as explained above, the intensity of light varies with time since the amount of by-products deposited on the window 130 (refer to FIG. 1) increases with time. However, the intensity decrease rate of light is relativelyconstant in the measurement wavelength band regardless of the thickness of the by-products accumulated on the window 130. That is, in the measurement wavelength band, the decrease rate of the transmittance of light passing through the window 130 may besubstantially independent of the thickness of the by-products accumulated on the window 130.
FIG. 7 is another experimental graph showing transmittance characteristics of light in a measurement wavelength band of an embodiment of the present invention. More specifically, the experimental results summarized in FIG. 7 show that theintensity of light varies in a measurement wavelength band independently of the wavelength of the light. In the experiment, the relative intensity of light was measured on December 10th, 15th, and 20th in a wavelength range from about 900 nm to about1700 nm.
Referring to FIG. 7, the intensity of the spectra decreases with time like the case of FIG. 6. However, the shapes of the spectra do not vary with dates of measurement. In other words, the transmittance of light in the wavelength band of about900 nm to about 1700 nm is slightly dependent on time but is independent on wavelength. That is, the wavelength range of about 900 nm to about 1700 nm satisfies the above-described requirements for a measurement wavelength band.
FIG. 8 is a graph for explaining advantages attained by using light having a wavelength in a measurement wavelength band according to an embodiment of the present invention. More specifically, the graph of FIG. 8 is obtained by normalizing thespectra of FIG. 7 based on the intensity of 1505-nm light measured on December 7th.
The advantages of the embodiments described herein are attained by sensing light emitted from a plasma chamber in a predetermined wavelength band (i.e., a measurement wavelength band) where the transmittance of the light is independent of thewavelength of the light. Furthermore, the advantages are attained by normalizing measured spectrum data to remove the effect of a time-dependent decrease of the transmittance of the light.
As described above, the state of a plasma chamber is checked by sensing light emitted from a plasma chamber in a predetermined wavelength band (i.e., a measurement wavelength band) where the transmittance of the light is independent of thewavelength of the light. When the transmittance of light is independent of the wavelength of the light, although the intensity of the light decreases with time, the decrease rate is substantially constant and independent of the wavelength of the light. Therefore, although contamination of a window increases with time, the state of the plasma chamber can be reliably evaluated.
Furthermore, according to embodiments of the present invention, spectra are measured in a wavelength band where the transmittance of light is independent of the wavelength of the light. Then, the spectra are normalized, and the state of theplasma chamber is evaluated using the normalized spectra. As explained above, in the wavelength band where the transmittance of light is independent of the wavelength of the light, a decrease rate of the intensity of the light is substantially constantand independent of the wavelength of the light. Thus, the effect of the time-dependent decrease of the intensity of the light is not included in the normalized spectra as shown in FIG. 8. As a result, the state of the plasma chamber can be reliablymonitored and evaluated although contamination of the window can increase with time.
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