US20050023132A1 - Device for measuring the profile of a metal film sputter deposition target, and system and method employing same - Google Patents
Device for measuring the profile of a metal film sputter deposition target, and system and method employing same Download PDFInfo
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- US20050023132A1 US20050023132A1 US10/923,233 US92323304A US2005023132A1 US 20050023132 A1 US20050023132 A1 US 20050023132A1 US 92323304 A US92323304 A US 92323304A US 2005023132 A1 US2005023132 A1 US 2005023132A1
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- target surface
- energy beam
- sensor
- target
- reflection
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/34—Gas-filled discharge tubes operating with cathodic sputtering
- H01J37/3476—Testing and control
- H01J37/3482—Detecting or avoiding eroding through
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/3407—Cathode assembly for sputtering apparatus, e.g. Target
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/54—Controlling or regulating the coating process
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/54—Controlling or regulating the coating process
- C23C14/542—Controlling the film thickness or evaporation rate
- C23C14/543—Controlling the film thickness or evaporation rate using measurement on the vapor source
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/56—Apparatus specially adapted for continuous coating; Arrangements for maintaining the vacuum, e.g. vacuum locks
- C23C14/564—Means for minimising impurities in the coating chamber such as dust, moisture, residual gases
Definitions
- the present invention relates generally to sputter deposition on substrate surfaces. More specifically, the present invention relates to methods and apparatus for measuring the profile of a sputtering target.
- FIG. 1 illustrates a cross-sectional schematic of a typical sputtering apparatus 10 comprising a vacuum chamber 12 having a gas inlet 14 and a gas outlet 16 .
- the sputtering apparatus 10 further comprises a substrate support pedestal 24 and a metallic target 22 attached to a sputtering cathode assembly 18 , each located within the vacuum chamber 12 .
- the pedestal 24 may be configured to secure a substrate 26 thereto with a biasable electrostatic chuck, a vacuum chuck, a clamping structure, or a combination of methods.
- the substrate 26 may be transported to and from the pedestal 24 manually or with a robotic arm or blade (not shown).
- the vacuum chamber 12 is filled with an inert gas, such as argon, through the gas inlet 14 and then reduced to a near vacuum through the gas outlet 16 .
- the target 22 is negatively charged to cause electrons to be emitted from an exposed surface 23 of the target 22 and move toward an anode (not shown). A portion of the moving electrons strike atoms of the inert gas, causing the atoms to become positively ionized and move towards the negatively charged target 22 .
- the electrons, inert gas atoms, and ions form a plasma which is typically intensified and confined over the target surface 23 by a magnetic field generated by a magnet assembly 20 located proximate the target 22 .
- the magnet assembly 20 may comprise one or more permanent magnets or electromagnets located behind and/or to the side of the target 22 .
- a portion of the ions discharging from the plasma strike the target surface 23 at a high velocity, causing atoms or small particles of the target 22 material to be ejected from the target surface 23 .
- the ejected atoms or small particles then travel through the vacuum chamber 12 until they strike a surface, such as the surface of the substrate 26 , forming a thin metallic film thereon.
- the magnetic field formed over the target surface 23 by the magnet assembly 20 confines the electrons emitted from the target 22 to an area near the target surface 23 . This greatly increases the electron density and the likelihood of collisions between the electrons and the atoms of the inert gas in the space near the target surface 23 . Therefore, there is a higher rate of ion production in plasma regions near the target surface 23 where the magnetic field intensity is stronger. Varying rates of ion production in different plasma regions causes the target surface 23 to erode unevenly.
- the configuration of the magnet assembly 20 produces a radial variation of thick and thin areas, or grooves, within a diameter of the target surface 23 .
- FIG. 2 illustrates a cross-sectional perspective view of a typical erosion profile of a cylindrical metallic target 22 , such as the metallic target 22 shown in FIG. 1 , which has been used in a sputtering process.
- FIG. 2 illustrates a target surface 23 before erosion has occurred as well as a target surface 32 that has eroded unevenly across the length of a diameter bounded by an outside edge 25 of the target 22 . Due to the geometry of a magnetic field surrounding the target 22 , the target surface 32 has eroded nearly symmetrically about a center line 30 dividing the length of the diameter.
- the target 22 may comprise a rare metal, such as gold, platinum, palladium or silver, or may comprise, for example, aluminum, titanium, tungsten or any other target material conventionally employed in the semiconductor industry. Therefore, it is advantageous to consume as much of the target 22 material during sputter deposition processes as possible before replacing an eroded target 22 . Further, replacing an eroded target 22 before the end of its useful life may be a difficult and time-consuming task. However, it is important to replace the target 22 before a groove “punches through” the target 22 material and exposes portions of the cathode assembly 18 to erosion, causing damage to the cathode assembly 18 and contaminating the sputtering apparatus 10 . For example, the target 22 material in the area of groove 28 shown in FIG. 2 may erode before the remainder of the target 22 material and expose the cathode assembly 18 to ionic bombardment from the surrounding plasma.
- a rare metal such as gold, platinum, palladium or silver
- the useful life of a metallic sputtering target 22 is typically estimated by determining the cumulative deposition time for the target 22 .
- a deposition time is chosen to guarantee that the target 22 material will never be completely removed at any given location and may take into account the thickness of the target 22 , the material used for the target 22 , and the effect of intensifying and confining the plasma over the target surface 32 by a magnetic field generated by the magnet assembly 20 in a predetermined configuration.
- the characteristics of the plasma distribution change due to, for example, reconfiguring the magnet assembly 20 to produce a magnetic field with a different geometry, the erosion of the target surface 32 may be changed and could result in localized enhanced metal removal and the possible punching through to the cathode assembly 18 before the expiration of the estimated deposition time.
- Directly measuring the target surface 23 is difficult and time consuming. Opening the vacuum chamber 12 to inspect the target surface 23 requires several hours of idle time while the vacuum chamber 12 is baked out under post-vacuum inspection. Accurate measurement of the target surface 23 while the sputtering apparatus 10 is under vacuum is difficult because the gap distance d between the target 22 and the pedestal 24 may be as small as 25 millimeters. Typical measurement devices are too large to be inserted into the gap d between the target 22 and the pedestal 24 to profile the target surface 23 while the vacuum chamber 12 is under vacuum. Further, measurement devices placed near the target 22 during a sputtering process may be damaged by exposure to metal deposition.
- the present invention relates to methods and apparatus for measuring the erosion of a metallic sputtering target.
- An apparatus comprises a sensor configured to emit an energy beam toward a target surface and to detect a reflection of the energy beam from the target surface.
- the sensor may be coupled to a thin profile arm configured to move or transport the sensor over the target surface between the target and a substrate support pedestal to a plurality of measurement locations.
- the arm may be configured to attach to a robotic device.
- the sensor and the arm are configured, positioned and sized to be inserted into a narrow gap existing between the target surface and the pedestal.
- the arm may also be configured to remove the sensor from the gap and to shield the sensor during a sputtering process.
- the senor comprises a source element configured to emit a collimated light beam and a plurality of detectors arranged in a linear array.
- the source element may be positioned so as to emit the collimated light beam at an acute angle with respect to the linear array of detectors.
- the detectors are positioned relative to the source element so that one of the detectors in the array will be illuminated by a reflection of the collimated light beam.
- the distance from the sensor to the target surface or the percentage of target erosion may be calculated by determining which detector in the array is illuminated by the reflection of the collimated light beam.
- the senor comprises a transmitter optically coupled to a source collimator configured to collimate a light beam as it exits an optical fiber.
- the sensor may further comprise a receiver optically coupled to a plurality of collection collimators, each of the plurality of collection collimators being configured to collect the reflection of the light beam incident thereon into a corresponding optical fiber.
- the present invention also encompasses a sputter deposition system incorporating the sensors of the present invention and a method of profiling a sputtering surface target.
- the method comprises emitting an energy beam, illuminating a first location on the target surface, detecting a reflection of the energy beam from the at least one location, and analyzing the detected reflection of the energy beam to determine a distance from the point of emission to the first location.
- FIG. 1 is a cross-sectional side view schematic of a sputtering apparatus
- FIG. 2 is a cross-sectional perspective side view of an erosion profile of a cylindrical, metallic target
- FIG. 3 is a cross-sectional side view schematic according to one embodiment of the present invention of a portion of a sputtering apparatus comprising a sensor configured, sized and positioned to be inserted between a target surface and a pedestal;
- FIG. 4 is a top view schematic of a sensor according to one embodiment of the present invention.
- FIG. 5 is a side view schematic of the sensor of FIG. 4 and a portion of a sputtering apparatus
- FIG. 6 is a block diagram of a sputter deposition system comprising a sensor assembly according to one embodiment of the present invention.
- FIG. 7 is a block diagram of a sensor assembly according to one embodiment of the present invention.
- FIG. 3 illustrates a cross-sectional schematic of a portion of a sputtering apparatus, such as the sputtering apparatus 10 shown in FIG. 1 , according to one embodiment of the present invention.
- a sensor 50 coupled to a thin profile arm 44 is configured and sized to be inserted into a gap between a target 22 and a pedestal 24 .
- the arm 44 may be configured to detachably attach to a chamber robot 40 configured to translate the sensor 50 over the target surface 23 , or at least a portion thereof.
- the chamber robot 40 may further be configured to protect the sensor 50 during the sputtering process by removing the sensor 50 from the sputtering area or by shielding the sensor 50 .
- the arm 44 may be interconnected to the chamber robot 40 through an articulating arm 42 configured to provide movement in at least one plane.
- the sensor 50 may detachably attach to a substrate pickup arm (not shown) connected to the chamber robot 40 and configured to transport a substrate (not shown) to and from the pedestal 24 using a pickup device (not shown), such as a clamp, vacuum chuck or electrostatic chuck, to attach the substrate thereto.
- the sensor 50 may be configured to attach directly to the pickup device.
- the sensor 50 is configured to transmit a signal 46 toward the target 22 and to receive a reflected signal 48 from the target surface 23 .
- the transmitted signal 46 may be an energy beam selected from the group comprising a visible light beam, an ultraviolet light beam, an infrared light beam, a radio frequency (“RF”) beam, a microwave beam and an ultrasound beam.
- RF radio frequency
- the reflected signal 48 may be analyzed to determine a relative distance between the sensor 50 and the target surface 23 . It may not be necessary to measure the relative distance between the sensor 50 and the target surface 23 at every point on the target surface 23 .
- the relative distance between the sensor 50 and the target surface 23 is measured by measuring the time delay between the emission of the transmitted signal 46 and detection of the reflected signal 48 , multiplying the measured time delay by the speed of the transmitted signal 46 and dividing by two.
- the chamber robot 40 may be configured to position the sensor 50 at a plurality of locations relative to the target surface. Further, the sensor 50 may be configured, such as by using a multiplexor, to scan a portion (as opposed to a single point) on the target surface 23 while positioned at one location relative to the target surface 23 .
- the distance between the sensor 50 and the target surface 23 may be determined by indirectly establishing the time delay by measuring a phase difference between the transmitted signal 46 and the reflected signal 48 .
- the transmitted signal 46 may comprise a modulated signal.
- the transmitted signal 46 may be a pulsed signal and the reflected pulse signal 48 may be detected only during a predetermined time window such that increased time delay between transmission and detection causes less of the pulse to be detected.
- the detected power level of the reflected pulse signal 48 is inversely proportional to the distance traveled.
- Other embodiments for measuring the distance between the sensor 50 and the target surface 23 may also be employed.
- FIG. 4 illustrates a top view schematic of a sensor 52 according to one embodiment of the present invention.
- the sensor 52 is attached to a thin profile arm 44 , such as the arm 44 shown in FIG. 3 .
- Sensor 52 comprises a source element 54 and a detector array 55 .
- the source element 54 has a thin profile so as to fit between the target 22 and the pedestal 24 , as shown in FIG. 3 .
- the source element 54 is configured to generate a collimated light beam.
- the source element 54 may comprise a laser diode.
- the source element 54 may comprise a collimator, such as a lens, configured to collimate or focus light exiting an optical fiber to a desired beam diameter or spot size.
- the collimated light emitted from the source element 54 minimizes extraneous reflections and enhances signal detection.
- Use of a collimated light beam as an energy beam is currently preferred, although the invention is not so limited.
- the detector array 55 comprises a plurality of detectors 56 (ten shown) disposed side by side in a linear array, each detector 56 having a thin profile so as to fit between the target 22 and the pedestal 24 , as shown in FIG. 3 .
- Each detector 56 in the detector array 55 is configured to produce an electronic sensory signal related to the magnitude of the radiation received thereon.
- each detector may comprise a photodiode or a charge coupled device (“CCD”).
- CCD charge coupled device
- each detector 56 in the detector array 55 may comprise a collimator, such as a lens, configured to collect light into an optical fiber.
- FIG. 5 illustrates a side view schematic of the sensor 52 and arm 44 shown in FIG. 4 .
- the source element 54 is positioned so as to emit a transmitted beam 60 at a predetermined transmission angle a in relation to the arm 44 .
- FIG. 5 also illustrates the sensor 52 positioned in relation to a portion of a target 22 , such as the target 22 shown in FIG. 2 .
- the number of detectors 56 in the detector array 55 and the position of each detector 56 relative to the source element 54 are dependent upon the distance between the sensor 52 and the target 22 .
- three surfaces 23 , 32 , 70 are referenced in FIG. 5 corresponding to different target 22 erosion states.
- the first target surface 23 corresponds to a new or unused target 22 that has not yet been exposed to a sputtering process.
- the transmitted beam 60 illuminates the new target surface 23 and reflects back toward the detector array 55 as reflected beam 62 .
- the vertical distance z between the new target surface 23 and the sensor 52 may be predetermined.
- the incident angle ⁇ of the transmitted beam 60 and the reflected angle ⁇ ′ of the reflected beam 62 are equal
- the next target surface 32 shown in FIG. 5 corresponds to a target 22 that has been used in a sputtering process wherein approximately one-third of the target 22 material has been eroded.
- the target surface 32 has eroded unevenly.
- the transmitted beam 60 now represented by dashed line 64 , illuminates the eroded target surface 32 and reflects back toward the detector array 55 as reflected beam 66 .
- the reflected beam 66 illuminates a detector 56 in the detector array 55 located approximately one-third of the distance between the detector 56 located nearest the source element 54 and the detector 56 located farthest from the source element 54 . Therefore, it may be determined that approximately one-third of the target 22 material has been eroded at the measured location along the target surface 32 .
- the next target surface 70 shown in FIG. 5 corresponds to the interface between the target 22 and the cathode assembly 18 , as shown in FIG. 1 .
- the transmitted beam 60 now represented by dashed line 68 , illuminates the target interface surface 70 and reflects back toward the detector array 55 as reflected beam 72 .
- the reflected beam 72 illuminates a detector 56 in the detector array 55 located farthest from the source element 54 .
- it may be determined that substantially all of the target 22 material has been eroded at the measured location along the target interface surface 70 .
- use of the present invention to detect target consumption prevents the target interface surface 70 from being punched through and exposing portions of the cathode assembly 18 to erosion from the sputtering process. Therefore, it may be advantageous to replace the target 22 before the target interface surface 70 is detected.
- FIG. 6 is a block diagram of a sputter deposition system 80 according to the present invention.
- the sputter deposition system 80 comprises a controller 82 electrically coupled to chamber circuitry 90 , sensor circuitry 100 , an input device 84 , an output device 86 and a data storage device 88 .
- FIGS. 4 and 5 illustrate the sensor circuitry 100 comprising a sensor 52 attached to an arm 44 , according to one embodiment of the present invention.
- the sensor 52 comprises a source element 54 and a plurality of detectors 56 (ten shown) forming a linear array 55 .
- the controller 82 is configured to communicate an electronic transmit signal to the source element 54 .
- the source element 54 Upon receipt of the transmit signal from the controller 82 , the source element 54 is configured to transmit a beam of collimated light.
- the beam of collimated light may be a pulsed beam of collimated light.
- Each detector 56 is configured to generate an electronic sensory signal related to the magnitude of the radiation received thereon.
- the controller 82 is configured to receive and compare each of the sensory signals to determine which one of the detectors 56 was illuminated with the greatest magnitude of radiation.
- the controller 82 may be configured to receive the sensory signals during a predefined time window in relation to the communication of the transmit signal to the source element 54 .
- the controller 82 is further configured to determine the relative distance from the sensor 52 to a target surface 23 , 32 , 70 .
- the controller 82 may be configured to estimate the relative amount of erosion at a location along the target surface 23 , 32 , 70 according to the relative position of the detector 56 in the detector array 55 illuminated with the greatest amount of radiation. For example, if a detector 56 located at the center of the detector array is determined by the controller 82 to be illuminated by a reflected beam, then the controller 82 may be configured to estimate that half of the target 22 material has been eroded at the position along the target surface 23 , 32 , 70 being measured.
- FIG. 7 illustrates a block diagram of a sensor assembly 102 , such as the sensor circuitry 100 shown in FIG. 6 , according to another embodiment of the present invention.
- the sensor assembly 102 shown in FIG. 7 comprises a source element 110 and a plurality of reception elements 112 (four shown) attached to a thin profile arm 114 , similar to the arm 44 shown in FIG. 3 .
- the source element 110 comprises a collimator, such as a lens, configured to collimate or focus light exiting an optical fiber 116 to a desired beam diameter or spot size.
- Each reception element 112 comprises a collimator, such as a lens, configured to collect light incident thereon into an optical fiber assembly 118 .
- the sensor assembly 102 further comprises a transmitter 104 coupled to the source element 110 through the optical fiber 116 and a receiver 106 coupled to each of the plurality of reception elements 112 through the optical fiber assembly 118 .
- the optical fiber assembly 118 comprises a plurality of optical fibers, each optical fiber configured to couple to one reception element 112 .
- the transmitter 104 is configured to receive a transmit signal from the controller 82 and to transmit a beam of collimated light to the source element 110 through the optical fiber 116 .
- the beam of collimated light may be a pulsed beam of collimated light.
- the receiver 106 is configured to receive a light beam through the optical fiber assembly 118 and to generate an electronic sensory signal related to the magnitude of the radiation collected at the respective reception element 112 .
- the receiver 106 is further configured to transmit each of the sensory signals to the controller 82 .
- the controller 82 is configured to receive and compare each of the sensory signals to determine which one of the reception elements 112 was illuminated with the greatest magnitude of radiation.
- the controller 82 may be configured to receive the sensory signals during a predefined time window in relation to the communication of the transmit signal to the source element 110 .
- the controller 82 is further configured to determine the relative distance from the source element 110 to an object (not shown), as described above.
- the controller 82 may be configured to interface with the chamber circuitry 90 , including chamber robot circuitry 92 , to control the position of the sensor circuitry 100 relative to a target 22 in the vacuum chamber 12 , the placement and removal of a substrate 26 on the pedestal 24 , sputter processing times, and other sputtering process and vacuum chamber 12 operations.
- the controller 82 may further be configured to perform computer functions such as executing software to perform desired calculations and tasks.
- the input device 84 may include, by way of example only, an Internet or other network connection, a mouse, a keypad or any device that allows an operator to enter data into the controller 82 .
- the output device 86 may include, by way of example only, a printer or a video display device.
- the data storage device 88 may include, by way of example only, drives that accept hard and floppy discs, tape cassettes, CD-ROM or DVD-ROM.
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Abstract
An apparatus and method for measuring the erosion profile of a metallic target in a sputtering device are provided by inserting a thin sensor into a gap between the target and a substrate pedestal. The sensor is configured to emit an energy beam toward the surface of the target and to detect a reflection of the energy beam. The sensor may comprise a source element configured to emit a collimated light beam and a plurality of detectors arranged in a linear array. The sensor may also comprise optical fibers configured to reduce the size of the sensor. The detectors are positioned relative to the source element so that one of the detectors in the array will be illuminated by a reflection of the collimated light beam. The distance from the sensor to the target may be derived from the position of the detector illuminated by the reflected beam.
Description
- This application is a continuation of application Ser. No. 10/352,699, filed Jan. 27, 2003, pending.
- 1. Field of the Invention
- The present invention relates generally to sputter deposition on substrate surfaces. More specifically, the present invention relates to methods and apparatus for measuring the profile of a sputtering target.
- 2. State of the Art
- A thin film of metallic material may be deposited on a substrate using a sputter deposition process wherein a metallic target is attacked with ions causing atoms or small particles of the target to be ejected from the target and deposited on the substrate surface.
FIG. 1 illustrates a cross-sectional schematic of a typicalsputtering apparatus 10 comprising avacuum chamber 12 having agas inlet 14 and agas outlet 16. Thesputtering apparatus 10 further comprises asubstrate support pedestal 24 and ametallic target 22 attached to a sputteringcathode assembly 18, each located within thevacuum chamber 12. Thepedestal 24 may be configured to secure asubstrate 26 thereto with a biasable electrostatic chuck, a vacuum chuck, a clamping structure, or a combination of methods. Thesubstrate 26 may be transported to and from thepedestal 24 manually or with a robotic arm or blade (not shown). - During the sputtering process, the
vacuum chamber 12 is filled with an inert gas, such as argon, through thegas inlet 14 and then reduced to a near vacuum through thegas outlet 16. Thetarget 22 is negatively charged to cause electrons to be emitted from an exposedsurface 23 of thetarget 22 and move toward an anode (not shown). A portion of the moving electrons strike atoms of the inert gas, causing the atoms to become positively ionized and move towards the negativelycharged target 22. The electrons, inert gas atoms, and ions form a plasma which is typically intensified and confined over thetarget surface 23 by a magnetic field generated by amagnet assembly 20 located proximate thetarget 22. Themagnet assembly 20 may comprise one or more permanent magnets or electromagnets located behind and/or to the side of thetarget 22. A portion of the ions discharging from the plasma strike thetarget surface 23 at a high velocity, causing atoms or small particles of thetarget 22 material to be ejected from thetarget surface 23. The ejected atoms or small particles then travel through thevacuum chamber 12 until they strike a surface, such as the surface of thesubstrate 26, forming a thin metallic film thereon. - The magnetic field formed over the
target surface 23 by themagnet assembly 20 confines the electrons emitted from thetarget 22 to an area near thetarget surface 23. This greatly increases the electron density and the likelihood of collisions between the electrons and the atoms of the inert gas in the space near thetarget surface 23. Therefore, there is a higher rate of ion production in plasma regions near thetarget surface 23 where the magnetic field intensity is stronger. Varying rates of ion production in different plasma regions causes thetarget surface 23 to erode unevenly. Typically, the configuration of themagnet assembly 20 produces a radial variation of thick and thin areas, or grooves, within a diameter of thetarget surface 23.FIG. 2 illustrates a cross-sectional perspective view of a typical erosion profile of a cylindricalmetallic target 22, such as themetallic target 22 shown inFIG. 1 , which has been used in a sputtering process.FIG. 2 illustrates atarget surface 23 before erosion has occurred as well as atarget surface 32 that has eroded unevenly across the length of a diameter bounded by anoutside edge 25 of thetarget 22. Due to the geometry of a magnetic field surrounding thetarget 22, thetarget surface 32 has eroded nearly symmetrically about acenter line 30 dividing the length of the diameter. - Referring now to
FIGS. 1 and 2 , thetarget 22 may comprise a rare metal, such as gold, platinum, palladium or silver, or may comprise, for example, aluminum, titanium, tungsten or any other target material conventionally employed in the semiconductor industry. Therefore, it is advantageous to consume as much of thetarget 22 material during sputter deposition processes as possible before replacing aneroded target 22. Further, replacing aneroded target 22 before the end of its useful life may be a difficult and time-consuming task. However, it is important to replace thetarget 22 before a groove “punches through” thetarget 22 material and exposes portions of thecathode assembly 18 to erosion, causing damage to thecathode assembly 18 and contaminating thesputtering apparatus 10. For example, thetarget 22 material in the area ofgroove 28 shown inFIG. 2 may erode before the remainder of thetarget 22 material and expose thecathode assembly 18 to ionic bombardment from the surrounding plasma. - The useful life of a
metallic sputtering target 22 is typically estimated by determining the cumulative deposition time for thetarget 22. A deposition time is chosen to guarantee that thetarget 22 material will never be completely removed at any given location and may take into account the thickness of thetarget 22, the material used for thetarget 22, and the effect of intensifying and confining the plasma over thetarget surface 32 by a magnetic field generated by themagnet assembly 20 in a predetermined configuration. However, if the characteristics of the plasma distribution change due to, for example, reconfiguring themagnet assembly 20 to produce a magnetic field with a different geometry, the erosion of thetarget surface 32 may be changed and could result in localized enhanced metal removal and the possible punching through to thecathode assembly 18 before the expiration of the estimated deposition time. - Directly measuring the
target surface 23 is difficult and time consuming. Opening thevacuum chamber 12 to inspect thetarget surface 23 requires several hours of idle time while thevacuum chamber 12 is baked out under post-vacuum inspection. Accurate measurement of thetarget surface 23 while thesputtering apparatus 10 is under vacuum is difficult because the gap distance d between thetarget 22 and thepedestal 24 may be as small as 25 millimeters. Typical measurement devices are too large to be inserted into the gap d between thetarget 22 and thepedestal 24 to profile thetarget surface 23 while thevacuum chamber 12 is under vacuum. Further, measurement devices placed near thetarget 22 during a sputtering process may be damaged by exposure to metal deposition. - In view of the shortcomings in the art, it would be advantageous to prevent premature replacement and over consumption of the
target 22 by providing a technique and device to measure thetarget surface 23 while thevacuum chamber 12 is under vacuum. - The present invention relates to methods and apparatus for measuring the erosion of a metallic sputtering target.
- An apparatus according to one embodiment of the present invention comprises a sensor configured to emit an energy beam toward a target surface and to detect a reflection of the energy beam from the target surface. The sensor may be coupled to a thin profile arm configured to move or transport the sensor over the target surface between the target and a substrate support pedestal to a plurality of measurement locations. The arm may be configured to attach to a robotic device. The sensor and the arm are configured, positioned and sized to be inserted into a narrow gap existing between the target surface and the pedestal. The arm may also be configured to remove the sensor from the gap and to shield the sensor during a sputtering process.
- In another embodiment of the present invention, the sensor comprises a source element configured to emit a collimated light beam and a plurality of detectors arranged in a linear array. The source element may be positioned so as to emit the collimated light beam at an acute angle with respect to the linear array of detectors. The detectors are positioned relative to the source element so that one of the detectors in the array will be illuminated by a reflection of the collimated light beam. The distance from the sensor to the target surface or the percentage of target erosion may be calculated by determining which detector in the array is illuminated by the reflection of the collimated light beam.
- In a further embodiment of the present invention, the sensor comprises a transmitter optically coupled to a source collimator configured to collimate a light beam as it exits an optical fiber. The sensor may further comprise a receiver optically coupled to a plurality of collection collimators, each of the plurality of collection collimators being configured to collect the reflection of the light beam incident thereon into a corresponding optical fiber.
- The present invention also encompasses a sputter deposition system incorporating the sensors of the present invention and a method of profiling a sputtering surface target. The method comprises emitting an energy beam, illuminating a first location on the target surface, detecting a reflection of the energy beam from the at least one location, and analyzing the detected reflection of the energy beam to determine a distance from the point of emission to the first location.
- Other features and advantages of the present invention will become apparent to those of ordinary skill in the art through consideration of the ensuing description, the accompanying drawings, and the appended claims.
- The drawings, which illustrate what are currently considered to be the best modes for carrying out the invention:
-
FIG. 1 is a cross-sectional side view schematic of a sputtering apparatus; -
FIG. 2 is a cross-sectional perspective side view of an erosion profile of a cylindrical, metallic target; -
FIG. 3 is a cross-sectional side view schematic according to one embodiment of the present invention of a portion of a sputtering apparatus comprising a sensor configured, sized and positioned to be inserted between a target surface and a pedestal; -
FIG. 4 is a top view schematic of a sensor according to one embodiment of the present invention; -
FIG. 5 is a side view schematic of the sensor ofFIG. 4 and a portion of a sputtering apparatus; -
FIG. 6 is a block diagram of a sputter deposition system comprising a sensor assembly according to one embodiment of the present invention; and -
FIG. 7 is a block diagram of a sensor assembly according to one embodiment of the present invention. -
FIG. 3 illustrates a cross-sectional schematic of a portion of a sputtering apparatus, such as thesputtering apparatus 10 shown inFIG. 1 , according to one embodiment of the present invention. As shown inFIG. 3 , asensor 50 coupled to athin profile arm 44 is configured and sized to be inserted into a gap between atarget 22 and apedestal 24. Thearm 44 may be configured to detachably attach to achamber robot 40 configured to translate thesensor 50 over thetarget surface 23, or at least a portion thereof. Thechamber robot 40 may further be configured to protect thesensor 50 during the sputtering process by removing thesensor 50 from the sputtering area or by shielding thesensor 50. Thearm 44 may be interconnected to thechamber robot 40 through an articulatingarm 42 configured to provide movement in at least one plane. In another embodiment of the present invention, thesensor 50 may detachably attach to a substrate pickup arm (not shown) connected to thechamber robot 40 and configured to transport a substrate (not shown) to and from thepedestal 24 using a pickup device (not shown), such as a clamp, vacuum chuck or electrostatic chuck, to attach the substrate thereto. In yet another embodiment, thesensor 50 may be configured to attach directly to the pickup device. - The
sensor 50 is configured to transmit asignal 46 toward thetarget 22 and to receive a reflectedsignal 48 from thetarget surface 23. The transmittedsignal 46 may be an energy beam selected from the group comprising a visible light beam, an ultraviolet light beam, an infrared light beam, a radio frequency (“RF”) beam, a microwave beam and an ultrasound beam. To determine the amount of erosion at any location on thetarget surface 23, the reflectedsignal 48 may be analyzed to determine a relative distance between thesensor 50 and thetarget surface 23. It may not be necessary to measure the relative distance between thesensor 50 and thetarget surface 23 at every point on thetarget surface 23. Due to the radial symmetry of the erosion of thetarget surface 23, it is only necessary to determine the relative distance between thesensor 50 and thetarget surface 23 at points located linearly between thecenter line 30 of thetarget surface 23 and anoutside edge 25 of thetarget surface 23, as shown inFIG. 2 . Thus, in measuring the relative distance between thesensor 50 and thetarget surface 23 approximately every ten millimeters linearly between thecenter line 30 and anoutside edge 25 may provide sufficient resolution to prevent punching through atarget 22 having a diameter of approximately thirty centimeters. - In one embodiment of the present invention, the relative distance between the
sensor 50 and thetarget surface 23 is measured by measuring the time delay between the emission of the transmittedsignal 46 and detection of the reflectedsignal 48, multiplying the measured time delay by the speed of the transmittedsignal 46 and dividing by two. To profile thetarget surface 23, thechamber robot 40 may be configured to position thesensor 50 at a plurality of locations relative to the target surface. Further, thesensor 50 may be configured, such as by using a multiplexor, to scan a portion (as opposed to a single point) on thetarget surface 23 while positioned at one location relative to thetarget surface 23. In another embodiment, the distance between thesensor 50 and thetarget surface 23 may be determined by indirectly establishing the time delay by measuring a phase difference between the transmittedsignal 46 and the reflectedsignal 48. In aphase measurement sensor 50, the transmittedsignal 46 may comprise a modulated signal. In yet another embodiment, the transmittedsignal 46 may be a pulsed signal and the reflectedpulse signal 48 may be detected only during a predetermined time window such that increased time delay between transmission and detection causes less of the pulse to be detected. Thus, the detected power level of the reflectedpulse signal 48 is inversely proportional to the distance traveled. Other embodiments for measuring the distance between thesensor 50 and thetarget surface 23, as presently known in the art, may also be employed. -
FIG. 4 illustrates a top view schematic of asensor 52 according to one embodiment of the present invention. Thesensor 52 is attached to athin profile arm 44, such as thearm 44 shown inFIG. 3 .Sensor 52 comprises asource element 54 and adetector array 55. Thesource element 54 has a thin profile so as to fit between thetarget 22 and thepedestal 24, as shown inFIG. 3 . Thesource element 54 is configured to generate a collimated light beam. By way of example only, and not by limitation, thesource element 54 may comprise a laser diode. Alternatively, thesource element 54 may comprise a collimator, such as a lens, configured to collimate or focus light exiting an optical fiber to a desired beam diameter or spot size. As will be seen below, the collimated light emitted from thesource element 54 minimizes extraneous reflections and enhances signal detection. Use of a collimated light beam as an energy beam is currently preferred, although the invention is not so limited. - The
detector array 55 comprises a plurality of detectors 56 (ten shown) disposed side by side in a linear array, eachdetector 56 having a thin profile so as to fit between thetarget 22 and thepedestal 24, as shown inFIG. 3 . Eachdetector 56 in thedetector array 55 is configured to produce an electronic sensory signal related to the magnitude of the radiation received thereon. By way of example only, and not by limitation, each detector may comprise a photodiode or a charge coupled device (“CCD”). Alternatively, eachdetector 56 in thedetector array 55 may comprise a collimator, such as a lens, configured to collect light into an optical fiber. -
FIG. 5 illustrates a side view schematic of thesensor 52 andarm 44 shown inFIG. 4 . As shown inFIG. 5 , thesource element 54 is positioned so as to emit a transmittedbeam 60 at a predetermined transmission angle a in relation to thearm 44. Although not shown, it may also be advantageous to position eachdetector 56 of thedetector array 55 at an angle in relation to thearm 44 so as to align with a corresponding reflected beam, such as reflectedbeams -
FIG. 5 also illustrates thesensor 52 positioned in relation to a portion of atarget 22, such as thetarget 22 shown inFIG. 2 . The number ofdetectors 56 in thedetector array 55 and the position of eachdetector 56 relative to thesource element 54 are dependent upon the distance between thesensor 52 and thetarget 22. For illustration purposes, threesurfaces FIG. 5 corresponding todifferent target 22 erosion states. Thefirst target surface 23 corresponds to a new orunused target 22 that has not yet been exposed to a sputtering process. The transmittedbeam 60 illuminates thenew target surface 23 and reflects back toward thedetector array 55 as reflectedbeam 62. To configure the dimensions of thedetector array 55, the vertical distance z between thenew target surface 23 and thesensor 52 may be predetermined. Thus, assuming the incident angle β of the transmittedbeam 60 and the reflected angle β′ of the reflectedbeam 62 are equal, the distance x between thesource element 54 and thenearest detector 56 in the detector array 55 (i.e., thedetector 56 illuminated by the reflected beam 62) is given by: - The
next target surface 32 shown inFIG. 5 corresponds to atarget 22 that has been used in a sputtering process wherein approximately one-third of thetarget 22 material has been eroded. As discussed above in relation toFIG. 2 , thetarget surface 32 has eroded unevenly. The transmittedbeam 60, now represented by dashedline 64, illuminates the erodedtarget surface 32 and reflects back toward thedetector array 55 as reflectedbeam 66. The reflectedbeam 66 illuminates adetector 56 in thedetector array 55 located approximately one-third of the distance between thedetector 56 located nearest thesource element 54 and thedetector 56 located farthest from thesource element 54. Therefore, it may be determined that approximately one-third of thetarget 22 material has been eroded at the measured location along thetarget surface 32. - The
next target surface 70 shown inFIG. 5 corresponds to the interface between thetarget 22 and thecathode assembly 18, as shown inFIG. 1 . The transmittedbeam 60, now represented by dashedline 68, illuminates thetarget interface surface 70 and reflects back toward thedetector array 55 as reflectedbeam 72. The reflectedbeam 72 illuminates adetector 56 in thedetector array 55 located farthest from thesource element 54. Thus, it may be determined that substantially all of thetarget 22 material has been eroded at the measured location along thetarget interface surface 70. As discussed above, use of the present invention to detect target consumption prevents thetarget interface surface 70 from being punched through and exposing portions of thecathode assembly 18 to erosion from the sputtering process. Therefore, it may be advantageous to replace thetarget 22 before thetarget interface surface 70 is detected. -
FIG. 6 is a block diagram of asputter deposition system 80 according to the present invention. Thesputter deposition system 80 comprises acontroller 82 electrically coupled tochamber circuitry 90,sensor circuitry 100, aninput device 84, anoutput device 86 and adata storage device 88.FIGS. 4 and 5 illustrate thesensor circuitry 100 comprising asensor 52 attached to anarm 44, according to one embodiment of the present invention. Thesensor 52 comprises asource element 54 and a plurality of detectors 56 (ten shown) forming alinear array 55. Thecontroller 82 is configured to communicate an electronic transmit signal to thesource element 54. Upon receipt of the transmit signal from thecontroller 82, thesource element 54 is configured to transmit a beam of collimated light. The beam of collimated light may be a pulsed beam of collimated light. Eachdetector 56 is configured to generate an electronic sensory signal related to the magnitude of the radiation received thereon. Thecontroller 82 is configured to receive and compare each of the sensory signals to determine which one of thedetectors 56 was illuminated with the greatest magnitude of radiation. Thecontroller 82 may be configured to receive the sensory signals during a predefined time window in relation to the communication of the transmit signal to thesource element 54. - Referring to
FIGS. 5 and 6 , thecontroller 82 is further configured to determine the relative distance from thesensor 52 to atarget surface FIG. 5 , thecontroller 82 may be configured to estimate the relative amount of erosion at a location along thetarget surface detector 56 in thedetector array 55 illuminated with the greatest amount of radiation. For example, if adetector 56 located at the center of the detector array is determined by thecontroller 82 to be illuminated by a reflected beam, then thecontroller 82 may be configured to estimate that half of thetarget 22 material has been eroded at the position along thetarget surface sensor 52 to thetarget surface source element 54 and thedetector 56 being illuminated. For example, if the transmission angle a and the distance x between thesource element 54 and thenearest detector 56 inFIG. 5 are known, then equation (1) above may be used (assuming the incident angle β of the transmittedbeam 60 and the reflected angle β′ of the reflectedbeam 62 are equal) to determine the distance z between thesensor 52 and thetarget surface 23 as: -
FIG. 7 illustrates a block diagram of asensor assembly 102, such as thesensor circuitry 100 shown inFIG. 6 , according to another embodiment of the present invention. Thesensor assembly 102 shown inFIG. 7 comprises asource element 110 and a plurality of reception elements 112 (four shown) attached to athin profile arm 114, similar to thearm 44 shown inFIG. 3 . Thesource element 110 comprises a collimator, such as a lens, configured to collimate or focus light exiting anoptical fiber 116 to a desired beam diameter or spot size. Eachreception element 112 comprises a collimator, such as a lens, configured to collect light incident thereon into anoptical fiber assembly 118. Thesensor assembly 102 further comprises atransmitter 104 coupled to thesource element 110 through theoptical fiber 116 and areceiver 106 coupled to each of the plurality ofreception elements 112 through theoptical fiber assembly 118. Theoptical fiber assembly 118 comprises a plurality of optical fibers, each optical fiber configured to couple to onereception element 112. - Referring to
FIGS. 6 and 7 , thetransmitter 104 is configured to receive a transmit signal from thecontroller 82 and to transmit a beam of collimated light to thesource element 110 through theoptical fiber 116. The beam of collimated light may be a pulsed beam of collimated light. For eachreception element 112, thereceiver 106 is configured to receive a light beam through theoptical fiber assembly 118 and to generate an electronic sensory signal related to the magnitude of the radiation collected at therespective reception element 112. Thereceiver 106 is further configured to transmit each of the sensory signals to thecontroller 82. Thecontroller 82 is configured to receive and compare each of the sensory signals to determine which one of thereception elements 112 was illuminated with the greatest magnitude of radiation. Thecontroller 82 may be configured to receive the sensory signals during a predefined time window in relation to the communication of the transmit signal to thesource element 110. Thecontroller 82 is further configured to determine the relative distance from thesource element 110 to an object (not shown), as described above. - Referring to
FIGS. 1 and 6 , thecontroller 82 may be configured to interface with thechamber circuitry 90, includingchamber robot circuitry 92, to control the position of thesensor circuitry 100 relative to atarget 22 in thevacuum chamber 12, the placement and removal of asubstrate 26 on thepedestal 24, sputter processing times, and other sputtering process andvacuum chamber 12 operations. Thecontroller 82 may further be configured to perform computer functions such as executing software to perform desired calculations and tasks. - The
input device 84 may include, by way of example only, an Internet or other network connection, a mouse, a keypad or any device that allows an operator to enter data into thecontroller 82. Theoutput device 86 may include, by way of example only, a printer or a video display device. Thedata storage device 88 may include, by way of example only, drives that accept hard and floppy discs, tape cassettes, CD-ROM or DVD-ROM. - While the invention may be susceptible to various modifications and alternative forms, specific embodiments have been shown by way of example in the drawings and have been described in detail herein. However, it should be understood that the invention is not intended to be limited to the particular forms disclosed. Rather, the invention includes all modifications, equivalents, and alternatives falling within the spirit and scope of the invention as defined by the following appended claims.
Claims (31)
1. A sputtering apparatus, comprising:
a chamber;
a sputtering target located within the chamber; and
a sensor associated with the chamber and configured to measure at least one characteristic of a target surface of the sputtering target, wherein the sensor comprises:
a source element configured to project an energy beam onto the target surface of the sputtering target; and
a plurality of detectors disposed in a linear array and configured to detect a reflection of the energy beam from the surface of the sputtering target.
2. The apparatus of claim 1 , wherein the at least one characteristic comprises an erosion profile of the target surface.
3. The apparatus of claim 1 , wherein each of the plurality of detectors is configured to generate an electronic sensory signal related to an angle of the reflection of the energy beam incident thereon.
4. The apparatus of claim 1 , wherein each of the plurality of detectors comprises a collimator configured to collect the reflection of the energy beam incident thereon into a corresponding optical fiber.
5. The apparatus of claim 4 , further comprising a receiver optically coupled to each collimator through its corresponding optical fiber, the receiver configured to generate an electronic sensory signal for each collimator related to an angle of the reflection of the energy beam incident thereon.
6. The apparatus of claim 1 , wherein the energy beam is a collimated light beam.
7. The apparatus of claim 1 , wherein the source element comprises a collimator configured to collimate the energy beam as it exits an optical fiber.
8. The apparatus of claim 7 , further comprising a transmitter optically coupled to the source element through the optical fiber, the transmitter configured to transmit the energy beam to the collimator.
9. The apparatus of claim 1 , wherein the plurality of detectors comprises a first detector located in relation to the source element so as to be illuminated by the reflection of the energy beam when substantially none of the target surface at a target surface location is eroded.
10. The apparatus of claim 9 , wherein the plurality of detectors comprises a second detector located in relation to the source element so as to be illuminated by the reflection of the energy beam when substantially all of the target surface at the target surface location is eroded.
11. The apparatus of claim 10 , wherein the plurality of detectors comprises at least one intermediate detector positioned between the first detector and the second detector with a proportional distance relationship to the first detector and the second detector, and located in relation to the source element so as to be illuminated by the reflection of the energy beam when the target surface at the target surface location is partially eroded such that the proportional distance relationship correlates to the partially eroded amount.
12. A sputtering erosion sensor, comprising:
a sensor configured to emit an energy beam toward a target surface of a sputtering target and to detect a reflection of the energy beam from the target surface; and
a transporter configured to detachably bear the sensor and transport the sensor relative to the target surface.
13. The sensor of claim 12 , wherein the transporter is further configured as a substrate pickup arm configured to pick up and place a substrate on a pedestal.
14. The sensor of claim 13 , wherein the substrate pickup arm includes a pickup device selected from the group consisting of a clamp, a vacuum chuck, and an electrostatic chuck.
15. The sensor of claim 12 , wherein the transporter is an articulating arm configured for attachment to a robot.
16. The sensor of claim 12 , wherein the transporter is further configured to transport the sensor substantially parallel to the target surface along a substantially linear path between substantially a center of the target and substantially an outer edge of the target.
17. The sensor of claim 12 , wherein the sensor comprises a source element configured to emit the energy beam and a plurality of detectors disposed in a linear array.
18. The sensor of claim 17 , wherein the plurality of detectors comprises a first detector located in relation to the source element so as to be illuminated by the reflection of the energy beam when substantially none of the target surface at a target surface location is eroded.
19. The sensor of claim 18 , wherein the plurality of detectors comprises a second detector located in relation to the source element so as to be illuminated by the reflection of the energy beam when substantially all of the target surface at the target surface location is eroded.
20. The sensor of claim 19 , wherein the plurality of detectors comprises at least one intermediate detector positioned between the first detector and the second detector with a proportional distance relationship to the first detector and the second detector, and located in relation to the source element so as to be illuminated by the reflection of the energy beam when the target surface at the target surface location is partially eroded such that the proportional distance relationship correlates to the partially eroded amount.
21. A method of measuring at least one sputtering characteristic, comprising:
providing a sputtering target within a chamber;
providing a sensor within the chamber, the sensor comprising a source element and a plurality of detectors disposed in a linear array;
directing an energy beam from the source element onto a target surface of the sputtering target; and
detecting a reflection of the energy beam from the target surface of the sputtering target with at least one detector of the plurality of detectors.
22. The method of claim 21 , wherein the at least one sputtering characteristic comprises an erosion amount of the sputtering target.
23. The method of claim 21 , further comprising estimating an erosion amount of the target surface at a target surface location by measuring a time delay between emitting the energy beam and detecting the reflection of the energy beam.
24. The method of claim 21 , further comprising estimating an erosion amount of the target surface at a target surface location by measuring a phase difference between the energy beam and the reflection of the energy beam.
25. The method of claim 21 , further comprising estimating an erosion amount of the target surface at a target surface location by comparing a power level of the energy beam with a power level of the reflection of the energy beam.
26. The method of claim 21 , further comprising estimating an erosion amount of the target surface at a target surface location by detecting a location on the sensor illuminated by the reflection of the energy beam by using the plurality of detectors disposed in the linear array.
27. A method of developing a sputtering erosion profile, comprising:
transporting a sensor near a target surface location along a substantially linear path between substantially a center of a sputtering target and substantially an outer edge of the sputtering target;
illuminating the target surface location with an energy beam emitted from a source element born by the sensor;
detecting a reflection of the energy beam from a surface of the sputtering target at the target surface location with at least one detector born by the sensor; and
repeating the transporting, illuminating, and detecting for at least one additional target surface location along the substantially linear path to develop a sputtering erosion profile.
28. The method of claim 27 , further comprising estimating an erosion amount of the target surface at the target surface location by measuring a time delay between emitting the energy beam and detecting the reflection of the energy beam.
29. The method of claim 27 , further comprising estimating an erosion amount of the target surface at the target surface location by measuring a phase difference between the energy beam and the reflection of the energy beam.
30. The method of claim 27 , further comprising estimating an erosion amount of the target surface at the target surface location by comparing a power level of the energy beam with a power level of the reflection of the energy beam.
31. The method of claim 27 , further comprising estimating an erosion amount of the target surface at the target surface location by detecting a location on the sensor illuminated by the reflection of the energy beam by using a plurality of detectors disposed in a linear array.
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US10/923,233 US20050023132A1 (en) | 2003-01-27 | 2004-08-19 | Device for measuring the profile of a metal film sputter deposition target, and system and method employing same |
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US10/923,233 US20050023132A1 (en) | 2003-01-27 | 2004-08-19 | Device for measuring the profile of a metal film sputter deposition target, and system and method employing same |
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Also Published As
Publication number | Publication date |
---|---|
US6974524B1 (en) | 2005-12-13 |
US20060054497A1 (en) | 2006-03-16 |
US6811657B2 (en) | 2004-11-02 |
US20040144638A1 (en) | 2004-07-29 |
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