WO2018200139A1 - Improved laser light energy and dose control using repetition rate based gain estimators - Google Patents

Improved laser light energy and dose control using repetition rate based gain estimators Download PDF

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Publication number
WO2018200139A1
WO2018200139A1 PCT/US2018/025921 US2018025921W WO2018200139A1 WO 2018200139 A1 WO2018200139 A1 WO 2018200139A1 US 2018025921 W US2018025921 W US 2018025921W WO 2018200139 A1 WO2018200139 A1 WO 2018200139A1
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Prior art keywords
laser
repetition rate
voltage
gain estimator
gain
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PCT/US2018/025921
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French (fr)
Inventor
Yingbo Zhao
Kevin Michael O'brien
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Cymer LLC
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Cymer LLC
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Priority to CN201880026865.1A priority Critical patent/CN110546579B/en
Priority to KR1020197031397A priority patent/KR102274904B1/en
Priority to JP2019550185A priority patent/JP6948403B2/en
Publication of WO2018200139A1 publication Critical patent/WO2018200139A1/en
Anticipated expiration legal-status Critical
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/10069Memorized or pre-programmed characteristics, e.g. look-up table [LUT]
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70008Production of exposure light, i.e. light sources
    • G03F7/70025Production of exposure light, i.e. light sources by lasers
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03FPHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70Microphotolithographic exposure; Apparatus therefor
    • G03F7/70483Information management; Active and passive control; Testing; Wafer monitoring, e.g. pattern monitoring
    • G03F7/7055Exposure light control in all parts of the microlithographic apparatus, e.g. pulse length control or light interruption
    • G03F7/70558Dose control, i.e. achievement of a desired dose
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/10038Amplitude control
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/131Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/10038Amplitude control
    • H01S3/10046Pulse repetition rate control
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/102Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
    • H01S3/104Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling the active medium, e.g. by controlling the processes or apparatus for excitation in gas lasers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/1306Stabilisation of the amplitude

Definitions

  • the disclosed subject matter is in the field of laser light control and more specifically in the field of controlling the energy of a laser generated by a laser light source as may be used in semiconductor photolithography processes.
  • Photolithography is a commonly used process in the semiconductor industry.
  • Modem photolithography typically uses a laser light source, also known as a laser system, to provide very narrow band light pulses that illuminate a mask thus exposing photo-resistive material on silicon wafers, also known as substrates, in stepper-scanner devices, also known as scanners.
  • a laser light source also known as a laser system
  • stepper-scanner devices also known as scanners.
  • Advances in semiconductor device parameters have put increasing demands on the performance characteristics of the laser light sources and stepper-scanners used. Improvements in precision and speed of operation of these devices are increasingly needed.
  • the laser light source communicates desired laser light parameters to the laser light source to achieve a desired dosage of laser light energy for use in the photolithographic process.
  • the laser light source generates the laser light and outputs it to the stepper-scanner.
  • challenges in performing these operations For example, it can take some time for the generated laser light to stabilize on the desired parameters. Further, because of noise and other disturbances in the laser light source, it can be difficult to accurately generate the laser light at the desired energy level. What is needed are further improvements in how the laser tight source quickly and accurately generates the laser light to meet the desired parameters.
  • a system and method for laser light energy control and resulting dose control creates and uses a set of gain estimators, one for each of a range of laser light pulse repetition rates. When a new repetition rate is specified, its corresponding gain estimator is retrieved and used to adjust and fire the laser source. The resulting generated laser light thereby reduces convergence delay and, further, can repeatedly do so with subsequently specified repetition rates.
  • a method of laser light energy control comprising: receiving, in a laser system controller, a first laser trigger command and a voltage command; converting, by the laser system controller, the voltage command to a first energy target; determining, by the laser system controller, a first laser repetition rate based on a difference between the first laser trigger command and a previous laser trigger command; retrieving, by the laser system controller, a first repetition rate gain estimator corresponding to the first laser repetition rate; determining, by the laser system controller, a first laser voltage using the first energy target and the first repetition rate gain estimator; directing, by the laser system controller, a laser source to fire using the first laser voltage; receiving, in the laser system controller, a subsequent laser trigger command and a subsequent voltage command; converting, by the laser system controller, the subsequent voltage command to a second energy target; determining, by the laser system controller, a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the
  • a laser system for laser light energy control comprising: a laser system controller configured to: receive a first laser trigger command and a voltage command; convert the voltage command to a first energy target; determine a first laser repetition rate based on a difference between the first iaser trigger command and a previous laser trigger command; retrieve a first repetition rate gain estimator corresponding to the first iaser repetition rate; determine a first iaser voltage using the first energy target and the first repetition rate gain estimator; direct a iaser source to fire using the first iaser voltage; receive a subsequent Iaser trigger command and a subsequent voltage command; convert the subsequent voltage command to a second energy target; determine a second Iaser repetition rate based on a difference between the subsequent Iaser trigger command and the first Iaser trigger command, wherein the second iaser repetition rate is different than the first Iaser repetition rate; retrieve a second repetition rate gain estimator corresponding to the second laser repetition rate;
  • FIG. 1 is a block diagram of an exemplary Iaser system and scanner as may be used in one embodiment.
  • FIG. 2 is a graph showing characteristics of a generated iaser light as may be used in one embodiment.
  • FIG. 3 is a block diagram of a laser system controller as may be used in one embodiment.
  • FIG.4 is a flowchart of various embodiments of the present method of setting, updating, and using a set of gain estimators.
  • Described herein is a system and method for controlling the energy of a laser light source generated laser.
  • the desired energy of the Iaser light is achieved more rapidly and more accurately than with known approaches thus improving dose control in the photolithography process.
  • the operations and elements of this system and method will now be described.
  • FIG. 1 a block diagram 100 of a laser system 110 and scanner 140 as may be used in a modem deep ultraviolet ("DUV, e.g., having wavelengths in the range of 5 - 250 nanometers (nm) photolithography process and with the present approach can be seen.
  • DUV modem deep ultraviolet
  • the source of the laser light in laser system 110 is a laser source 120, which can be a single or dual chamber system, controlled by a controller 130 via communication 125.
  • laser source 120 fires the resulting laser light 115 travels to scanner 140, which is responsible for exposing the semiconductor wafer.
  • scanner 140 sends to laser system 110 via communication 135 desired parameters for the laser light to be generated by laser system 110.
  • photolithography process typically include such things as laser light wavelength, energy level and a timing trigger for when the laser system is to fire the laser.
  • the laser system generates the laser light 115 based on those parameters.
  • scanner 140 communicates additional desired parameters for further laser light to be generated by laser system 110.
  • FIG. 2 characteristics of the generated laser light can be seen in a graph form.
  • scanner 140 has communicated a series of differing timing triggers which resulted in laser system 110 generating laser light at a RepRate of 2000, then 6000, then 5990 and then 4000 laser pulses per second.
  • the actual de/dv (the inverse of the above-described dv/de), in degrees represented by a series of x's in the figure, is different at each of the differing RepRates.
  • the resulting estimated de/dv in degrees represented by a series of o's in the figure, converges to within a small deviation from the actual de/dv within approximately 100,000 (100k) laser pulses.
  • the present approach overcomes this problem by creating and storing a set of gain estimators each operable for a differing RepRate. Then, whenever the laser system is asked to fire the laser with a differing timing trigger interval, i.e., at a differing RepRate, a gain estimator to be operable at that RepRate can be used without waiting for convergence to the new de/dv. Hie benefit of this approach is then furthered when there are frequent changes in the RepRate because the convergence lag is avoided with each change.
  • controller 130 of FIG. 1 is shown having a stored RepRate Gain Estimator ("RRGE") table 301.
  • RRGE RepRate Gain Estimator
  • each row is a range of RepRates (e.g., 450 - 549, 550 - 649, etc.) with a corresponding RepRate Gain Estimator (e.g., RRGE 1, RRGE 2, RRGE 3, etc.) to be used with a RepRate in that range.
  • a gain estimator is a collection of data and a series of steps (i.e., logic and operations) that act on that data and the inputs to output the result.
  • steps i.e., logic and operations
  • One example of such a gain estimator is:
  • each stored gain estimator i.e., each RRGE in the table
  • values Xi and X2 which are the state of the estimator that get updated each time the estimator executes
  • k refers to 'Value before the update' while k+1 refers to "value after the update”
  • a, b, and c are constants determined by the system creator.
  • FIG. 4 a flowchart of a process 400 of setting, updating, and using a set of gain estimators according to various embodiments will now be described.
  • step 401 the gain estimators are set to default values. In one
  • the gain estimators i.e., the RepRate Gain Estimators
  • the RepRate Gain Estimators in the RepRate Gain Estimator Table 301 of laser controller 130 are set to default values by initially setting the data "X" state values, as discussed above with respect to FIG. 3.
  • the default values are set so that the RepRate Gain Estimators will output an average of typical dv/de values, which typically range from 0.02 to 0.2, and therefore the default values are set so tile RRGEs will output an average value of 0.11. It is to be understood that other default values can likewise be used and, further, that each gain estimator need not be set to the same default value.
  • step 403 a laser trigger (also known as a laser firing trigger) and a voltage command are received from the scanner by the laser system.
  • a laser trigger also known as a laser firing trigger
  • a voltage command are received from the scanner by the laser system.
  • this laser trigger and voltage command are received from scanner 140 by laser system 110 via communication 135 and the voltage command is determined by scanner 140 based on a desired laser energy level and its knowledge of the dv/de relationship, as described above. It is to be understood that the laser trigger and the voltage command can be sent as a single communication from the scanner to the laser source or can be sent as separate communications from the scanner to the laser source in any sequence or order. In various embodiments, other command signals (e.g., digitally encoded signals) may be used in place of a voltage command.
  • other command signals e.g., digitally encoded signals
  • step 405 the laser system converts the voltage command to an energy target. In one embodiment, this conversion is performed by laser system 110, and more particularly by laser system controller 130, based on its greater knowledge of the dv/de relationship within operations of the laser system and as is understood by one of skill in the art.
  • step 407 the laser system determines the RepRate of the laser. In one embodiment, this determination is performed by laser system 110, and more particularly by laser system controller 130, based on a difference between the received laser trigger command received from scanner 140 and a previously received laser trigger command from scanner 140.
  • step 409 the gain estimator for the determined RepRate is retrieved. In one embodiment, this is performed by retrieving a RRGE n in RRGE Table 301 corresponding to the determined RepRate.
  • step 411 the voltage with which to fire the laser, referred to herein as the laser voltage, is determined using the energy target and the retrieved gain estimator, in one embodiment, this is performed by laser system controller 130 in laser system 110 and, according to various embodiments, is performed according to the following formula:
  • the laser is fired.
  • the laser is fired by controller 130 directing laser source 120 to fire at the laser voltage, that is, the voltage computed by the RRGE corresponding to the trigger received from scanner 140.
  • the gain estimator is updated.
  • the gain estimator is updated by controller 130 calculating a new gain estimator tor the current laser pulse, based on a measured resulting energy from tie current laser pulse and using gain estimator calculation techniques known in the art, and the calculated new gain estimator is then stored in RRGE Table 301 corresponding to the RepRate determined in step 407.
  • all gain estimators are updated on each laser pulse by storing the calculated new gain estimator as new gain estimator values in RRGE Table 301 corresponding to all RepRates in the table. Updating all gain estimators on each laser pulse may provide a more accurate gain estimator for each RepRate than using any previously stored gain estimator (including the default gain estimator).
  • step 401 The process then returns to step 401 to receive a new laser trigger and voltage command.
  • the set of gain estimators is instead created without receiving commands from a scanner, in this embodiment, the voltage command and laser trigger is either generated internally within the laser system or by laser system operator input. Regardless of whether this embodiment or the one described with reference to FIG. 4 is used, the process of creating and updating the set of gain estimators can be considered a training mode for the laser system and, as such, need not actually involve any exposure of the generated laser light to a wafer in a scanner.
  • a static set of stored gain estimators corresponding to various RepRates, previously set and updated as described above with reference to FIG.4, are then used to fire the laser without continuing to update the gain estimators as described above with reference to step 415 of FIG. 4.
  • step 413 of firing the laser then returns to step 403 of receiving a laser trigger and voltage command without performing step 415 of updating gain estimators.
  • laser system controller 130 can be any computing system comprising a processor and memory, including a personal computer, server, or other processing system, that runs software instructions for performing the described operations which instructions may themselves have come from or reside on a computer readable storage medium.
  • laser system controller 130 can be any dedicated hardware such as an application specific integrated circuit (ASIC) or other hardwired device, with or without firmware, that is specifically configured to perform the described operations.
  • ASIC application specific integrated circuit
  • a method of laser light energy control comprising:
  • a laser system for laser light energy control comprising:
  • a laser system controller configured to:
  • [00077] determine a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the first laser repetition rate;
  • [00080] direct the laser source to fire using the second laser voltage.
  • a method of laser light energy control comprising:
  • each gain estimator in said set of gain estimators corresponding to a range of laser repetition rates
  • activating said laser source to generate laser light said activating being responsive to a laser voltage determined using said first gain estimator.
  • each gain estimator pertains to the relationship between an amount of voltage applied to said laser source and an amount of energy in laser light generated by said laser source.
  • a method of laser light energy control for a laser light source comprising:
  • each of said training-mode laser activation signal including at least a training-mode laser trigger command and training-mode voltage command
  • each gain estimator pertains to the relationship between an amount of voltage applied to said laser source and an amount of energy in laser light generated by said laser source.

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
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  • Optics & Photonics (AREA)
  • General Physics & Mathematics (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
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Abstract

A laser system's laser light energy control and resulting dose control is improved by creating and using a set of gain estimators, one for each of a set or range of laser Sight pulse repetition rates. When a new repetition rate is used, its corresponding gain estimator is retrieved, used to compute the voltage to fire the Iaser source, and updated. The resulting generated Iaser light thereby avoids the convergence delay inherent in prior iaser systems and, further, can repeatedly do so with subsequent specified repetition rates.

Description

IMPROVED LASER LIGHT ENERGY AND DOSE CONTROL USING REPETITION
RATE. BASED GAIN ESTIMATORS
CROSS-REFERENCE TO RELATED APPLICATION
[00013 This application claims priority of US application 15/495,245 which was filed on April 24, 2017 and which is incorporated herein in its entirety by reference.
BACKGROUND FIELD OF THE INVENTION
[0002] The disclosed subject matter is in the field of laser light control and more specifically in the field of controlling the energy of a laser generated by a laser light source as may be used in semiconductor photolithography processes.
RELATED ART
[0003] Photolithography is a commonly used process in the semiconductor industry. Modem photolithography typically uses a laser light source, also known as a laser system, to provide very narrow band light pulses that illuminate a mask thus exposing photo-resistive material on silicon wafers, also known as substrates, in stepper-scanner devices, also known as scanners. Advances in semiconductor device parameters have put increasing demands on the performance characteristics of the laser light sources and stepper-scanners used. Improvements in precision and speed of operation of these devices are increasingly needed.
[0004] As is known in the art, the stepper-scanner device periodically
communicates desired laser light parameters to the laser light source to achieve a desired dosage of laser light energy for use in the photolithographic process. In turn, the laser light source generates the laser light and outputs it to the stepper-scanner. There are, however, numerous challenges in performing these operations. For example, it can take some time for the generated laser light to stabilize on the desired parameters. Further, because of noise and other disturbances in the laser light source, it can be difficult to accurately generate the laser light at the desired energy level. What is needed are further improvements in how the laser tight source quickly and accurately generates the laser light to meet the desired parameters. SUMMARY
[0005] A system and method for laser light energy control and resulting dose control creates and uses a set of gain estimators, one for each of a range of laser light pulse repetition rates. When a new repetition rate is specified, its corresponding gain estimator is retrieved and used to adjust and fire the laser source. The resulting generated laser light thereby reduces convergence delay and, further, can repeatedly do so with subsequently specified repetition rates.
[0006] In one embodiment is a method of laser light energy control comprising: receiving, in a laser system controller, a first laser trigger command and a voltage command; converting, by the laser system controller, the voltage command to a first energy target; determining, by the laser system controller, a first laser repetition rate based on a difference between the first laser trigger command and a previous laser trigger command; retrieving, by the laser system controller, a first repetition rate gain estimator corresponding to the first laser repetition rate; determining, by the laser system controller, a first laser voltage using the first energy target and the first repetition rate gain estimator; directing, by the laser system controller, a laser source to fire using the first laser voltage; receiving, in the laser system controller, a subsequent laser trigger command and a subsequent voltage command; converting, by the laser system controller, the subsequent voltage command to a second energy target; determining, by the laser system controller, a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the first laser repetition rate; retrieving, by the laser system controller, a second repetition rate gain estimator corresponding to the second laser repetition rate; determining, by the laser system controller, a second laser voltage using the second energy target and tine second repetition rate gain estimator; and, directing, by the laser system controller, the laser source to fire using the second laser voltage.
[0007] In another embodiment is a laser system for laser light energy control comprising: a laser system controller configured to: receive a first laser trigger command and a voltage command; convert the voltage command to a first energy target; determine a first laser repetition rate based on a difference between the first iaser trigger command and a previous laser trigger command; retrieve a first repetition rate gain estimator corresponding to the first iaser repetition rate; determine a first iaser voltage using the first energy target and the first repetition rate gain estimator; direct a iaser source to fire using the first iaser voltage; receive a subsequent Iaser trigger command and a subsequent voltage command; convert the subsequent voltage command to a second energy target; determine a second Iaser repetition rate based on a difference between the subsequent Iaser trigger command and the first Iaser trigger command, wherein the second iaser repetition rate is different than the first Iaser repetition rate; retrieve a second repetition rate gain estimator corresponding to the second laser repetition rate; determine a second laser voltage using the second energy target and the second repetition rate gain estimator; and, direct the iaser source to fire using the second iaser voltage.
BRIEF DESCRIPTION OF THE DRAWING
[0008] Various embodiments are disclosed in the following detailed description and the accompanying drawing.
[0009] FIG. 1 is a block diagram of an exemplary Iaser system and scanner as may be used in one embodiment.
[00010] FIG. 2 is a graph showing characteristics of a generated iaser light as may be used in one embodiment.
[00011] FIG. 3 is a block diagram of a laser system controller as may be used in one embodiment.
[00012] FIG.4 is a flowchart of various embodiments of the present method of setting, updating, and using a set of gain estimators.
[00013] Described herein is a system and method for controlling the energy of a laser light source generated laser. In the present approach, the desired energy of the Iaser light is achieved more rapidly and more accurately than with known approaches thus improving dose control in the photolithography process. The operations and elements of this system and method will now be described. [00014] Referring now to FIG. 1 , a block diagram 100 of a laser system 110 and scanner 140 as may be used in a modem deep ultraviolet ("DUV, e.g., having wavelengths in the range of 5 - 250 nanometers (nm) photolithography process and with the present approach can be seen. The source of the laser light in laser system 110 is a laser source 120, which can be a single or dual chamber system, controlled by a controller 130 via communication 125. When laser source 120 fires the resulting laser light 115 travels to scanner 140, which is responsible for exposing the semiconductor wafer.
[00015] As is known in the art, scanner 140 sends to laser system 110 via communication 135 desired parameters for the laser light to be generated by laser system 110. The parameters, intended to achieve a desired exposure in the
photolithography process, typically include such things as laser light wavelength, energy level and a timing trigger for when the laser system is to fire the laser. In turn, the laser system generates the laser light 115 based on those parameters. This process then continues as scanner 140 communicates additional desired parameters for further laser light to be generated by laser system 110.
[00016] As is known in the art, there is a relationship between the amount of voltage applied to laser source 120, as specified by controller 130 via communication 125, and the resulting energy in the generated laser light. This relationship is commonly represented as dv/de, which is the derivative of voltage with respect to energy. U.S. Patent No 7,756,171 and U,S. Patent Application No. 11/900,527, each incorporated herein by reference, describe these aspects known in the art. It is known in the art to use what is called a gain estimator, an algorithm for estimating the dv/de relationship. As stated above, there is a relationship between the amount of voltage applied to laser source 120 and the resulting energy in the generated laser light. In general, the greater the applied voltage the greater the resulting energy. However, this relationship is affected by noise and other disturbances in the laser system. As such, rather than simply presuming a given voltage will always result in the same energy, a gain estimator algorithm is created by varying (or dithering, i.e., dv) the voltage locally and then using the corresponding response in energy (i.e., de) to compute de/dv as an output. This de/dv, which is the output of the gain estimator, is then used to compute the final voltage value that the laser system then uses to generate the laser light at the desired energy level. U.S. Patent No 8102,889, incorporated herein by reference herein, describes these aspects known in the art.
[00017] However, while such known usage of a gain estimator can reduce or eliminate error or variability of the laser light energy, it still fails to address the problem of the generated laser light not providing the desired energy level during the transient phase or convergence lag. In other words, should the scanner request laser light at a different repetition rate (i.e., the number of laser pulses fired in a second, hereinafter "RepRate" or "rr", as dictated by the timing trigger received from scanner 140), laser energy performance will be temporarily worse until the gain estimator finds the new de/dv again because, as shown in FIG. 2, RepRate affects the de/dv gain.
[00018] Referring now to FIG. 2, characteristics of the generated laser light can be seen in a graph form. In this example, scanner 140 has communicated a series of differing timing triggers which resulted in laser system 110 generating laser light at a RepRate of 2000, then 6000, then 5990 and then 4000 laser pulses per second. As shown, the actual de/dv (the inverse of the above-described dv/de), in degrees represented by a series of x's in the figure, is different at each of the differing RepRates. As also shown, the resulting estimated de/dv, in degrees represented by a series of o's in the figure, converges to within a small deviation from the actual de/dv within approximately 100,000 (100k) laser pulses. Other experiments have shown that it can take up to about 30 seconds for this convergence to occur (with time ·=. number of laser pulses divided by laser pulse RepRate, it takes about 16.67 seconds for 100k laser pulses to occur at a RepRate of 6,000 and about 50 seconds for 100k laser pulses to occur at a RepRate of 2,000, thus confirming that 30 seconds is a reasonable estimate). This convergence lag, that is, the number of laser pulses and/or the time between when the laser source is directed to fire at a new RepRate and the generated laser light achieves the desired energy level, detrimentally affects the desired wafer dose in scanner 140.
[00019] The present approach overcomes this problem by creating and storing a set of gain estimators each operable for a differing RepRate. Then, whenever the laser system is asked to fire the laser with a differing timing trigger interval, i.e., at a differing RepRate, a gain estimator to be operable at that RepRate can be used without waiting for convergence to the new de/dv. Hie benefit of this approach is then furthered when there are frequent changes in the RepRate because the convergence lag is avoided with each change.
[00020] Referring now to FIG. 3, controller 130 of FIG. 1 is shown having a stored RepRate Gain Estimator ("RRGE") table 301. As shown in table 301, each row is a range of RepRates (e.g., 450 - 549, 550 - 649, etc.) with a corresponding RepRate Gain Estimator (e.g., RRGE 1, RRGE 2, RRGE 3, etc.) to be used with a RepRate in that range.
[00021] As further explanation, and as would be understood by one of skill in the art in light of the teachings herein, a gain estimator is a collection of data and a series of steps (i.e., logic and operations) that act on that data and the inputs to output the result. One example of such a gain estimator is:
Figure imgf000008_0001
[00022] where each stored gain estimator (i.e., each RRGE in the table) thus includes this data denoted as values Xi and X2), which are the state of the estimator that get updated each time the estimator executes, k refers to 'Value before the update' while k+1 refers to "value after the update", and a, b, and c are constants determined by the system creator.
[00023] In this way, any time a new RepRate is desired or specified, again via the timing trigger received by the laser system from the scanner, a corresponding RRGE can immediately be retrieved and used without incurring any convergence lag. !t is to be understood that the correspondence between RepRate ranges and corresponding RepRate Gain Estimators can be stored in any data storage format, structure or layout and is not limited to the specific form of the table shown in the figure. Further, the particular RepRate range or quantum of values corresponding to a given RepRate Gain Estimator can be as broad or narrow as desired as they are only limited by available storage capacity.
[00024] Referring now to FIG. 4, a flowchart of a process 400 of setting, updating, and using a set of gain estimators according to various embodiments will now be described.
[00025] in step 401 , the gain estimators are set to default values. In one
embodiment, the gain estimators (i.e., the RepRate Gain Estimators) in the RepRate Gain Estimator Table 301 of laser controller 130 are set to default values by initially setting the data "X" state values, as discussed above with respect to FIG. 3. In one still further embodiment, the default values are set so that the RepRate Gain Estimators will output an average of typical dv/de values, which typically range from 0.02 to 0.2, and therefore the default values are set so tile RRGEs will output an average value of 0.11. It is to be understood that other default values can likewise be used and, further, that each gain estimator need not be set to the same default value.
[00026] In step 403 a laser trigger (also known as a laser firing trigger) and a voltage command are received from the scanner by the laser system. In one
embodiment this laser trigger and voltage command are received from scanner 140 by laser system 110 via communication 135 and the voltage command is determined by scanner 140 based on a desired laser energy level and its knowledge of the dv/de relationship, as described above. It is to be understood that the laser trigger and the voltage command can be sent as a single communication from the scanner to the laser source or can be sent as separate communications from the scanner to the laser source in any sequence or order. In various embodiments, other command signals (e.g., digitally encoded signals) may be used in place of a voltage command.
[00027] In step 405, the laser system converts the voltage command to an energy target. In one embodiment, this conversion is performed by laser system 110, and more particularly by laser system controller 130, based on its greater knowledge of the dv/de relationship within operations of the laser system and as is understood by one of skill in the art. [00028] In step 407, the laser system determines the RepRate of the laser. In one embodiment, this determination is performed by laser system 110, and more particularly by laser system controller 130, based on a difference between the received laser trigger command received from scanner 140 and a previously received laser trigger command from scanner 140.
[00029] In step 409, the gain estimator for the determined RepRate is retrieved. In one embodiment, this is performed by retrieving a RRGE n in RRGE Table 301 corresponding to the determined RepRate.
[00030] In step 411 , the voltage with which to fire the laser, referred to herein as the laser voltage, is determined using the energy target and the retrieved gain estimator, in one embodiment, this is performed by laser system controller 130 in laser system 110 and, according to various embodiments, is performed according to the following formula:
Figure imgf000010_0001
[00031]
[00032]
[00033]
[00034]
[00035]
[00036]
[00037]
Figure imgf000010_0002
[00038] In step 413, the laser is fired. In one embodiment, the laser is fired by controller 130 directing laser source 120 to fire at the laser voltage, that is, the voltage computed by the RRGE corresponding to the trigger received from scanner 140.
[00039] In step 415, the gain estimator is updated. In one embodiment, the gain estimator is updated by controller 130 calculating a new gain estimator tor the current laser pulse, based on a measured resulting energy from tie current laser pulse and using gain estimator calculation techniques known in the art, and the calculated new gain estimator is then stored in RRGE Table 301 corresponding to the RepRate determined in step 407. In other embodiments all gain estimators are updated on each laser pulse by storing the calculated new gain estimator as new gain estimator values in RRGE Table 301 corresponding to all RepRates in the table. Updating all gain estimators on each laser pulse may provide a more accurate gain estimator for each RepRate than using any previously stored gain estimator (including the default gain estimator).
[00040] The process then returns to step 401 to receive a new laser trigger and voltage command.
[00041] In an alternative embodiment, the set of gain estimators is instead created without receiving commands from a scanner, in this embodiment, the voltage command and laser trigger is either generated internally within the laser system or by laser system operator input. Regardless of whether this embodiment or the one described with reference to FIG. 4 is used, the process of creating and updating the set of gain estimators can be considered a training mode for the laser system and, as such, need not actually involve any exposure of the generated laser light to a wafer in a scanner.
[00042] In an alternative embodiment, a static set of stored gain estimators corresponding to various RepRates, previously set and updated as described above with reference to FIG.4, are then used to fire the laser without continuing to update the gain estimators as described above with reference to step 415 of FIG. 4. In such an embodiment (comprising steps 403 through 413), step 413 of firing the laser then returns to step 403 of receiving a laser trigger and voltage command without performing step 415 of updating gain estimators.
[00043] The embodiments discussed herein are illustrative of the present invention. As these embodiments of the present invention are described with reference to illustrations, various modifications or adaptations of the methods and or specific structures described may become apparent to those skilled in the art. Ail such modifications, adaptations, or variations that rely upon the teachings of the present invention, and through which these teachings have advanced the art, are considered to be within the spirit and scope of the present invention. Hence, the description and the drawing should not be considered in a limiting sense, as it is understood that the present invention is in no way limited to only the embodiments illustrated.
[00044] It is also to be understood that alternative sequences and mathematical formulas could be used within the spirit and meaning of the present invention as described herein.
[00045] Likewise, it is to be understood that laser system controller 130 can be any computing system comprising a processor and memory, including a personal computer, server, or other processing system, that runs software instructions for performing the described operations which instructions may themselves have come from or reside on a computer readable storage medium. Alternatively, laser system controller 130 can be any dedicated hardware such as an application specific integrated circuit (ASIC) or other hardwired device, with or without firmware, that is specifically configured to perform the described operations. Other aspects of the invention are set out in the following number clauses.
[00046] 1. A method of laser light energy control comprising:
[00047] receiving, in a laser system controller, a first laser trigger command and a voltage command;
[00048] converting, by the laser system controller, the voltage command to a first energy target;
[00049] determining, by the laser system controller, a first laser repetition rate based on a difference between the first laser trigger command and a previous laser trigger command;
[00050] retrieving, by the laser system controller, a first repetition rate gain estimator corresponding to the first laser repetition rate;
[00051] determining, by the laser system controller, a first laser voltage using the first energy target and the first repetition rate gain estimator;
[00052] directing, by the laser system controller, a laser source to fire using the first laser voltage;
[00053] receiving, in the laser system controller, a subsequent laser trigger command and a subsequent voltage command; [00054] converting, by the laser system controller, the subsequent voltage command to a second energy target;
[00055] determining, by the laser system controller, a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the first laser repetition rate;
[00056] retrieving, by the laser system controller, a second repetition rate gain estimator corresponding to the second laser repetition rate;
[00057] determining, by the laser system controller, a second laser voltage using the second energy target and the second repetition rate gain estimator; and,
[00058] directing, by the laser system controller, the laser source to tire using the second laser voltage.
[00059] 2. The method of clause 1 further comprising before the steps of clause 1:
[00060] setting tine first repetition rate gain estimator and the second repetition rate gain estimator to a default value.
[0006] ] 3. The method of clause 2 further comprising:
[00062] updating the first repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
[00063] updating the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
[00064] 4. The method of clause 2 further comprising:
[00065] updating the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
[00066] updating the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command. [00067] 5. A laser system for laser light energy control comprising:
[00068] a laser system controller configured to:
[00069] receive a first laser trigger command and a voltage command;
[00070] convert the voltage command to a first energy target;
[00071] determine a first laser repetition rate based on a difference between the first laser trigger command and a previous laser trigger command;
[00072] retrieve a first repetition rate gain estimator corresponding to the first laser repetition rate;
[00073] determine a first laser voltage using the first energy target and the first repetition rate gain estimator;
[00074] direct a laser source to fire using the first laser voltage;
[00075] receive a subsequent laser trigger command and a subsequent voltage command;
[00076] convert the subsequent voltage command to a second energy target
[00077] determine a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the first laser repetition rate;
[00078] retrieve a second repetition rate gain estimator corresponding to the second laser repetition rate;
[00079] determine a second laser voltage using the second energy target and the second repetition rale gain estimator; and,
[00080] direct the laser source to fire using the second laser voltage.
[0008] ] 6. Hie laser system of clause 5, wherein the laser system controller is further configured to set the first repetition rate gain estimator and the second repetition rate gain estimator to a default value before receiving the first laser trigger command and the voltage command.
[00082] 7. The laser system of clause 6, wherein the laser system controller is further configured to:
[00083] update the first repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and, [00084] update the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
[00085] 8. The laser system of clause 6, wherein the laser system controller is further configured to:
[00086] update the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
[00087] update the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
[00088] 9. In a photolithography system, said photolithography system having at least a laser source and scanner, a method of laser light energy control comprising:
[00089] providing a set of gain estimators, each gain estimator in said set of gain estimators corresponding to a range of laser repetition rates;
[00090] receiving communication from said scanner of said photolithography system, said communication including a laser trigger command and a voltage
command;
[00091] determining a first laser repetition rate corresponding to said
communication;
[00092] retrieving a first gain estimator from said set of gain estimators, said first gain estimator being associated with a first range of laser repetition rates, said first range of laser repetition rates includes said first laser repetition rate; and
[00093] activating said laser source to generate laser light, said activating being responsive to a laser voltage determined using said first gain estimator.
[00094] 10. The method of clause 9 wherein said photolithography system is a deep UV (DUV) photolithography system. [00095] 11 - Hie method of clause 9 wherein said each gain estimator pertains to the relationship between an amount of voltage applied to said laser source and an amount of energy in laser light generated by said laser source.
[00096] 12. The method of clause 9 further comprising updating said first gain estimator after said activating, said updating includes obtaining a measured energy in said laser light and calculating an updated gain estimator value based on at least said measured energy.
[00097] 13. The method of clause 9 further comprising updating said set of gain estimators after said activating, said updating includes obtaining a measured energy in said laser light and calculating updated gain estimator values for said set of gain estimators based on at least said measured energy.
[00098] 14. A method of laser light energy control for a laser light source, comprising:
[00099] creating a set of gain estimators, each gain estimator in said set of gain estimators corresponding to a range of laser repetition rates, said creating including at least:
[000100] a) generating a training-mode laser activation signal, each of said training- mode laser activation signal including at least a training-mode laser trigger command and training-mode voltage command,
[000101] b) determining a laser repetition rate corresponding to said training-mode laser activation signal,
[000102] c) activating said laser source responsive to said training-mode laser activation signal to generate laser pulses,
[000103] d) varying a voltage level supplied to said laser source to cause an energy level of said laser pulses to reach a desired energy level,
[000104] e) employing the voltage level that causes said energy of said laser pulses to reach said desired energy level to calculate a gain estimator for said laser repetition rate, and
[000105] f) repeating steps a) to e) with different training-mode laser activation signals to obtain said set of gain estimators; and [000106] employing said set of gain estimators to generate laser light for performing wafer photolithography.
[000107] 15. The method of clause 14 wherein said employing comprising:
[000108] receiving communication from a scanner of a photolithography system, said communication including a laser trigger command and a voltage command;
[000109] determining a first laser repetition rate corresponding to said
communication;
[000110] retrieving a first gain estimator from said set of gain estimators, said first gain estimator being associated with a first range of laser repetition rates, said first range of laser repetition rates includes said first laser repetition rate; and
[00011] ] activating said laser source to generate said laser light, said activating being responsive to a laser voltage determined using said first gain estimator.
[000112] 16. The method of clause 15 wherein said photolithography system is a deep UV (DUV) photolithography system.
[000113] 17. The method of clause 15 wherein said each gain estimator pertains to the relationship between an amount of voltage applied to said laser source and an amount of energy in laser light generated by said laser source.
[000114] 18. The method of clause 15 further comprising updating said first gain estimator after said activating, said updating includes obtaining a measured energy in said laser light and calculating an updated gain estimator value based on at least said measured energy.
[000115] 19. The method of clause 15 further comprising updating said set of gain estimators after said activating, said updating includes obtaining a measured energy in said laser light and calculating updated gain estimator values for said set of gain estimators based on at least said measured energy.

Claims

CLAIMS What is claimed is:
1. A method of laser light energy control comprising:
receiving, in a laser system controller, a first laser trigger command and a voltage command;
converting, by the laser system controller, the voltage command to a first energy target;
determining, by the laser system controller, a first laser repetition rate based on a difference between the first laser trigger command and a previous laser trigger command;
retrieving, by the laser system controller, a first repetition rate gain estimator corresponding to the first laser repetition rate;
determining, by the laser system controller, a first laser voltage using the first energy target and the first repetition rate gain estimator;
directing, by the laser system controller, a laser source to fire using the first laser voltage;
receiving, in the laser system controller, a subsequent laser trigger command and a subsequent voltage command;
converting, by the laser system controller, the subsequent voltage command to a second energy target;
determining, by the laser system controller, a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the first laser repetition rate;
retrieving, by the laser system controller, a second repetition rate gain estimator corresponding to the second laser repetition rate;
determining, by the laser system controller, a second laser voltage using tine second energy target and the second repetition rate gain estimator; and,
directing, by the laser system controller, the laser source to fire using the second laser voltage.
2. The method of claim 1 further comprising before the steps of claim 1 : setting the first repetition rate gain estimator and the second repetition rate gain estimator to a default value.
3. The method of claim 2 further comprising:
updating the first repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
updating the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
4. The method of claim 2 further comprising:
updating the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
updating the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
5. A laser system for laser light energy contra! comprising:
a laser system controller configured to:
receive a first laser trigger command and a voltage command;
convert the voltage command to a first energy target;
determine a first laser repetition rate based on a difference between the first laser trigger command and a previous laser trigger command;
retrieve a first repetition rate gain estimator corresponding to the first laser repetition rate; determine a first laser voltage using the first energy target and the first repetition rate gain estimator;
direct a laser source to fire using the first laser voltage;
receive a subsequent laser trigger command and a subsequent voltage command;
convert the subsequent voltage command to a second energy target;
determine a second laser repetition rate based on a difference between the subsequent laser trigger command and the first laser trigger command, wherein the second laser repetition rate is different than the first laser repetition rate;
retrieve a second repetition rate gain estimator corresponding to the second laser repetition rate;
determine a second laser voltage using the second energy target and the second repetition rate gain estimator; and,
direct the laser source to fire using the second laser voltage.
6. The laser system of claim 5, wherein the laser system controller is further configured to set the first repetition rate gain estimator and the second repetition rate gain estimator to a default value before receiving the first laser trigger command and the voltage command.
7. The laser system of claim 6, wherein the laser system controller is further configured to:
update the first repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
update the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
8. The laser system of claim 6, wherein the laser system controller is further configured to: update the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the first laser voltage and before receiving the subsequent laser trigger command and the subsequent voltage command; and,
update the first repetition rate gain estimator and the second repetition rate gain estimator after directing the laser source to fire using the second laser voltage and before receiving any other laser trigger command and any other voltage command.
9. In a photolithography system, said photolithography system having at least a laser source and scanner, a method of laser light energy control comprising: providing a set of gain estimators, each gain estimator in said set of gain estimators corresponding to a range of laser repetition rates;
receiving communication from said scanner of said photolithography system, said communication including a laser trigger command and a voltage command;
determining a first laser repetition rate corresponding to said communication; retrieving a first gain estimator from said set of gain estimators, said first gain estimator being associated with a first range of laser repetition rates, said first range of laser repetition rates includes said first laser repetition rate; and
activating said laser source to generate laser light, said activating being responsive to a laser voltage determined using said first gain estimator,
10. The method of claim 9 wherein said photolithography system is a deep U V (DU V) photolithography system.
11. The method of claim 9 wherein said each gain estimator pertains to the relationship between an amount of voltage applied to said laser source and an amount of energy in laser light generated by said laser source.
12. The method of claim 9 further comprising updating said first gain estimator after said activating, said updating includes obtaining a measured energy in said laser tight and calculating an updated gain estimator value based on at least said measured energy.
13. The method of claim 9 further comprising updating said set of gain estimators after said activating, said updating includes obtaining a measured energy in said laser light and calculating updated gain estimator values for said set of gain estimators based on at least said measured energy.
14. A method of laser light energy control for a laser light source, comprising: creating a set of gain estimators, each gain estimator in said set of gain estimators corresponding to a range of laser repetition rates, said creating including at least:
a) generating a training-mode laser activation signal, each of said training-mode laser activation signal including at least a training-mode laser trigger command and training-mode voltage command,
b) determining a laser repetition rate corresponding to said training-mode laser activation signal,
c) activating said laser source responsive to said training-mode laser activation signal to generate laser pulses,
d) varying a voltage level supplied to said laser source to cause an energy level of said laser pulses to reach a desired energy level,
e) employing the voltage level that causes said energy of said laser pulses to reach said desired energy level to calculate a gain estimator for said laser repetition rate, and
f) repeating steps a) to e) with different training-mode laser activation signals to obtain said set of gain estimators; and
employing said set of gain estimators to generate laser light for performing wafer photolithography.
15. The method of claim 14 wherein said employing comprising: receiving communication from a scanner of a photolithography system, said communication including a laser trigger command and a voltage command;
determining a first laser repetition rate corresponding to said communication; retrieving a first gain estimator from said set of gain estimators, said first gain estimator being associated with a first range of laser repetition rates, said first range of laser repetition rates includes said first laser repetition rate; and
activating said laser source to generate said laser light, said activating being responsive to a laser voltage determined using said first gain estimator.
16. The method of claim 15 wherein said photolithography system is a deep UV (DUV) photolithography system.
17. The method of claim 15 wherein said each gain estimator pertains to the relationship between an amount of voltage applied to said laser source and an amount of energy in laser light generated by said laser source.
18. The method of claim 15 further comprising updating said first gain estimator after said activating, said updating includes obtaining a measured energy in said laser light and calculating an updated gain estimator value based on at feast said measured energy.
19. The method of claim 15 further comprising updating said set of gain estimators after said activating, said updating includes obtaining a measured energy in said laser light and calculating updated gain estimator values for said set of gain estimators based on at least said measured energy.
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