The present application claims priority from Japanese Patent Application No. 2009-122647 filed on May 21, 2009, the contents of which are incorporated herein by reference in their entirety.
1. Field of the Invention
The present invention relates to an apparatus and a method for measuring and controlling a trajectory (track) of a droplet target to be used for generating plasma radiating EUV (extreme ultraviolet) light in a chamber apparatus of an LPP (laser produced plasma) type EUV light source apparatus for generating EUV light to be used for exposure of semiconductor wafers or the like.
2. Description of a Related Art
In recent years, as semiconductor processes become finer, photolithography has been making rapid progress toward finer fabrication. In the next generation, microfabrication at 60 nm to 45 nm, further, microfabrication at 32 nm and beyond will be required. Accordingly, in order to fulfill the requirement for microfabrication at 32 nm and beyond, for example, exposure equipment is expected to be developed by combining an EUV light source for generating EUV light having a wavelength of about 13 nm and reduced projection reflective optics.
As the EUV light source, there are three kinds of light sources, which include an LPP (laser produced plasma) light source using plasma generated by irradiating a target with a laser beam, a DPP (discharge produced plasma) light source using plasma generated by discharge, and an SR (synchrotron radiation) light source using orbital radiation. Among them, the LPP light source has advantages that extremely high intensity close to black body radiation can be obtained because plasma density can be considerably made larger, and that the light of only the particular waveband can be radiated by selecting the target material. Further, the LPP light source has advantages that an extremely large collection solid angle of 2π to 4π steradian can be ensured because it is a point light source having substantially isotropic angle distribution and there is no structure such as electrodes surrounding the plasma light source and so on. Therefore, the LPP light source is considered to be predominant as a light source for EUV lithography, which requires power of more than several tens of watts.
Here, a principle of generating EUV light in the LPP light source will be explained. A target material supplied into a chamber is irradiated with a driver laser beam, and thereby, the target material is excited and turned into plasma. From the plasma, various wavelength components including EUV light are radiated. Then, EUV light is reflected and collected by using an EUV collector mirror for highly reflecting a specific wavelength component (for example, a component having a wavelength of 13.5 nm), and outputted to a device using EUV light (for example, exposure unit). For the purpose, on a reflection surface of the EUV collector mirror, for example, a multilayer coating (Mo/Si multilayer coating) in which molybdenum (Mo) thin coatings and silicon (Si) thin coatings are alternately stacked is formed.
In the LPP light source, as the target material to be used for generating plasma radiating EUV light, liquid tin is considered to be a predominant material. Accordingly, in the LPP light source, a target delivery mechanism is provided for injecting tin melted at a high temperature from a target injection nozzle and supplying it in a droplet state to a predetermined plasma generation position. Here, the predetermined plasma generation position is a position on which a pulse laser beam is focused by using a laser beam focusing optics, and, when the target material passing through the position is irradiated with the pulse laser beam, plasma is generated.
According to one aspect of the present invention, there is provided an apparatus for measuring and controlling a target trajectory within a chamber apparatus for generating extreme ultraviolet light from plasma generated by irradiating a droplet target supplied from a target injection nozzle with a driver laser beam from an external driver laser, and the apparatus includes: a nozzle adjustment mechanism for adjusting at least one of a position and an angle of the target injection nozzle; a target trajectory measuring unit for measuring a target trajectory formed by a droplet target supplied from the target injection nozzle to obtain trajectory information on the target trajectory; a target trajectory angle detecting unit for obtaining a value related to an angle deviation between the target trajectory represented by the trajectory information obtained by the target trajectory measuring unit and a predetermined target trajectory; and a nozzle adjustment controller for controlling the nozzle adjustment mechanism based on the value related to the angle deviation obtained by the target trajectory angle detecting unit such that the droplet target passes through a predetermined position.
Further, according to another aspect of the present invention, there is provided a method of measuring and controlling a target trajectory within a chamber apparatus for generating extreme ultraviolet light from plasma generated by irradiating a droplet target supplied from a target injection nozzle with a driver laser beam from an external driver laser, and the method includes the steps of: (a) measuring a target trajectory formed by a droplet target supplied from the target injection nozzle to obtain trajectory information on the target trajectory; (b) obtaining a value related to an angle deviation between the target trajectory represented by the trajectory information obtained at step (a) and a predetermined target trajectory; and (c) adjusting at least one of a position and an angle of the target injection nozzle based on the value related to the angle deviation obtained at step (b) such that the droplet target passes through a predetermined position.
Hereinafter, embodiments of the present invention will be explained in detail by referring to the drawings. The same reference numerals are assigned to the same component elements and the duplicated explanation thereof will be omitted.
The driver laser 101 is a high-power laser apparatus such as a carbon dioxide laser for generating a driver laser beam (pulsed laser beam) to be used for turning the target material into plasma.
The EUV light generation chamber 102 is a chamber in which EUV light is generated. The EUV light generation chamber 102 is evacuated by a vacuum pump 105 for prevention of absorption of EUV light. Further, in the EUV light generation chamber 102, a window 106 for introducing a laser beam 120 generated from the driver laser 101 into the EUV light generation chamber 102 is attached. Furthermore, within the EUV light generation chamber 102, a target injection nozzle 103a as a part of the target delivery mechanism 103, a target collecting unit 107, and an EUV light collector mirror 108 are provided.
The target delivery mechanism 103 supplies the target material to be used for generating EUV light into the EUV light generation chamber 102 via the target injection nozzle 103a. As a target material, a molten metal of tin (Sn), lithium (Li), or the like may be used. The target delivery mechanism 103 melts the metal and pressurizes it with an inert gas such as argon (Ar), and thereby, ejects the molten metal through a minute hole of about several tens of micrometers of the target injection nozzle 103a.
The molten metal ejected from the minute hole may be formed into droplets having a uniform size at a certain distance from the target injection nozzle 103a by providing periodic vibration to the target injection nozzle 103a by using a piezoelectric element or the like. The produced droplet target 109 is irradiated with a laser beam when it passes through a predetermined laser beam irradiation position 130, and a part of it turns into plasma 131 generating light having various wavelength components including EUV light. Among the supplied droplet targets 109, the targets that have not been turned into plasma may be collected by the target collecting unit 107.
The laser beam focusing optics 104 may include a mirror 104a for reflecting the laser beam 120 outputted from the driver laser 101 in a direction of the EUV light generation chamber 102, a mirror adjustment mechanism 104b for adjusting the position and the angle (elevation angle) of the mirror 104a, a focusing element 104c for focusing the laser beam 120 reflected by the mirror 104a, and a focusing element adjustment mechanism 104d for moving the focusing element 104c along the optical axis of the laser beam. The laser beam 120 focused by the laser beam focusing optics 104 may pass through the window 106 and the opening formed at the center of the EUV light collector mirror 108 to reach the trajectory of the droplet target 109. The laser beam focusing optics 104 focuses the laser beam 120 to form a focus on the trajectory of the droplet target 109. Thereby, the droplet target 109 supplied from the target injection nozzle 103a is excited and turned into plasma, and EUV light 121 is generated from the plasma.
The EUV light collector mirror 108 is a concave mirror having a spheroidal reflection surface on which, for example, a Mo/Si coating for reflecting light having a wavelength of 13.5 nm at high reflectance is formed. The EUV light collector mirror 108 reflects the generated EUV light 121 to collect it to an intermediate focusing point (IF). The EUV light 121 reflected by the EUV light collector mirror 108 may pass through a gate valve 110 provided in the EUV light generation chamber 102. Further, the EUV light 121 may pass through a spectral purity filter (SPF) 111 for removing unnecessary light (electromagnetic waves or light having shorter wavelengths than that of EUV light, and light having longer wavelengths than that of EUV light, for example, violet light, visible light, infrared light, and so on) from the light generated from the plasma 131, and transmitting only specific EUV light, for example, light having a wavelength of 13.5 nm. Then, the EUV light 121 collected on the IF (intermediate focusing point) may be guided to an exposure unit or the like via a transmission optics.
Here, in the case where plasma is generated from the same point as the point at which the droplet target 109 has first been irradiated with the laser beam 120, the laser beam irradiation point coincides with the plasma generation position. On the other hand, there is a method of generating EUV light by irradiating the droplet target 109 with a pre-pulse laser beam to expand it, and then, irradiating the expanded target with a main-pulse laser beam to generate plasma. In this case, the first laser beam irradiation point may not necessarily coincide with the plasma generation position. Accordingly, in this application, the position where the droplet target 109 is first irradiated with the laser beam 120 is referred to as “predetermined laser beam irradiation position”.
By the way, the tin droplet target having a diameter of 10 μm to 60 μm passes through a predetermined plasma generation position at a high speed of about 30 m/s to about 60 m/s, for example. In this regard, the droplet target is irradiated with a pulsed laser beam having a repetition rate of, for example, 50 kHz to 100 kHz in a plasma generation region having a diameter of, for example, about several tens of micrometers. Therefore, in order to generate EUV light, it is necessary that the pulse timing of the pulsed laser beam and the generation timing of the droplet target are synchronized and the trajectory of the droplet target passes through the predetermined plasma generation position for stabilization of the output of the EUV light source and the plasma generation position (emission point of EUV light). The trajectory of the droplet target may vary due to various factors such as the temperature change and wear-out of the nozzle part for injecting the target material, and therefore, it is desirable to measure and control the three-dimensional spatial position thereof.
A general LPP light source control system includes an imaging device (CCD camera) for supplying an image of a target stream path as output, and a stream path error detector for detecting the position error of the target stream path imaged by the imaging device. The stream path error detector detects the position error of the target stream path. The position error of the target stream path is a position error in a direction of an axis substantially perpendicular to the target stream path from the desired target stream path intersecting the desired plasma start site (plasma generation position). Further, two imaging devices may be arranged such that the optical axes are orthogonal to each other, and perceive the two-dimensional position error.
As shown in
However, in the real operation, the radiation direction of the droplet target injected from the target injection nozzle may change and tilt relative to the predetermined injection direction. It is estimated that this is because the tip end of the target injection nozzle is corroded by heat and the channel is deflected or the solid produced by the reaction of a part of the target material, for example, tin oxide or tin compound adheres to the channel or the outer part of the target injection nozzle, and thereby, the injection direction of the droplet target is changed.
On the other hand, in the case where the plasma generation position is reflected within the image obtained by the imaging device, the brightness in the plasma generation position is extremely higher and it is difficult to accurately detect the position of the droplets having lower brightness. Therefore, the position error of the target trajectory in the predetermined plasma generation position is estimated by using the position error in the position apart from the plasma generation position, that is, the position nearer to the plasma generation position between the target injection nozzle and the plasma generation position.
As shown in
Further, when tin is used as the target material, the molten tin is heated to nearly 300° C. in the target delivery mechanism. In this regard, the part near to the tip end of the target injection nozzle for injecting the molten tin may be thermally deformed and displaced from the designed position or the channel of the target injection nozzle may be deflected. In this case, if the configuration in which the target delivery mechanism is mounted on a linear stage or the like and moved is used, when the real target trajectory is shifted relative to the predetermined target trajectory, only a part of the target trajectory may be imaged. That may cause inaccurate evaluation of the amount of movement of the target delivery mechanism or the change of the injection direction of the droplet target.
Here, it is assumed that the target injection nozzle is located above the predetermined plasma generation position in the drawing (broken line). In this case, the position error δ of the target trajectory from the predetermined plasma generation position can be obtained based on the position error δ′ of the target trajectory that can be read from the image obtained by the imaging device. However, in the case where the real nozzle position is shifted from the designed nozzle position, it may be difficult to control the droplet target to pass through the predetermined plasma generation position even by moving the nozzle position of the target delivery mechanism to the left in the drawing by the distance δ.
Further, in order to minimize the debris of tin produced after the droplet target is irradiated with the driver laser beam, production of a mass-limited target formed by reducing the diameter of the droplet target (to the diameter of about 10 μm) is proposed. With reduction of the diameter of the droplet target, the control with higher accuracy may be required for the trajectory on which the droplet target passes. As below, “the trajectory on which the droplet target passes” may be simply referred to as “the target trajectory”.
In the embodiment, in the EUV light generation chamber apparatus of the LPP light source, the apparatus for measuring and controlling a target trajectory is provided such that stable supply of EUV light can be maintained by adjusting the position or the angle of the target injection nozzle even in the case where the injection direction of the droplet target injected from the target injection nozzle tilts from the predetermined injection direction. A target trajectory measuring unit for measuring the target trajectory may be provided inside or outside of the chamber. However, in the case where there is a possibility that the chamber is thermally deformed, in order to reduce the measurement error, it is desirable that the target trajectory measuring unit is provided outside the chamber and in another frame separate from the chamber.
A nozzle adjustment controller 18 controls the nozzle adjustment mechanism 113 at least based on the value related to the angle deviation obtained by the target trajectory angle detecting unit 15 such that the droplet target 109 passes through the predetermined laser beam irradiation position 130. Further, the nozzle adjustment controller 18 may control the nozzle adjustment mechanism 113 based on output signals of displacement gauges 21 and 22 such that the position of the target injection nozzle 103a coincides with the reference position.
Furthermore, the LPP light source, to which the apparatus for measuring and controlling a target trajectory according to the embodiment is applied, may include a trigger timing adjusting unit 33 . To the driver laser 101, the trigger timing adjusting unit 33 sends out a trigger signal for adjusting the trigger timing of the driver laser 101 such that the driver laser 101 irradiates the droplet target 109 with the driver laser beam in the predetermined laser beam irradiation position (plasma generation position) 130 in synchronization with the timing when the droplet target 109 reaches the predetermined laser beam irradiation position 130.
In the configuration example as shown in
Referring to
The nozzle angle adjustment mechanism 113b may preferably have a first rotational axis and a second rotational axis orthogonal to each other within the two-dimensional plane substantially orthogonal to the predetermined target trajectory, and can adjust the angle of the target injection nozzle 103a by the two rotational axes according to the control signal outputted from the nozzle angle adjustment controller 16. The imaging devices 11 and 13 may be arranged such that the optical axes of the imaging devices 11 and 13 are in parallel to the first and second rotational axes of the nozzle angle adjustment mechanism 113b, respectively. In this case, the angle of the target injection nozzle 103a can be adjusted by rotating respective one rotational axis with respect to each imaging device.
Referring to
First, at step S1 as shown in
In the left drawing of
Even in the case where the target injection nozzle 103a and the predetermined laser beam irradiation position 130 are not contained in the images obtained by the imaging devices 11 and 13, if the measurement position (Z=Z1) is determined and the positions of the target trajectory measured in the measurement position (Z=Z1) and the predetermined target trajectory are contained in the images, the angle deviation θ can be obtained by using the amount of deviation X2−X1 of the target trajectory 112 calculated from the images. At step S2 as shown in
Then, at step S3 as shown in
The right drawing of
By performing the same control as above based on the image obtained in the X-axis direction, the tilt of the target trajectory 112 in the Y-direction can be corrected. In the case of using the first technique as shown in
In the left drawing of
According to the second technique as shown in
In the above configuration, when the angle of the target injection nozzle 103a is changed by the nozzle angle adjustment mechanism 113b, the position of the injection opening of the tip end of the target injection nozzle 103a may move in the horizontal direction in the drawing. In this case, additionally, it may be necessary to compensate for the movement in the horizontal direction in the drawing to maintain the position of the injection opening to the original position by the action of the nozzle position adjustment system or the like. However, even in the case without the control of the nozzle position adjustment controller 23, if the nozzle angle adjustment controller 16 performs the more sophisticated computation to grasp the relationship between the tilt of the target injection nozzle 103a and the horizontal movement of the tip end position and controls the nozzle position adjustment mechanism 113a together with the nozzle angle adjustment mechanism 113b, the injection opening can be held in the original position. Alternatively, a gonio stage tilting around the injection opening position of the center of the tip end of the target injection nozzle 103a may be used as the nozzle angle adjustment mechanism 113b. The gonio stage is a stage for moving an object along a circumference around a point located in a space.
By the way, it is enough that the target trajectory measuring unit 17 as shown in
X
G
=D×(I2−I1)/(I1+I2)
Since the position sensitive detector obtains the position of the light spot by the computation of analog voltages, the position of the target trajectory can be measured at an extremely high speed with high resolving power. In the case where the position of the target trajectory is measured by using plural position sensitive detectors, at least two position sensitive detectors may be provided in at least two locations along the target trajectory, respectively.
The two displacement gauges 21 and 22 are provided such that their measurement axes are in different directions from each other, and can measure the position of the target injection nozzle 103a within the two-dimensional plane orthogonal to the predetermined target trajectory. It is desirable that the optical axes of the two displacement gauges 21 and 22 are orthogonal to each other. As each of the displacement gauges 21 and 22, a laser displacement gauge, a laser interferometer, or the like for performing noncontact and high-accuracy position measurement may be used.
Since the target material is heated to about 300° C., the tip end position of the target injection nozzle 103a may be displaced from the original position due to thermal deformation of parts or the like. Even in such a case, in order to supply the target to the predetermined laser beam irradiation position 130, it is preferable that the position of the target injection nozzle 103a is measured without the influence of the mechanical displacement due to heat. Accordingly, the nozzle position adjustment system may include the displacement gauges 21 and 22 fixed to an independent frame separated from the mechanical displacement of the target delivery mechanism 103 due to the heat. Thereby, the position of the tip end of the target injection nozzle 103a can be measured without the influence of heat (step S11 as shown in
Further, the nozzle position adjustment controller 23 calculates the deviation of the current position of the target injection nozzle 103a relative to the reference position (original position) of the target injection nozzle 103a where the droplet target reaches the predetermined laser beam irradiation position 130 (step S12). The nozzle position adjustment controller 23 compares the deviation of the position of the target injection nozzle 103a with the predetermined threshold value, and determines whether the deviation exceeds a threshold value or not (step S13). If the deviation does not exceed the predetermined threshold value (NO at step S13), the process returns to the first step S11. On the other hand, if the deviation exceeds the predetermined threshold value (YES at step S13), the nozzle position adjustment controller 23 controls the nozzle position adjustment mechanism 113a to move the target injection nozzle 103a in a direction in which the deviation is eliminated and they coincide with each other (step S14).
The nozzle position adjustment mechanism 113a translates the target injection nozzle 103a to adjust the position of the target injection nozzle 103a. The nozzle position adjustment mechanism 113a may adjust the position of the target injection nozzle 103a by moving the target delivery mechanism 103 mounted on a linear stage or the like. In this manner, the position of the target injection nozzle 103a is adjusted to coincide with the original position where the droplet target can be supplied to the predetermined laser beam irradiation position 130. The flowcharts as shown in
By using the nozzle position adjustment system and the target trajectory angle adjustment system in combination and respectively performing feedback control of them, control results with high quality can be obtained. In this case, first, the nozzle position adjustment system may perform control of providing the position of the target injection nozzle 103a in the reference position (original position). Then, the target trajectory angle adjustment system may perform control of compensating for the tilt of the target trajectory. Further, two kinds of control may be repeatedly performed. By the separation of the two kinds of control, the target trajectory 112 can be accurately maintained in the predetermined laser beam irradiation position 130.
Further, the target injection nozzle 103a may not be tilted. Since the position of the target injection nozzle 103a can be measured with relatively high accuracy by the displacement gauges 21 and 22, the target trajectory may be adjusted to pass through the predetermined laser beam irradiation position 130 by only translating the target injection nozzle 103a.
If the angle deviation θ of the target trajectory 112 from the predetermined target trajectory has been obtained by the target trajectory angle detecting unit 15 (
Referring to
The trigger timing adjustment system may include a detector laser 31, a light receiving element 32, and a trigger timing adjusting unit 33. The detector laser 31 applies a detector laser beam 35 for search toward the trajectory of the droplet target 109. The light receiving element 32 detects the detector laser beam 35 passing between the droplet targets or the detector laser beam 35 reflected by the droplet target. The trigger timing adjusting unit 33 senses the timing when the droplet target 109 passes through the predetermined laser beam irradiation position 130 based on the detection signal supplied from the light receiving element 32. Further, the trigger timing adjusting unit 33 generates a trigger signal for adjusting the trigger timing of the driver laser 101 such that the driver laser 101 irradiates the droplet target 109 with a driver laser beam 120 in the predetermined laser beam irradiation position 130, and outputs the trigger signal to the driver laser 101. The driver laser 101 may generate the driver laser beam 120 in synchronization with the trigger signal.
In the case where the scattering light by the driver laser beam 120 is relatively strong or the case where the droplet target is small, the transmitted light or the reflected light of the detector laser beam 35 is relatively weak and the light receiving element 32 may not accurately detect the detector laser beam 35. In such a case, the detector laser beam 35 may be applied toward the position above the predetermined laser beam irradiation position 130 (toward the target injection nozzle 103a side) instead of the vicinity of the predetermined laser beam irradiation position 130. The trigger timing adjusting unit 33 senses the timing when the droplet target passes through the detection position, and then, the trigger timing adjusting unit 33 may activate the trigger signal to be supplied to the driver laser 101 with the timing when the droplet target reaches the predetermined laser beam irradiation position 130. Thereby, even the small droplet target 109 is irradiated with the driver laser beam 120, and the droplet target 109 is turned into plasma.
The nozzle position adjustment system and the target trajectory angle adjustment system include the nozzle position adjustment mechanism 113a, the nozzle angle adjustment mechanism 113b, the target trajectory measuring unit 17, the target trajectory angle detecting unit 15, the displacement gauges 21 and 22, and a nozzle adjustment controller 24. The nozzle position adjustment mechanism 113a adjusts the position of the target injection nozzle 103a. The nozzle angle adjustment mechanism 113b adjusts the angle of the target injection nozzle 103a. The target trajectory measuring unit 17 measures the target trajectory by using a sensor selected from among various sensors cited above. The target trajectory angle detecting unit 15 obtains the value related to the angle deviation between the target trajectory represented by the trajectory information and the predetermined target trajectory based on the trajectory information obtained by the target trajectory measuring unit 17, and thereby, detects the tilt of the target trajectory 112. The displacement gauges 21 and 22 measure the position displacement of the tip end of the target injection nozzle 103a. The nozzle adjustment controller 24 controls the nozzle position adjustment mechanism 113a and the nozzle angle adjustment mechanism 113b to respectively perform the position adjustment of the target injection nozzle 103a and the angle adjustment of the target trajectory based on the output signals of the displacement gauges 21 and 22 and the value related to the angle deviation obtained by the target trajectory angle detecting unit 15.
In the nozzle position adjustment system and the target trajectory angle adjustment system, the displacement gauges 21 and 22 directly measure the displacement of the tip end of the target injection nozzle 103a, and the nozzle adjustment controller 24 generates the control signal of the nozzle position adjustment mechanism 113a and the control signal of the nozzle angle adjustment mechanism 113b based on the measurement result and the information on the tilt of the target trajectory 112. For example, the nozzle adjustment controller 24 may first perform control of providing the position of the target injection nozzle 103a in the reference position, and then, perform control of compensating for the tilt of the target trajectory. Further, the nozzle adjustment controller 24 may repeatedly perform the two kinds of control. Thereby, the target trajectory 112 can be accurately controlled to pass through the predetermined laser beam irradiation position 130. According to the mode, high-accuracy control can be performed compared to the mode of adjusting the horizontal position of the target injection nozzle 103a according to the position error of the target trajectory 112.
On the basis of the information, a nozzle adjustment controller 25 controls the nozzle position adjustment mechanism 113a. The nozzle adjustment controller 25 further maintains the tip end of the target injection nozzle 103a in the original position and controls the nozzle angle adjustment mechanism 113b. Thereby, the nozzle adjustment controller 25 compensates for the tilt of the target injection nozzle 103a and maintains the target trajectory 112 of the droplet target injected from the target injection nozzle 103a in the Z-axis direction. Accordingly, the target trajectory 112 of the target injected from the target injection nozzle 103a can pass through the predetermined laser beam irradiation position 130. In the third mode as shown in
The nozzle position adjustment system and the target trajectory angle adjustment system as shown in
The nozzle position adjustment controller 26 controls the nozzle position adjustment mechanism 113a based on the position deviation of the target injection nozzle 103a and the measured tilt of the target trajectory 112. Thereby, the target injection nozzle 103a can be translated such that the target trajectory 112 passes through the predetermined laser beam irradiation position 130.
According to the one embodiment of the invention, in the chamber apparatus of the LPP light source, even in the case where the injection direction of the droplet target injected from the target injection nozzle of the target delivery mechanism tilts from the predetermined injection direction, the angle deviation between the measured target trajectory and the predetermined target trajectory can be obtained and at least one of the position and the angle of the target injection nozzle can be adjusted based on the angle deviation such that the droplet target passes through the predetermined position.
Furthermore, according to some embodiments, the following merits may be obtained.
In addition, in the above described embodiment, the case where the present invention is applied to the LPP type EUV light source apparatus for generating EUV light by focusing the driver laser beam to the predetermined laser beam irradiation position, where the droplet target passes, to generate plasma has been explained, but the present invention is not limited to the embodiment. For example, the present invention can be also applied to an LPP type EUV light source apparatus for generating EUV light by irradiating the droplet target with a pre-pulse laser beam for expanding the target or weakly turning it into plasma, and then, irradiating the expanded target or the weak plasma with a main-pulse laser beam to generate plasma.
Number | Date | Country | Kind |
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JP 2009-122647 | May 2009 | JP | national |