CIOMP got a High Power CO2 laser patent.
In order to solve the above problems, the present invention provides a CO 2 laser power stabilization method and device for extreme ultraviolet lithography light sources, which solves the problem that the existing CO 2 laser power stabilization method needs to break the thermal balance of the laser system, through precise closed-loop control The time delay of injecting seed laser of the same frequency into the laser amplifier can significantly regulate the gain extraction efficiency of the seed laser and improve the power stability of the main pump CO 2 laser.
The invention provides a CO 2 laser power stabilization method applied to extreme ultraviolet lithography light sources . A laser amplifier with the same repetition frequency as the seed laser is used to amplify the seed laser. Without changing the discharge excitation power of the laser amplifier, Change the time delay of the seed laser entering the laser amplifier to improve the gain extraction efficiency of the seed laser.
Preferably, a certain time delay is selected, the seed laser is injected into the laser amplifier, the amplified laser pulse energy output by the laser amplifier is measured, and the amplified laser pulse energy is compared with the preset range:
When the amplified laser pulse energy is higher than the maximum value of the preset range, increase the time delay until the amplified laser pulse energy is within the preset range;
When the amplified laser pulse energy is lower than the minimum value of the preset range, the time delay is reduced until the amplified laser pulse energy is within the preset range.
A CO 2 laser power stabilization device used in extreme ultraviolet lithography light sources , including: CO 2 seed laser, CO 2 laser amplifier, control center and photodetector;
CO 2 seed laser outputs seed laser;
The CO 2 laser amplifier amplifies the power of the seed laser and outputs the amplified laser. The discharge excitation frequency of the CO 2 laser amplifier is the same as the pulse frequency of the seed laser;
The photodetector measures the pulse energy of the amplified laser and feeds the pulse energy back to the control center. The control center controls the time delay of the CO 2 seed laser output seed laser based on the relationship between the pulse energy and the preset range.
Preferably, it also includes a beam delivery unit composed of a fixed-magnification beam expander to match the beam characteristic size of the seed laser with the CO 2 laser amplifier to improve the power extraction efficiency of the CO 2 laser amplifier.
Preferably, the amplified laser is sampled through a laser sampling mirror, and the photodetector measures the pulse energy of the amplified laser
Preferably, a tin droplet target generator is also included. The tin droplet target generator generates micro-sized tin droplets with the same frequency as the CO2 seed laser, and the amplified laser interacts with the tin droplets to radiate high-efficiency EUV light .
Preferably, the control center provides trigger signals for the CO 2 seed laser, CO 2 laser amplifier and tin droplet target generator, and the time delay between each other is adjustable, and the adjustment accuracy is not less than 1 ns.
Compared with the existing technology, the present invention can achieve the following beneficial effects:
Without breaking the thermal balance of the laser system, the present invention solves the current problem of poor power stability adjustment accuracy of the main oscillation power amplifier of the pulse system, and significantly improves the stability of the power/pulse energy of the high-repetition-frequency, narrow-pulse-width CO2 laser . It meets the application requirements of high-stability EUV lithography light source for CO 2 laser power stability.
The CO 2 laser power stabilization method applied to extreme ultraviolet lithography light sources provided by the present invention mainly solves the problem that the existing CO 2 laser power stabilization method needs to break the thermal balance of the laser system. Since the laser amplifier is capable of increasing energy under repetitive frequency discharge excitation conditions, Level gas molecules relax without radiation transition. Within a pulse period, spontaneous emission, collision relaxation and other processes will occur after the discharge excitation is stopped, and the CO 2 laser gain will gradually decrease. Therefore, without changing the discharge excitation power of the laser amplifier, through precise closed-loop control of the time delay of seed laser injection of the same frequency into the laser amplifier, the seed laser gain extraction efficiency can be significantly adjusted and the stability of the main pump CO 2 laser power can be significantly improved. .
As shown in Figure 1, the embodiment of the present invention combines the CO 2 laser power stabilization method and device used in extreme ultraviolet lithography light sources. The device includes a CO 2 seed laser 1, a beam delivery unit 2, a CO 2 laser amplifier 3, Control center 4, tin droplet target generator 5, tin droplet 6, laser targeting EUV luminous area 7, laser sampling mirror 8 and photodetector 9, including:
CO 2 seed laser 1 provides high repetition frequency, narrow pulse width seed laser for the main pump CO 2 laser. It can use acousto-optic Q-switching, electro-optical Q-switching or electro-optical cavity emptying technology to achieve high repetition frequency and narrow pulse CO The output of the 2 seed laser, CO 2 seed laser 1 is controlled by the trigger signal from the control center 4.
After the CO 2 seed laser 1 outputs the seed laser, the seed laser enters the beam delivery unit 2. The beam delivery unit 2 is used to match the output beam characteristic size of the CO 2 seed laser 1 with the gain space of the CO 2 laser amplifier 3 to improve gain filling. factor, thereby effectively improving the power extraction efficiency of the CO 2 laser amplifier 3. The beam delivery unit 2 is composed of a fixed magnification beam expander.
The seed laser enters the CO 2 laser amplifier 3 for laser amplification. The CO 2 laser amplifier 3 can use radio frequency fast axial flow, radio frequency fast cross flow, radio frequency slab and other high-power laser amplifiers. The discharge excitation frequency of the CO 2 laser amplifier 3 is consistent with the seed laser. The pulse frequency is the same, or the same as the discharge excitation frequency of the CO 2 seed laser 1, and the discharge excitation duty cycle is adjustable. Under the control of the trigger signal, it can realize discharge excitation with a gate frequency of 10kHz-100kHz, and the discharge excitation duty cycle can be adjusted from 1% to 90%.
The control center 4 is used to provide precisely controllable trigger signals for the CO 2 seed laser 1, the beam delivery unit 2 and the CO 2 laser amplifier 3, and the time delay between them is precisely adjustable, and the adjustment accuracy is not less than 1 ns. Under the control sequence of the control center 4, the seed laser output by the CO 2 seed laser 1 is amplified by the CO 2 laser amplifier 3, and then lasered with the tin droplets 6 generated by the tin droplet target generator 5 in the laser targeting EUV luminous area 7 For target shooting, plasma EUV light is generated. The droplet target generator 5 uses a piezoelectric ceramic excitation capillary generator, which can spray spherical tin droplet targets with a frequency of 10kHz-100kHz and a size of 10μm-100μm. A laser sampling mirror 8 is provided on the optical path before laser target shooting. The laser sampling mirror 8 is a ZnSe material coated sampling mirror with a sampling rate of <0.2%. The laser sampling mirror 8 samples a part of the amplified seed laser, and passes this part of the sample into the high-sensitivity photodetector 9 to facilitate laser power monitoring. The photodetector 9 measures the pulse energy of the amplified laser in real time, and it comes with a fixed magnification The power attenuator avoids the energy saturation distortion of the detection signal. The photoelectric detector 9 feeds it back to the control center 4. The control center 4 performs signal collection and calculation comparison to determine the relationship between the actual measured energy value of the amplified laser pulse and the preset range. According to the energy determination result, the triggering moment of the pulse output signal of the CO 2 seed laser 1 is adjusted in real time to improve the power stability of the main pump CO 2 laser