Embodiments of the invention relate to a method for monitoring a laser optical unit of a laser system. Embodiments of the invention also relate to a laser system for carrying out such a method.
In optical units for high-performance laser applications, defects arising during operation, such as penetration burns or increase of absorption due to soiling, are a frequently occurring cause of unplanned maintenance issues or damage to machines. Embodiments of the invention are used for early detection of slowly accumulated defects (for example, continuously increasing degree of soiling) and/or individual incidents (for example, the occurrence of penetration burns on coatings and optical units due to occurring pulse peaks or particle burn off). Machine failures can thus be avoided early.
Monitoring the operation of a laser optical unit by checking a coolant temperature is known to the applicant. If a defect occurs in the laser optical unit, it heats up, which can be detected by monitoring the coolant temperature. An increase of the coolant temperature can often only be detected with a severe time delay, however.
Furthermore, monitoring a laser optical unit by means of light source and photodiode is known to the applicant. However, such monitoring is susceptible to flashes from particles which run through the laser optical unit, but do not result in defects of the laser optical unit.
Furthermore, monitoring starting variables of the laser system, for example, to compare setpoint and actual values of the laser power, is known. However, defects are also only detected comparatively late in this case.
Embodiments of the present invention provide a method for monitoring a laser optical unit of a laser system. The method includes guiding a laser beam through the laser optical unit, performing a first measurement of vibrations arising in the laser optical unit, structure-borne sound arising in the laser optical unit, and/or sound arising in the laser optical unit by using a sensor, and generating an output of the first measurement, and/or an output of a change of the vibrations, of the structure-borne sound, and/or of the sound.
Subject matter of the present disclosure will be described in even greater detail below based on the exemplary figures. All features described and/or illustrated herein can be used alone or combined in different combinations. The features and advantages of various embodiments will become apparent by reading the following detailed description with reference to the attached drawings, which illustrate the following:
Embodiments of the invention provide a method which permits rapid and reliable monitoring of a laser system in a simply designed manner. Embodiments of the invention also provide a laser system for carrying out such a method.
According to some embodiments, a method for monitoring a laser optical unit of a laser system comprising the following method steps:
A laser-induced vibration/structure-borne sound and/or sound arises/arise at a defect. Laser power is absorbed at the defect in this case, which results in a temperature increase and therefore a thermal expansion of the laser optical unit, and structure-borne sound, sound, and/or vibrations are generated in the laser optical unit. Such a defect can arise, for example, due to ablation of material of the laser optical unit.
If a sudden temperature increase occurs, e.g., due to particle burnoff, fracture of the laser optical unit, damage to coatings of the laser optical unit by pulse peaks, plasma breakthroughs in the surrounding medium or on the laser optical unit or its coating itself, it can be that a measurable shockwave will be generated in the laser optical unit. If the laser optical unit is located in an atmosphere, a sound wave will additionally also be emitted, which is likewise detectable.
Such an event can be concluded on the basis of the time curve of the detected vibrations, the detected sound, and/or structure-borne sound, for example, the occurrence of peaks in the detected signal.
In pulsed lasers or power-modulated lasers, the modulation of the laser power results in a modulation of the absorbed power and therefore in a pulsating heat source, which in turn results in a pulsating thermal expansion and therefore in turn vibrations, structure-borne sound, and sound emission. A sound, vibration, or structure-borne sound source localized around the absorbing defect is therefore to be expected, the frequency of which corresponds to the modulation frequency of the incident laser beam (for example, the pulse repetition rate in the case of pulsed lasers or the modulation/regulation frequency in the case of power-regulated continuous lasers). An amplitude increase can therefore be measured in the relevant frequency range in the frequency spectrum of the emitted sound, structure-borne sound, and/or vibrations. The intensity and therefore the amplitude of this sound, structure-borne sound, and/or these vibrations is proportional to the mean absorbed power. The absorbed power can therefore be concluded directly on the basis of the amplitude increase.
The sensors are preferably fastened on the laser optical unit in this case.
The vibrations, structure-borne sound, and/or sound arising in the laser optical unit are preferably detected by means of at least three sensors. The at least three sensors detect sound, structure-borne sound, and/or vibrations at different times in each case in case of a defect. The position of the defect in the volume of the laser optical unit can be concluded by triangulation from time-of-flight measurements (in case of a shockwave) or phase differences (in case of a frequency-based evaluation).
Therefore, chronologically discrete defect events can be concluded in the time range by monitoring the vibrations, the structure-borne sound, and/or the sound, while the analysis of the amplitude distribution in the frequency range enables a detection of slower events, for example, an absorption increase due to accumulated soiling. Both evaluation methods are complementary here and can be applied alternatively or simultaneously.
Defects occurring in the laser optical unit can be simply identified reliably and early by the detection of the vibrations, structure-borne sound, and/or sound emitted by the laser optical unit. In other words, the method according to embodiments of the invention enables efficient monitoring of a laser optical unit, wherein little installation space is required for the monitoring.
The output, preferably optical and/or acoustic, can take place on an output unit. The output can comprise an alarm if the output exceeds predefined threshold values.
The measurement in method step D) is preferably reduced to a modulation frequency range of the laser beam, in particular to a pulse frequency of the laser beam. The restriction can be carried out by a bandpass filter. The bandpass filter can be provided in the form of hardware and/or software. The modulation frequency range of the laser beam is preferably between 10 kHz and 150 kHz, in particular between 20 kHz and 130 kHz, preferably between 30 kHz and 120 kHz.
In a preferred embodiment of the method, the method additionally comprises the following method steps:
In this way, the vibrations generated in optimum operation, the structure-borne sound generated in optimum operation, and the sound generated in optimum operation can remain unconsidered and the unpredicted deviations can be recognized easily. In one preferred embodiment of the invention, the output is first generated when the deviation of the two measurements exceeds a predefined threshold value.
The vibrations, structure-borne sound, and/or sound arising in the laser optical unit in optimum operation are preferably detected depending on the laser power. In this way, signal variations which occur due to a deliberate increase of the laser power are calibrated out.
The measurement in method step B), in particular as in method step D), is preferably reduced to a modulation frequency range of the laser beam, in particular to a pulse frequency of the laser beam. In this way, background vibrations, background structure-borne sound, and/or background sound can be suppressed.
A MEMS vibrometer and/or a laser triangulation sensor can be used as a sensor in the method according to embodiments of the invention. Alternatively or additionally, the following sensor/the following sensors can be provided for this purpose:
In one preferred embodiment of the invention, the method comprises the following method step:
Embodiments of the invention also provide a laser system, in particular for carrying out a method described here, having a laser optical unit for guiding a laser beam, wherein the laser system comprises a sensor for monitoring the laser optical unit, wherein the sensor is designed in the form of
The laser system can comprise a target material that can be irradiated using the laser beam to generate EUV radiation.
The method features mentioned for carrying out the method described here also refer to the device (laser system) and vice versa to avoid repetitions.
Further advantages of the embodiments of the invention are evident from the description and the drawing. Similarly, the features mentioned above and the features still to be explained may each be used on their own or together in any desired combinations according to embodiments of the invention. The embodiments shown and described should not be understood as an exhaustive list, but rather as being of an exemplary character.
A sensor 24 is arranged on the laser optical unit 16, for example, on a lens or a mirror. The sensor 24 is designed to measure vibrations, structure-borne sound, and/or sound. The sensor 24 is connected in a wireless and/or wired manner to an output unit 26. The data measured using the sensor 24 are output in processed and/or unprocessed form in the output unit 26.
Since the sound signal is excited with the frequency and phase of the laser beam incident on the laser optical unit, a similar picture as in
As described above, embodiments of the invention relate to a method 12 for monitoring a laser optical unit 16. At least one sensor 24 measures the vibrations, structure-borne sound, and/or sound originating from the laser optical unit 16. The measurement can be restricted to a modulation frequency of a laser beam 18 conducted through the laser optical unit 16. Alternatively or additionally thereto, the measurement can be compared to a measurement in optimum operation. Embodiments of the invention also relate to a laser system 10, in particular for carrying out such a method 12.
While subject matter of the present disclosure has been illustrated and described in detail in the drawings and foregoing description, such illustration and description are to be considered illustrative or exemplary and not restrictive. Any statement made herein characterizing the invention is also to be considered illustrative or exemplary and not restrictive as the invention is defined by the claims. It will be understood that changes and modifications may be made, by those of ordinary skill in the art, within the scope of the following claims, which may include any combination of features from different embodiments described above.
The terms used in the claims should be construed to have the broadest reasonable interpretation consistent with the foregoing description. For example, the use of the article “a” or “the” in introducing an element should not be interpreted as being exclusive of a plurality of elements. Likewise, the recitation of “or” should be interpreted as being inclusive, such that the recitation of “A or B” is not exclusive of “A and B,” unless it is clear from the context or the foregoing description that only one of A and B is intended. Further, the recitation of “at least one of A, B and C” should be interpreted as one or more of a group of elements consisting of A, B and C, and should not be interpreted as requiring at least one of each of the listed elements A, B and C, regardless of whether A, B and C are related as categories or otherwise. Moreover, the recitation of “A, B and/or C” or “at least one of A, B or C” should be interpreted as including any singular entity from the listed elements, e.g., A, any subset from the listed elements, e.g., A and B, or the entire list of elements A, B and C.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10 2022 205 579.9 | Jun 2022 | DE | national |
This application is a continuation of International Application No. PCT/EP2023/064128 (WO 2023/232652 A1), filed on May 25, 2023, and claims benefit to German Patent Application No. DE 10 2022 205 579.9, filed on Jun. 1, 2022. The aforementioned applications are hereby incorporated by reference herein.
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/EP2023/064128 | May 2023 | WO |
| Child | 18963576 | US |