Patent Application
20240168306
Embodiments of the present invention relate to a focusing device for focusing at least two laser beams onto a target material moving in a target region for generating extreme ultraviolet (EUV) radiation, for lithography purposes. Embodiments of the present invention also relate to an EUV beam generating apparatus comprising such a focusing device.
Focusing devices and EUV beam generating apparatuses have been disclosed by WO 2015/036024 A1 and WO 2015/036025 A1.
In those focusing devices and beam generating apparatuses, the efficiency of the target irradiation is reduced as a result of the respective laser beams being focused onto the target material at different positions in the target region from different directions in each case.
Embodiments of the present invention provide a focusing device for focusing at least two laser beams onto a moving target material in a target region for generating extreme ultraviolet (EUV) radiation. The focusing device includes a first focusing element for focusing a first laser beam onto the target material at a first position in the target region, a second focusing element for focusing a second laser beam onto the target material at a second position in the target region, and a reflective optical element for reflecting the EUV radiation generated by the target material. An optical axis of the first focusing element and/or an optical axis of the second focusing element are aligned approximately parallel or congruently with respect to an optical axis of the reflective optical element.
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 focusing device and an EUV beam generating apparatus which enable more efficient irradiation of the target material.
According to embodiments of the present invention, a focusing device includes:
This results in an image plane of the first focusing element and/or an image plane of the second focusing element being aligned perpendicularly or approximately perpendicularly to the optical axis of the reflective optical element. In particular, the target material can move in a plane (target plane) which is approximately perpendicular or perpendicular to the optical axis of the reflective optical element and thus approximately parallel, parallel or congruent with respect to one of the image planes of the two focusing elements. As a result of the optical axis of at least one of the focusing optical elements being aligned approximately parallel, parallel or congruently with respect to the optical axis of the reflective optical element, the target material is irradiatable effectively.
In this case, the reflective optical element is suitable in particular for reflecting EUV radiation emitted during the irradiation of the target material with laser radiation. The reflective optical element can be embodied e.g. as a near-normal incidence collector mirror having a reflective surface in the form of an ellipsoid of revolution, wherein the reflective optical element has a first focal point near or in a region in which the target material is irradiated with the laser beam(s).
According to embodiments of the invention, at least one, preferably both optical axes of the two focusing elements be aligned perpendicularly or almost perpendicularly to a flight direction or trajectory of the target material, with the target material moving from a first position to a second position in the target region. In this case, the first laser beam can be guided into the target region on a first beam path of the focusing device. The second laser beam can be guided into the target region on a second beam path of the focusing device. In this case, the principal axis of the first and/or second beam path can be parallel and offset or tilted with respect to the optical axis of the focusing element. By contrast, in the case of a “traditional” imaging, the optical axis is coaxial with respect to the principal axis of the beam path of the laser beam. As a result, the two optical axes have to be tilted with respect to one another in order to spatially separate the laser beams in the near field and to superimpose them in the far field.
In one preferred embodiment, the focusing elements can have parallel or identical, in particular with a margin of ±4°, preferably with a margin of ±2°, parallel or identical optical axes. This results in approximately parallel, parallel or congruent image planes for the two focusing elements. The target material is irradiatable effectively as a result.
The first focusing element can be embodied in the form of an element group. As an alternative or in addition thereto, the second focusing element can be embodied in the form of an element group.
The principal axis of the first beam path preferably does not extend coaxially with respect to the optical axis of the first focusing element. The principal axis of the second beam path preferably does not extend coaxially with respect to the optical axis of the second focusing element.
The respective principal axes of the beam paths can be collimated and collinear upstream of the focusing elements. In a possible alternative configuration, the individual collimated laser beams can also be arranged non-parallel to one another.
In the case of one or more of the laser beams having been imaged obliquely in the beam path upstream of the respective focusing element (e.g. upon passing through a collimating lens, the optical axis of which is aligned obliquely with respect to a direction of propagation of the laser beam), the focusing element, in accordance with the Scheimpflug condition, is preferably tilted relative to a plane perpendicular to the principal axis of the beam path of the laser beam in order to align the image plane in the plane in which the target material is moving. In the case, too, of the individual collimated laser beams being arranged non-parallel to one another, the focusing elements, in particular their principal planes, in accordance with the Scheimpflug condition, are preferably tilted relative to a plane perpendicular to the principal axis of the beam path of the laser beam in order to align the focus plane in the plane in which the target material is moving.
The target material is preferably embodied in the form of a tin droplet. A plasma that emits EUV radiation can be generated in the tin droplet by way of the irradiation with laser radiation.
It is further preferred for the principal axis of the first beam path and/or the principal axis of the second beam path to be offset, in particular in parallel fashion, with respect to the optical axis of the respective focusing element. One focusing element or both focusing elements is/are thereby embodied as rotationally asymmetrical with respect to their respective optical axes. A distortion-free projection in the image plane can be achieved as a result. By way of example, a cross-sectionally circular laser beam or cross-sectionally circular laser beams can have a circular projection.
Preferably, at least one focusing element is embodied in the form of a segment of a rotationally symmetrical focusing element. As a result, the focusing device is of simple constructional design and the beam paths are calculable comparatively easily.
If the principal axes of the beam paths are offset, a moving target material can be irradiated by the two laser beams with a temporal offset. In other words, a moving target material can be impinged on with a temporal (and thus also spatial) offset by virtue of the optical axes of the two focusing optical elements being displaced parallel to one another so that each optical axis passes through the respective target material. The optical axes of the focusing elements are offset with respect to one another by preferably less than 3 mm, in particular less than 1 mm.
With further preference, at least one focusing element, in particular both beam shaping elements, can be embodied in the form of a lens or a mirror. In the case of a mirror, in particular an off-axis parabolic mirror or a combination of off-axis parabolic mirror and off-axis ellipsoidal mirror can be used.
The first beam shaping element and/or the second beam shaping element can be arranged within a vacuum chamber. The vacuum chamber can have a first opening for the first laser beam to enter the vacuum chamber and/or a second opening for the second laser beam to enter the vacuum chamber.
A deflection mirror, in particular a double mirror arrangement, can be provided in the first beam path and/or in the second beam path. The double mirror arrangement leads to a significant, preferably even complete, reduction of astigmatism (cf. Seunghyuk Chang: Linear astigmatism of confocal off-axis reflective imaging systems with N-conic mirrors and its elimination; Journal of the Optical Society of America A, Vol. 32, No. 5/May 2015, pages 852-859). In the case of this arrangement, however, the laser beam to be imaged is not guided on a theoretical optical axis that results in an imaging free of astigmatism, but rather on an entrance side (collimated entrance beam) is offset parallel thereto in order to achieve the desired effect of a tilted principal axis on an exit side with an image plane parallel to the target plane. In the equivalent model of a lens optical unit, this corresponds to the displacement of the principal axis of the beam path of the laser beam with respect to the optical axis of the lens. In this case, the angle of the principal axis of the beam path of the laser beam on the exit side corresponds to the tangent of the distance of the principal axis of the beam path of the laser beam on the entrance side divided by the effective focal length EFL.
The focusing device can have a third beam path for guiding a third laser beam into the target region. The target material can be irradiated on its path firstly by the first laser beam, subsequently by the third laser beam and finally by the second laser beam. The third laser beam can impinge on the first focusing element at an angle of more than 2°, in particular of more than 4°, with respect to the first laser beam. As a result, the third beam path and hence the third laser beam likewise has an image plane extending approximately parallel, parallel or congruently with respect to the plane in which the target material is moving. The principal axis of the third beam path and hence of the third laser beam—in particular after passing through the first focusing element—preferably does not extend coaxially with respect to the optical axis of the first focusing element. Alternatively, the third beam path or further beam paths can also have a third focusing element and thus a spatially separate optical axis with the same constraints as the first two beam paths.
Embodiments of the invention also provide an EUV beam generating apparatus comprising a vacuum chamber, into which the target material is introducible into the target region for the purpose of generating EUV radiation, wherein the EUV beam generating apparatus comprises the focusing device described here and also a first beam source for generating the first laser beam and a second beam source for generating the second laser beam.
In this case, principal axes of the respective laser beams preferably correspond to the principal axes of the respective beam paths along which they are guided.
The laser beams can have different wavelengths. In particular, the first laser beam can have a wavelength of between 500 nm and 1200 nm and the second laser beam can have a wavelength of between 8 μm and 12 μm. In particular in the case of the wavelengths mentioned, the first optical element is preferably embodied in the form of a lens composed of quartz glass, borosilicate crown glass, sapphire glass, or in the form of a mirror composed of aluminum or silicon carbide or copper. In particular in the case of the wavelengths mentioned, the second optical element is preferably embodied in the form of a lens composed of zinc selenide or (artificial) diamond, or in the form of a mirror composed of copper. The materials mentioned have good optical properties in conjunction with good processability and good cooling capacity.
In a preferred embodiment of the invention, the first laser beam and/or the second laser beam are/is pulsed. This makes it possible, inter alia, for the power introduced into the target material and hence the power of the emitted EUV radiation to be high.
The EUV beam generating apparatus can comprise a third beam source for generating the third laser beam, wherein the principal axis of the third laser beam preferably corresponds to the principal axis of the third beam path.
The third laser beam can be pulsed. The pulsed third laser beam can be used for generating an intermediate pulse between a pulse as a result of the first laser beam and pulse as a result of the second laser beam onto the target material.
Further advantages of the invention are evident from the description and the drawing. Likewise, according to embodiments of the invention, the features mentioned above and those that will be explained still further can be used in each case individually by themselves or as a plurality in any desired combinations. The embodiments shown and described should not be understood as an exhaustive enumeration, but rather are of exemplary character for outlining the invention.
The focusing device 10 comprises a target material 12 moving in a target plane 14 in flight direction 16. The target material 12 is irradiated by a first laser beam 18 and a second laser beam 20. The irradiation of the target material 12 gives rise to EUV radiation that is reflected by a reflective optical element 70. The reflective optical element 70 has an optical axis 72, on which in particular a first and a second focal point of the reflective optical element 70 are arranged. In particular, the target material 12 is irradiated in such a way that the EUV radiation arises at the first focal point and is focused onto the second focal point by the reflective optical element 70. The target material preferably moves in a target plane 14 extending perpendicularly to the optical axis 72 of the reflective optical element 70. The first laser beam 18 is guided in a first beam path 22 and the second laser beam 20 is guided in a second beam path 24. A first focusing element 26 is arranged in the first beam path 22. A second focusing element 28 is arranged in the second beam path 24. The focusing elements 26, 28 are each embodied in the form of optically focusing elements. The focusing elements 26, 28 can have different focal lengths.
The focusing elements 26, 28 have optical axes 30, 32 extending coaxially with respect to the principal axes of the beam paths 22, 24 of the laser beams 18, 20. The laser beams 18, 20 are not superimposable on account of their wavelength and/or polarization. The optical axes 30, 32 are therefore at an angle of more than 4° with respect to one another and with respect to the optical axis 72 of the reflective optical element 70. As a result, the image planes 34, 36 are also at an angle of more than 4° with respect to the target plane 14. This results in distorted imagings 38 of the laser beams 18, 20 on the target material 12 (when viewed in the plane of the flight direction). When the target material 12 is viewed in viewing direction 40, for example cross-sectionally circular laser beams 18, 20 are imaged elliptically if the target material 12 is not spherical, but rather deformed. A deformation occurs here in particular as a result of the irradiation. An ineffective irradiation of the target material 12 takes place as a result.
As is evident from
In the present case, furthermore, the principal axes 42, 44 of the beam paths 22, 24 along which the laser beams 18, 20 are guided after passing through the focusing elements 34, 36 are offset with respect to the optical axes 30, 32. Alternatively, it is also possible for only one of the principal axes 42, 44 of the beam paths 22, 24 to extend offset with respect to the respective optical axis 30, 32. As indicated by dashed lines in
The focusing elements 26, 28 are preferably embodied in the form of optically focusing elements, in particular each in the form of a converging lens or a collecting mirror. Alternatively, it is also possible for only one of the focusing elements 26, 28 to be preferably embodied in the form of an optically focusing element, in particular in the form of a converging lens or a collecting mirror.
Deflection mirror(s) 46, 48 can be arranged in one or both beam paths 22, 24, said deflection mirrors merely being indicated schematically in
In the exemplary embodiment in accordance with
The laser beams 18, 20, 50 can cause the target material 12 to partly vaporize. As a result, the movement of the target material 12 can take place only approximately in the target plane 14 in some cases. The deviations of the trajectory of the target material 12 from the target plane 14 are illustrated schematically in an exaggerated manner, however, in the figures.
The first laser beam 18 and optional third laser beam 50 shown in
As described above, embodiments of the invention relate to a focusing device 10, in particular for generating EUV radiation. The focusing device 10 is designed to illuminate target material 12 on a target plane 14. The focusing device 10 comprises, at the very least, at least one beam shaping element 26, 28, the optical axis 30, 32 thereof being perpendicular to the target plane 14. As a result, the image plane of a laser beam 18, 20 guided by one of the focusing elements 26, 28 is aligned parallel to the target plane 14. This enables the efficient irradiation of the target material 12. A completely distortion-free imaging of at least one laser beam 18, 20 can be achieved by means of the principal axis of the beam path of said laser beam 18, 20 being offset with respect to the optical axis 30, 32 of the focusing element 26, 28 by which said laser beam 18, 20 is guided. One of the focusing elements 26, 28 can guide a third laser beam 50 for intermediate irradiation of the target material 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 |
|---|---|---|---|
| 21188167.7 | Jul 2021 | EP | regional |
This application is a continuation of International Application No. PCT/EP2022/071088 (WO 2023/006821 A1), filed on Jul. 27, 2022, and claims benefit to European Patent Application No. EP 21 188 167.7, filed on Jul. 28, 2021. The aforementioned applications are hereby incorporated by reference herein.
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/EP2022/071088 | Jul 2022 | US |
| Child | 18420916 | US |
