Abstract:
An imaging optical system has a plurality of mirrors which image an object field in an object plane in an image field in an image plane. The imaging optical system has a pupil obscuration. The last mirror in the beam path of the imaging light between the object field and the image field has a through-opening for the passage of the imaging light. A penultimate mirror of the imaging optical system in the beam path of the imaging light between the object field and the image field has no through-opening for the passage of the imaging light. The result is an imaging optical system that provides a combination of small imaging errors, manageable production and a good throughput for the imaging light.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
       [0001]    This application is a continuation of, and claims benefit under 35 USC 120 to, international application PCT/EP2010/000602, filed Feb. 2, 2010, which claims benefit under 35 USC 119 of German Application No. 10 2009 008 644.7, filed Feb. 12, 2009 and under 35 USC 119(e) of U.S. Ser. No. 61/151,871, filed Feb. 12, 2009 and U.S. Ser. No. 61/264,472, filed Nov. 25, 2009. International application PCT/EP2010/000602 is hereby incorporated by reference in its entirety. 
     
    
     FIELD 
       [0002]    The disclosure relates to an imaging optical system with a plurality of mirrors, which image an object field in an object plane into an image field in an image plane. Furthermore, the disclosure relates to a projection exposure installation with an imaging optical system of this type, a method for producing a microstructured or nanostructured component with a projection exposure system of this type, and a microstructured or nanostructured component produced by this method. 
       BACKGROUND 
       [0003]    Imaging optical systems are known from US 2006/0232867 A1 and US 2008/0170310 A1. 
       SUMMARY 
       [0004]    The disclosure provides an imaging optical system having a combination of small imaging errors, manageable production and good throughput for the imaging light are achieved. 
         [0005]    According to the disclosure, it is recognised that without relatively large losses in the imaging quality, it is possible, in a pupil-obscured system, in other words in an imaging optical system with a pupil obscuration, to configure the penultimate mirror with a continuous reflective face, in other words without a through-opening within the optically used region of the penultimate mirror. This facilitates the production of this penultimate mirror with an adequate mirror thickness and also allows an adequately large spacing between the side of the penultimate mirror facing the image plane and the image plane while at the same time minimising the size of the pupil obscuration. This facilitation of production is particularly important if this penultimate mirror is arranged on a mirror body and/or a mirror carrier which is thin in comparison to the other mirrors. 
         [0006]    The numerical value for the pupil obscuration is produced by the ratio of the area within the exit pupil masked because of the pupil obscuration relative to a total area of an exit pupil of the imaging optical system. A pupil obscuration, which is less than 5%, makes possible a pupil obscured imaging optical system with a particularly high light throughput. Furthermore, the small obscuration according to the disclosure may lead to a small or negligible influence on an imaging quality of the imaging optical system, in particular on the imaging contrast. The pupil obscuration may be less than 10%. The pupil obscuration may, for example, be 4.4% or 4.0%. The pupil obscuration may be less than 4%, may be less than 3%, may be less than 2% and may even be less than 1%. The pupil obscuration of the imaging optical system may be predetermined by one of the mirrors, for example by a through-opening thereof or by an outer edging thereof, or by an obscuration stop or diaphragm, which is arranged in the beam path of the imaging light between the object field and the image field. 
         [0007]    At least one of the mirrors of the imaging optical system according to one of the two aspects described above may have a reflection face, which is designed as a free-form face which cannot be described by a rotationally symmetrical function. 
         [0008]    A working spacing of the penultimate mirror additionally facilitates its production. The working spacing may be at least 22 mm, at least 40 mm, at least 60 mm, at least 80 mm and may even be 85 mm. Even larger values for the working spacing are possible. The working spacing is defined as the spacing between the image plane and the portion closest thereto of a used reflection face of the closest mirror, in other words the penultimate mirror of the projection optical system. The image plane is the field plane, which is adjacent to the penultimate mirror, of the imaging optical system. 
         [0009]    A maximum angle of incidence facilitates the configuration of a highly reflective coating on this mirror. This is advantageous, in particular, if imaging light with a small wavelength is used, for example with DUV (Deep Ultraviolet), VUV (Vacuum Ultraviolet), or EUV (Extreme Ultraviolet) wavelengths. A multi-layer coating with a small acceptance band width of the angle of incidence and a correspondingly high reflection may then be used, in particular. The maximum angle of incidence of the imaging light on the penultimate mirror in the beam path may be 34.5°, 30°, 25°, 20°, 16.9° or 15.9° in the meridional section of the imaging optical system. 
         [0010]    An arrangement of the penultimate mirror leads to the possibility that a holder, which holds this penultimate mirror and mirrors of the imaging beam path in front of the imaging beam path section, between the third to last mirror and the penultimate mirror, may be relatively compact in design. 
         [0011]    As an alternative to this, an arrangement of the penultimate mirror is possible. 
         [0012]    An arrangement of the third to last and the sixth to last mirror back to back leads to a compact structure of the imaging optical system with good utilisation of the installation space. 
         [0013]    Basically, instead of a back to back mirror arrangement, an arrangement is also possible in which reflection faces are provided on both sides of a monolithic base body, which correspond to the mirror faces of the mirror arrangement then replaced. 
         [0014]    At least one intermediate image leads to the possibility of guiding an imaging beam path section of the beam path of the imaging light between the object field and the image field closely past further components of the imaging optical system. The intermediate image may, in particular, be arranged in the region of the through-opening of the last mirror, which makes a small pupil obscuration possible. The imaging optical system may also have more than one intermediate image and may, in particular, have two intermediate images in the beam path of the imaging light between the object field and the image field. 
         [0015]    A plurality of intermediate images may also be used to for correcting imaging errors or simplifying the design of the mirror forms involved. 
         [0016]    At least one crossing or intersection region allows compact beam guidance. The imaging optical system may also have more than one intersection region of this type, in particular two, three or four intersection regions, between imaging beam path sections. One or all of the intersection regions may spatially overlap one another at least in portions. An intersection region is taken to mean the region in which the imaging beam path sections intersect in total. In the reflection on a mirror, the imaging beam path sections therefore, according to definition, do not intersect in an intersection region of this type. 
         [0017]    A numerical aperture allows high resolution of the imaging optical system. The numerical aperture may be at least 0.4 and may also be at least 0.5. 
         [0018]    A rectangular field facilitates the conducting of the lithography process when using the imaging optical system. A rectangular field of this type may be achieved, in particular, by the use of non-rotationally symmetrical free-form faces as reflection faces of the mirrors of the imaging optical system. At least one of the mirrors may be configured as a free-form face of this type. The image field may have dimensions of 2 mm×26 mm or of 2.5 mm×26 mm. 
         [0019]    When using the imaging optical system as a projection optical system its advantages stand out, in particular. 
         [0020]    The imaging optical system according to the disclosure may have precisely six mirrors. 
         [0021]    The advantages of a projection exposure installation according to the disclosure correspond to those which were stated above with respect to the imaging optical system according to the disclosure. The light source of the projection exposure installation may be wide band in design and for example have a band width, which may be greater than 1 nm, which is greater than 10 nm or which is greater than 100 nm. In addition, the projection exposure installation may be designed such that it can be operated with light sources of different wavelengths. Light sources for other wavelengths used, in particular, for microlithography, can be used in conjunction with the imaging optical system according to the disclosure, for example light sources with the wavelengths 365 nm, 248 nm, 193 nm, 157 nm, 126 nm, 109 nm and, in particular, also with wavelengths, which are less than 100 nm, for example between 5 nm and 30 nm. 
         [0022]    The light source of the projection exposure installation may be configured to produce illumination light with a wavelength of between 5 nm and 30 nm. A light source of this type uses reflection coatings on the mirrors which, in order to fulfil a minimum reflectivity, have only a small angle of incidence acceptance band width. Together with the imaging optical system according to the disclosure, this desire a small angle of incidence acceptance band width can be fulfilled. 
         [0023]    Corresponding advantages apply to a production method according to the disclosure and the microstructured or nanostructured component produced thereby. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0024]    An embodiment of the disclosure will be described in more detail below with the aid of the drawings, in which: 
           [0025]      FIG. 1  schematically shows a projection exposure installation for EUV microlithography; 
           [0026]      FIG. 2  shows, in a meridional section, an embodiment of an imaging optical system, which can be used as a projection lens system in the projection exposure installation according to  FIG. 1 , the imaging beam path being shown (virtually) for the main beams and being shown for the upper and lower coma beam of a plurality of selected field points; 
           [0027]      FIGS. 3 to 21  show further embodiments of the imaging optical system in a view similar to  FIG. 2 . 
       
    
    
     DETAILED DESCRIPTION 
       [0028]    A projection exposure installation  1  for microlithography has a light source  2  for illumination light or imaging light  3 . The light source  2  is an EUV light source which produces light in a wavelength range of, for example, between 5 nm and 30 nm, in particular between 5 nm and 15 nm. The light source  2  may, in particular, be a light source with a wavelength of 13.5 nm or a light source with a wavelength of 6.9 nm. Other EUV wavelengths are also possible. In general, any wavelengths, for example visible wavelengths or else other wavelengths, which can be used in microlithography and are available for the suitable laser light sources and/or LED light sources (for example 365 nm, 248 nm, 193 nm, 157 nm, 129 nm, 109 nm), are even possible for the illumination light  3  guided in the projection exposure installation  1 . A beam path of the illumination light  3  is shown extremely schematically in  FIG. 1 . 
         [0029]    An illumination optical system  6  is used to guide the illumination light  3  from the light source  2  to an object field  4  in an object plane  5 . The object field  4  is imaged in an image field  8  in an image plane  9  with the predetermined reduction scale using a projection optical system or an imaging optical system  7 . The image field  8 , in the x-direction, has an extent of 26 mm and, in the y-direction, an extent of 2 mm. The object field  4  and the image field  8  are rectangular. One of the embodiments shown in  FIG. 2   ff . can be used for the projection optical system  7 . The projection optical system  7  according to  FIG. 2  reduces by a factor of 4. Other reduction scales are also possible, for example 5×,  8 × or else reduction scales which are greater than 8×. The image plane  9 , in the projection optical system  7  in the embodiments according to  FIG. 2   ff . is arranged parallel to the object plane  5 . Imaged here is a portion, which coincides with the object field  4 , of a reflection mask  10 , which is also called a reticle. 
         [0030]    The imaging by the projection optical system  7  takes place on the surface of a substrate  11  in the form of a wafer, which is carried by a substrate holder  12 .  FIG. 1  schematically shows, between the reticle  10  and the projection optical system  7 , a beam concentration  13  of the illumination light  3  running therein, and, between the projection optical system  7  and the substrate  11 , a beam concentration  14  of the illumination light  3  leaving the projection optical system  7 . A numerical aperture (NA) on the image field side of the projection optical system  7  in the embodiment according to  FIG. 2  is 0.50. This is not represented to scale in  FIG. 1 . 
         [0031]    To facilitate the description of the projection exposure installation  1  and the various embodiments of the projection optical system  7 , a Cartesian xyz-coordinate system is given in the drawing, from which the respective position reference of the components shown in the figures emerges. In  FIG. 1 , the x-direction runs perpendicular to the plane of the drawing and into it. The y-direction extends to the right and the z-direction downward. 
         [0032]    The projection exposure installation  1  is of the scanner type. Both the reticle  10  and the substrate  11  are scanned during operation of the projection exposure installation  1  in the y-direction. A stepper type of the projection exposure installation  1 , in which a stepwise displacement of the reticle  10  and the substrate  11  in the y-direction takes place in between individual exposures of the substrate  11 , is possible. 
         [0033]      FIG. 2  shows the optical design of a first embodiment of the projection optical system  7 .  FIG. 2  shows the beam path of three respective individual beams  15 , which issue from five object field points spaced apart from one another in the y-direction in  FIG. 2 . The three individual beams  15 , which belong to one of these five object field points, are in each case associated with three different illumination directions for the two object field points. Main beams  16 , which run through the centre of a pupil in a pupil plane  17  of the projection optical system  7 , are drawn in  FIG. 2  only for graphical reasons as these are not real, but virtual imaging beam paths of the projection optical system  7  because of a central pupil obscuration of the projection optical system  7 . These main beams  16  firstly run divergently, proceeding from the object plane  5 . This is also called a negative back focal distance of an entry pupil of the projection optical system  7  below. The entry pupil of the projection optical system  7  according to  FIG. 2  is not located within the projection optical system  7 , but in the beam path in front of the object plane  5 . This makes it possible, for example, to arrange a pupil component of the illumination optical system  6  in the entry pupil of the projection optical system  7  in the beam path in front of the projection optical system  7 , without further imaging optical components having to be present between this pupil component and the object plane  5 . 
         [0034]    The projection optical system  7  according to  FIG. 2  has a total of six mirrors, which are numbered consecutively by M 1  to M 6  in the order of their arrangement in the beam path of the individual beams  15 , proceeding from the object field  4 .  FIG. 2  shows the calculated reflection faces of the mirrors M 1  to M 6  or M 5 , M 6 . Only a small region of these calculated reflection faces is used, as can be seen in the view of  FIG. 2 . Only this actually used region of the reflection faces is actually present in the real mirrors M 1  to M 6 . These useful reflection faces are carried in a known manner by mirror bodies. 
         [0035]    All six mirrors M 1  to M 6  of the projection optical system  7  are designed as free-form faces which cannot be described by a rotationally symmetrical function. Other embodiments of the projection optical system  7  are also possible, in which at least one of the mirrors M 1  to M 6  has a free-form reflection face of this type. 
         [0036]    A free-form face of this type may also be produced from a rotationally symmetrical reference face. Free-form faces of this type for reflection faces of the mirrors of projection optical systems of projection exposure installation for microlithography are known from US 2007-0058269 A1. 
         [0037]    The free-form face can be described mathematically by the following equation: 
         [0000]    
       
         
           
             
               
                 
                   Z 
                   = 
                   
                     
                       
                         cr 
                         2 
                       
                       
                         1 
                         + 
                         
                           
                             1 
                             - 
                             
                               
                                 ( 
                                 
                                   1 
                                   + 
                                   k 
                                 
                                 ) 
                               
                                
                               
                                 c 
                                 2 
                               
                                
                               
                                 r 
                                 2 
                               
                             
                           
                         
                       
                     
                     + 
                     
                       
                         ∑ 
                         
                           j 
                           = 
                           2 
                         
                         N 
                       
                        
                       
                           
                       
                        
                       
                         
                           C 
                           j 
                         
                          
                         
                           X 
                           m 
                         
                          
                         
                           Y 
                           n 
                         
                       
                     
                   
                 
               
               
                 
                   ( 
                   1 
                   ) 
                 
               
             
           
         
       
     
         [0000]    wherein there applies: 
         [0000]    
       
         
           
             
               
                 
                   j 
                   = 
                   
                     
                       
                         
                           
                             ( 
                             
                               m 
                               + 
                               n 
                             
                             ) 
                           
                           2 
                         
                         + 
                         m 
                         + 
                         
                           3 
                            
                           
                               
                           
                            
                           n 
                         
                       
                       2 
                     
                     + 
                     1 
                   
                 
               
               
                 
                   ( 
                   2 
                   ) 
                 
               
             
           
         
       
     
         [0000]    Z is the rising height (sagitta) of the free-form face at the point x, y 
         [0000]      ( x   2   +y   2   =r   2 ). 
         [0000]    c is a constant, which corresponds to the vertex curvature of a corresponding asphere. k corresponds to a conical constant of a corresponding asphere. C j  are the coefficients of the monomials X m Y n . Typically, the values of c, k and C j  are determined on the basis of the desired optical properties of the mirror within the projection optical system  7 . The order of the monomial, m+n, may be varied as desired. A monomial of a higher order may lead to a design of the projection optical system with improved image error correction, but is more complex to calculate. m+n may adopt values of between 3 and more than 20. 
         [0038]    Free-form faces can also be described mathematically by Zernike polynomials, which are described, for example, in the manual of the optical design programme CODE V®. Alternatively, free-form faces may be described with the aid of two-dimensional spline surfaces. Examples of this are Bezier curves or non-uniform rational basis splines (NURBS). Two-dimensional spline surfaces may, for example, be described by a network of points in an xy-plane and associated z-values or by these points and gradients associated with them. Depending on the respective type of spline surface, the complete surface is obtained by interpolation between the network points using, for example, polynomials or functions, which have specific properties with regard to their continuity and differentiability. Examples of this are analytical functions. 
         [0039]    The mirrors M 1  to M 6  have multiple reflection layers to optimise their reflection for the impinging EUV illumination light  3 . The reflection can be optimised all the better, the closer the impingement angle of the individual beams  15  on the mirror surface lies to the perpendicular incidence. The projection optical system  7  has small reflection angles overall for all the individual beams  15 . 
         [0040]    The optical design data of the reflection faces of the mirrors M 1  to M 6  of the projection optical system  7  can be inferred from the following tables. The first of these tables gives, for the optical surfaces of the optical components and for the aperture diaphragm, the respective reciprocal value of the vertex curvature (radius) and a spacing value (thickness), which corresponds to the z-spacing of adjacent elements in the beam path, proceeding from the object plane. The second table gives the coefficients C, of the monomials X m Y n  in the free-form face equation given above for the mirrors M 1  to M 6 . Nradius is in this case a standardisation factor. According to the second table, the amount is still given in mm, along which the respective mirror, proceeding from a mirror reference design, has been decentred (Y-decentre) and rotated (X-rotation). This corresponds to a parallel displacement and a tilting in the free-form face design method. The displacement takes place here in the y-direction and the tilting is about the x-axis. The rotation angle is given in degrees here. 
         [0000]    
       
         
               
               
               
               
             
               
               
               
               
             
           
               
                   
               
               
                 Surface 
                 Radius 
                 Spacing value 
                 Operating mode 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 Object plane 
                 INFINITE 
                 815.666 
                   
               
               
                 M1 
                 −1153.305 
                 −615.656 
                 REFL 
               
               
                 M2 
                 222.516 
                 319.520 
                 REFL 
               
               
                 M3 
                 382.480 
                 −319.520 
                 REFL 
               
               
                 M4 
                 558.747 
                 1485.905 
                 REFL 
               
               
                 M5 
                 701.517 
                 −770.248 
                 REFL 
               
               
                 M6 
                 875.932 
                 810.223 
                 REFL 
               
               
                 Image plane 
                 INFINITE 
                 0.000 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
             
           
               
                   
               
               
                 Coef- 
                   
                   
                   
                   
                   
                   
               
               
                 ficient 
                 M1 
                 M2 
                 M3 
                 M4 
                 M5 
                 M6 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 K 
                 −2.605966E+00 
                 −5.961575E−01 
                 1.802738E+00 
                 −4.147176E−01 
                 5.283440E+00 
                 −8.773495E−03 
               
               
                 Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2 
                 9.076785E−06 
                 −2.333474E−03 
                 9.771997E−05 
                 −1.351961E−04 
                 −3.072793E−04 
                 −3.218741E−05 
               
               
                 Y2 
                 −1.262804E−05 
                 −2.351151E−03 
                 −4.280681E−04 
                 −2.063652E−04 
                 −4.778011E−05 
                 −1.825268E−05 
               
               
                 X2Y 
                 5.547212E−08 
                 1.113508E−06 
                 1.714986E−06 
                 4.601654E−08 
                 −7.454541E−07 
                 −3.779820E−09 
               
               
                 Y3 
                 7.260181E−08 
                 9.449646E−07 
                 1.271140E−06 
                 8.751761E−08 
                 −2.182587E−07 
                 4.618324E−09 
               
               
                 X4 
                 −2.717367E−10 
                 −5.643202E−09 
                 1.100027E−10 
                 2.753993E−11 
                 1.011144E−10 
                 −1.051777E−11 
               
               
                 X2Y2 
                 −4.717758E−10 
                 −1.285056E−08 
                 −1.176444E−08 
                 −6.509076E−11 
                 −5.621785E−10 
                 −2.181974E−11 
               
               
                 Y4 
                 −1.535374E−10 
                 −5.716571E−09 
                 −8.317888E−09 
                 −1.255759E−10 
                 1.083353E−10 
                 −7.220214E−12 
               
               
                 X4Y 
                 4.620639E−14 
                 2.908858E−12 
                 −2.838235E−11 
                 −5.428510E−14 
                 −3.027549E−13 
                 2.004008E−15 
               
               
                 X2Y3 
                 1.354365E−13 
                 2.499768E−12 
                 −4.853945E−11 
                 1.768342E−14 
                 3.032599E−12 
                 4.901143E−15 
               
               
                 Y5 
                 9.758474E−14 
                 −8.026135E−12 
                 −2.371972E−11 
                 1.039111E−13 
                 6.346065E−12 
                 6.164413E−15 
               
               
                 X6 
                 −1.650739E−19 
                 −1.746162E−14 
                 −4.622947E−14 
                 4.561474E−17 
                 −1.475643E−15 
                 −4.982818E−18 
               
               
                 X4Y2 
                 1.411917E−16 
                 −4.021338E−14 
                 −1.679149E−13 
                 4.396111E−16 
                 −2.334912E−15 
                 −7.006257E−18 
               
               
                 X2Y4 
                 4.293001E−16 
                 3.421095E−14 
                 −2.624283E−13 
                 4.785171E−16 
                 2.028609E−14 
                 −2.259935E−18 
               
               
                 Y6 
                 3.538529E−16 
                 1.283163E−14 
                 3.276365E−14 
                 9.873439E−16 
                 1.117653E−14 
                 8.963014E−19 
               
               
                 X6Y 
                 −2.078486E−19 
                 −1.183867E−16 
                 −3.132075E−16 
                 2.806498E−19 
                 1.669547E−17 
                 3.910845E−21 
               
               
                 X4Y3 
                 −2.392439E−19 
                 −3.921710E−16 
                 −1.722114E−16 
                 3.083030E−19 
                 2.773189E−17 
                 1.616941E−20 
               
               
                 X2Y5 
                 3.774411E−19 
                 −4.353032E−16 
                 4.633354E−16 
                 1.078201E−18 
                 2.004813E−17 
                 1.540131E−20 
               
               
                 Y7 
                 −7.122980E−18 
                 −3.967812E−17 
                 6.639885E−16 
                 −2.211631E−18 
                 −8.876500E−17 
                 4.032079E−21 
               
               
                 X8 
                 −1.403258E−22 
                 −5.276488E−20 
                 −1.503485E−18 
                 1.126741E−22 
                 −3.102183E−20 
                 −3.780424E−24 
               
               
                 X6Y2 
                 −1.352342E−21 
                 5.134116E−19 
                 −9.187180E−18 
                 −4.302896E−22 
                 3.184593E−20 
                 −4.432214E−24 
               
               
                 X4Y4 
                 −2.843591E−21 
                 8.052424E−19 
                 −1.538670E−17 
                 −9.478150E−22 
                 1.108150E−20 
                 1.149988E−24 
               
               
                 X2Y6 
                 3.933427E−21 
                 2.988855E−19 
                 −7.353139E−18 
                 −1.034931E−20 
                 −1.498632E−19 
                 1.296327E−24 
               
               
                 Y8 
                 −1.881220E−20 
                 −5.733234E−19 
                 −1.441529E−18 
                 2.416028E−21 
                 −4.165554E−19 
                 −1.440139E−24 
               
               
                 X8Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y3 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y5 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y7 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y9 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X10 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y10 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Nradius 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
               
             
           
               
                   
               
               
                 Coef- 
                   
                   
                   
                   
                   
                   
                 Image 
               
               
                 ficient 
                 M1 
                 M2 
                 M3 
                 M4 
                 M5 
                 M6 
                 plane 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 Y-decentre 
                 −4.633 
                 −32.903 
                 −307.827 
                 −405.254 
                 −609.190 
                 −503.476 
                 0.000 
               
               
                 X-rotation 
                 −2.685 
                 −19.040 
                 −11.876 
                 4.571 
                 −7.815 
                 −3.906 
                 0.000 
               
               
                   
               
             
          
         
       
     
         [0041]    The mirrors M 1 , M 2 , M 4  and M 6  are configured as concave mirrors. The radius of curvature of the mirror M 2  is so large that it almost looks like a planar mirror in  FIG. 2 . The mirrors M 3  and M 5  are configured as convex mirrors. 
         [0042]    The mirrors M 1  and M 6  and M 3  and M 6  are arranged back to back with regard to the orientation of their reflection faces. 
         [0043]    The optically used regions of the mirrors M 1  to M 5  have no through-opening within the optically used region for the passage of imaging light, in other words are not obscured. The mirror M 5 , in other words the penultimate mirror in the beam path of the illumination light  3  between the object field  4  and the image field  8 , also has no through-opening for the passage of the imaging light or illumination light  3 . The mirror M 5 , in other words, has an uninterrupted used reflection face. 
         [0044]    In the imaging beam path between the mirrors M 4  and M 5 , the individual beams  15  pass through a through-opening  18  in the mirror M 6 . The mirror M 6  is used around the through-opening  18 . The mirror M 6  is thus an obscured mirror. 
         [0045]    The pupil plane  17 , in the imaging beam path in the projection optical system  7 , lies between the mirrors M 2  and M 3 . The pupil plane  17  also lies in the imaging beam path between the object field  4  and the through-opening  18  of the mirror M 6 . An obscuration stop or diaphragm for central shading of a pupil of the projection optical system  7  may be arranged in the pupil plane  17 . The obscuration diaphragm thus shades the central region of the imaging light  3  in the pupil plane  17  which does not contribute to the imaging of the object field  4  because of the through-opening  18 . 
         [0046]    An intermediate image plane  19  of the projection optical system  7  is located in the imaging beam path between the mirrors M 4  and M 5 . The associated intermediate image is located adjacent to the through-opening  18  in the mirror M 6 . As a result it is possible to make this through-opening  18  small in comparison to the used reflection face of the mirror M 8 . A central pupil obscuration, in other words the ratio of an area blanked by the through-opening  18  or the obscuration diaphragm in the pupil plane  17  within an exit pupil of the projection optical system  7  relative to an overall face of this exit pupil, is 4.4% in the projection optical system  7 . 
         [0047]    A working spacing d w  between the image plane  9  and the portion closest to the image plane of a used reflection face of the mirror M 5  is 22 mm. A ratio of this working spacing d w  to the overall length of the projection optical system  7 , in other words to the spacing between the object field  4  and the image field  8 , is 1.3%. 
         [0048]    A further pupil plane  20  of the projection optical system  7  is located in the imaging beam path in the region of the mirror M 5 . A diaphragm may also be arranged here. 
         [0049]    The angle of incidence of the individual beams  15  on the mirror M 3  in the meridional plane, which is shown in  FIG. 2 , is a maximum of 34.5°. 
         [0050]    An imaging beam path section  21  runs between the third to last mirror M 4  in the imaging beam path and the penultimate mirror M 5  in the imaging beam path. This imaging beam path section  21  begins at the reflection on the mirror M 4  and ends at the reflection on the mirror M 5 . The imaging beam path in the projection optical system  7  in front of the imaging beam path section  21 , in other words the imaging beam path between the object field  4  and the mirror M 4 , on the one hand, and an imaging light bundle  22  in the region of the image field  8 , on the other hand, are guided on the same side of the imaging beam path section  21 . Accordingly, the object field  4  and the penultimate mirror M 5  are arranged on different sides of a main plane  23  which extends centrally through the image field  8  and is perpendicular to the meridional plane, in other words the plane of the drawing of  FIGS. 2 to 4 . 
         [0051]      FIG. 3  shows a further embodiment of the projection optical system  7 . Components, which correspond to those of the projection optical system  7  according to  FIG. 2 , have the same reference numerals and are not discussed again in detail. 
         [0052]    The optical design data of the projection optical system  7  according to  FIG. 3  can be inferred from the following tables, which correspond to the tables on the projection optical system  7  according to  FIG. 2  with respect to their structure. 
         [0000]    
       
         
               
               
               
               
             
               
               
               
               
             
           
               
                   
               
               
                 Surface 
                 Radius 
                 Spacing value 
                 Operating mode 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 Object plane 
                 INFINITE 
                 986.270 
                   
               
               
                 M1 
                 −815.021 
                 −716.283 
                 REFL 
               
               
                 M2 
                 −1692.737 
                 1034.499 
                 REFL 
               
               
                 M3 
                 805.634 
                 −904.485 
                 REFL 
               
               
                 M4 
                 1745.655 
                 1800.135 
                 REFL 
               
               
                 M5 
                 186.402 
                 −695.651 
                 REFL 
               
               
                 M6 
                 818.011 
                 795.967 
                 REFL 
               
               
                 Image plane 
                 INFINITE 
                 0.000 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
               
             
           
               
                   
               
               
                 Coef- 
                   
                   
                   
                   
                   
                   
                 Image 
               
               
                 ficient 
                 M1 
                 M2 
                 M3 
                 M4 
                 M5 
                 M6 
                 plane 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 K 
                 −1.238679E−01 
                 −1.791231E+01 
                 −1.198325E+00 
                 −2.530823E−01 
                 −1.020467E−02 
                 5.662681E−02 
                   
               
               
                 X2 
                 1.225388E−04 
                 −1.219365E−03 
                 −9.215303E−04 
                 −2.476431E−04 
                 −1.451018E−03 
                 −6.707230E−06 
               
               
                 Y2 
                 3.086233E−04 
                 3.281365E−04 
                 −2.291446E−04 
                 5.508666E−05 
                 −1.225948E−03 
                 −2.358417E−06 
               
               
                 X2Y 
                 3.520023E−08 
                 −2.237558E−06 
                 4.383580E−08 
                 −5.980784E−10 
                 1.944652E−06 
                 5.208464E−10 
               
               
                 Y3 
                 −3.914904E−09 
                 8.665292E−08 
                 3.997990E−07 
                 5.130872E−09 
                 −9.275351E−07 
                 −5.831866E−09 
               
               
                 X4 
                 5.262082E−11 
                 −5.336536E−08 
                 2.120561E−11 
                 −2.198962E−11 
                 −7.191540E−09 
                 6.478133E−13 
               
               
                 X2Y2 
                 1.459216E−10 
                 −7.004312E−10 
                 5.077070E−10 
                 1.326969E−10 
                 −1.229590E−08 
                 −1.283249E−12 
               
               
                 Y4 
                 1.690794E−10 
                 −3.956379E−10 
                 6.068550E−10 
                 2.595291E−11 
                 −4.780182E−09 
                 −3.237182E−12 
               
               
                 X4Y 
                 −2.099690E−14 
                 −1.842852E−11 
                 1.225213E−13 
                 1.180341E−13 
                 1.310535E−11 
                 −2.534706E−15 
               
               
                 X2Y3 
                 3.021789E−14 
                 −1.362668E−11 
                 −4.690792E−13 
                 −1.357904E−13 
                 1.637678E−11 
                 −8.678287E−16 
               
               
                 Y5 
                 1.894306E−13 
                 2.933573E−13 
                 −6.894643E−12 
                 −5.680668E−14 
                 −6.265372E−12 
                 −1.795660E−15 
               
               
                 X6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y3 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y5 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y7 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y3 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y5 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y7 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y9 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X10 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y10 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Nradius 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
                 0.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
               
               
                 Y-decentre 
                 −28.611 
                 −158.244 
                 −344.671 
                 −406.391 
                 −114.284 
                 −227.166 
                 0.000 
               
               
                 X-rotation 
                 1.129 
                 0.021 
                 −3.156 
                 6.560 
                 9.217 
                 4.608 
                 0.000 
               
               
                   
               
             
          
         
       
     
         [0053]    In the projection optical system  7  according to  FIG. 3 , the mirror M 5 , in comparison to the projection optical system  7  according to  FIG. 2 , is present mirrored about the main plane  23 . The penultimate mirror M 5  and the object field  4  are arranged on the same side of the main plane  23 . The imaging beam path between the object field  4  and the mirror M 2 , on the one hand, and the imaging light bundle  22  in the region of the image field  8  of the projection optical system  7  according to  FIG. 3 , on the other hand, are guided on different sides of the imaging beam path section  21 . The imaging beam path section  21  and a further imaging beam path section  24  between the mirrors M 2  and M 3  intersect in the imaging beam path of the projection optical system  7  according to  FIG. 3 . 
         [0054]    In the projection optical system  7  according to  FIG. 3 , the mirror M 2  is configured as a convex mirror. Because of the very large radius of curvature of the mirror M 2 , the latter appears virtually to be a planar mirror in  FIG. 3 . 
         [0055]    The intermediate image plane  19 , in the projection optical system  7  according to  FIG. 3 , lies practically precisely at the level of the through-opening  18  in the mirror M 6 . 
         [0056]    The central pupil obscuration in the projection optical system  7  according to  FIG. 3  is 4.0%. The working spacing d w  between the image plane  9  and the portion of the used reflection face of the mirror M 5  closest to the image plane is 85 mm. A radio of this working spacing d w  to the overall length of the projection optical system  7  according to  FIG. 3  is 3.7%. The angle of incidence of the individual beams  15  on the mirror M 5  in the meridional plane, which is shown in  FIG. 3 , is a maximum of 16.9°. 
         [0057]      FIG. 4  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 and 3  have the same reference numerals and are not discussed again in detail. 
         [0058]    The optical design data of the projection optical system  7  according to  FIG. 4  can be inferred from the following tables, which correspond to the tables on the projection optical system  7  according to  FIGS. 2 and 3  with regard to their structure. 
         [0000]    
       
         
               
               
               
               
             
               
               
               
               
             
           
               
                   
               
               
                 Surface 
                 Radius 
                 Spacing value 
                 Operating mode 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 Object plane 
                 INFINITE 
                 485.884 
                   
               
               
                 M1 
                 573.309 
                 −385.884 
                 REFL 
               
               
                 M2 
                 856.474 
                 1014.613 
                 REFL 
               
               
                 M3 
                 −619.480 
                 −508.729 
                 REFL 
               
               
                 M4 
                 601.504 
                 1294.117 
                 REFL 
               
               
                 M5 
                 256.986 
                 −685.388 
                 REFL 
               
               
                 M6 
                 838.548 
                 785.387 
                 REFL 
               
               
                 Image plane 
                 INFINITE 
                 0.000 
               
               
                   
               
             
          
         
       
     
         [0000]    
       
         
               
               
               
               
               
               
               
               
             
               
               
               
               
               
               
               
               
             
           
               
                   
               
               
                 Coef- 
                   
                   
                   
                   
                   
                   
                 Image 
               
               
                 ficient 
                 M1 
                 M2 
                 M3 
                 M4 
                 M5 
                 M6 
                 plane 
               
               
                   
               
             
             
               
                   
               
             
          
           
               
                 K 
                 −5.356880E−02 
                 8.027989E−02 
                 2.215137E+00 
                 −5.038784E−01 
                 4.907814E−02 
                 1.120410E−01 
                   
               
               
                 Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2 
                 −4.675062E−04 
                 −2.669898E−05 
                 1.839305E−03 
                 −2.126518E−04 
                 −9.700568E−04 
                 7.232599E−06 
               
               
                 Y2 
                 −1.320900E−03 
                 −5.452804E−04 
                 7.818071E−04 
                 −4.431611E−04 
                 −8.012468E−04 
                 1.044012E−05 
               
               
                 X2Y 
                 1.229247E−06 
                 4.121203E−07 
                 −2.381957E−06 
                 −9.694733E−08 
                 −1.199882E−06 
                 −5.510251E−09 
               
               
                 Y3 
                 −7.423640E−08 
                 −8.613636E−08 
                 4.979224E−08 
                 −2.077214E−08 
                 1.739231E−07 
                 −1.476529E−09 
               
               
                 X4 
                 −2.550932E−10 
                 −5.351417E−11 
                 1.281481E−08 
                 −4.388472E−11 
                 −2.188996E−09 
                 2.529523E−13 
               
               
                 X2Y2 
                 −2.178964E−10 
                 −2.067816E−10 
                 8.488864E−09 
                 −1.254954E−10 
                 −2.292180E−09 
                 2.688243E−13 
               
               
                 Y4 
                 −8.677437E−10 
                 −8.009019E−10 
                 1.878436E−09 
                 −1.372181E−10 
                 −1.320127E−09 
                 1.277954E−12 
               
               
                 X4Y 
                 −3.215827E−13 
                 1.670802E−13 
                 −1.372762E−10 
                 4.754789E−14 
                 −6.365774E−12 
                 −2.679463E−16 
               
               
                 X2Y3 
                 −1.228117E−12 
                 3.874349E−13 
                 −2.437182E−11 
                 −1.718101E−13 
                 −6.070058E−12 
                 −1.679816E−15 
               
               
                 Y5 
                 −1.148542E−13 
                 2.500543E−13 
                 1.577671E−12 
                 5.427575E−13 
                 −6.442309E−12 
                 −1.838497E−15 
               
               
                 X6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y3 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y5 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y7 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8Y 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y3 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y5 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y7 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y9 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X10 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X8Y2 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X6Y4 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X4Y6 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 X2Y8 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Y10 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
                 0.000000E+00 
               
               
                 Nradius 
                 1.000000E+00 
                 0.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
                 1.000000E+00 
               
               
                 Y-decentre 
                 172.287 
                 276.185 
                 336.270 
                 167.562 
                 379.550 
                 267.210 
                 0.000 
               
               
                 X-rotation 
                 −3.535 
                 −5.840 
                 10.868 
                 13.825 
                 9.306 
                 4.657 
                 0.000 
               
               
                   
               
             
          
         
       
     
         [0059]    The imaging beam path between the intermediate image plane  19  and the image field  8 , in the projection optical system  7  according to  FIG. 4 , corresponds to that of the projection optical system  7  according to  FIG. 3 . 
         [0060]    The object field  4  and the mirror M 5  are arranged on different sides of the main plane  23 . 
         [0061]    The mirrors M 1  and M 4  on the one hand, and the mirrors M 3  and M 6 , on the other hand, in the projection optical system  7  according to  FIG. 4 , are arranged back to back. 
         [0062]    The mirrors M 1 , M 3  and M 6  are concave. The mirror M 5  is convex. The mirrors M 2  and M 4  have a radius of curvature which is so great that they appear virtually to be a planar mirror in  FIG. 4 . 
         [0063]    In the projection optical system  7  according to  FIG. 4 , an aperture diaphragm may be arranged in the region of the pupil plane  17  between the mirrors M 2  and M 3 . 
         [0064]    The central pupil obscuration, in the projection optical system  7  according to  FIG. 4 , is 4.0%. The working spacing d w  between the image plane  9  and the portion of the used reflection face of the mirror M 5  closest to the image plane is 85 mm in the projection optical system according to  FIG. 4 . A ratio of this working spacing d w  to the overall length of the projection optical system  7  according to  FIG. 4  is 4.25%. The angle of incidence of the individual beams  15  on the mirror M 5  in the meridional plane, which is shown in  FIG. 4 , is a maximum of 15.9°. 
         [0065]    In the following table, characteristics of the projection optical system 
         [0066]    (PO) according to  FIGS. 2 ,  3  and  4  are summarised again: 
         [0000]    
       
         
               
               
               
               
             
               
               
               
               
             
           
               
                   
                   
               
               
                   
                 PO accord- 
                 PO accord- 
                 PO accord- 
               
               
                   
                 ing to 
                 ing to 
                 ing to 
               
               
                   
                 FIG. 2 
                 FIG. 3 
                 FIG. 4 
               
               
                   
                   
               
             
             
               
                   
               
             
          
           
               
                 NA 
                 0.5 
                 0.5 
                 0.5 
               
               
                 Image field size 
                 2 × 26 
                 2 × 26 
                 2 × 26 
               
               
                 y times x [mm × mm] 
               
               
                 Reduction scale 
                 4× 
                 4× 
                 4× 
               
               
                 Pupil obscuration 
                 4.4 
                 4.0 
                 4.0 
               
               
                 (exit pupil) [%] 
               
               
                 Overall length [mm] 
                 1726 
                 2300 
                 2000 
               
               
                 max. angle of incidence of 
                 28.8 
                 10.2 
                 11.5 
               
               
                 the central main beam [°] 
               
               
                 max. angle of incidence in 
                 34.5 
                 16.9 
                 15.9 
               
               
                 the meridional section 
               
               
                 Main beam angle in the 
                 8 
                 8 
                 8 
               
               
                 reticle for central 
               
               
                 field point [°] 
               
               
                 Spacing of the centre of 
                 22 
                 85 
                 85 
               
               
                 the mirror M5 from the 
               
               
                 image plane [mm] 
               
               
                   
               
             
          
         
       
     
         [0067]    The main beam is the main beam  16  of a central point of the object field  4 . This central point is defined as the point which is located in the centre between the two edge object field points in the meridional section. 
         [0068]      FIG. 5  shows a further embodiment of the projection optical system  7 . Components, which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 4  have the same reference numerals and are not discussed again in detail. 
         [0069]    The imaging beam path between the object field  4  and the image field  8  in the projection optical system  7  according to  FIG. 5  is reminiscent of the imaging beam path of the embodiment according to  FIG. 4 . In comparison to the imaging beam path of the configuration according to  FIG. 4 , that according to  FIG. 5  with regard to the guidance of the imaging beams between the object field  4  and the mirror M 4 , appears mirrored about a plane lying virtually parallel to the xz-plane. In the imaging beam path of the projection optical system  7  according to  FIG. 5 , a part of the imaging beam path adjacent to the mirror M 3  lies on the same side of the imaging beam path section  21  as the imaging light bundle  22  in the region of the image field  8 . In the embodiment according to  FIG. 5 , a pupil plane  17  lies in the imaging beam path between the mirrors M 2  and M 3  and an intermediate image plane  19  lies between the mirrors M 4  and M 5 . 
         [0070]    The projection optical system  7  according to  FIG. 5  has a numerical aperture NA on the image side of 0.33. The image field  8  has an extent of 26 mm in the x-direction and of 2.5 mm in the y-direction. The image field  8  is rectangular. A wave front error of the projection optical system  7  according to  FIG. 5  is in the region between 0.2 and 0.5λ (rms, Root Mean Square). This wave front error is given for a wavelength λ, of 13.5 nm. 
         [0071]      FIG. 6  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 5  have the same reference numerals and will not be discussed again in detail. 
         [0072]    The imaging beam path between the object field  4  and the image field  8  in the projection optical system  7  according to  FIG. 6  is comparable to the imaging beams path in the embodiment according to  FIG. 5 . The numerical aperture on the image side and the image field size and the image field form correspond to that which was described above in conjunction with the embodiment according to  FIG. 5 . 
         [0073]    The projection optical system  7  according to  FIG. 6  has a numerical aperture NA on the image side of 0.33. The image field  8  has an extent of 26 mm in the x-direction and 2.5 mm in the y-direction. The image field  8  is rectangular. 
         [0074]    The projection optical system  7  according to  FIG. 6  has an overall length of 1180 mm between the object plane  5  and the image plane  9 . 
         [0075]    The pupil plane  17  in the imaging beam path between the mirrors M 2  and M 3  is accessible from all sides in the embodiment according to  FIG. 6 . 
         [0076]    A maximum angle of incidence on the mirror M 4  may be 21° in the embodiment according to  FIG. 6 . The angle of incidence is a maximum angle of incidence here on the mirror M 4  in the plane of the drawing of  FIG. 6 . 
         [0077]      FIG. 7  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 6  have the same reference numerals and will not be discussed again in detail. 
         [0078]    In the projection optical system  7  according to  FIG. 7 , the imaging beam path between the object field  4  and the mirror M 4  in total runs on the side of the imaging beam path section  21  opposing the imaging light bundle  22  between the mirrors M 4  and M 5 . 
         [0079]    In the imaging beam path of the embodiment according to  FIG. 7 , no overall intersecting imaging beam path sections are present between the object field  4  and the mirror M 4 . The fact that individual beams of the imaging beam path sections intersect in the reflection path during the reflection on the mirrors M 1  to M 4  does not represent intersecting imaging beam path sections overall of the imaging beam path. 
         [0080]    An imaging beam path section  25  extending between the mirrors M 3  and M 4  is guided past the mirror M 6  in the embodiment according to  FIG. 7 . A further intermediate image plane  26  in the imaging beam path section  25  lies in the region of this guiding past. The projection optical system  7  according to  FIG. 7  thus has, in addition to the intermediate image plane  19 , which lies close to the through-opening  18  in the imaging beam path, the further intermediate image plane  26 . Thus, two intermediate images are present in the imaging beam path between the object field  4  and the image field  8  in the projection optical system  7  according to  FIG. 7 . 
         [0081]      FIG. 8  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 7  have the same reference numerals and will not be discussed again in detail. 
         [0082]    In the projection optical system  7  according to  FIG. 8 , a portion of the imaging beam path associated with the reflection on the mirror M 3  is guided on the side of the imaging beam path section  21  opposing the imaging light bundle  22 . 
         [0083]    An intermediate image plane  26  lies in an imaging beam path section  27  between the mirrors M 1  and M 2 . The second intermediate image plane  19  is arranged, as in the above-described embodiments, in the region of the through-opening  18 . 
         [0084]    In the imaging beam path of the embodiment according to  FIG. 8 , the imaging beam path section  24  between the mirrors M 2  and M 3 , intersects an imaging beam path section  28  between the object field  4  and the mirror M 1  in a first intersection region  29 . The imaging beam path section  21  between the mirror M 4  and M 5  in turn intersects the imaging beam path section  24  between the mirrors M 2  and M 3  in a further intersection region  30 . 
         [0085]    The projection optical systems according to  FIGS. 8 to 17  may have a numerical aperture NA of 0.33. An image field size of these projection optical systems may be 2.5 mm in the x-direction and 26 mm in the y-direction. 
         [0086]      FIG. 9  shows a further embodiment of the projection optical system  7 . Components which correspond to those which were already described above with reference to the projection optical system  7  from  FIGS. 2 to 8  have the same reference numerals and will not be discussed again in detail. 
         [0087]    The imaging beam path in the embodiment of the projection optical system  7  according to  FIG. 9  substantially corresponds to the imaging beam path of the embodiment according to  FIG. 8 . A difference lies in the guidance of the imaging beam path section  28 : this imaging beam path section  28  between the object field  4  and the mirror M 1 , in the embodiment according to  FIG. 9 , does not only intersect the imaging beam path section  24  between the mirrors M 2  and M 3 , but also the imaging beam path section  25  between the mirrors M 3  and M 4  and the imaging beam path section  21  between the mirrors M 4  and M 5 . An intersection region  31  of the intersection last mentioned between the imaging beam path section  28  and the imaging beam path section  21  in portions overlaps with the intersection regions  29  and  30 . In the imaging beam path of the embodiment according to  FIG. 9 , the intersection regions  29  and  30  also overlap one another. 
         [0088]    An intersection region  32  of the intersection between the imaging beam path sections  28  and  25  is separated from the intersection regions  29  and  30  and partially overlaps with the intersection or crossing region  31 . 
         [0089]      FIG. 10  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 9 , have the same reference numerals and will not be described in detail again. 
         [0090]    An imaging beam path of the embodiment of the projection optical system  7  according to  FIG. 10 , apart from an arrangement mirrored about an xz-plane, is similar to the imaging beam path of the embodiment according to  FIG. 2 . In contrast to the imaging beam path according to  FIG. 2 , in the embodiment according to  FIG. 10 , the mirror M 3  is located closer to the mirror M 6  than the mirror M 1 . In the embodiment of the projection optical system  7  according to  FIG. 2 , the situation is precisely vice versa: there, the mirror M 1  is closer to the mirror M 6  than the mirror M 3 . In addition, in the embodiment of the projection optical system  7  according to  FIG. 10 , the mirror M 2  is located significantly closer to the object plane  5  than the mirror M 4 . 
         [0091]    In the imaging beam path section  24  between the mirrors M 2  and M 3 , in the embodiment according to  FIG. 10 , a diaphragm or stop  33  may be arranged in the region of a pupil plane of the projection optical system  7  according to  FIG. 10 . The imaging beam path section  24  is freely accessible from all sides in the region of this arrangement of the diaphragm  33 . 
         [0092]      FIG. 11  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 10  have the same reference numerals and are not discussed again in detail. 
         [0093]    The imaging beam path in the embodiment of the projection optical system  7  according to  FIG. 11  corresponds to the imaging beam path of the embodiment according to  FIG. 8 . In the projection optical systems according to  FIGS. 11 to 14 , mirrors M 1  to M 6  may be used that have different radii of curvature in two directions that are orthogonal to one another, in other words, on the one hand, in the xz-plane and, on the other hand, in the yz-plane. 
         [0094]    The projection optical system  7  according to  FIG. 11  is telecentric on the object side. 
         [0095]      FIG. 12  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described with reference to the projection optical system  7  from  FIGS. 2 to 11  have the same reference numerals and will not be discussed again in detail. 
         [0096]    The imaging beam path in the embodiment of the projection optical system  7  according to  FIG. 12  is similar to that of the embodiment according to  FIG. 2 , apart from a view which is mirror-inverted about an xz-plane. In contrast to the embodiment according to  FIG. 2 , in the embodiment of the projection optical system  7  according to  FIG. 12 , in the imaging beam path section  27  between the mirrors M 1  and M 2 , there is an intermediate image in an intermediate image plane  26  in addition to the further intermediate image in the intermediate image plane  19 , which is located adjacent to the through-opening  18 . In the embodiment of the projection optical system  7  according to  FIG. 12 , the mirror M 3  is located closer to the mirror M 6  than the mirror M 1 . This also distinguishes the imaging beam path of the projection optical system  7  according to  FIG. 12  from that of the embodiment according to  FIG. 2 , where the mirror M 1  is closer to the mirror M 6  than the mirror M 3 . 
         [0097]    The projection optical system  7  according to  FIG. 12  is telecentric on the object side. 
         [0098]      FIG. 13  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 12  have the same reference numerals and are not discussed again in detail. 
         [0099]    The imaging beam path, in the embodiment of the projection optical system  7  according to  FIG. 12 , is similar to the imaging beam path of the embodiment according to  FIG. 8 . In contrast to the embodiment according to  FIG. 8 , in the imaging beam path of the projection optical system  7  according to  FIG. 13 , in the imaging beam path section  25  between the mirrors M 3  and M 4 , there is an intermediate image in an intermediate image plane  26 , in addition to the intermediate image plane  19 , which is located in the region of the through-opening  18 . 
         [0100]    The projection optical system  7  according to  FIG. 13  is telecentric on the object side. 
         [0101]      FIG. 14  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 13  have the same reference numerals and are not discussed again in detail. 
         [0102]    The imaging beam path in the embodiment of the projection optical system  7  according to  FIG. 14  is similar to the imaging beam path of the embodiment according to  FIG. 9 . In contrast to the embodiment according to  FIG. 9 , an intermediate image is present in the imaging beam path of the projection optical system  7  according to  FIG. 14 , in the imaging beam path section  25  between the mirrors M 3  and M 4  and not between the mirrors M 1  and M 2 , in an intermediate image plane  26  in addition to the intermediate image plane  19 , which is located in the region of the through-opening  18 . 
         [0103]      FIG. 15  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 14  have the same reference numerals and will not be discussed again in detail. 
         [0104]    The imaging beam path of the projection optical system  7  according to  FIG. 15 , between the mirror M 2  and the image field  8 , is similar to the imaging beam path of the embodiment according to  FIG. 5 . 
         [0105]    The imaging beam path section  27  between the mirrors M 1  and M 2 , in the embodiment of the projection optical system  7  according to  15 , is guided past both the mirror M 6  and the mirror M 4 . Arranged adjacent to the mirror M 4  in the imaging beam path section  27  is an intermediate image in an intermediate image plane  26  in addition to the intermediate image in the intermediate image plane  19 , which is located close to the through-opening  18 . 
         [0106]      FIG. 16  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 15  have the same reference numerals and will not be discussed again in detail. 
         [0107]    The imaging beam path of the projection optical system  7  according to  FIG. 16  is similar to the imaging beam path according to  FIG. 13 . In contrast to the imaging beam path of the embodiment according to  FIG. 13 , in the projection optical system  7  according to  FIG. 16 , the imaging beam path section  24  between the mirrors M 2  and M 3  is guided past the mirror M 6 . In the embodiment according to  FIG. 13 , the mirrors M 3  and M 6  are arranged back to back. 
         [0108]      FIG. 17  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 16  have the same reference numerals and will not be discussed again in detail. 
         [0109]    The imaging beam path of the projection optical system  7  according to  FIG. 17 , from the mirror M 3 , is similar to the imaging beam path of the embodiment according to  FIG. 13 . In contrast to this, the imaging beam path section  28  between the object field  4  and the mirror M 1  intersects the imaging beam path section  24  between the mirrors M 2  and M 3 . A further difference between the embodiments according to  FIGS. 17 and 3  is that in the embodiment according to  FIG. 17  in the imaging beam path section  25  between the mirrors M 3  and M 4 , an intermediate image is arranged in an intermediate image plane  26 . This intermediate image is present in turn in addition to the intermediate image in the intermediate image plane  19  close to the through-opening  18 . 
         [0110]      FIG. 18  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 17  have the same reference numerals and will not be discussed again in detail. 
         [0111]    The imaging beam path in the embodiment according to  FIG. 18  between the object field  4  and the mirror M 4  is guided in total on a side of the imaging beam path section  21  opposing the imaging light bundle  22  between the mirrors M 4  and M 5 . The imaging beam path of the embodiment according to  FIG. 18  differs in this regard from that of the embodiment of  FIG. 2 . The course of the imaging beam path between the object field  4  and the mirror M 4  is otherwise reminiscent of the course of the imaging beam path in the projection optical system  7  according to  FIG. 2 . A further difference is that in the embodiment according to  FIG. 18 , a pupil plane  17  is arranged in the imaging beam path section  27  between the mirrors M 1  and M 2 . Between these two mirrors, the imaging beam path section  27  is accessible in broad regions from all sides. 
         [0112]    The projection optical system  7  according to  FIG. 18  has a numerical aperture NA on the image side of 0.33. The image field has an extent of 26 mm in the x-direction and of 2.5 mm in the y-direction. The image field  8  is rectangular. 
         [0113]    The projection optical system  7  according to  FIG. 18  has a wave front error in the range between 0.03 and 0.10λ (rms) over the image field  8 . 
         [0114]    The mirrors M 1  to M 6  are designed as free-form faces of the tenth order. 
         [0115]    The mirror M 6  has a diameter of 460 mm. The projection optical system  7  according to  FIG. 18  has an overall length of 1630 mm between the object plane  5  and the image plane  9 . 
         [0116]    The maximum angle of incidence on one of the mirrors M 1  to M 6  may be 17°. The angle of incidence here is a maximum angle of incidence in the drawing plane of  FIG. 18 . 
         [0117]    The imaging beam path section  27  is guided past the mirror M 6 . The mirrors M 3  and M 6  are arranged back to back. 
         [0118]      FIG. 19  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 18  have the same reference numeral and will not be discussed again in detail. 
         [0119]    The imaging beam path in the embodiment of the projection optical system  7  according to  FIG. 19  is similar to that of the embodiment according to  FIG. 18 . 
         [0120]    The projection optical system  7  according to  FIG. 19  has a numerical aperture NA on the image side of 0.50. The image field has an extent of 26 mm in the x-direction and of 2.5 mm in the y-direction. The image field  8  is rectangular. 
         [0121]    The wave front error in the embodiment according to  FIG. 19  is a maximum of 0.25% (rms) over the image field  8 . 
         [0122]    The mirrors M 1  to M 6  are designed as free-form faces of the tenth order. 
         [0123]    The mirror M 6  in the embodiment according to  FIG. 19  has a diameter of 700 mm. The overall length of the projection optical system  7  according to  FIG. 19  between the object plane  5  and the image plane  9  is 1800 mm. 
         [0124]      FIG. 20  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 19  have the same reference numerals and will not be discussed again in detail. 
         [0125]    The imaging beam path of the projection optical system  7  according to  FIG. 20  corresponds to that of the embodiment according to  FIG. 18 . 
         [0126]      FIG. 21  shows a further embodiment of the projection optical system  7 . Components which correspond to those which have already been described above with reference to the projection optical system  7  from  FIGS. 2 to 20  have the same reference numerals and will not be discussed again in detail. 
         [0127]    The imaging beam path of the projection optical system  7  according to  FIG. 21  corresponds to that of the embodiment according to  FIG. 18 . 
         [0128]    No back to back arrangements are present in the embodiments according to  FIGS. 18 to 21  in the imaging beam path between the object field  4  and the mirror M 4 . In particular the mirrors M 1  and M 4  are not arranged back to back with respect to one another. 
         [0129]    To produce a microstructured or nanostructured component, the projection exposure installation  1  is used as follows: firstly, the reflection mask  10  or the reticle and the substrate or the wafer  11  are provided. A structure on the reticle  10  is then projected onto a light-sensitive layer of the wafer  11  with the aid of the projection exposure installation. By developing the light-sensitive layer, a microstructure or nanostructure is then produced on the wafer  11  and therefore the microstructured component.