the general method for compensating the proximity effect in electron beam projection systems consists in dividing a complex exposure pattern into individual partial patterns , and to determine for each partial pattern the additional exposure ( electron beam dosage ) required to compensate the proximity effect . this additional irradiation dosage depends on the respective surroundings of each partial pattern . depending on the irradiation dosage found , and on the form of the partial pattern an opening in an exposure mask is defined with which the partial pattern is exposed for a second time , with an electron beam of the intensity of the initial exposure . fig2 shows this method with an example of an exposure pattern as described in connection with fig1 . the longitudinal partial pattern 20 is split into two areas b1 , b2 , with b1 being provided opposite partial pattern c , reference number 21 . partial patterns b1 and c each receive scattering electrons of the other partial pattern , and for compensating the proximity effect they therefore require only a relatively small additional exposure dosage ; this additional dosage is supplied by means of a second exposure in the hatched areas 22 , 23 . isolated partial pattern b2 receives no ( or less ) scattering electrons of other partial patterns so that the total irradiation dosage available for its exposure is clearly less than in partial patterns b1 and c . the additional exposure for compensating the proximity effect is therefore to be effected with a higher dosage ; accordingly , ( hatched ) area 24 applied in the second exposure is larger than in partial patterns b1 and c . the exact size and the exact position of the hatched areas of second exposure has to be precisely determined for each individual case , taking into consideration all losses and contributions of the proximity effect for each partial pattern . this can be calculated ( with algorithms or tables for standard patterns ), or it can be effected in experiments by measuring the respectively required additional dosage . a measuring method for the proximity effect will be described in detail below . the consequences of the proximity effect , and of the additional correction exposure onto a ridge - shaped profile in the photoresist are represented in fig3 . in fig3 a , irradiation dosage ( d ) is given over a local coordinate ( x ); dashed line 30 represents the distribution of the irradiation dosage when there is no electron scattering in the photoresist ; solid line 31 represents the case with electron scattering . the minimum dosage required for exposing the photoresist is assumed to have value d o ; the line width in the developed photoresist is obtained from the intersection of dosage distribution and minimum dosage d o . fig3 a shows that width b , which results in the case without scattering ( corresponding to the respective nominal width ) is not reached when there are scattering effects , but only a reduced width b &# 39 ;. for compensating this proximity effect , the invention suggests to use instead of a distribution of the irradiation dosage according to line 30 , an intensity profile in accordance with fig3 b ; within the desired line width b , an additional exposure ( electron irradiation ) is provided in an area k , e . g ., with a second exposure mask with openings of width k . ( the trapezoid shape of the dosage curve instead of the theoretically expected vertical limitations is due to inevitable electron - optical effects ). the resulting exposure profile of the two superimposed exposures is shown in fig3 c at reference number 32 . this curve intersects the horizontal of minimum exposure d o at the respective points of intersection so that after the exposure of the photoresist nominal width b is obtained . the double exposure for correcting the proximity effect can , e . g ., be carried out in a second exposure step , with an exposure mask having openings corresponding to the double exposure patterns . such a second exposure step suitable for proximity effect correction only is avoided in connection with complementary masks as described in applicants &# 39 ; german pat . no . 27 39 502 corresponding to u . s . pat . no . 4 , 169 , 230 . owing to the strong interactions of electrons and matter , the mask patterns in electron beam projection systems cannot be provided on a &# 34 ; transparent &# 34 ; substrate ; instead , the mask openings are preferably real holes in the mask . however , isolated pattern elements cannot be made in this manner since they do not have a support . this problem can be solved through the superposition of two complementary masks in that the isolated structure is divided into suitably formed and supported partial structures . the above described correction of the proximity effect can in complementary masks be achieved as a by - product without any additional exposure step . after the division of the mask pattern into two complementary masks the respective additional correction exposure is determined for each partial pattern thus formed , and a corresponding opening is made in the other complementary mask . the principle of complementary masks is shown schematically in fig4 ; dotted ring 40 is to be exposed , centerpiece 41 &# 39 ; is not to be exposed . for forming complementary masks a and b , ring 40 is divided into four partial areas 40a to 40d , and two respective of these partial areas ( 40a , 40c , 40b , 40d , respectively ) are arranged on an exposure mask ( b and / or c ). through the superposition of the two masks b , c the annular exposure area 40 is obtained without there being any mechanical stability problems for center area 41 &# 39 ;. for correcting the proximity effect in the annular exposure area of fig4 a , double exposures are necessary in those areas which in fig5 a are hatched , and marked with reference numbers 50a to 50d . fig5 b and 5c represent correction masks that may be used when for each complementary mask an additional exposure step would be carried out to correct the proximity effect . the correction mask with reference number 51 in fig5 b , and with apertures 50b , 50d is provided to correct complementary mask 42 with areas 40b , 40d , and accordingly correction mask 52 in fig5 c with apertures 50a , 50c to correct complementary mask 41 with areas 40a , 40c . these additional correction masks , however , are not necessary when the correction mask for a complementary mask is integrated in the respective other complementary mask . the combinations of complementary and correction masks are shown in fig5 d and 5e . complementary mask 41 thus comprises correction or compensating openings 50b , 50d for complementary mask 42 , and vice versa complementary mask 42 comprises correction or compensating openings 50a , 50c for complementary mask 41 . by superimposing the two supplemented masks 41 , 42 in fig5 d and 5e , fig5 a with the respective areas of double exposure is obtained . to ensure the mechanical stability of the masks in accordance with fig5 e and 5d the correction openings have to be slightly smaller than the associated exposure openings . in masks 41 , 42 of fig5 d , 5e between the actual exposure openings ( e . g . 40a ) and correction openings ( e . g . 50b ), there consequently remain sufficient ridges to separate these partial patterns . ridge widths of 0 . 3 to 0 . 4 μm will be enough for the mask stability . in the method of compensating the proximity effect with two exposure steps of the same intensity , as described here , a partial pattern can receive as correction dosage only once more the dosage used for the initial exposure ( i . e ., when the opening of the correction mask corresponds to the opening of the partial pattern ). this restriction of the applicable correction exposure is most evident in isolated pattern elements ( e . g . small squares ), and it restricts the application of the method to patterns with a maximum resolution of 0 . 5 μm . with even smaller dimensions of the structure to be imaged the losses through the proximity effect are greater than the maximum applicable correction irratiation . in that case , compensation would have to involve the additional exposure with higher intensity and / or another separate mask . the exact determination of position and form of the double exposure pattern part requires the precise measuring of the range of the proximity effect . below , a method will be described permitting a direct measuring of this scope . according to this method , a test pattern is imaged on a radiation sensitive ( photoresist ) layer and developed which consists of several groups of lines of equal width but where from group to group there is a slight increase of line width ( approximately 1 / 8 μm ). the ratio of line width d to the range of the proximity effect in the photoresist determines the shape of the line edges after the photoresist development . fig6 is a schematic representation of the influence of the proximity effect on edge profiles . fig6 uses as a test object an extended photoresist area 60 with an edge 61 , as well as a ridge 62 with edges 63 and 64 and a width d . owing to the proximity effect edge 61 receives a back - scattering dosage on one side only ( from exposed area 65 ); the dosage at edge 63 , on the other hand , depends on whether width d of the ridge is bigger or smaller than the range of the proximity effect . in the latter case , e . g . with a smaller width , edge 63 receives scattering electrons from exposed area 65 as well as from exposed area 66 . therefore the profile of edge 63 will alter , compared with the profile of edge 61 as soon as thickness d adopts a value that is comparable with the range of the proximity effect . fig6 a represents the situation after a full development of the photoresist when width d is greater than the proximity effect . fig6 b shows a ridge with width d &# 39 ; smaller than the proximity effect range ; after a full development of the photoresist there is &# 34 ; sub - etching &# 34 ; at edges 63 and 64 owing to the proximity effect . distinguishing the various edge profiles can in principle be effected photomicroscopically , or with a scanning electron microscope ( which latter case would involve the destroying of the sample ). to distinguish various profiles in the limit zone ( i . e ., line width d ≲ range of the proximity effect ) is , however , very complicated as there are only minor deviations or only a small asymmetry of edges 61 and 63 , 64 . for an easier detection of the profiles , particularly in photomicroscopic observation it is therefore suggested not to develop fully the above - mentioned exposed line pattern in the usual manner , but to discontinue the developing process prematurely , e . g ., after approximately 70 to 80 % of the full developing time . instead of the profile in fig6 a there will be a profile of the type shown in fig6 c and instead of the profile of fig6 b the profile according to fig6 d will be obtained . the distinguishing of the profiles between 6c and 6d can now be made photomicroscopically much more easily and clearly than that of the profiles according to fig6 a , b . any changes of edge profile 63 owing to the proximity effect can be easily ascertained in that the symmetry in profiles 61 and 63 is compared . if with a decreasing ridge width d a deviation in the symmetry of the two edges appears for the first time this ridge width corresponds to the range of the proximity effect . since asymmetries in the edge profile are very easily found by optical means this method of interrupted development represents a direct and quick measuring of the range of the proximity effect . in fig7 the two evaluation methods for line test patterns are compared . the microscopic photographs 7a and 7b represent test objects where developing had been interrupted after 70 % of the developing period . partial fig7 c and 7d represent the same test patterns after a 100 % development . the exposed and etched areas are marked 70 to 79 . in fig7 a , ridge width d is smaller than the range of the proximity effect . consequently , the left and right edges of etched area 70 are asymmetrical so that there appears another thin line at the left edge of area 70 . in fig7 b width d precisely corresponds to the range of the proximity effect so that in the stepwise widening of ridge width d both edges of area 70 appear symmetrical for the first time . fig7 c corresponds to fig7 a after a 100 % development , fig7 d corresponds to fig7 b after a 100 % development . in both fig7 c and 7d it is very difficult if not impossible to find any differences caused by the proximity effect , for an edge sub - etching is scarcely noticeable optically . while the invention has been particularly shown and described with reference to the preferred embodiments thereof , it will be understood by those skilled in the art that various changes in form and detail may be made therein without departing from the spirit and scope of the invention .