fig1 shows the schematic configuration of a projection apparatus having three radiation sources 100 , 200 and 300 . these radiation sources emit the beams 110 , 210 , and 310 . since the three radiation sources can not all be positioned at the same location , the beams of the sources of radiation 200 and 300 are deflected by means of the deflection mirrors 220 and 320 and aligned with beam 110 . the three beams hit the first mirror 400 which is movable . by means of the motion of the first mirror 400 the three beams 110 , 210 and 310 may be directed onto the projection screen 10 . by means of appropriate motion of the mirror 400 thus an image is generated spot by spot on the projection screen 10 . this method for projecting an image is also known as “ flying spot method ”. the three radiation sources 100 , 200 and 300 are lasers in a preferred embodiment , whereby the beams 110 , 210 and 310 are laser beams . it is favorable to choose the colors of the lasers to be red , blue and green . thus , any number of colors in the color spectrum may be generated . thereby a very versatile image may be generated on the projection screen 10 . in an ideal case the three beams 110 , 210 and 310 superimpose each other exactly by means of the configuration shown in fig1 , so that the desired reference impression results . however , minimal angular deviations caused by production lead to a deviation of the beams of each other , which results in an actual impression which deviates from the reference impression . such a deviation of angle d can be seen in fig2 . it is to be seen here that the three beams 110 , 210 and 310 show deviations of each other , which is also reflected on the projection screen 10 . in many cases it is impossible and very hard , respectively , to improve projection apparatuses mechanically to such an extent that such a angular deviation is avoided . in many cases the angles may also change during operation due to thermal stress . for this reason a measurement method and a measurement procedure , respectively , for positioning the beams is provided in the present invention as shown in fig3 . for example , in fig3 the measurement of the position of the beam 110 can be seen . this beam is deflected by means of the movable first mirror 400 and is projected onto the projection screen 10 . between first mirror 400 and projection screen 10 a further second mirror 600 is arranged . this may be semi - transparent , whereby a portion of the beam 110 may be further projected onto the projection screen 10 , another portion of the beam is however deflected by mirror 600 . the deflected beam 110 is projected onto a detector 500 . in the various embodiments of the invention it is feasible to determine the position of the beam 110 during the operation of the projection apparatus or prior to the operation of the projection apparatus . in a so called offline - operation in fact radiation in the direction of the projection screen is applied at the time of the measurement of the position of the beams , however , no image information is transmitted . the so called offline - operation is to mean , that the accomplishment of the measurement of the position of the beams is carried out during the projecting operation . with respect to fig3 both the offline - operation as well as the online - operation can be described . both during offline - operation as well as during online - operation two different methods may be applied . one method comprises a variable mirror position and a stationary detector , the other method a variable detector position with a fixedly defined mirror position . as a first exemplary embodiment the option for offline - operation having a stationary detector is to be described . in this connection , for the accomplishment of the measurement of the position of the beams only one single beam is operating at any one time . the second mirror 600 may be semi - transparent or non - transparent , since it is not required that the beam has to be projected onto the projection screen . the second mirror 600 , however , should be positioned such that it directs the respective beam , which is currently operating , at least partially onto a detector 500 having a fixed position . the respective beam directed onto the detector 500 thereby generates a projection on the detector . the first movable mirror 400 is now moved so long as to have an orientation in which a maximum intensity of the respective beam is measured at detector 500 . this is carried out individually for each beam , for example for the beam 110 , 210 and 310 . it is particularly favorable , if for each of the beams one further orientation of the first mirror 400 is determined where the maximum intensity of the beam is measured at the first detector 500 . this adds to an increase of the measurement accuracy . the respective orientations of the first mirror 400 may respectively be measured contactless by means of the capacitance between the first mirror 400 and a counterpart . it is also feasible to measure the orientations of the first mirror 400 by means of a mechanical sensor . furthermore , the orientation of the mirror may respectively be determined thus that the first mirror 400 is irradiated with an additional beam whose deflection is determined by means of a second detector . in doing so , it is favorable if the additional beam at any one time is arranged having an inclined angle in relation to the beam which is currently operating . from the orientations of the first mirror 400 measured , in the following differences may be calculated from the orientations of the mirror for the first beam , a second and a third beam . the determination of the orientation of the mirror and of the difference of the orientations of the mirror for the respective beams serves to determine the actual deviation of the beams of each other . the measurement of the position of the beams may thus be carried out internal or external to the device . from the difference of the orientations of the mirror for the respective beams a angular deviation between the beams may be determined . a further embodiment of the invention is the measurement method of the beam position during offline - operation with variable detector position . in this connection , the first mirror 400 is held in at least one fixed orientation for each beam . detector 500 is brought into one respective position for each beam , for example for the beams 110 , 210 and 310 , in which a maximum intensity of the respective beam is measured at the detector . the measurement of the position of the detector may be carried out internal or external to the device . the measurement internal to the device is carried out contactless by means of the capacitance between the detector and a counterpart or by means of a mechanical sensor . if it is desired to avoid the measurement of the detector position , instead of a single detector a plurality of detectors ( detector array ) may further be used for the determination of the positions of the projections of the beams . in doing so , the plurality of detectors is positioned such that all positions of the projections of the beams on the plurality of detectors may be measured without having to move the plurality of detectors . by consecutively measuring the positions of the projection of the beams on the plurality of detectors a angular deviation between the beams is determined which is used for determining the actual deviation of the beams of each other on the projection screen . during online - operation the second mirror 600 is semi - transparent and installed permanently in order to particularly favorable direct a portion of the beams onto the projection screen to generate an image and to simultaneously direct another portion of the beams onto the detectors to determine the deviation of the beams of each other . in other words , all colors are operating simultaneously , which is to mean that an image is generated on the projection screen 10 while simultaneously the position of the beams on a detector 500 is measured . the deflection of the beams , for example of the beams 110 , 210 and 310 , onto the detector 500 is carried out by means of the second mirror 600 . since all beams are operating simultaneously it is required to provide certain elements in the beam path for separating the beams in front of the detector 500 . for this purpose , a wavelength selective filter is suitable for example , which is provided between the second mirror 600 and detector 500 . this filter allows for only one beam to reach the detector 500 at any one time , while the other beams are blocked . thus , the respective position of the projection of one beam may be measured . a further possibility to separate the beams is a diffractive element which is provided behind the second mirror 600 . a diffractive element will take care that the beams are directed into different directions and thus also will be separated . during online - operation with a stationary detector a plurality of detectors is used as the detector . the respective beam which is directed onto the plurality of detectors generates a projection on this plurality of detectors . the first mirror 400 again is brought into different orientations in which the respective beams on the plurality of detectors may be measured by means of an intensity maximum . this may advantageously again be carried out several times for each beam and respectively a new orientation of the mirror may be determined . the orientations of mirror 400 may respectively be measured internal or external to the device . these are , for example , the contactless measurement by means of the capacitance between the mirror 400 and a counterpart or the measurement by means of a mechanical sensor . as an external option it may be used the irradiation with an additional beam whose deflection is determined by means of a further detector . this additional beam is advantageously arranged having an angle inclined with respect to the remaining beams . the orientations of the first mirror 400 determined such are used to determine differences of mirror orientations for the respective beams . from these differences again angular deviations between the respective beams are determined and from these the actual deviation of the beams on the projection screen is calculated . during online - operation it is further feasible to bring the first mirror 400 into defined orientations for each beam . a detector 500 may be brought into a position for each beam in which a maximum intensity of the respective beam is measured at the detector . the measurement of the position of the detector may be carried out internal or external to the device . the internal measurement is the contactless measurement by means of the capacitance between the detector and a counterpart or the measurement by means of a mechanical sensor . further , a plurality of detectors may be used which are positioned such that all projections of the beams may be measured simultaneously . in doing so , a motion of the plurality of detectors is not required . from the positions of the projections of the beams on the plurality of detectors a angular deviation between the respective beams may be determined . in turn , using the angular deviation the actual deviation of the beams of each other on the projection screen 10 may be determined . the difference between the two methods during online - operation , once with stationary detector and once with movable mirror exists in that with the stationary detector a signal is sent when the detector indicates a maximum intensity maximum . if the mirror has a defined orientation , a signal is sent if the mirror has this defined orientation . both signals make sure that the temporal intensity variation of the control of the radiation sources is carried out . from fig4 the focusing of the beams in front of the detector can be seen schematically . the provision of a lens 700 between the second mirror 600 and detector 500 is particularly favorable in order to achieve an improvement of the measurement accuracy . each , foe example beam 110 , has a technically conditioned width a . this width may be minimized by means of the provision of a lens . by further providing an aperture 750 between lens 700 and detector 500 the correct position of the beam may further be defined . due to motion of mirror 600 the position of the projection of beam 110 is moved and may be brought into an orientation where the beam exactly meets detector 500 through the aperture . a focused beam results in a exact finding concerning the position of its projection on the detector . the application of an aperture and a lens may reduce the beam diameter to about 20 to 30 μm or even less . from fig5 an example for the determination of the deviation of the projections of the beams on the projection screen 10 can be seen . the projections of the beams 110 , 210 and 310 can be seen as spots 110 a , 210 a and 310 a on the projection screen 10 . the three spots have two deviations each if for example a reference point 110 a is chosen . spot 210 a deviates from spot 110 a in x and y directions . the differences are designated 210 a - y and 210 a - x . similarly , the projection of beam 310 , 310 a has a deviation in y direction and x direction in relation to the spot of the projection 110 a . these deviations are designated 310 a - y and 310 a - x . therefore relative deviations of the projections in relation to a chosen reference projection spot are achieved . from these deviations angular deviations may be determined . for example , the assumption that a pixel misalignment by one row and one column with a resolution of 1024 × 768 , a projection distance of 1 . 5 m and a image size of 42 cm × 29 . 7 cm results in a angular deviation of 0 . 015 ° in the row and 0 . 016 ° in the column . the angular deviations in turn result in the determination of the actual deviations of the projections on the projection screen . from the angular deviations a phase shift of the beams in relation to each other may be determined . the phase shift relates to the electronic signals for the activation of the respective beams . if the electronic signals of the respective beams are modulated by the phase shift determined , which is to mean a temporal delay of the single beams , the desired color effect on projection screen 10 may be reconstructed . fig6 schematically shows the implementation of the above described exemplary embodiments of the invention into an embodiment of a projection apparatus . here , a projection apparatus can be seen which comprises a video electronics 800 , which results in projecting motion pictures or still pictures . furthermore , a central control unit 900 is provided , preferably on a semiconductor chip . the video electronics 800 feeds data to the electronic control 30 for the radiation sources . the electronic control 30 for the radiation sources may be comprised of delay elements 130 a , 230 a and 330 a for each source of radiation 100 , 200 and 300 and of drivers for each source of radiation 130 b , 230 b and 330 b . the radiation sources , which advantageously are lasers , send the beams 110 , 210 and 310 to a movable first mirror 400 . this first mirror 400 is actuated by a first electronic driver 450 . the first mirror 400 directs the beams onto a projection screen . arranged between the mirror 400 and a detection device 550 for the accomplishment of the measurements of the beam positions is a second mirror 600 which directs the beams in the desired direction . the detection device 550 is designed according to the above described exemplary embodiments and may in particular comprise a first detector or a plurality of detectors . control unit 900 is connected to the first mirror 400 , to the detection device 550 and to the electronic signal 800 for generating an image via read data lines . this means control unit 900 receives data concerning the orientation of mirror 400 , concerning the progress of the electronic signals for generating an image and concerning the results of the measurements of detection device 550 . furthermore , control unit 900 is connected via write data lines with the driver of the first mirror 450 , the electronic control 30 for the radiation sources and the electronic signal 800 for generating an image . this means control unit 900 may , from the determined data , which it has received from the read lines , send revised data to the driver of the first mirror 450 for an updated orientation of the mirror , to the electronic control for the radiation sources for regulating the beams 110 , 210 and 310 and to the electronic signal 800 for generating an image for temporal intensity variation of the signals , which are required in light of the new conditions . as an example , the delay elements 130 a , 230 a and 330 a may such assure that the radiation sources 100 , 200 and 300 send beams with modulated intensity at modulated points in time in order to improve the image quality on the projection screen 10 . from the mirror orientations determined for each beam phase shifts are determined , from which control signals are sent to the delay elements . the above method and the above projection apparatus are not limited to correct undesired angular deviations of superimposed beams on the projection screen , but may particularly favorable also be used to correct angular deviations of beams on the projection screen , if the angular deviation is predetermined . for this purpose fig7 sketchily shows an embodiment of a projection apparatus 1001 , which comprises three laser sources in each case adjusted with an angle in relation to each other , namely a red emitting laser diode 1002 , a green radiating laser diode 1003 and a blue radiating laser diode 1004 . by way of the angled orientation of lasers 1002 , 1003 , 1004 also the respective emitted laser beams 1005 , 1006 , 1007 are arranged having predefined angles with respect to each other , and such are non - collinear . in this example the angle between the red beam of light 1005 and the green beam of light 1006 is designated α 1 , and the one between the green beam of light 1006 and the blue beam of light 1007 is designated α 2 . the beams of light 1002 , 1003 , 1004 without further deflection non - collinearily hit a scanning mirror 1008 ( for example analogous to the scanning mirror 400 of the above figs ), which as indicated by the arrow and the dotted line is deflectable by an operational maximum mechanical angle of deflection β in the viewing plane . the exemplary embodiment is shown represented only in one plane for the purpose of better clarity . generally the laser diodes 1002 , 1003 , 1004 may be arranged in any order in relation to each other . furthermore , also several laser sources 1002 , 1003 , 1004 may be used for each color , wherein the colors do not have to be limited to red , green and blue . in order to form beam characteristics furthermore one or several optical elements , such as lenses , collimators and so on , arranged in the beam path may be used . in the exemplary embodiment shown the following constraint is met for the angular deviations αi between two beams 1005 , 1006 , 1007 : the sum of the angular deviations αi between two beams 1005 , 1006 , 1007 is smaller than the operational maximum mechanical angle of deflection β of the scanning mirror 1008 minus 10 °, thus σ αi = β − 10 °. this constraint applies to the viewing in a plane and analogously may be transferred to a second plane perpendicular to this plane . fig8 sketchily shows a projection apparatus 1009 according to a second embodiment . this embodiment now comprises a convolution of two beam paths 1010 , 1011 for the red laser diode 1002 and the blue laser diode 1004 , respectively . for this purpose separate deflection elements are used for the single laser beams 1010 , 1011 , such as mirror 1012 . in an alternative embodiment deflection mirrors 1012 may for example be used for one or two other colors . the arrangement shown may be implemented more compact than the one of fig7 . fig9 sketchily shows a projection apparatus 1013 according to a third embodiment , where now a deflection of the beams of light , here of all beams of light 1014 , 1015 , 1016 , is carried out by means of a single mirror array 1017 having identically implemented and arranged single mirrors 1018 . here , the arrangement of the light sources 1002 , 1003 , 1004 is again not limited to one plane , but may be realized two - dimensionally . fig1 sketchily shows a projection apparatus 1019 according to a fourth embodiment having stacked laser sources , namely a red laser source 1002 and a green laser source 1004 . these may , for example stacked as a bar or “ submount ”, be accommodated on a shared semiconductor chip or module . however , the projection apparatus 1019 may generally comprise also three or several laser sources in the form of submounts , among them also green laser sources . beamforming and directional control of the laser beams 1020 , 1021 onto the scanner mirror 1008 is carried out by means of a micro - optical element 1022 arranged in the beam path , for example a array of lenses , a phase changing element or a optical element having a refractive index gradient . by means of the micro - optical element 1022 the beams of light 1020 , 1021 at first emitted collinearily by the lasers 2 , 4 are deflected with an angle α 3 with respect to each other and non - collinearily radiated onto the scanner mirror 1008 . since appropriate green laser sources are not yet available in the form of stackable laser sources a green laser source ( without representation ), preferably without further deflection , will be directed non - collinearily with respect to the other beams of light 1020 , 1021 onto the scanner mirror 1008 . the above mentioned exemplary embodiments for the predetermined angular deviation have the advantages that they do not require optical elements which let pass a defined spectral range and reflect a second spectral range . this has the advantage that optical losses may be minimized and thus a brighter image effect is achieved on the screen . in addition , without considering the polarization state any number of sources of a color may be directed onto the scanner mirror , whereby again a brighter image effect may be achieved . the non - collinear beamguiding furthermore makes it feasible to implement a laser projector having small dimensions . in addition , this laser projector may be manufactured with low production efforts by means of resigning a collinear beamguiding , since the effort for the collinear adjustment ( typically in the dimension of micro - optics ) is omitted . furthermore an accuracy of illustration is increased . the method of using the angular deviation is not limited to a coaction with the deviation reducing method for projecting an image described in fig1 to fig6 , but is also a separate invention , in which the image projection may be carried out in all forms known to a person skilled in the art , in particular in all further forms of deviation reduction known to a person skilled in the art . the invention generally is not limited by the description on the basis of the exemplary embodiments . rather the invention comprises each new characteristic as well as any combination of characteristics , which in particular includes each combination of characteristics from the patent claims , even if this characteristic or this combination by oneself is not explicitly provided in the patent claims or the exemplary embodiments .