referring now to the drawings , wherein like reference numerals refer to the same or corresponding parts throughout the several views , an example of multiple beam scanning apparatus construction employing two laser diodes is described in reference to fig1 a , which is an exploded perspective view showing the construction of optical elements of the multiple beam scanning apparatus of the present invention . as shown in fig1 a , the laser diodes 11 and 12 are respectively fixed on the supporters 13 and 14 , and assembled with the rear surface of the base body 15 with the screws 18 and 19 so as to coincide with the optical axis of collimator lenses 16 and 17 . the collimator lenses 16 and 17 are accommodated in and engaged with tightly engaging holes 15a and 15b of the base body 15 performing the positional adjustment respectively with the laser diodes 11 and 12 , and bonded to the holes 15a , 15b by binding agent , etc . the collimator lenses 16 and 17 convert the respective light fluxes from the laser diodes 11 , 12 to parallel light fluxes . the light rays emitted from the collimator lenses 16 and 17 are form - shaped by respective circular slits of the iris plate 20 for the respective light rays and composed by a beam composing medium 21 . moreover , although the iris plate 20 is provided separately in the present embodiment , the engaging holes 15a and 15b engaging the collimator lenses 16 and 17 can be commonly used as the iris plate . next , the beam composing medium 21 is described referring to fig1 a and 1b . the laser diodes 11 and 12 are arranged on a common plane with the p - n junction surfaces thereof abutting each other . the polarization of either one of the beams ( beam of the laser diode 11 ) is rotated by 90 ° by half wavelength plate 22 mounted on the incident surface of the beam composing medium 21 , and the beam passes through on the polarized beam splitter surface 21b of the beam composing medium 21 . fig1 c shows the respective waveforms of the light beams before and after passing through the half wavelength plate 22 . furthermore , the beam of the laser diode 12 is internally reflected on the slanted surface 21a of the beam composing medium 21 and further reflected on the polarized beam splitter surface 21b of the beam composing medium 21 . the reflected beam is composed with the beam of the laser diode 11 near the optical axis of the laser diode 11 serving as the standard . optical axes relating to the respective laser diodes 11 and 12 are set so as to be inclined with respect to each other by the angle α , as shown at the output side of the beam composing medium 21 , i . e ., slightly deviated from each other by the small angle a in the main scanning direction . the angle α is obtained , for example , by displacing the laser diode 12 in relation to the collimator lens 17 to produce an eccentricity in the emitted beam from the collimator 17 . the beams emerging from the beam composing medium 21 are in parallel . the beam composing medium 21 and the iris plate 20 are supported at a predetermined position on the rear surface of the flange member 23 and fixed on the base body 15 with screws 24 and 25 . the respective members in the optical path from the laser diodes 11 and 12 to the flange member 23 are unitarily fixed on the substrate 26 on which the driving circuits of the laser diodes 11 and 12 are provided , and those members serve as a light source unit . the light source unit is rotatable about the optical axis of the laser diode 11 by means of a rotating mechanism ( not shown ). an aperture 27 is rotatively supported in the cylinder portion 23a of the flange member 23 , as also shown in the enlarged perspective view of fig2 . fig3 is a cross sectional view showing assembly of the multiple beam scanning apparatus shown in fig1 a . the aperture 27 is provided with snapping claws 27b and 27c supported in a groove formed on the external circumference of the cylindrical portion 23a of the flange member 23 such that the aperture 27 can rotate around the flange member 23 . the aperture 27 is installed into the groove 28a of the apparatus frame 28 and is fixed thereon and circumscribes the optical axis . in the construction above described , the flange member 23 is slightly moved rotatively by an angle θ around the cylindrical portion 23a , and the light source unit 10 is rotated and adjusted on the basis of the standard inner circumference surface of the aperture 27 to achieve a desired light intensity . as the result of the rotation θ , the pitch in the sub - scanning direction of the respective axes is adjusted , and further , in order to obtain the desired dimension and shape of the light flux , the light beam is shaped by the aperture 27 . more particularly , fig6 a is a schematic illustration of how pitch p is varied by rotation θ of the light source unit 10 . fig6 b is a graph illustrating the relationship between the rotational angle θ and the pitch p . where po is the ideal value of pitch , p is the measured value of pitch , and l is the distance between the beam spots from the lasers 11 , 12 , as shown in fig6 a . the light source unit is fixed with the screws to the apparatus frame 28 at the rotative position where a predetermined pitch in the sub - scanning direction is obtained . in such manner , troublesome optical axis adjustment is avoided , and when the light beam is rotatively adjusted by rotating the light source unit , the position of only the aperture 27 is kept constant regardless of rotational movement of the light source , whereby the parallel orientation of the light flux with respect to the scanning lens is also maintained after passing through the aperture 27 . thereby a predetermined beam spot diameter can be obtained on the surface to be scanned . furthermore , since the rectangular aperture 27 is unitarily supported together with the light source unit , when the beam spot diameter is changed , it is possible to change the light source unit by adjusting the light beam . consequently , it is possible to change the beam spot diameter only by adjusting or exchanging and readjusting the light source unit 10 . therefore the adjustment can be largely facilitated . furthermore , in the present embodiment , although the aperture 27 is employed as the beam shaping medium , other components such as a prism , a beam compressor , etc . having the same function can be employed in place of the aperture 27 . in the aforementioned embodiment , two laser diodes are employed . however , instead a plurality of light emitting sources arranged as an array can be used . next , an example of controlling operation performed by the multiple beam scanning apparatus is described . fig4 shows a system including a multiple scanning apparatus and an example of a first controlling apparatus . in fig4 the light source unit 10 is constructed with the respective members arranged in the optical path from the laser diodes 11 and 12 to the flange member 23 as shown in fig1 . the respective beams emitted from the light source portion 10 are transmitted to a polarizing medium including a cylinder lens 30 and reflecting a multiple - surface mirror 31 . the light beams thus transmitted are repeatedly polarized in the main scanning direction by rotating the above multiple - surface mirror 31 . the light beams reflected on the multiple - surface mirror 31 are further projected as light spots on the predetermined scanning / recording surface by use of the scanning lens constructed with a ƒ - θ lens 32 and a partial doughnut - shaped lens 33 . at this time , the respective beams are deviated by one pitch p in the sub - scanning direction , and thereby two scanning lines are written at the same time . a photo - sensor 34 employed as a light intensity sensing medium is disposed at a position near the surface to be scanned and detects the intensity of the scanning beam in a margin area which is not to be written into . the operating unit 35a receives the detected intensity data and calculates an intensity deviation shifted from an initial value in comparison with the predetermined standard value . the laser diode controlling unit 36a controls the beam output of the laser diode driving circuit in order to decrease the above deviation . the above - mentioned photo - sensor 34 and laser diode controlling unit 36a perform the operation of light intensity change control . the rotation drive unit 37 is constructed of , for instance , a stepping motor , etc ., and rotates the light source unit 10 and generates an encoding pulse in accordance with the rotation thereof . a rotation variation detecting unit 38 is constructed with , for instance , a rotary encoder , and the control unit 39a receives the encoded data and the rotation drive unit 37 causes the light source portion 10 to rotate to a desired position . the desired position can be manually determined by operator entry of a suitable code . alternatively , the desired position can be automatically determined by detecting the positions of the light beam spots and thereby measuring the pitch p of the light beams on the photosensitive member , and then determining the required angle θ based on the measured value of pitch p and the desired value of pitch po using the relationship above described . pitch p can be measured by means of a ccd sensor ( not shown ) provided in the margin of the photosensitive member . consequently , the intensity of exposure does not change even in the case of rotatively adjusting the light beam and automatically compensating the scanning line pitch , etc . fig5 shows a second example of the control apparatus in the multiple beam scanning apparatus of the present invention . in fig5 the control unit cause the light source portion 10 to rotate to a desired position , and at the same time , receives the data from the rotation change detecting unit 38 and outputs the installment angle data of the light source unit 10 to the operational unit 35b , as in the case of performing the control operation of fig4 . fig6 c is a graph showing the relationship between the installment angle θ of the light source unit 10 and the intensity of the emitted light rays on the surface to be scanned , i . e ., the intensity of the light beams passing through the aperture 27 . since the light beams entering the aperture 27 have a defined beam shape before passing through the aperture 27 , and since the aperture is stationary in relation to rotation of the light source unit 10 , the amount of light ( light intensity ) of the beams emitted from the aperture 27 can be changed either by rotating the light source unit 10 or adjusting the aperture 27 . in fig5 the previously measured value of light intensity measured by sensor 34 is memorized in the operating unit 35b . the operating portion 35b determines the installment angle θ based on the measured light intensity using the relationship shown in fig6 c , calculates the deviation of the measured installment angle from a standard installment angle and further calculates the variation of the light intensity . the operational unit 35b controls the laser diode controlling unit 36b in order to compensate for variations in the light intensity . the control unit 36b of the laser diode , as in the case of control unit 36a , controls the beam output of the laser diode driving circuit . consequently , the intensity of exposing does not change even in the case of automatically compensating the scanning line pitch , etc . according to a first aspect of the present invention , the light source unit is rotated around the optical axis and adjusted , and thereby the pitch of the respective optical axes in the sub - scanning direction is determined . consequently , the adjustment of pitch is greatly facilitated . further , according to a second aspect of the present invention , since the respective light beams are shaped by the circular iris plate , the light flux diameter of the light beam passing through the beam shaping medium is kept to a predetermined value at the time of rotating the light source unit and rotatively adjusting the light beam , and thereby a predetermined beam spot can be obtained on the surface to be scanned . according to a third aspect of the present invention , since the beam shaping medium is unitarily supported together with the light source unit , and the beam shaping medium can be rotatively moved around the optical axis thereof relative to the light source unit , it is sufficient only to change the light source unit by the rotative adjustment of the light beam at the time of changing the beam spot diameter . consequently , the diameter of the beam spot can be changed only by exchanging the light source unit , whereby assembling and maintenance of the apparatus can be largely improved . according to a fourth aspect of the present invention , since the beam shaping medium is unitarily supported together with the light source unit , and the beam shaping medium can be rotatively moved around the optical axis thereof relative to the light source unit , it suffices only to change the light source unit to perform rotative adjustment of the light beam . according to a fifth aspect of the present invention , the beam shaping medium is constructed with a rectangular aperture . therefore , it suffices only to exchange the light source unit at the time of changing the beam spot diameter . furthermore , since the number of the parts employed for the beam shaping medium is small and the extent of the influence upon the optical axis variation is also small , assembly is facilitated and the apparatus can be small - sized . according to a sixth aspect of the present invention , there is provided a light intensity change controlling medium for variably controlling the intensity of the light rays emitted from the laser diode in accordance with the installment angle resulting from the rotative adjustment of the light source unit . therefore , the exposure intensity does not change at the time of rotatively adjusting the light beam and a stable precise image intensity can be obtained . according to a seventh aspect of the present invention , since the light intensity change controlling medium is provided with a light intensity detecting medium for detecting the light intensity variation of the respective beams at the surface to be scanned , the intensity of exposing does not change even in the case of rotatively adjusting the light beam and automatically compensating the scanning line pitch , etc ., and a stable image can be obtained . according to a eighth aspect of the present invention , in the sixth status , since the light intensity change controlling medium is provided with a light intensity change calculating medium for calculating variation in the intensity of the emitted light rays in accordance with the installment angle of the light source , the exposure intensity does not change and a stable and preferable image can be obtained even in the case of automatically compensating the scanning line pitch . obviously , numerous modifications and variations of the present invention are possible in light of the above teachings . it is therefore to be understood that within the scope of the appended claims , the invention may be practiced otherwise than as specifically described herein .