fig1 is a schematic representation of a partial cross section side view of x - ray tube 10 within which electron bombarded and x - ray generating structure 12 of anode 14 is attached to and cooled by a base structure , which is heat pipe 16 , while generating x - ray beam 18 . such a tube is constructed with cathode 20 mounted within evacuated envelope 24 and interconnected to suitable power supplies ( not shown ) by cathode connections 26 which penetrate envelope 24 . electron beam 22 originates at cathode 20 and bombards x - ray generating structure 12 . fig1 also schematically depicts a structure which can be used to control electron beam 22 . magnetic coil 28 is a device which can deflect electron beam 22 in any direction along bombarded structure 12 , as indicated by beam lines 22 a and 22 b . however , it should be appreciated that there are other devices in the art , such as electrostatic plates , which can also be used to deflect electron beam 22 and scan it across structure 12 . heat pipe 16 penetrates envelope 24 and is sealed to it at vacuum seals 30 by conventional means . heat pipe 16 eliminates the need to rotate anode 14 because heat pipe 16 is capable of cooling bomdarded structure 12 well enough to prevent thermal damage to structure 12 by the electron beam . in this embodiment , in order to sufficiently cool bombarded structure 12 , heat pipe 16 is constructed with a tungsten casing , lithium fluid , and a niobium powder wick for high power density operation . heat pipe 16 removes the heat generated at the spots at which electron beam 22 bombards structure 12 . cooling coil 32 , located at the condenser end of heat pipe 16 , and through which a cooling fluid is pumped , then moves the heat from heat pipe 16 to a remote heat exchanger ( not shown ). elimination of the need to rotate anode 14 complements the ability to deflect electron beam 22 because it permits full electronic control of the location of the spots which generate x - ray beam 34 . with the structure shown in fig1 the electron beam can be moved around structure 12 instead of requiring the rotation of anode 14 . furthermore , with the rotation of the anode eliminated , the invention is not restricted to circular layouts for x - ray generating structure 12 . thus , it is quite practical to construct anode 14 and heat pipe 16 with rectangular plan views , and with the concave cross section of structure 12 as shown in fig1 to generate x - rays which yield a linear configuration on the illuminated surface . however , the present invention also uses special material for x - ray generating structure 12 which gives x - ray beam 34 special characteristics and increased versatility . structure 12 is constructed as a single crystal or a highly oriented coating of a material such as tungsten . such a highly oriented coating can be produced by chemical vapor deposition , a process well understood in the art of material coating . for the preferred embodiment , structure 12 is a single crystal structure of tungsten with a thickness of 0 . 001 to 0 . 010 inch . however , many other materials can be produced as single crystal structures , and each material has different x - ray generating characteristics such as wavelength and beam orientation . these characteristics of materials are well documented in the literature dealing with x - rays . the characteristic of such a single crystal structure is that there are a limited number of exit paths available to the photons generated within the crystal lattice of the material , and that all the photon emission paths originating from any location on the structure are parallel to the emission paths originating at all the other locations . thus , for a flat structure , although photons are emitted at several specific angles to the surface , all locations on the structure will emit photons at only the same few limited angles at which every other location emits photons , and the result will be many parallel beams of photons leaving the structure at each of the limited number of angles . in the simplest case which is illustrated in fig1 if one of the exit path angles for a particular material is perpendicular to structure 12 , any spot of structure 12 which is bombarded by electron beam 22 will generate , along with a limited number of other x - ray beams , an x - ray beam 18 exiting perpendicular to structure 12 . therefore , when structure 12 is shaped as a parabola or a small radius sphere approximating a parabola , the x - ray beams from all locations of structure 12 exit perpendicular to parabolic structure 12 . those beams , such as beams 18 a and 18 b , then meet at focal point 34 , after exiting tube 10 through window 36 , regardless of where on structure 12 they originated . it should be appreciated that parabolic structure 12 is not functioning as a reflector as might be first supposed , but rather as a parabolic radiation generator . moreover , structure 12 need not necessarily be a parabola , but can be any curved structure to focus a beam at a particular location or locations . a deviation in the curved structure is particularly helpful when the exit angles of the beams from structure 12 which are being used is other than perpendicular . one such variation of the electron bombarded and x - ray generating structure of an anode is depicted in fig2 . fig2 is a side view of an alternate embodiment of the x - ray generating anode 40 of the invention in which structure 42 is flat and , as in many x - ray tubes , angled to deliver x - ray beam 44 out the side of the tube wall 46 . as in fig1 an electron beam 48 bombards x - ray generating structure 42 , and electron beam 48 can be moved over entire structure 42 as is indicated by beam lines 48 a and 48 b by a deflection coil ( not shown ). however , anode 40 in fig2 differs from anode 14 in fig1 because x - ray generating structure 42 is flat so there is no focusing action and also because the angles of exit of x - ray beams 44 , 44 a , and 44 b from structure 42 are not perpendicular to structure 42 . nevertheless , when x - ray beams 44 , 44 a , and 44 b originate from single crystal structure 42 , or any highly oriented coating , they are all collimated and parallel to each other regardless of the origin points of the beams . the structure of fig2 therefore makes it possible to illuminate areas equivalent in size to structure 42 itself with x - rays . as previously discussed , such illumination is useful in exposing masked areas in photolithography to x - rays . fig2 also shows an alternate structure for cooling the x - ray generating structure of the anode . in fig2 x - ray generating structure 42 is attached to hollow casing 50 , and high velocity , high turbulence liquid is pumped into casing 50 through input pipe 52 which extends into casing 50 until near structure 42 . output pipe 54 removes the heated liquid from casing 50 and is interconnected to an external heat exchanger ( not shown ) where the liquid is cooled for return to input pipe 52 by a pump ( not shown ). it is to be understood that the form of this invention as shown is merely a preferred embodiment . various changes may be made in the function and arrangement of parts ; equivalent means may be substituted for those illustrated and described ; and certain features may be used independently from others without departing from the spirit and scope of the invention as defined in the following claims . for example , various materials can be used in single crystal form to generate different wavelengths of x - rays , and to yield x - ray beams with different exit angles from the single crystal . furthermore , as previously discussed , materials can be coated onto the anode for the x - ray emitting structure by means of chemical vapor deposition . such coated materials are also capable of generating highly collimated x - rays .