Patent Number: 
Section: claims

1. A method for producing resist profiled elements with an electron beam lithography system, which produces the electron beam with a primary energy, the beam axis of which is largely perpendicular to a resist layer in which the resist profile is produced, comprising the steps of:providing the resist layer in the form of a negative resist on a substrate;exposing surfaces of a selected resist system of substrate, resist and thickness of the resist layer with different doses and determining a contrast curve after development the measured residual thickness of the resist layer;determining for a later defined adjustment of the electron beam lithography system a scattering cone and a size thereof in relation to the resist system, wherein a plurality of single lines are scribed in the resist layer with a probe size as small as possible and thereby obtaining a residual resist thickness distribution which is dependent on the site of incidence of the electron beam and being converted with the help of the contrast curve into an electron dose distribution that is the scattering cone;determining from the contrast curve the electron dose distribution of the scattering cone the resulting resist thickness distribution, which depends from several parameters;adjusting the electron beam with regard to parameters including the electron surface dose, width of the generated resist profile, thickness of the resist layer, and/or the primary energy of the electron beam, such that a non-orthogonal resist profile is produced and the probe size is the smallest possible structure size; andadjusting the probe size is quasi-continuously, whereby the primary energy of the electron beam is continuously changeable, a lower energy limit of the primary electrons is 1 keV, and an upper energy limit of the primary electrons is 20 keV. 2. The method according to claim 1, wherein the electron surface dose is defined by parameters such as the type of substrate, type of resist, resist thickness, development rule, and primary energy of the electron beam, and wherein the electron beam is adjusted according to these parameters. 3. The method according to claim 1, wherein the resist profile comprises a grating structure that consists of an array of depressions and elevations. 4. The method according to claim 1, wherein a gradation curve of the used resist is taken. 5. The method according to claim 1, wherein with the primary energy of the electron beam, the development process, and the resist thickness held constant, a gradation of the resist is applied as a function of a standard resist thickness in relation to the standard electron surface dose used is applied before electron irradiation. 6. The method according to claim 5, wherein the gradation  S  =            (                        Δ          ⁢                                          ⁢          d                          d          0                    )        /          (                        Δ          ⁢                                          ⁢          D                          D          max                    )      does not exceed the value of 1.5. 7. The method according to claim 6, wherein surfaces in the resist layer are exposed with a variable electron dose, and wherein the appropriate electron dose for the pertaining and residual resist thickness is determined after the development process. 8. The method according to claim 1, wherein one element of the profile of the grating structure consisting of depressions and elevations is determined by the electron surface dose      D    B    =            (                        D          0                          (                                    2              ⁢                                                          ⁢              n                        +            1                    )                    )        ×                  ∑                  i          =          1                          i          =          n                    ⁢              [                                            f              e                        ⁡                          (              x              )                                +                                    f              e                        ⁡                          (                              x                -                                  i                  ×                  b                                            )                                +                                    f              e                        ⁡                          (                              x                +                                  i                  ×                  b                                            )                                      ]            to be used. 9. The method according to claim 1, wherein a diameter of a scattering cone is produced by the amplitude of the primary energy of the electron beam in the resist layer around the site of incidence of the electron beam, whereby the diameter of the scattering cone is inversely proportional to the primary energy of the electron beam. 10. The method according to claim 1, wherein the electron surface dose is defined by the parameters such as type of substrate, type of resist, resist thickness, development rule, and primary energy of the electron beam.