fig1 shows a schematic circuit diagram of an x - ray generator implemented in inverter technology . the voltage applied to the x - ray tube 7 between anode a and cathode k is a direct - current voltage . the direct - current voltage may be obtained by a power rectifier 1 and an intermediate circuit filter 2 . the direct - current voltage may be converted into an alternating - current voltage by a series resonant circuit inverter 3 . the alternating - current voltage may be transformed by a high - voltage transformer 4 into a high voltage , which is converted into a direct - current voltage , for the x - ray tube 7 by a high - voltage rectifier 5 and filtered by a high - voltage capacitor 6 . the high voltage at the x - ray tube 7 may be 75 kv and more relative to ground or reference potential . as shown in fig2 , the high - voltage rectifier 6 is assembled from an array of commercially available high - voltage diodes connected in series . fig2 illustrates a diode chain ( diodes d 1 . . . dn ) of a high - voltage rectifier . the polarity of the high voltage originating from the high - voltage transformer may be such that the high - voltage diodes are in the conducting state . if the polarity of the applied high voltage changes , the high - voltage diodes transition to the cut - off state . however , the transition to the cut - off state does not take place arbitrarily quickly , since the minority charge carriers contained in the depletion layer of the high - voltage diodes are first eliminated . during this time interval , a reverse voltage is present at the diodes . because current continues to flow through the diodes due to the charge carriers present , a high power loss , referred to as the turn - off loss , occurs momentarily . particularly in the case of x - ray generators which operate in the higher frequency range , the high - voltage diodes may be subject to a heavy load due to the turn - off losses . fig2 shows parasitic capacitors or parasitic capacitances ( cp 1 . . . cp n - 1 ). during the transition from the conducting ( forward - biased ) to the non - conducting ( reverse - biased ) state , the topmost partial capacitance cp 1 is charged up first and then the other partial capacitances in turn . accordingly , almost all of the externally applied voltage is present initially at the topmost high - voltage diode , until the other partial capacitances are then charged up in turn . particularly high turn - off power losses occur at the topmost high - voltage diode and then at the other upper high - voltage diodes . high - voltage diodes having “ controlled - avalanche characteristics ,” which are able to withstand these high peak loads , may be used . to reduce the heavy load on the upper partial capacitances and prevent malfunctions in these switching elements , a potential control is provided to allow the turn - off power losses to be distributed uniformly over all of the high - voltage diodes . the potential control may include a diode chain that is embedded between two transversely mounted conductive plates p 1 and p 2 , of which one ( p 1 ) is connected to the potential of the top diode and the other ( p 2 ) to the potential of the bottom diode . the electric field between the diode chain and the plates may lead to the formation of spatially distributed capacitances , which are represented by dashed lines in fig3 . the distributed capacitances may be capacitances per unit length . such a capacitance per unit length may increase the closer the plate is to the resistance . accordingly , a capacitive voltage divider corresponding to the partial ratio at the diode chain is located at each point of the diode chain . the dynamic voltage distribution at the diodes is roughly equal to the total voltage divided by the number of diodes . during the transition from the conducting to the non - conducting state there results a uniform voltage distribution controlled by the capacitances , which ensures that the turn - off losses are distributed virtually uniformly over all of the diodes . in one embodiment , as shown in fig4 and 5 , an intermediate electrode may lie at a partial voltage . in high - voltage generators of x - ray generators , the x - ray tube voltage may be disposed symmetrically relative to the reference potential . accordingly , the assemblies , including the high - voltage cables , may have high - voltage insulation . in one embodiment , high voltage may be disposed unilaterally relative to the reference potential . accordingly , high - voltage insulation is difficult to ensure . fig4 shows lines that are connected to the potential of the total voltage . as shown in fig4 , a wire 11 has a thickness of 7 mm . the wire 11 lies at a potential of 150 kv . an edge or a limit of the x - ray device 12 is shown . the edge lies at reference potential . the distance between the wire 11 and the edge 12 is 100 mm . potential lines are drawn in the figure at intervals of 10 kv . the density of the potential lines is a measure for the field strength . the field strength is at its highest close to the wire 11 , where it amounts to max 9 kv / mm . the peak effect of the electric field strength may cause excessive field strengths at the lines lying at high - voltage potential , such as , for example , wire 11 , which have a relatively small diameter compared to the other dimensions . excessive field strengths may be field strength values , which due to their size , are a hazard potential ( e . g . spark formation or corona discharges , voltage breakdowns ). to reduce the high field strength to harmless values , a great distance between the lines and the reference potential may be required . accordingly , a disproportionately great distance would be necessary , since the distance is included in the high field strength at the small radii only via its logarithm . the high field strengths may be beneficially reduced by way of a greater diameter of the lines , which in turn gives rise to production problems , since lines with a large diameter are unwieldy to install and in addition — since they are to be provided with a high - voltage insulation — are not widely established components . in one embodiment , an intermediate electrode 13 is used . a voltage between the reference potential and the total voltage is applied to the intermediate electrode 13 . the voltage between the reference potential and the total voltage may be half the total voltage , which may be available due to the circuit layout ( fig5 ). fig5 shows a wire 11 . the wire 11 may have a thickness of 7 mm , which is at a potential of 150 kv . to reduce the field strength , an intermediate electrode 13 may be provided . the intermediate electrode 13 may lie at 75 kv . the edge 13 may lie at reference potential . the distance between the wire 11 and the edge 12 may be 100 mm . as a result of the intermediate electrode 13 , the maximum field strength is reduced to 6 kv / mm . this is also apparent from the potential lines which have a distance of 10 kv . the field strength between the reference electrode and the intermediate electrode amounts to 2 kv / mm . for example , the measure of the intermediate electrode 13 may reduce field strength excess at the tight radii of the equipotential lines . the intermediate electrode 13 may enclose the components , which lie at the total voltage , like an electric cage , insofar as this is constructionally possible . instead of using one control electrode , a potential control may be implemented by a plurality of control electrodes , which lie , for example , at different partial potentials . in fig6 to 9 illustrate potential control used in conjunction with a high - voltage connector . the high - voltage connector may present a particular problem in the case of high voltage . a high - voltage connector is shown in fig6 . a connector 31 ( horizontally hatched area ) may be introduced into a receptacle 32 ( diagonally hatched area ), such that a contact is established . an internal conductor 33 of the connector 31 is indicated to illustrate the contacting . a narrow air gap 34 remains between connector 31 and receptacle 32 after the two parts are connected . the casting material from which connector 31 and receptacle 32 are made is loaded to breakdown . although the casting material may not present a problem ( provided the casting process has been performed cleanly and free of voids , i . e ., without holes ), the leakage current load in the air gap between connector and receptacle may cause a problem . the leakage current resistance of high - voltage installations is inherently lower than the dielectric strength . it is essential to ensure a homogeneous distribution of the electric field strength along the leakage path . if excessive field strengths occur locally , this may lead to limited discharge processes at these points . the limited discharge processes at these points may damage the surface of the insulation material and over the long term result in a flashover along the leakage path . a simple connector is shown in fig6 . if the simple connector is used , then excessive field strengths may occur along the leakage path at the upper part of the air gap , as is shown by the simulation result of the field distribution in the high - voltage connector system shown in fig7 . a long connector and / or additional insulation materials ( e . g . silicone stocking ) may be disposed in the air gap . control electrodes may be used to achieve a uniform field distribution along the air gap between high - voltage connector and receptacle to prevent the breakdown mechanism . for example , four control electrodes or control elements 36 , 39 having defined potential may be used . in this scheme the control electrode 36 and the control rings 37 and 38 lie at reference potential . the control element 39 lies at high - voltage potential . the control electrode 36 may effect a capacitive voltage division between itself , the air gap , and the internal conductor 31 . the voltage along the air gap 34 may be uniformly reduced . the principle of operation corresponds to that of fig3 . in one embodiment , the optimal characteristics of the control electrode may be as long as the high - voltage connector and may have a shape similar to that of a spherical cap . however , simulation tests have shown that results that are only marginally less good are achieved using the variant shown in fig8 , which is easier to produce . the control rings 37 and 38 effect a field harmonization at the top and bottom edges and contribute to a more uniform field distribution . simulation results for the connector system from fig8 are shown in fig9 . the field distribution in the high - voltage connector system may be homogenized by the field control . the uniform field distribution achieves a constant field strength within the air gap . accordingly , it is possible to operate with higher voltages without undesirable leakage currents occurring .