in one embodiment , the present invention aims at detecting an electric field asymmetry in the icr cell and eliminating it by compensating and correcting the electric field . the existence of the magnetron motion in the cell produces normally very weak sidebands around the main ion cyclotron resonance signal of an ion measured at the frequency v r which are on the frequency scale in a distance of the magnetron frequency v m and 2v m . additionally , in the mass spectrum a peak with half the mass , i . e ., with the doubled reduced cyclotron frequency ( 2v r ) appears , this is the peak of the second harmonic . another signal with comparable abundance appears in the direct vicinity of the 2v r signal , which is a satellite peak with a frequency of ( 2v r + v m ). this satellite peak is separated from the second harmonics by just a magnetron frequency ( v m ). the mass difference is e . g ., at m / z 351 about 0 . 007 dalton . depending on conditions , also other satellite signals with even less abundance can appear in distances of mv m ( m = 2 , 3 , 4 , . . . ), which are of insignificant abundance under regular measurement conditions , however , can in principle also be used for the electric field correction if sufficiently abundant . in the frequency spectrum or mass spectrum these distances are extremely small , since the magnetron frequency v m under the applied electric and magnetic field conditions is in general less than 10 hz . in fig4 a to 4 d an example of unfavorable conditions in a dynamically harmonized icr cell containing leaf and inverse leaf electrodes is shown : an asymmetric electric field is here artificially generated by using a special set of voltages at the four pairs of the leaf electrodes ( as shown in fig3 a - 3 b ). under these circumstances ions circle on large and offset magnetron orbits . fig4 a shows the full ft - icr mass spectrum 400 of sodium trifluoroacetate in the icr cell with a slightly offset electric field axis and , thus , under unfavorable conditions in terms of position and size of the magnetron orbit to demonstrate the effect . the peak with m / z = 702 . 87 da 401 is selected for a closer view and displayed in fig4 b . in the abscissa of the spectrum in fig4 b the scale is converted from mass scale to a frequency scale ( therefore the numbers increase to the left ) and the peaks are shown with their measured cyclotron frequencies . the reduced cyclotron frequency of the selected main peak with m / z = 702 . 87 da 401 is called v r ′. it has three visibly abundant sidebands at frequencies v r ′+ v m 412 , v r ′+ 2v m 411 , and v r − v m 413 . sidebands indicate the existence of significantly large magnetron orbits and confirm the unfavorable conditions in the icr cell during the acquisition of these spectra . fig4 c shows the second harmonics 421 of the main peak at m / z = 702 . 87 da ( 401 ) at twice its measured cyclotron frequency 2v r ′, therefore , at the half of its m / z value . the abscissa of the spectrum in fig4 c is again converted to the frequency scale and all peaks are shown with their measured cyclotron frequencies . the second harmonics has a set of satellite peaks 422 , 423 , 424 and 425 in distances equal to multiples of the magnetron frequency v m . the satellite peak with highest abundance has the frequency 2v r + v m 422 . in principle , some or all of these satellite peaks 423 , 424 and 425 can be used to perform the electric field correction . the intensity of the second harmonics peak with the frequency of 2v r ′ is related to the position of the magnetron motion . if the center of the magnetron orbit approaches the cell axis , the intensity of the second harmonics is reduced . if the magnetron axis virtually coincides with the cell axis , the second harmonics peak virtually disappears , that is , is hardly detectable above the noise . additionally , the intensity of the satellite peak with the frequency 2v r ′+ v m is related to the size of the magnetron orbit . if the magnetron radius is large , as in this example , this satellite peak is considerably abundant a comparison of the scales of the ordinates of fig4 b and 4 c shows that the second harmonics and its major satellite peak are by more than an order of magnitude smaller than the main signal . the distribution of the second harmonics peaks 402 can even be seen in the broadband spectrum shown in fig4 a ( see the dashed ellipse ). in an ft - icr measurement , it is basically advantageous if the magnetron orbit has a relatively small diameter or if it does not exist at all . unfortunately , experimental methods to reduce the magnetron motion with cooling using a resonant buffer gas are not generally applicable since they are mass selective and require the introduction of relatively high amounts of gas into the ultrahigh vacuum chamber . in addition , it is also desirable that the axis of the magnetron orbit be as close as possible to the axis of the icr cell . in the best case , it should be coaxial with the cell axis . a compromise would be a small magnetron orbit close to the cell axis . if the electric field in the cell is asymmetric , its axis may be radially displaced against the cell axis . in this case , the magnetron orbit is also shifted and located around this radially displaced electric field axis . one aim of the electric field correction is that the ions in the cell circle on magnetron orbits that have a diameter as small as possible and are as central as possible . simulations of the ion motion in the icr cell show that the second harmonics with the frequency 2v r disappears if the magnetron orbit is concentric with the cell , i . e ., if its center is on the cell axis . if the electric field axis does not coincide with the cell axis , i . e ., if it is radially displaced , this will also shift the magnetron orbit radially and the second harmonics peak will appear . on the other hand , the intensity of the satellite peak ( 2v r + v m ) of the second harmonics increases with the magnetron radius . in order to achieve small magnetron orbits which are as central as possible , in an embodiment according to the present invention it is proposed correcting or compensating electric field conditions by using varying compensation voltages at the various mantle electrodes so that the intensities of the second harmonics and its satellite peak become as small as possible . ion motion simulations show , that during the cyclotron excitation process of an ion which is not at the cell axis , the center of the cyclotron motion shifts radially . if , at the start of the cyclotron excitation , the ion is located in the quadrant of an excitation electrode , the center of its cyclotron path is shifted away from the excitation electrode to the axis of the cell . this means the ion will continue orbiting on a slightly smaller magnetron orbit after the cyclotron excitation . the magnetron motion is de - excited or relaxed . if the ion , however , is located , at the start of the cyclotron excitation , in the quadrant of a detection electrode , the center of its cyclotron path is shifted in direction to the detection electrode , away from the axis of the cell . this means , after this cyclotron excitation , the ion continues circling on a larger magnetron orbit . its magnetron motion is excited during the cyclotron excitation period . an increase of the size ( or diameter ) of the magnetron orbit leads to a stronger satellite peak ( 2v r + v m ) of the second harmonics ( 2v r ). thus , in a complete magnetron cycle around the cell axis there are two phases where a cyclotron excitation increases the intensity of the satellite peak ( 2v r + v m ) and two phases where a cyclotron excitation decreases the intensity of the satellite peak ( 2v r + v m ). fig5 a shows the result of a simulation . in the cross sectional view 150 of a cylindrical icr cell with excitation electrodes 160 and 161 and detection electrodes 162 and 163 , a simulated cyclotron path 151 is depicted . prior to its cyclotron excitation , the ion is not on axis of the icr cell , but on a position 154 in the quadrant of one of the excitation electrodes 160 due to its large and excited , or offset , magnetron orbit . after the cyclotron excitation the center of the excited cyclotron orbit is no longer at the same position 154 but it is now somewhat closer to the center of the cell . the difference 157 is shown between the two dashed lines 155 and 156 in fig5 a . fig5 b also shows the result of a simulation . in the cross section view 170 of a cylindrical icr cell with excitation electrodes 160 and 161 and detection electrodes 162 and 163 a simulated cyclotron path 171 is depicted . prior to its cyclotron excitation , the ion is not on axis of the icr cell , but at a position 174 in the quadrant of one of the detection electrodes 162 due to its large and excited , or offset , magnetron orbit . after the cyclotron excitation , the center of the excited cyclotron orbit is no longer at the same position 174 but it is now somewhat closer to the detection electrode 162 . the difference 177 is shown between the two dashed lines 175 and 176 in fig5 b . compared to the cyclotron motion , the magnetron motion is very slow . thus , when an ion is cyclotron - excited on its magnetron orbit , after the excitation , the ion practically does not move further on its magnetron path . if between the capture of the ion in the cell and the excitation of the cyclotron motion a variable delay ( post capture delay , pcd ) is inserted into the experiment sequence , the ion can be monitored on its magnetron orbit with the satellite peak ( nv r + mv m ) of an even - numbered harmonics , such as the second harmonic with n = 2 . if after a certain post capture delay time the ion arrives in the quadrant of a detection electrode , where the resonant cyclotron excitation takes place , the monitored intensity of the ( 2v r + v m ) peak increases to a maximum . after a still larger post capture delay time the ion arrives in the quadrant of an excitation electrode when the resonant cyclotron excitation takes place , and the monitored intensity of the ( 2v r + v m ) peak decreases , for example to a minimum . the measured dependence of the relative intensity of the ( 2v r + v m ) peaks on the post capture delay ( pcd ) can be used to obtain information about the displacement ( or shift ) of the magnetron orbit and about the symmetry of the dc electric field in the cell . pcd diagrams of ions on magnetron orbits around the cell axis show two equally high maxima and two equally high minima within one magnetron period . if the maxima are not equally high , this is a sign that the magnetron orbit is shifted , i . e ., that the electric field axis no longer coincides with the cell axis . relatively small magnetron orbits result in flat and shallow pcd curves with low intensity . larger magnetron orbits are responsible for the higher maxima and deeper minima magnetron orbits which are shifted completely to one side of the cell result in pcd curves with one single maximum and one single minimum within a magnetron period . small magnetron orbits which are completely off axis and shifted to a quadrant of the cell , which however , due to their small size still are very close to the cell axis , form flat pcd curves with a single maximum and a single minimum within a magnetron period and still deliver good ft - icr spectra . it has to be noted that the relative intensity of the ( 2v r + v m ) peak changes often very strongly with the variation of the post capture delay , while the relative intensity of the second harmonics ( 2v r ) shows no significant change vs . the variation of the post capture delay time . fig6 shows a pcd diagram 250 in which the change of the relative intensity of the peak with the measured frequency ( 2v r + v m ) is plotted as a function of the post capture delay time of the ions in the cell . as described above the pcd curve 251 shows maxima 260 , 262 , 264 and minima 261 , 263 . the distance between a first maximum 260 and a third maximum 262 corresponds to the period 252 of the magnetron motion , which is in this case about 200 ms . this in turn corresponds to a magnetron frequency of about 5 hz . in the lower half of the figure the corresponding positions of an ion in the cell are shown , at which the cyclotron excitation took place . here , the excitation electrodes 160 and 161 and the detection electrodes 162 and 163 can be seen in the cross sectional views of icr cells . in these simulated pictures , ions start the cyclotron excitation always at an ion position which is not on the cell axis . starting positions of the ion cyclotron excitations are marked as white dots 270 , 280 and the shift direction of the center of the cyclotron orbit during the excitation process is shown by white arrows 271 , 281 . as described above , this shift is in direction 281 to a detection electrode 162 if the excitation process takes place near a detection electrode 162 . this in turn means an excitation of the magnetron motion during the cyclotron excitation . however , if a cyclotron excitation is in the quadrant of an excitation electrode 160 , the center of the cyclotron path is shifted away from the excitation electrode 160 , in direction 271 to the cell center . this in turn means a de - excitation or a relaxation of the magnetron motion during the cyclotron excitation . if the axis of the dc field coincides with the icr cell axis the cyclotron motion winds as a magnetron orbit on a circle around the cell axis . in this case , the maxima in the pcd curve should be equally high . however , in fig6 the maxima in the pcd curve 251 are not equally high . they are alternatingly higher and lower . this means that the magnetron does not circle around the cell axis since the electric field axis is shifted . by compensating the shifted electric field , the field axis can be moved back close to the geometric axis of the cell , in the best case even such that it coincides with the geometric axis . in one embodiment , for correcting an asymmetric electric field inside a dynamically harmonized icr cell , the inverse leaf electrodes are used , which anyway carry a common dc potential . this dc potential can be re - adjusted in order to shim the shifted field axis back to the geometric axis of the cell . fig7 shows the effect of the electric field correction in a dynamically harmonized icr cell ( 50 ) from fig3 a on a different pcd diagram ( 300 ). the first pcd curve ( 320 ) shows alternating low and high maxima . prior to plotting this curve in a dynamically harmonized icr cell , a dc voltage of 1500 mv is connected to all inverse leaf - shaped electrodes of the cylinder mantle . for the electric correction , the voltage applied to a pair of the inverse leaf electrodes in the excitation ( 61 and 63 in fig3 b ) is varied , while the others are kept at 1500 mv . before plotting the curve 321 the voltage of the electrode pair 61 and 63 is reduced to 1485 mv . upon this change the lower maxima become slightly higher . the curves 322 and 323 are plotted with voltages of this electrode pair at 1475 mv and at 1465 mv , respectively . finally , at 1450 mv a pcd curve 324 is observed , which contains approximately equally high maxima . the field compensation is accomplished and the axis of the magnetron orbit is now close to concentric with the cell axis . as mentioned above , a pcd curve with all equally sized maxima is a sign for a central magnetron motion , i . e ., a practically central electric field axis . however , it can also be desirable that the magnetron orbit has a relatively small radius . thus , the intensity of the satellite peak with frequency for example ( 2v r + v m ) needs to be as small as possible , which in turn means the intensity of the pcd curve must be as small as possible . experience shows that pcd curves which remain within an intensity range of a few percent , such as up to 2 - 3 % or even more , are a sign for an acceptable field correction state of the icr cell . even a small magnetron orbit which is a little shifted away from the cell axis , and is completely in the quadrant of e . g ., a detection electrode so that it produces a pcd curve with a single maximum within a magnetron period , is also an acceptable compromise . fig8 shows a pcd diagram 340 with the curve 341 , which shows only one maximum and one minimum within a magnetron period after a field correction is applied . in the same figure , as a comparison , another pcd curve 342 is shown which contains , after a different compensation voltage adjustment , two maxima and two minima within a magnetron period . fig9 a to 9 d show the effect of the field correction on the ft - icr spectrum in a dynamically harmonized icr cell . the spectrum 410 with the selected peak 401 before the application of the field correction is known from fig4 b . as mentioned above , this spectrum is shown to illustrate the effects under unfavorable electric field conditions in the icr cell . the sidebands 411 , 412 , and 413 are an indication of a significantly large magnetron orbit . fig9 a shows the same part of the ft - icr spectrum 430 after the application of a field correction according to an embodiment of the invention . voltage differences applied to the inverse leaf electrodes for correction were − 10 mv at the electrode pair 57 and 59 , − 100 mv at electrode pair 61 and 63 , + 10 mv at the electrode pair 66 and 68 , and + 100 mv at the electrode pair 70 and 72 ( numerals as in fig3 b ). the only visible peak in the spectrum after this correction is the main peak with the frequency v r ′ 401 a , the sidebands are no longer visible . furthermore , the absolute intensity of the main peak v r ′ 401 a is here larger than before the correction 401 ; fig4 b . with the reduced magnetron radius , possible ion losses during cyclotron excitations are avoided . fig4 c depicts a spectrum 420 of the second harmonics 2v r ′ 421 and its satellite peaks 422 , 423 , 424 and 425 before field correction . fig9 b , on the other hand , depicts a spectrum 440 after field correction . there are only two peaks left , the second harmonics 421 a now less than a fifth of 421 in fig4 c , and the largest satellite peak 422 a , now about 10 % of the corresponding peak 422 in fig4 c . fig9 c shows the full ft - icr mass spectrum 400 a of natfa after the field correction . not only is the intensity of the selected peak 401 increased , but also all other peaks are more abundant after the field correction . the intensity of the second harmonics peaks group 402 below m / z 1 , 000 is also reduced 402 a ( dashed ellipse ) in the field - corrected spectrum 400 a . fig9 d summarizes the changes at the second harmonics peak and its satellites during the field correction on the same intensity scale . the extracted partial spectrum 420 a at the bottom shows the second harmonics 421 of the ion with m / z 702 . 87 da ( on a frequency scale ) and its major satellite peak 422 in artificially generated asymmetric field conditions . the partial spectrum 450 in the middle shows the situation during the field correction when the voltages of all inverse leaf electrodes are exactly the same (+ 1 . 5v ), i . e ., a perfectly symmetric voltage case . the intensities of the second harmonics 421 b and its satellite 422 b are already much less . the top spectrum 440 a shows the two peaks when the field correction is accomplished . the second harmonics 421 a and its satellite 422 a are significantly smaller than in the starting spectrum 420 a . an interesting point here is that after the accomplished field correction and minimizing the second harmonics and its satellite peak , the final voltage setting is not symmetric either . however , they are differently asymmetric than the initial setting . in other words , the pattern of compensation voltages is not homogeneous over the set of different electrodes . the unfavorable starting conditions ( fig4 b , c ) were due to an artificial asymmetric voltage setting in the cell . these initial voltage values before field correction were : 1 . 50v at the electrode pair 57 and 59 , 1 . 55v at the electrode pair 61 and 63 , 1 . 50v at the electrode pair 66 and 68 , and 1 . 45v at the electrode pair 70 and 72 ( numerals as in fig3 b ). the final voltage values after field correction were : 1 . 49v at the electrode pair 57 and 59 , 1 . 45v at the electrode pair 61 and 63 , 1 . 51v at the electrode pair 66 and 68 , and 1 . 55v at the electrode pair 70 and 72 . since this setting is providing the smallest second harmonics ( 2v r ′), smallest satellite peak ( 2v r ′+ v m ) and the smallest sidebands of the main peak , it is obviously the preferred way for forming a symmetric electric field when the axis coincides ( or nearly coincides ) with the cell axis . the experience shows that the correction voltages usually deviate from the previous uncorrected voltage settings between about ± 10 and 100 mv , but can also be higher or lower in individual cases . observations also show that the amplitude of the irradiated rf electric field for the excitation of the ion cyclotron motion also influences the shape of the pcd curves . pcd curves with equally high maxima within a magnetron period can start showing low and high maxima if the excitation amplitude is changed , e . g ., doubled . therefore , it is advantageous to perform field correction processes at the excitation amplitudes which will be used in an actual experiment series . a shift of the electric field axis is not only observed in dynamically harmonized icr - cells . also conventional cylindrical icr - cells , as shown at ( 200 ) in fig1 a , can have a shifted electric field axis . an asymmetrically contaminated trapping electrode in a classical icr cell , for instance , can cause a slightly asymmetric electric field . since in conventional icr cells no extra longitudinal electrodes exist to which dc voltages are connected , the correction or compensation of the asymmetry is different here . in these cells , according to further embodiments of the invention , the electric field correction can be performed by connecting variable voltages to the excitation electrodes ( one of them visible , 211 ) and to the detection electrodes 210 and 212 . detection electrodes are usually sensitive and often generate a noisy signal if a dc voltage is applied to them . however , if a battery is used as power source , for example , the noise can be reduced ( e . g ., minimized ) also in this case due its very stable output . another alternative embodiment according to the invention would be to modify a conventional cylindrical icr cell with additional electrodes that carry the necessary dc voltage for an electric field axis correction . since most of the voltages used for a successful correction are less than 100 mv , a disturbance of the icr cell operation would be relatively minimal . the embodiment in fig1 b shows such a cylindrical cell 201 with a total of four longitudinal correction electrodes e . g ., 230 and 231 between excitation electrodes ( one of them visible , 221 ) and detection electrodes 220 and 222 . four longitudinal correction electrodes , in this case symmetrically arranged about the cell axis at 90 ° intervals , can basically move the electric field axis back to the geometric cell axis if the field axis was uniformly shifted in a radial direction . uniform means here that the general form of the electric field is conserved . it is just shifted in the radial direction but the electric field axis remains essentially parallel to the geometric axis . in this simplest case , the field axis is not bent , rippled or tilted . in some cases ft - icr cells with a larger number of excitation and / or detection electrodes are used . using multiple pairs of detection electrodes helps acquiring higher resolution ft - icr spectra . in the cells for these applications also a larger number of correction electrodes can be used . in an ft - icr cell with four excitation and four detection electrodes , also eight correction electrodes can be placed between each of these ft - icr mantle ( excite and detect ) electrodes . even if the cell is not used for higher frequency detection , excitation and detection electrodes can still be divided longitudinally into two or more parts and a thin longitudinal correction electrode can be placed between each of them . fig1 c shows as example a cell 301 with eight ft - icr mantle electrodes with longitudinal correction electrodes ( total of 8 ) placed between each of them . in this figure in a 90 ° angle between the dashed - dotted lines 305 and 306 an excitation electrode 320 , a correction electrode 330 , a detection electrode 321 , and a second correction electrode 331 are fitted . the electrode 322 is another excitation , and 319 another detection electrode while 329 is again a correction electrode . element 205 and 206 are the axial trapping electrodes of the icr cell . unfortunately , sometimes electric field disturbances in the icr cell appear which are more complicated than just a simple linear shift of the field axis . the reason may be a more complex distribution of the electrode surface charging which not only shows a radial non - uniformity but also an axial one . in this non - linear case a linear axis correction , e . g ., using the inverse leaf electrodes 61 and 63 of a dynamically harmonized cell 50 as shown in fig3 b , cannot be successful , as these longitudinal electrodes are parallel to the cell axis . using these electrodes only a radial field correction can be made , but not an axial one . in order to also correct field errors with axial components , the use of segmented ( correction ) electrodes in the icr cell is suggested . segmented electrodes can also be used to correct the electric field , if the field axis is perturbed non - uniformly , such as by bending , rippling or tilting . a bent , rippled or tilted electric field axis is formed , for instance , if at different axial positions the center of the electric field is radially shifted by different amounts . in a dynamically harmonized cell 50 as shown in fig3 a - 3 b the inverse leaf shaped electrodes ( e . g ., 57 ) can be segmented . fig1 shows , according to another embodiment of the invention , a modified dynamically harmonized cell 100 in which the inverse leaf shaped cylinder mantle electrodes are divided . divided inverse leaf electrodes visible in this figure have the partial electrodes 107 a , 107 b , 107 c , 107 d , 107 e , and 109 a , 109 b , 109 c , 109 d , and 109 e , as well as 111 a , 111 b , 111 c , 111 d , 111 e . only two partial electrodes 105 a and 105 b are visible from a further inverse leaf electrode family 105 a - 105 e . each of these partial electrodes is supplied with an independent and variable dc voltage . the configuration depicted in fig1 is one of the possible embodiments and contains inverse leaf electrodes divided in five parts . inverse leaf electrodes including more parts can be made . in this configuration leaf electrodes ( e . g ., 58 ) as well as the half - leaf electrodes ( e . g ., 56 a and 56 b ) remained unchanged as in the original version of the dynamically harmonized cell 50 illustrated in fig3 a . in order to correct non - linear field distortions in a modified cylindrical icr cell 201 as shown in fig1 b this can be further modified by dividing the correction electrodes 230 and 231 . such a further modified cell 202 is shown in fig1 as another embodiment according to the invention . axial distortion components of an asymmetric electric field can be compensated using these correction electrodes which are in this particular embodiment divided into five segments 230 a , 230 b , 230 c , 230 d , 230 e , and 231 a , 231 b , 231 c , 231 d , 231 e . to each segment of the divided correction electrodes an independently variable dc voltage is connected . the number of electrode segments is not limited to the number five as in this embodiment but can be varied . fig1 shows as an example a cylindrical ion cyclotron resonance cell 301 with two pairs of excitation electrodes and two pairs of detection electrodes and longitudinal correction electrodes ( total of 8 ) placed between each of them . each correction electrode in this figure is divided into seven segments . the excitation electrode 320 , a segmented correction electrode with the segments 330 a , 330 b , 330 c , 330 d , 330 e , 330 f , 330 g , a detection electrode 321 and a second segmented correction electrode with the segments 331 a , 331 b , 331 c , 331 d , 331 e , 331 f , 331 g are fitted within a 90 ° angle between the dashed - dotted lines 305 and 306 . element 322 is another excitation electrode and element 319 yet another detection electrode , while the electrode divided in segments 329 a , 329 b , 329 c , 329 d , 329 e , 329 f and 329 g is again a correction electrode . the process of the asymmetry correction of the electric field can be performed beginning with standard voltage settings at the ( correction ) electrodes . initially , an ft - icr spectrum is acquired and one of the major peaks of interest is chosen as the object of the optimization . then , further ft - icr spectra are acquired under varied post capture delay times until a pcd - diagram for the relative intensity of the satellite peak of an even - numbered harmonics with the frequency of nv r ± mv m , such as 2v r ± 1v m , for over at least two periods of the magnetron motion is completed . it is to be mentioned here that the chosen ion does not have to be isolated for the iteration . measurements can proceed with all available ions within the icr cell . the pcd curve shows maxima and minima . a delay time in the pcd diagram at or near a maximum of the curve is selected . keeping this pcd time , now all ( correction ) electrode voltages are varied in a multidimensional search in order to find an optimum voltage combination that leads to a common minimum of the relative intensities of the even - numbered harmonics with the frequency nv r and its satellite peak with the frequency nv r ± mv m , such as n = 2 : the second harmonics and m = 1 : the closest satellite peak . after finding this local common minimum , the obtained voltage values corresponding to this minimum are used and the post capture delay time is varied again , a partial or complete pcd curve is acquired . then it is checked if the relative intensities of the even - numbered harmonics and the satellite peak at the maxima of the curve are reduced below the values obtained with the previous voltage setting . if they are not reduced in this pcd diagram , one has to go back and pick another point near a maximum at the initial pcd curve and start over again . if the relative intensities of the even - numbered harmonics and the satellite peak at the maxima of the curve are reduced , one starts with another iteration at the new curve &# 39 ; s maximum . again here , a maximum of this pcd curve is selected and the variation of the voltages for a multidimensional search is repeated and optimized again . these iterations are repeated until the global common minimum of the two peaks is found , i . e ., the even - numbered harmonics with the frequency nv r and its satellite peak with the frequency e . g . nv r + mv m . the process of the asymmetry correction of the electric field can be automated . a computer program can be used with an algorithm that begins with standard voltage settings at the ( correction ) electrodes . it acquires ft - icr spectra , selects one of the major peaks of interest , varies the post capture delay time , acquires again ft - icr spectra until it completes a pcd - diagram for the relative intensity of the satellite peak of an even - numbered harmonics with the frequency of nv r ± mv m , e . g . n = 2 and m = 1 , for over at least two periods of the magnetron motion . the pcd curve shows maxima and minima . the algorithm selects a delay time in the pcd diagram at or near a maximum of the curve . keeping this pcd time , it now varies all ( correction ) electrode voltages in a multidimensional search to find an optimum voltage combination that leads to a common minimum of the relative intensities of the even - numbered harmonics with the frequency nv r and its satellite peak with the frequency nv r ± mv m . after finding this local common minimum it uses the obtained voltage values corresponding to this minimum , goes back and varies the post capture delay time , acquires a complete pcd curve , and checks if the relative intensities of the even - numbered harmonics and the satellite peak at the maxima of the curve are reduced below the values obtained with the previous voltage setting . if they are not reduced in this pcd diagram , the program goes back and picks another point near a maximum in the initial pcd curve and starts over again . if the relative intensities of the even - numbered harmonics and the satellite peak at the maxima of the curve are reduced , the program starts another loop at the new curve &# 39 ; s maximum . the program again selects a maximum of this pcd curve and repeats the variation of the voltages for a multidimensional search and the optimization again . it repeats these iterative loops until it finds the global common minimum of the two peaks , i . e ., the even - numbered harmonics with the frequency nv r and its satellite peak with the frequency e . g ., nv r ± mv m . a slightly different method of the optimization , preferably performed in an automated manner , would be the following : the program acquires ft - icr spectra , selects one of the major peaks of interest and checks the intensities of an even - numbered harmonics ( nv r ) and the satellite peaks ( nv r ± mv m ) of the even - numbered harmonics therein in dependence of the compensation voltages . by independently varying the compensation voltages of all available ( correction ) electrodes the algorithm performs a multidimensional search for a common minimum of these two peaks . after finding the voltages for obtaining minimal peaks , the algorithm goes back and changes now the post capture delay time , then repeats the multidimensional voltage search again and finds the common minimum of the peaks now in dependence of this new delay time , and so on . these iterative loops continue until the global common minimum of the two peaks , i . e ., the even - numbered harmonics with the frequency nv r and its satellite peak with the frequency nv r ± mv m is found . in complex cases where also axial components of the distorted electric field need to be compensated , the correction algorithm will include the voltage values of the individual segments of the corresponding electrodes . such an optimization program can always be applied , if an electric field asymmetry is suspected . automated runs can also be implemented for diagnostic purposes . here the program would acquire in periodic times a post capture delay curve just for testing the size ( or diameter ) and the symmetry of the magnetron motion and deriving the conclusion about the position of the axis of the electric field in the icr cell . the invention has been described with reference to various embodiments . it will be understood , however , that various aspects or details of the invention may be changed , or various aspects or details of different embodiments may be arbitrarily combined , if practicable , without departing from the scope of the invention . generally , the foregoing description is for the purpose of illustration only , and not for the purpose of limiting the invention which is defined solely by the appended claims . although the present invention has been illustrated and described with respect to several preferred embodiments thereof , various changes , omissions and additions to the form and detail thereof , may be made therein , without departing from the spirit and scope of the invention .