Patent Number: 
Section: claims

1. A method of identifying an optimal landing energy of a probe current in a scanning electronic microscope for use in obtaining an optimal topographic image of a sample, comprising the steps of:(a) directing the probe current to the sample at a selected landing energy to produce a signal electron beam from the sample;(b) measuring the probe current;(c) providing a signal electron beam current detector;(d) receiving the signal electron beam at the signal electron beam current detector to obtain a signal electron beam current measurement;(e) calculating a ratio of the signal electron beam current measurement to the measured beam energy of the probe current;(f) repeating steps (a) through (e) at a landing energy other than the selected landing energy; and(g) comparing the calculated ratios at each landing energy to identify the optimal landing energy as a landing energy corresponding to a ratio having a value proximate “1”;(h) selecting the identified optimal landing energy; and(i) obtaining substantially the entire topographic image of the sample by directing the probe current to the sample at a single landing energy which is the optimal landing energy, and directing a resulting signal electron beam to an imaging detector. 2. The method of claim 1, wherein said providing step comprises applying to the sample a voltage having a value proximate a value of the voltage of the probe current, and using the signal electron beam to locate a desired position for the signal electron beam current detector. 3. The method of claim 1, wherein said measuring step (b) comprises disposing a probe current detector in a path of the probe current. 4. The method of claim 1, wherein said receiving step comprises directing the signal electron beam to said signal electron beam current detector. 5. The method of claim 4, wherein said step of directing the signal electron beam further comprises employing a Wein filter disposed in the path of the signal electron beam. 6. The method of claim 1, wherein said steps (d) and (h) are performed by employing a Wien filter disposed in the path of the signal electron beam for selectively directing the signal electron beam to one of said imaging detector and said signal electron beam current detector. 7. The method of claim 1, further comprising the step of selectively positioning said signal electron beam current detector within the path of the signal electron beam. 8. The method of claim 7, wherein said step (c) of providing a signal electron beam detector comprises the step of positioning the signal electron beam detector coplanar with, and at a 180° angle from, said imaging detector. 9. The method of claim 3, wherein said measuring step (b) further comprises using a Faraday cup as the probe current detector. 10. The method of claim 1, wherein said providing step (c) further comprises providing a Faraday cup as the signal electron current detector. 11. The method of claim 7, wherein said selectively positioning step further comprises applying a voltage to one of said signal electron beam and said imaging detector. 12. A system for identifying an optimal landing energy of a probe current in a scanning electronic microscope for use in obtaining an optimal topographic image of a sample, comprising:means for directing the probe current to the sample at a selected landing energy to produce a signal electron beam from the sample;a probe current detector for measuring the probe current;a signal electron beam current detector for obtaining a measurement of the signal electron beam;means for calculating a ratio of the signal electron beam current measurement to the measured beam energy of the probe current;means for obtaining a plurality of signal currents at different landing energies;means for comparing the calculated ratios at each landing energy to identify the optimal landing energy as a landing energy corresponding to a ratio having a value proximate “1”;means for selecting the identified optimal landing energymeans for obtaining substantially the entire topographic image of the sample by directing the probe current to the sample at a single landing energy which is the optimal landing energy, and directing a resulting signal electron beam to an imaging detector.