396B. Spengler et al.: Laser Mass Analysis in Biology arise from the eventual need to increase the chooping frequency to improve the spatial resolution. This will decrease the signal.Considerable improvements to the present experiments can be made when one considers the use of radiation resistant phosphors such as the compound semiconductors [4,9, lo]. We are presently pursuing this line of investigation.We feel that LEM should be able to compete well with IR microscopy, since this latter technique, although chemically selective, is limited to a resolution somewhat larger than the operating wavelength, confocal and other recent o p t i d configurations notwithstanding. The LEM should be superior to spontaneous Raman microscopy because of the sample heating problem for most materials with spontaneous Raman. The sophistication necessary in the design of the optical train is considerably simplified as well.Compared to our earlier work on coherent Raman microscopy, namely the CARS microscope [ll], the present technique shouid be able to eventually achieve considerably improved spatial resolution, probably be easier to implement in a turnkey operation, but requires vacuum over the sample and more extensive sample preparation than needed for the CARS microscope.The LEM should be able to perform analyses which can not be done using well known electron beam microprobe or microimaging methods such as X-ray fluorescence, SIMS, Auger, PES, etc. These conventional methods tend to be strongest in providing atomic species, not molecular information. While some of them do give some molecular specificity, they are incapable of the spectral resolution of a laser based method. In principle, if one sought to image a species such as the extremely narrow bandwidth zero phonon lines of a solid, this should be out possible for the LEM.Even using the simple carbon dioxide laser, there is a large range of applications open to this technique because of the many accidental coincidences in the 9 -11 micron portion of the spectrum [7,8]. These potential applications include: imaging organic residues in wafer production; viewing cured and uncured regions of photopolymers; defects, dislocations, etc. in semiconductors; imaging the distribution of non-ra-dioactive isotopic species; imaging crystalline phases differing only in stoichiometry.The authors wish to thank the following members of the staff of the Naval Research Laboratory: Mr. John Peele for the complete mechanical design, modifications and construction of the instrument: Dr. Claudia Randolph for initially suggesting the manganese difluoride phosphor; and Dr. Mark Seaver for many discussions and suggestions. We also wish to thank Dr. Howard Schlossberg of the Air Force Offce of Scientific Research for providing support and encouragement during various stages of this project.