“…The limitation of single dish measurements is always spatial resolution: a typical telescope with a diameter of 10 m has a spatial resolution of λ mm 30 , where λ mm is the observing wavelength in mm, and thus, e.g., a 10 m telescope operating at 90 GHz cannot resolve features smaller than about 100 . This problem has been circumvented in two ways: by observing eclipses, when the Moon's limb acts as a knife edge crossing the field of view, and the time dependence of the millimeter flux can be converted into (onedimensional) spatial resolution much finer than the telescope beam (e.g., Tolbert et al 1964;Hagen et al 1971;Beckman et al 1975;Swanson & Hagen 1975;Shimabukuro et al 1975;Roellig et al 1991;Ewell, Jr. et al 1993); and by going to submillimeter wavelengths (smaller λ), which is possible with the James Clerk Maxwell Telescope (JCMT) and Caltech Submillimeter Telescope (CSO) on Mauna Kea, Hawaii. These telescopes have been able to make images of the solar disk at submillimeter wavelengths with a spatial resolution as small as 20 (Horne et al 1981;Lindsey & Jefferies 1991;Bastian et al 1993a,b;.…”