Page 334 - Sami Franssila Introduction to Microfabrication
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Tools for Microfabrication 313



           are often much simpler than direct measurements: for  reaction products, such as SiF 4 or WF 6 . At the etching
           example, vacuum chamber base pressure is a good  end-point, free fluorine intensity increases because it
           indication of vacuum quality, but mass spectrometry  is not consumed by the reaction. A more selective
           (usually called RGA, for residual gas analysis) can  method would be the monitoring of reaction products
           actually identify the residual atoms and molecules,  themselves. This must be developed for every process
           which can be truly significant in understanding vacuum-  individually. Nitrogen signal (396 nm) is suitable for
           film interactions. Molecular recognition also helps in  monitoring nitride etching: there will be a sharp drop
           trouble-shooting leaks.                     in nitrogen signal when all the nitride has been etched
             Very few measurements are actually done on the  away. OES does not, however, measure wafers but,
           wafers during processing. This is understandable because  rather, the process.
           process chamber conditions are often harsh, for example,  One of the oldest applications of in situ monitoring
           RF-fields, corrosive gases or high temperatures. Wafer  is the quartz crystal microbalance (QCM) film-thickness
           temperature in RTA can be measured by pyrometry dur-  control during evaporation and sputtering. The QCM
           ing processing. In ultra-high vacuum conditions, sur-  is placed in the same atom flux as the wafers, and
           face spectroscopy can be used to monitor deposition  therefore it experiences the same film deposition. Mass
           processes in real time: reflection high-energy electron  change is detected as a frequency change and converted
           diffraction (RHEED) and low-energy electron diffrac-  to film thickness. The resonance frequency of the QCM
           tion (LEED) are routinely employed in MBE systems  is given by
           to check the crystallinity of the growing film. Unfor-        f = v tr /2x        (30.1)
           tunately, most deposition processes are operated under
           conditions in which such systems cannot be used. Film  For quartz wafer of 500 µm thickness with transverse
           thickness during deposition or etching can be measured  wave velocity of 3340 m/s, this translates to 3.3 MHz.
           by, for example, ellipsometry or interferometry, but such  The frequency drop due to thickness increase is given by
           systems are not commonplace.                                      2
                                                                     f = −2f  x/v tr        (30.2)
             Measurements can be classified into four categories
           according to their immediacy:                 Taking into account the fact that the deposited film
                                                       density differs from that of quartz (but neglecting that
           – in situ: during wafer processing in the process  its elastic properties differ), we get the thickness from
              chamber                                  the frequency change:
           – in-line: after wafer processing in the process tool                 2
                                                              x = (v tr ρ quartz ) f/(−2f ρ film )  (30.3)
              (e.g., exit load lock)
           – on-line: in the wafer fab by wafer fab personnel  With a 1 ppm frequency shift easily detectable, the
           – ex situ: outside the analytical laboratory by expert  minimum thickness change that can be seen is of the
              users.                                   order of angstroms. Temperature sensitivity of QCM
                                                               ◦
                                                       is 0.5 ppm/ C, which has to be accounted for because
             In situ resist development monitoring with an inter-  deposition is usually accompanied by temperature rise.
           ferometric end-point detector can improve linewidth  In-line tools are located, for example, in load
           control considerably. It can compensate for changes in  locks or cool down chambers, and they measure
           exposure dose, resist (de)composition, developer con-  wafers immediately after, but not during, processing.
           centration and temperature or resist bake drifts and  Having the instrument outside the process chamber
           shifts, which could easily result in 10% development  helps because the ambience is usually benign: nitrogen
           time differences.                           or vacuum atmosphere without RF-fields, plasmas or
             Plasma etching is almost always monitored in real  toxic gases.
           time, in order to determine the end point and to prevent  On-line measurements constitute the bulk of mea-
           excessive etching of the substrate or the underlying  surements in wafer fab. These include measurements
           film. Optical emission spectroscopy (OES) is commonly  of standard film-thickness (ellipsometry, reflectometry),
           used: the intensity of some suitable excited species in  sheet resistance, implant damage by thermal waves, step
           the plasma is monitored with optical systems, including  height by profilometer, and so on. Some measurements,
           a wavelength selective detector. In fluorine plasmas, a  such as those for sheet resistance or film thickness, are
           signal at λ = 704 nm (from excited fluorine atoms) can  performed in seconds; while some, such as those for
           be used. During etching, the signal is small because  sample preparation or pumpdown (SEM, AFM), require
           there is little free fluorine: most of it is bound as  a few minutes.
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