Page 333 - Sami Franssila Introduction to Microfabrication
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312 Introduction to Microfabrication



                                                           Heating (and cooling) can also be affected by direct
                          Clean
             atm press    resist     APCVD   th oxid     backside contact with a fluid. Argon is employed in
                  10 2                          epi      sputtering systems to ramp up wafers to 400 to 500 C,
                                                                                                ◦
                                                         in a timescale of 10 s. In etchers, the wafer backside is
                   10      PECVD    LPCVD                often cooled by helium flow. Some of these gases leak
                          RIE    poly, ox/nitr, metal    into the process chamber, and the type of heating/cooling
                       Cryo  MIE Sputt-dep               gas has to be compatible with the process. In a plasma
                Pressure (torr)  10 −4  ECR  UHV/CVD     etcher, energy is supplied to the wafer both from the
                   −2
                  10
                       etch
                                                         plasma and from exothermic etching reactions. If no
                                      Gas
                                                         clamping is done, the temperature can easily rise to
                                                           ◦
                                      MBE
                  10 −6     Evap     source              80 C during the first minute of plasma etching, and
                                                         reach the photoresist glass transition temperature of ca.
                                                         120 C in a few minutes. Steady-state temperatures can
                                                            ◦
                  10 −8                                               ◦
                                    MBE                  be kept below 40 C indefinitely by backside cooling.
                 10 −10
                         0   200  400  600  800  1000  1200  30.5 SIMULATION OF PROCESS EQUIPMENT
                        room   Temperature (°C)
                        temp                             Process simulation covers length scales of a few
            Figure 30.1 Equipment classified on temperature/pressure  micrometres in both lateral and vertical directions. In
            axes. Reproduced from Rubloff, G.W. & Boronaro, D.T.  process-equipment simulation, the length scale is defined
            (1992), by permission of IBM                 by the tool size, and it can be up to a metre. In
                                                         practice, this scale difference means that tool simulation
                                                         is carried out independently of process simulation. In
                     Table 30.2 Methods for heating
                                                         tool simulation, 3D is the norm, but of course, all
            Method                     Example           symmetries in the tool geometry are utilized to reduce
                                                         computational load.
            Resistance heating  Furnace                    Typical tool simulation includes temperature distribu-
            Induction heating  Epitaxial reactor         tion, flow patterns and plasma properties. Mass, momen-
            Photon heating    Rapid thermal processing RTP  tum, energy and charge balances are calculated. Plasma
            Conduction        Horizontal electrodes in PECVD  modelling is difficult because it involves so many param-
            Convection        Argon backside heating in a
                                                         eters: collision cross-sections, ionization, attachment,
                                sputtering system
                                                         recombination, dissociation, and so on. These plasma
                                                         reactions must then be combined with surface reactions
                                                         (deposition or etching). Taken together, these determine,
            inevitable air mattress between the wafer and the hot  for instance, PECVD film uniformity. For reactors oper-
            plate, today the degree of thermal contact can be con-  ating in the mass transport–limited regime, flow patterns
            trolled at will (with hot plate price tags up to $20 000).  are of utmost importance. For reactors operating in the
              In most tools, wafers lie horizontally on elec-  surface reaction–limited regime, thermal design is a
            trodes/susceptors, and the electrode or susceptor is  high priority.
            heated. Clamping the wafer to the substrate electrode
            is the simplest way of increasing thermal contact. Both
            mechanical clamping and electrostatic clamping (ESC)  30.6 MEASURING FABRICATION PROCESSES
            are used. In the former, pins hold the topside of the
            wafer, which limits usable wafer area, and there is the  There are three different aspects that can be measured
            danger of contamination from the clamp pins. Mechan-  in a fabrication process: tool, process and wafer. Tool
            ical clamping is widely used because it is much sim-  parameters such as RF power, mass flow, process time
            pler than ESC. Clamping is essential when wafers  or electrode temperature are easily measured. Process
            are processed in the vertical position (for instance,  measurements deal with ionic strength in a cleaning
            in ion implanters in which the long acceleration tube  solution, electron and ion energies in plasma or an
            (see Figure 15.6) can only be built horizontally) or  ion dose. In lithography, exposure time is usually set,
            when wafers are processed face down (as in CMP,  but exposure, of course, depends on the UV energy,
            Figure 16.2).                                which drifts with lamp lifetime. Indirect measurements
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