Page 105 - Sami Franssila Introduction to Microfabrication
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84 Introduction to Microfabrication



            temperatures, but the situation is really much more                   Mo
            complex because stress relaxation can occur during high-  Tension  Cr        Ta
            temperature deposition.
              The coefficient of thermal expansion (CTE) of silicon                             Pt
                     −6 ◦
            is 2.6 × 10 / C (around room temperature). The only
            other materials used in microfabrication that have
            smaller coefficients are silicon dioxide, silicon nitride
                                            −6 ◦
            and diamond which have CTEs 0.5 × 10 / C, 2.4 ×
                             −6 ◦
              −6 ◦
            10 / C and 1.1 × 10 / C, respectively. Oxide, nitride  Compression
            and diamond, are therefore the only materials that
            can develop compressive extrinsic stresses over silicon     0.1 Pa    1 Pa
            substrates. Aluminium CTE is 23 ppm, which is fairly                Pressure
            high, tungsten CTE is 4 ppm and polymers have CTE  Figure 7.11 Sputtering pressure and film stress. Atomic
            values in the range of 30 to 100 ppm.        masses: Cr 52, Mo 96, Ta 181, Pt 195. Redrawn after
              Intrinsic stresses are caused by many mechanisms that  Ohring, M. (1992), by permission of Academic Press
            are not fully understood. Deposited polycrystalline films
            are not at their energy minimum. An exceptionally low
            deposition temperature means that the arriving atoms do
            not have enough energy to find energetically favourable
            positions, and the film builds up without relaxation.
            Voids and incorporated foreign atoms contribute to
            intrinsic stresses. Bombardment during deposition has
            a pronounced effect on many film properties, including
            stresses, because the bombardment pinches off loosely
            bound atoms, resulting in a more uniform, less stressed
            film. Too high bombardment, on the other hand,        Tensile stress   Compressive stress
                                                                                  (negative)
            implants atoms into the film in a non-equilibrium     (positive)
                                                                    (a)                 (b)
            way, and compressive stresses build up. Crystallization
            and phase transitions, and other processes that lead  Figure 7.12 Thin-film stresses: a film that must be
            to volume changes, such as outgassing, lead to stress  elongated to fit a wafer is under tensile stress (positive) and
            changes.                                     a film that is compressed to fit a wafer, is under compressive
                                                         (negative) stress
              Evaporated metal films are usually under tensile
            stresses. Sputtered films can be under tensile or compres-
            sive stresses. Sputtering, with ion bombardment during
                                                           Stresses in thin films cause wafer curvature, as shown
            deposition, is a much more complex process than evap-
                                                         in Figure 7.12. Imagine a free film attached to a massive
            oration, and stress tailoring can be achieved by:
                                                         wafer and forcefit to the wafer size. Next, imagine,
                                                         stress relaxation through the wafer curvature. A film
            • bias power                                 under tensile stress will result in a concave shape,
            • argon pressure                             while a compressively stressed film will end up with
            • sputtering gas mass                        a convex profile.
            • temperature                                  Figure 7.12 gives a macroscopic depiction of stresses,
            • deposition rate.                           but the same reasoning works on the atomic level as
                                                         well: germanium lattice constant is 4.2% larger than that
            Sputtered film stress can be tailored by the deposition  of silicon, therefore germanium and silicon–germanium
            pressure: films are usually under compressive stress if  films on silicon are compressively stressed, and silicon
            deposited at low pressure (ca. 0.1 Pa in a magnetron  films on SiGe are under tensile stress.
            sputtering system) but turn to tensile stress as the  Stress at room temperature is a sum of intrinsic
            deposition pressure is raised (to ca. 1 Pa) (Figure 7.11).  and extrinsic stresses. Since extrinsic stresses are
            This crossover pressure increases with the atomic mass.  usually tensile (with the exception of oxide, nitride and
            However, this is not a universal solution, because  diamond), and total stresses can be close to zero, this
            pressure affects not only the film stress but also many  means that intrinsic stresses from the deposition process
            other properties such as deposition rate and film density.  are compressive. This is often the case.
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