Page 264 - Book Hosokawa Nanoparticle Technology Handbook
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4.5 STRUCTURE CONTROL OF NANOPARTICLE COLLECTIVES BY SINTERING AND BONDING   FUNDAMENTALS
                                                                 increasing carrier gas flow rate, which increased the
                                                                 deposition efficiency. The deposition efficiency was
                                                                 also strongly affected by properties of the starting
                                                                 particles, such as the average particle size and size
                                                                 distribution, and mechanical and surface properties
                                                                 [6]. The deposition efficiency of the AD method is
                                                                 about 30 times higher than conventional thin-film-
                                                                 formation methods such as sputtering, which have a
                                                                 deposition rate of only about 10 nm/min for an area
                                                                       2
                                                                 of 5 cm . Therefore, the AD method is attractive for
                                                                 manufacturing processes because it permits high
                                                                 throughput.
                                                                  In conventional thin-film and thermal spray-coating
                                                                 methods, surface cleaning before deposition is needed
                                                                 to achieve acceptable adhesion with a substrate. On
                                                                 the other hand, the AD method does not require such
                                                                 pre-cleaning, because during the initial stage of parti-
                                                                 cle impaction with the surface, similar to sand-blasting
                                                                 processes, surface contaminants such as dirt and oils
                  Figure 4.5.28
                  Influence of carry gas to transmittance of PZT layer  are removed by the initial particle collisions.
                  deposited at RT.                               Deposition automatically begins when the surface
                                                                 becomes sufficiently clean. The film adhesion strength
                                                                 to glass and metal substrates was in excess of 20 MPa.
                                                                 However, to realize maximum adhesive strength, suit-
                  Zirconate Titanate  (PZT:Pb(Zr ,Ti )O ) and    able hardness and elasticity of the substrate are
                                                      3
                                               52
                                                   48
                  Ni-Zn-Fe O , but also for non-oxide materials such  needed.
                         3
                            4
                  as AlN and MgB . In either case, particles with diam-  Ceramic film patterning can be achieved by using
                               2
                  eter greater than 80 nm and with single crystal struc-  a mask deposition method, in which a particle jet is
                  ture are needed to make films with acceptable  impacted onto the substrate through a pattern mask
                  hardness.  The crystal grain size of  As-deposited  that contains many openings, each of which is in the
                  films was less than 50 nm, which was smaller than  order of 50 
m. In this case, it is important to con-
                  that of the starting particles. The reason for this is  sider the aerosol jet flow in the deposition chamber
                  apparently that the starting particles break down dur-  and through the mask orifices. If the pressure in the
                  ing collisions and then each particle bonds together  deposition chamber is not sufficiently low, the parti-
                  to form a nanocrystal layer.                   cle jet is scattered by the edge of the openings in the
                    If the carrier gas and pressure in the deposition  mask and the resulting mask pattern is not preserved
                  chamber are properly selected so as to reduce the  on the substrate.
                  electrical discharge during particle deposition, trans-  The effect of ceramic particles sprayed onto a sub-
                  parent PZT and alumina films with transmission effi-  strate change from deposition to erosion [7],
                  ciencies of 60–80% at wavelengths ranging from  depending on the particle diameter, velocity, and
                  450–800 nm could be formed at room temperature  as  angle of incidence of the particle jet to the substrate.
                  shown in Fig. 4.5.28 [5].  The reason this can be  These factors also influence the layer density and
                  achieved is probably because during deposition the  surface roughness.  To achieve acceptable patterns
                  size of the defects in the starting particles is reduced  through a mask with acceptable detail, however, the
                  to crystal sizes that are smaller than those found in  angle of incidence of the particle jet must be kept
                  sintered, bulk materials, and that are also smaller than  within a specified range. This is because the angle of
                  the wavelength of visible light. Although distortions  incidence affects the flow patterns on the down-
                  were included inside the films, a rise of substrate tem-  stream side of the mask, which in turn affects the
                  perature due to particle collisions was not observed,  deposition efficiency and the degree to which the
                  and ceramic powders could be solidified at room tem-  mask profile is distorted. Figure 4.5.29 shows a
                  perature without the use of binders. Although the for-  thick, patterned PZT layer deposited onto Si, SUS,
                  mation of thin films using RTIC does not require  and Pt/Si substrates [8] under optimum deposition
                  sintering, it produces high-density films.     conditions. A ceramic microstructure with a 50-
m
                                                                 line width and aspect ratio greater than 1 can be pat-
                  3. Deposition properties and film patterning   terned by controlling the substrate heating tempera-
                  Deposition of PZT at film-deposition rates of  ture and strating particle properties. The AD method
                                               2
                  10–30 
m/min over an area 5 mm was achieved.   is useful for making piezoelectric films more than
                  The particle velocity and concentration in the  10  
m thick, for applications such as ultrasonic
                  aerosol jet downstream of the nozzle increased with  devices.

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