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FUNDAMENTALS                                           CH. 4 CONTROL OF NANOSTRUCTURE OF MATERIALS
                                                                 [2] A. Inoue, J. Fukuta,  Y. Matano and  Y. Matsumoto:
                                                                    J. Ceram. Soc. Jpn., 100(2), 208–210 (1992).
                                                                 [3] K. Kageyama, M. Enoki,  T. Kishi, K. Ikuina and
                                                                    M. Kimura: J. Jpn. Inst. Metals (in Japanese), 57(7),
                                                                    756–760 (1993).

                                                                 4.5.3 Nanostructure control of a joined interface
                                                                 A joined interface plays an important role to reveal
                                                                 high functionalities of materials including composite
                                                                 materials and electronic devices.
                                                                  It is a very important issue to clarify mechanism of
                                                                 revealing of high functionalities and to control high
                                                                 functionalities at the joined interface. Remarkable pro-
                                                                 gresses of measurement, evaluation, and analytical
                                                                 technology at atomistic level have been performed by
                                                                 progresses of quantum beam technologies such as an
                                                                 electron beam, a laser beam, and a synchrotron radia-
                                                                 tion, a nanoscale analytical technology and a simula-
                  Figure 4.5.13
                  Microstructure of LTCC of the Al O -glass-anorthite system.  tion method by a first principle molecular dynamics.
                                          2
                                           3
                                                                  Economos et al. reported more than 40 years ago
                                                                 that 4 types of joined interfaces between oxides and
                    The existence of an anorthite layer of thickness  metals, which are (1) a new phase is formed at the
                  1–2 
m around the Al O particles, as schematically  interface, (2) a ceramics is chemically attacked by
                                    2
                                      3
                  shown in Fig. 4.5.12, can be confirmed by observation  metal, (3) a metal penetrates along with grain bound-
                  of the microstructure of the sintered material of Al O 3  aries of ceramics and (4) a reaction zone is not
                                                          2
                  particles and glass. Energy dispersive X-ray analysis  observed at the interface, are observed by an optical
                  (EDX) reveals that the white particles, dark gray parts,  microscope [1]. But, progress of analytical and char-
                  and light gray layer around the particles are regarded  acterization technologies of interfaces revealed that
                  as Al O particles, glass, and the anorthite, respec-  joined interfaces cannot be classified into simple cat-
                      2
                        3
                  tively. Presumably the anorthite crystal emerges after  egories and formation of interface is affected by many
                  the reaction of the submicron Al O particles with the  factors such as a joining time, an atmosphere, and a
                                              3
                                            2
                  glass. Subsequently the lack of difference in the reac-  temperature. This has already been suggested by the
                  tive sintering performance within the nanosized region  study of wettability of Al O by liquid Ni [2].
                                                                                     2
                                                                                       3
                  is considered to have a significant influence on the  Many researchers have conducted direct observa-
                  structure of the final board and sintering control in a  tions and simulations of joined interface between
                  further finer region is required in future.    metal and ceramics. Especially, the interface structure
                    As mentioned above, the LTCC of the glass phase  between Nb and Al O have been studied as a model
                                                                                  3
                                                                                2
                  system shows different properties, depending upon the  system, since thermal expansion coefficient of Nb is
                  microstructure of ceramics and glass, like an aggre-  similar to that of Al O .The interface have been sys-
                                                                                   3
                                                                                 2
                  gate or generated crystal, even if the composition is  tematically investigated by using Al O single crystal
                                                                                             2
                                                                                               3
                  the same. To create a dense structure, for which the  which has different crystal orientation and by using
                  sintering in glass liquid phase plays a significant role,  samples made by a solid phase joining, an internal
                  the elucidation of the crystallization mechanism and  oxidation and a molecular beam epitaxial (MBE)
                  the control of the microstructure under a firing condi-  methods [2–4]. It has been revealed that Nb and Al O
                                                                                                         2
                  tion suitable for the electrode materials are needed, as  is directly joined without a formation of reaction layer 3
                  well as the densification. Above all, in order to acquire  and interface structures depend on a crystal orienta-
                  excellent electric properties, the microstructure and  tion of Al O and joining method [5]. An information
                                                                        2
                                                                          3
                  crystal need to be controlled more precisely, which  of bonding status between Nb and Al O has also been
                                                                                              2
                                                                                                3
                  requires technical advancement in the control of pow-  obtained by X-ray photo-emission spectroscopy
                  der properties from submicron to nanosized range and  (XPS) [6, 7]. Electrons in Nb atoms migrate to oxy-
                  the firing process in future.
                                                                 gen atoms that are the components of  Al O . The
                                                                                                      3
                                                                                                    2
                                                                 results obtained by XPS are in good agreement with
                                   References                    simulation result by Yamamoto et al. [8, 9].
                                                                  When joined interfaces between dissimilar materi-
                  [1] Electronic Materials Manufacturers  Association of  als such as metal–ceramics systems are in an epitax-
                     Japan:  Denshikairoyou koukinou seramikku kiban  (in  ial relationship, one of the important factors which
                     Japanese, Advanced Ceramic Board for Electric  affect interface characteristics is a lattice mismatch-
                     Circuit), Japan Industrial Publishing Co., Ltd., (1994).  ing. An interface structure is considerably affected by
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