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Correlation between subgrains and coherently scattering domains

Published online by Cambridge University Press:  01 March 2012

T. Ungár ,
G. Tichy ,
J. Gubicza  and
R. J. Hellmig
T. Ungár*
Affiliation:
Department of General Physics, Eötvös University, Pázmány Péter sétány 1A, Budapest H-1518 POB 32, Hungary
G. Tichy
Affiliation:
Department of Solid State Physics, Eötvös University, Pázmány Péter sétány 1A, Budapest H-1518 POB 32, Hungary
J. Gubicza
Affiliation:
Department of Solid State Physics, Eötvös University, Pázmány Péter sétány 1A, Budapest H-1518 POB 32, Hungary
R. J. Hellmig
Affiliation:
Institut für Werkstoffkunde und Werkstofftechnik, TU Clausthal, Agricolastr, 6, 38678 Clausthal-Zellerfeld, Germany
*
a)Electronic mail: [email protected]
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Abstract

Crystallite size determined by X-ray line profile analysis is often smaller than the grain or subgrain size obtained by transmission electron microscopy, especially when the material has been produced by plastic deformation. It is shown that besides differences in orientation between grains or subgrains, dipolar dislocation walls without differences in orientation also break down coherency of X-rays scattering. This means that the coherently scattering domain size provided by X-ray line profile analysis provides subgrain or cell size bounded by dislocation boundaries or dipolar walls.

Keywords

X-ray line profile analysistransmission electron microscopy (TEM)crystallite sizesubgrainsdipolar dislocation walls
Type
Invited Articles
Information
Powder Diffraction , Volume 20 , Issue 4 , December 2005 , pp. 366 - 375
Copyright
Copyright © Cambridge University Press 2005

INTRODUCTION

According to the kinematical theory of powder diffraction if the crystallites (coherently scattering domains) are strain-free and the average crystallite size is larger than a few microns, however, not much larger than about 10 μm, the physical line profiles of the diffraction peaks are delta functions (Warren, Reference Warren1990). In a polycrystalline structural material or in a realistic powder specimen several deviations from the ideal state can be present: (1) internal stresses, (2) stacking faults, (3) twinning, (4) crystallite smallness, (5) microstresses, (6) long-range internal stresses, (7) chemical heterogeneities, (8) anisotropic crystallite shape, or (9) anisotropic strain, etc. All these features and often their combinations comprise the microstructure of an investigated specimen. The presence of different microstructural features is manifested by different specific distortions of the ideal powder diffraction pattern. (i) Peak shift is related to internal stresses or planar faults, especially stacking faults or twinning. (ii) Peak broadening indicates crystallite smallness and microstresses, however, stress gradients and∕or chemical heterogeneities can also cause peak broadening. (iii) Peak asymmetries can be caused by long-range internal stresses (in particular gradients), planar faults or chemical heterogeneities. (iv) Anisotropic peak broadening can result from anisotropic crystallite shape or anisotropic strain. Here the anisotropic broadening means that the peak breadth is a nonmonotonous function of the momentum of the diffraction vector. There is no one-to-one correlation between the different peak profile features and the different microstructural properties. The interpretation of shape of peak profiles in terms of microstructural properties becomes more reliable if the results of other methods, e.g., transmission or scanning electron microscopy (TEM or SEM), are also used. On the other hand, the results of other methods, especially TEM or SEM, can be refined and∕or amended by using X-ray line profile analysis (XLPA).

The different microstructural properties from (1) to (9) can be treated on a well-established physical basis. Internal stresses are described by the elastic properties of crystals (Macherauch, Reference Macherauch1980; Noyan and Cohen, Reference Noyan and Cohen1987). Methods for the determination of probabilities of stacking faults and twinning from diffraction profiles have been elaborated for cubic and hexagonal crystals by Warren (Reference Cheary, Dooryhee, Lynch, Armstrong and Dligatch1990), Treacy et al. (Reference Treacy, Newsam and Deem1991), Scardi and Leoni (Reference Scardi and Leoni1999), Boulle et al. (Reference Boulle, Legrand, Guinebretière, Mercurio and Dauger2001), Estevez-Rams et al. (Reference Estevez-Rams, Leoni, Scardi, Aragon-Fernandez and Fuess2003), and Ustinov et al. (Reference Ustinov, Olikhovska, Budarina, Bernard, Mittemeijer and Scardi2004). Size broadening has been treated for spherical or nonspherical crystallites (Le Bail and Louër, Reference Le Bail and Louër1978; Louër et al., Reference Louër, Auffrédic, Langford, Ciosmak and Niepce1983; Langford et al., Reference Langford, Boultif, Auffrédic and Louër1993; van Berkum et al., Reference van Berkum, Vermuelen, Delhez, de Keijser and Mittemeijer1994; Langford et al., Reference Langford, Louër and Scardi2000; Leoni and Scardi, Reference Leoni and Scardi2004; Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001; Audebrand et al., Reference Audebrand, Raite and Louër2003; Ida et al., Reference Ida, Shimazaki, Hibino and Toraya2003). The evaluation of microstresses has been worked out in detail for dislocations (Krivoglaz, Reference Krivoglaz1996; Wilkens, Reference Wilkens1970; Gaál, Reference Gaál and Andersen1984; Groma et al., Reference Groma, Ungár and Wilkens1988, Ungár and Borbély, Reference Ungár and Borbély1996; Levine and Thomson, Reference Levine and Thomson1997; Groma, Reference Groma1998). Long-range internal stresses were related to the dipole polarization of dislocations (Mughrabi, Reference Mughrabi1983; Mughrabi et al., Reference Mughrabi, Ungár, Kienle and Wilkens1986, Groma et al., Reference Groma, Ungár and Wilkens1988). Anisotropic crystallite shape has been treated by Louër et al. (Reference Louër, Auffrédic, Langford, Ciosmak and Niepce1983) in the case of ZnO nanoparticles. Anisotropic peak broadening caused by strain is a general phenomenon which is closely related to the elastic properties of crystals and∕or the anisotropic strain field of dislocations (Ungár and Borbély, Reference Ungár and Borbély1996; Ungár and Tichy, Reference Ungár and Tichy1999; Scardi and Leoni, Reference Scardi and Leoni1999; Dinnebier et al., Reference Dinnebier, Von Dreele, Stephens, Jelonek and Sieler1999, Stephens, Reference Treacy, Newsam and Deem1999; Cheary et al., Reference Cheary, Dooryhee, Lynch, Armstrong and Dligatch2000).

One of the most frequent applications of XLPA is the determination of size or size distribution of crystallites. According to the theorem of Bertaut (Reference Bertaut1950) the profile of a size broadened peak can be obtained as the sum of the intensities diffracted by parallel and independent columns which build up the diffracting crystallites and aligned normal to the reflecting planes with unit cross-sectional area. The diffraction peak corresponding to one particular column is the squared Fourier transform of the form function pertaining to that column length. The final size-broadened peak is the volume-weighted sum of the individual peaks corresponding to the individual columns. The direct meaning of a size broadened peak is thus related to the (area and∕or volume) weighted column-length distribution in the specimen. The column-length distribution in the specimen depends on the size, the shape, and the size distribution of the crystallites. In order to obtain the (area and∕or volume weighted) mean size of crystallites or their distributions, specific assumptions have to be made about the shape and the size distribution of these objects (Langford and Louër, Reference Langford and Louër1996).

There is ample experimental evidence that the log-normal size distribution function, f(x), given by the median m and the variance σ, can describe crystallite size distribution in a wide range of bulk or loose powder materials (Valiev et al., Reference Valiev, Kozlov, Ivanov, Lian, Nazarov and Baudelet1994; Terwilliger and Chiang, Reference Terwilliger and Chiang1995; Krill and Birringer, Reference Krill and Birringer1998; Ungár et al., Reference Ungár, Borbély, Goren-Muginstein, Berger and Rosen1999; Langford et al., Reference Langford, Louër and Scardi2000; Scardi and Leoni, Reference Scardi and Leoni2002). Hinds (Reference Hinds1982) has shown that with m and σ the arithmetic-, the area-, and the volume-weighted mean crystallite diameters are

where k=0.5, 2.5, and 3.5 in the case of arithmetic-, area-, and volume-weighted mean and j stands for these different averages, respectively.

Crystallite size, grain size, or particle size are microstructural features which can be determined and even visualized by electron microscopy methods, e.g., TEM or SEM, and can also be determined by other methods, e.g., specific surface area measurement by Brunauer-Emmet-Teller (BET) procedure. In the present paper, size values provided by these methods are discussed in terms of the size values given by XLPA. It will be shown that when strain is caused either by dislocations or by other defects producing inhomogeneous strain, e.g., contact stresses between adjacent particles or triple junctions between three grain boundaries, crystallographic misorientation between the adjacent objects is not a prerequisite for breaking down coherency. Especially, in the case of dipolar dislocation walls it will be shown that, though the adjacent regions follow exactly the same crystallographic orientation, coherency is lost in most crystallographic directions.

THE CORRELATION BETWEEN CRYSTALLITE SIZE OR SIZE-DISTRIBUTIONS AS DETERMINED EITHER BY X-RAY LINE PROFILE ANALYSIS (XLPA) OR BY TRANSMISSION ELECTRON MICROSCOPY (TEM)

In the following some representative experimental results are reviewed where crystallite size has been determined by both the methods of XLPA and electron microscopy. These results are discussed within the two categories: (1) when X-ray and TEM sizes are in good agreement, and (2) when X-ray and TEM sizes show discrepancies.

When X-ray and TEM sizes are in good agreement

It has been shown in numerous papers that in nanostructured ceramic powders the crystallite size and the grain size values determined by XLPA and TEM, respectively, agree well within the experimental error (Louër et al., Reference Louër, Auffrédic, Langford, Ciosmak and Niepce1983; Langford et al., Reference Langford, Boultif, Auffrédic and Louër1993; Langford et al., Reference Langford, Louër and Scardi2000; Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Ribárik and Ungár2000a). For example Louër and co-workers have prepared loose powder of ZnO by the thermal decomposition of zinc-hydroxinitrate, Zn3(OH)4(NO3)2 (Louër et al., Reference Louër, Auffrédic, Langford, Ciosmak and Niepce1983). In order to avoid secondary growth after the first decomposition from the precursors the ambient conditions were carefully controlled. The TEM image obtained on ZnO powder shows well-defined cylindrical nanoparticles with aspect ratios of about 3. The Williamson-Hall plot of the full width at half maximum (FWHM) of the diffraction profiles revealed a strong anisotropy with the indices of reflections h k l, however, with clear indication for the absence of strain, e.g., FWHM values of the 002∕004 and 100∕300 pairs of reflections are identical within the experimental error in the reciprocal lattice scale. Based on this behaviour of the Williamson-Hall plot, authors evaluated the shape anisotropy in terms of a cylindrical particle model. The average cylinder diameter and height was obtained as 8 and 20 nm, respectively, in excellent agreement with the TEM results.

Langford and co-workers have studied the effect of size distribution on X-ray powder diffraction peak profiles (Langford et al., Reference Langford, Louër and Scardi2000). Nanocrystalline powder specimens of CeO2 were prepared from the decomposition of an oxide-nitrate, Ce2O(NO3)6.H2O, under N2 atmosphere with a heating rate of 3 K∕h up to 503 K. The specimen was additionally annealed for 24 h at the same temperature. The high resolution TEM (HREM) micrograph (see Figure 3, in Langford et al., Reference Langford, Louër and Scardi2000) has shown crystallites of the diameter of about 4 nm. Assuming log-normal size distribution the diffraction patterns were fitted by a Rietveld type whole powder pattern fitting procedure. The size distribution provided by the fitting procedure is in perfect agreement with the bar diagram obtained by evaluating the TEM micrographs (Langford et al., Reference Langford, Louër and Scardi2000; Scardi et al., Reference Scardi, Leoni and Delhez2004; Balzar et al., Reference Balzar, Audebrand, Daymond, Fitch, Hewat, Langford, Le Bail, Louër, Masson, McCowan, Popa, Stephens and Toby2004).

The crystallite size distribution in nanocrystalline silicon nitride ceramic loose powders has also been investigated by XLPA methods (Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Ribárik and Ungár2000a; Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Zsoldos and Ungár2000b). Two methods were used to produce Si3N4 powders. One of the two procedures was the gas-phase synthesis of silicon-tetrachloride and ammonia in thermal plasma reactor (Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Zsoldos and Ungár2000b). The majority (80 vol %) of the as-synthesized powder was amorphous. This powder was crystallized at 1500 °C for 2 h. After the crystallization heat-treatment an amorphous fraction of about 20% is still retained. Another powder was formed by nitridation of silicon and subsequent milling. The latter specimen was fully crystalline. Both powders were studied by XLPA and TEM. A TEM image for the powder crystallized at 1500 °C is shown in Figure 1. The grain size distribution obtained by TEM and the crystallite size distribution determined by XLPA are compared in Figure 2. The X-ray line profiles were evaluated by the Multiple Whole Profile (MWP) fitting method (Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001). A large number of TEM micrographs were evaluated for grain size. About 300 grains were chosen at random in different areas in different micrographs.

Figure 1. TEM micrograph of silicon nitride ceramic powder synthesized in thermal plasma and crystallized at 1500 °C.

The frequency of the measured diameters is shown in Figure 2 as bar graphs. The solid line in the figure is the size distribution function obtained by XLPA. The agreement between the size distributions obtained by TEM and X-rays is relatively good. The difference between the two distributions can be attributed to the smallest amorphous grains in the powder specimen (Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Zsoldos and Ungár2000b). Another reason is that the number of grains sampled in the present X-ray diffraction experiments is many orders of magnitude larger than the number evaluated in the TEM experiments. Similar comparison of the crystallite size distributions has been made for the nanodisperse Si3N4 powder formed by nitridation of silicon and subsequent milling. For this fully crystalline sample the agreement between the X-ray and TEM size distributions was better than for the powder obtained by thermal plasma synthesis. The area weighted mean crystallite size obtained from XLPA was compared with that calculated from the specific surface area determined by Brunauer-Emmett-Teller (BET) method (Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Ribárik and Ungár2000a). For both powders the area weighted mean size obtained from XLPA (93 and 62 nm for the plasma and nitridized powders, respectively) were in good agreement with those determined by BET method (94 and 71 nm for the plasma and nitrided powders, respectively, assuming spherical particles).

The relatively good correlation between the crystallite size determined by XLPA and the grain size obtained by TEM has also been shown for not only ceramic powders but also nanostructured metallic materials formed by electrodeposition, inert-gas condensation, or crystallization from amorphous precursors. For electrodeposited nanocrystalline Ni foils produced by pulse plating onto titanium substrate,

Figure 2. The grain size distribution obtained by TEM (bar diagram), and the crystallite size distribution determined by XLPA (solid line) (the vertical line is an estimated error bar).

XLPA provided ✩x✪area=12 nm and ✩x✪vol=38 nm for the area- and volume-weighted mean crystallite diameters, respectively (Tóth-Kádár et al., Reference Tóth-Kádár, Bakonyi, Sólyom, Hering, Konczos and Pavlyák1987; Bakonyi et al., Reference Bakonyi, Tóth-Kádár, Pogány, Cziráki, Geröcs, Varga-Josepovits, Arnold and Wetzig1996). Although the TEM micrograph obtained on the same specimen has not been evaluated quantitatively for crystallite or grain size, a good qualitative correlation between the X-ray and TEM results can be observed (Tóth-Kádár et al., Reference Tóth-Kádár, Bakonyi, Sólyom, Hering, Konczos and Pavlyák1987; Bakonyi et al., Reference Bakonyi, Tóth-Kádár, Pogány, Cziráki, Geröcs, Varga-Josepovits, Arnold and Wetzig1996). Similar agreement was found for electrodeposited Ni produced by Zhilyaev and co-workers (Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003). For this sample ✩x✪area=24 nm and ✩x✪vol=45 nm from XLPA while TEM experiments result in 35 nm as the area weighted mean grain size.

Nanocrystalline Pd pallets were prepared by inert-gas condensation and subsequent compaction (Krill and Birringer, Reference Krill and Birringer1998). Dark field TEM micrographs were evaluated quantitatively. The 111∕222 pair of X-ray diffraction peaks were evaluated by the classical Warren-Averbach method. From the area- and the volume-weighted mean crystallite size values the size distribution function has been determined. A good correlation between the bar-diagram obtained from the TEM micrographs and the size-distribution function provided by XLPA was observed. Similar good correlation was found between the TEM and X-ray size distribution functions for nanocrystalline Cu prepared by inert-gas condensation and subsequent hot compaction at Argonne National Laboratory (Sanders et al., Reference Sanders, Fougere, Thompson, Eastman and Weertman1997).

Nanocrystalline Ni5Hf particles were produced by careful crystallization from an amorphous precursor (Gubicza et al., Reference Gubicza, Ribárik, Bakonyi and Ungár2001). The amorphous ribbons of 3 mm width and 11 μm thickness were produced from a master alloy of Hf11Ni89 melted and fast quenched by the melt-spinning technique. The measured values of the median and variance obtained from XLPA are: m=3.3 nm and σ=0.82. The arithmetic-, the area-, and the volume-weighted mean crystallite size values calculated from m and σ are 5, 17, and 35 nm, respectively. They indicate a wide size distribution in good correlation with TEM observations. From the TEM micrograph the area weighted mean grain size has been determined to be about 10 nm in relatively good correlation with XLPA results.

When X-ray and TEM sizes show discrepancies

It is a general observation that in plastically deformed bulk metals the grain size determined by TEM is much higher than the crystallite size obtained by XLPA. In the following several examples of this phenomena are discussed.

The microstructure of a ferritic∕martensitic steel from the European Fusion Materials Technology Programme (EFMTP) was investigated by TEM by Marmy and co-workers (Marmy et al., Reference Marmy, Yuzhen and Victoria1991). It was found that the strength of the tempered martensite is caused by the carbide precipitates and by the lath structure which is strengthened by a high density of dislocations. After tensile deformation or low cycle fatigue a well-developed dislocation cell structure is formed leaving a small amount of the original dislocation density in the martensite. The TEM micrographs revealed strongly elongated laths of the ferritic∕martensitic material in which the laths are subdivided by dislocation cell walls. The dislocation densities and the mean crystallite diameters were determined for the normal state and after fatigue at room

Figure 3. TEM micrograph of a grain containing dislocation cells in ultrafine grained titanium formed by ECAP.

temperature and 250 °C by XLPA (Marmy et al., Reference Marmy, Yuzhen and Victoria1991). It is found that while the dislocation density increases during fatigue, especially at 250 °C, the mean crystallite size also increases considerably. This indicates that during fatigue, especially at higher temperatures, the dislocation density in the cell walls increases strongly, while simultaneously the dislocation cell size or the subgrain size increases too. The two parameters, i.e., the dislocation density and the area-weighted mean crystallite size, show similar tendency either determined from TEM micrographs or obtained by XLPA, but the grain size determined by TEM was much higher than the area-weighted crystallite size calculated from the X-ray line profiles.

Severe plastic deformation (SPD) methods are effective tools for producing bulk ultrafine grained metals. The two most frequently used SPD procedures are equal channel angular pressing (ECAP) and high pressure torsion (HPT). It has been shown for bulk ultrafine grained Al, Al-3%Mg, and Ni produced by SPD techniques that the grain size determined by TEM is about four to six times higher than the crystallite size obtained by XLPA (Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003; Gubicza et al., Reference Gubicza, Chinh, Horita and Langdon2004). When the strain has been increased by the combination of the different deformation procedures (ECAP, HPT, and cold rolling), the ratio of the two sizes was decreased down to about two to three. TEM investigations indicate that the grains in SPD materials are divided into subgrains and∕or dislocation cells which are separated from each other by low angle grain boundaries. The crystallite size in SPD metals obtained by X-ray diffraction is equivalent to the mean size of domains which scatter X-rays coherently. Consequently, X-ray diffraction makes a difference between the dislocation cells which are separated from each other by small differences in orientation, typically under 1°–2°. The usual TEM investigation (usually performed by visual observation) of SPD metals gives the size of the grains having high angle grain boundaries. As a consequence, the TEM grain size is higher than the dislocation cell size obtained by XLPA. When the different SPD methods are applied after each other to increase the applied strain, the differences in orientation between the dislocation cells or subgrains increase, and the ratio of the TEM grain size and coherently scattering domain size decreases.

Submicron grain-size titanium was produced by ECAP and subsequent cold rolling (Zhu et al., Reference Zhu, Huang, Gubicza, Ungár, Wang, Ma and Valiev2003). A detailed TEM study shows that the microstructure is inhomogeneous and shows a hierarchy, i.e., the grains contain subgrains which are further divided into dislocation cells. For example the large grains in Figure 3 consist of dislocation cells. The

Figure 4. The statistical size ranges of different structural features in ECAP processed titanium.

distribution of grain sizes is broad from less than 100 nm to over 600 nm. The structure of grains is dependent on their size but the size ranges of grains with different structures are overlapped. Figure 4 shows the statistical size ranges of different structural features. Grains containing subgrains are usually larger than 320 nm. Grains having dislocation cell structure without the intermediate subgrains are in the size range of 130–600 nm. Grains which have no dislocation cells are smaller than 150 nm. The dislocation cells are in the size range of 30–70 nm and the average cell size is 45 nm. The average grain size observed in TEM is much larger, about 270 nm (Zhu et al., Reference Zhu, Huang, Gubicza, Ungár, Wang, Ma and Valiev2003). The XLPA results in the area-weighted mean crystallite size of 41 nm which is several times smaller than the grain size obtained by TEM but it is in a relatively good correlation with the TEM cell size (see Figure 4).

A 99.98% copper specimen was extruded and subsequently deformed by ECAP in a single pass (Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001; Ribárik et al., Reference Ribárik, Ungár and Gubicza2001). TEM micrographs obtained on this specimen were evaluated in two steps. In a first step the well-defined, large angle grain boundaries were drawn into a contour map. This procedure was carried out on about ten similar micrographs. The linear intersection method was used to produce the bar graph of the distribution of crystallite diameters. It was established that the TEM size distribution gives much larger size values than the X-ray method. The median of the size distribution determined by XLPA was about 60 nm while that of the grains observed by TEM was about two to three times higher. In a second step typical grains in good contrast orientation were selected and finer contour maps were produced which corresponds to the dislocation cell structure. These contour maps were also evaluated by the linear intersection method and this size distribution was close to that determined from X-rays (Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001). This indicates that in a plastically deformed bulk metallic specimen the crystallite size and size distribution obtained by the X-ray method are close or almost equal to the dislocation cell size or size distribution.

The above-mentioned examples show that in the case of loose ceramic powders and metallic materials produced by inert-gas condensation or electrodeposition, as long as the grain diameter is within the sensitivity range of X-ray diffraction peak broadening, i.e., smaller than about 1 μm, TEM or HREM grain sizes are in good agreement with size and size-distribution results provided by XLPA. The grain size of SPD materials determined by TEM is generally several times higher than the crystallite size (or coherently scattering

Figure 5. The grain size determined by TEM (d TEM) vs the area-weighted mean crystallite size obtained from XLPA (✩x✪area) for plastically deformed metals and for metallic materials produced by inert-gas condensation or electrodeposition (a). The small grain size region of (a) is replotted in (b) where the different materials are indicated by different symbols: open square—Cu deformed by ECAP (Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001); closed circle—Ti processed by ECAP (Zhu et al., Reference Zhu, Huang, Gubicza, Ungár, Wang, Ma and Valiev2003); cross—Al-3%Mg formed by ECAP (Gubicza et al., Reference Gubicza, Chinh, Horita and Langdon2004); open circle—Ni specimens obtained by different SPD methods (Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003); open triangle—Cu formed by inert-gas condensation (Sanders et al., Reference Sanders, Fougere, Thompson, Eastman and Weertman1997); closed square—electrodeposited Ni (Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003).

domain size) obtained by XLPA. This is illustrated in Figure 5a where the TEM grain size is plotted versus the crystallite size determined by XLPA for metallic materials. The figure shows that for metals produced by electrodeposition or inert-gas condensation the two sizes are in good agreement while for metallic specimens formed by SPD the grain size is higher than the crystallite size. For better visibility, the small grain size region of Figure 5a is replotted in Figure 5b where the different materials are indicated by different symbols.

The reason for the difference between the TEM and XLPA sizes for SPD metals originates from the hierarchy of the microstructure. During SPD process the basic mechanisms of the grain refinement are the multiplication of dislocations and the subsequent arrangement into cell boundaries to minimise their strain energy. The dislocation cells have low-angle grain boundaries. As the deformation proceeds the dislocation density in the cell boundaries increases (even up to 1017–1018 m−2), the thickness of the boundaries decreases, and the difference in orientation between the neighboring cells also increase, i.e., the cell boundaries are transformed into high-angle grain boundaries. At a certain strain the microstructure contains low-angle cell boundaries [or incidental dislocation boundaries (IDBs)] and high-angle grain boundaries [geometrically necessary boundaries (GNBs)] simultaneously (Hughes and Hansen, Reference Hughes and Hansen2000). The grains confined by high-angle boundaries are subdivided into subgrains and∕or

Figure 6. The ratio of the grain size determined by TEM and the crystallite size obtained by XLPA vs the dislocation density: open square—Cu formed by inert-gas condensation (Sanders et al., Reference Sanders, Fougere, Thompson, Eastman and Weertman1997); open circle—Cu deformed by ECAP (Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001); open triangle—Ni specimens obtained by different SPD methods (Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003); closed inverted triangle—Ti processed by ECAP (Zhu et al., Reference Zhu, Huang, Gubicza, Ungár, Wang, Ma and Valiev2003); cross—pure Al and Al-3%Mg formed by ECAP (Gubicza et al., Reference Gubicza, Chinh, Horita and Langdon2004); closed square—electrodeposited Ni (Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003).

cells. The differences in orientation between cells is low (1°–2°) therefore there is no measurable contrast difference between them in TEM micrographs, i.e., they can be observed separately only by high-resolution TEM investigations. At the same time there is no coherency between the X-rays scattered from the different cells, therefore X-ray line profile analysis measures the size of these objects. As the strain increases the dislocation density also increases and the low-angle cell boundaries transformed to high-angle boundaries. Consequently, the TEM and XLPA sizes converge with increasing dislocation density as Figure 6 shows for different metals. In this figure the specimens formed by inert-gas condensation or electrodeposition are also plotted. The ratio of the two sizes corresponding to these samples is close to 1. Although in the case of SPD metals the lower crystallite size is associated with the higher dislocation density, there is no strict correlation between the two quantities obtained by XLPA as shown in Figure 7. The relationship between the dislocation density and the mean crystallite size can be described by power law with different exponents (n) depending on the type of materials (see Figure 7).

In the following section it is demonstrated that during SPD processes a special dislocation structure can develop which does not cause any differences in orientation but it

Figure 7. The dislocation density vs the area-weighted mean crystallite size for different series of plastically deformed materials: open circle—ball milled PbS (Ungár et al., Reference Ungár, Martinetto, Ribárik, Dooryhee, Walter and Anne2002); open square—Cu, Ti, Ni, and Al-3%Mg processed by SPD methods (Ungár et al., Reference Ungár, Gubicza, Ribárik and Borbély2001; Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003; Zhu et al., Reference Zhu, Huang, Gubicza, Ungár, Wang, Ma and Valiev2003; Gubicza et al., Reference Gubicza, Chinh, Horita and Langdon2004); cross—ball milled Al (Révész et al., Reference Révész, Lendvai and Ungár2000).

results in disappearance of the coherency between the different domains of grains. As a consequence, the smallest object size measured by careful TEM investigations is still much higher than the coherently scattering domain size determined by XLPA.

THE EFFECT OF DIPOLAR DISLOCATION WALLS ON COHERENT SCATTERING

Dipolar dislocation walls are one of the most common dislocation configurations in plastically deformed crystalline materials (Kuhlmann-Wilsdorf, Reference Kuhlmann-Wilsdorf, Nabarro and Duesbery2002). They do not cause tilt or twist between the two delineated regions (Wilkens et al., Reference Wilkens, Ungár and Mughrabi1987) therefore, it is not trivial whether they break down coherent scattering.

In materials, where deformation proceeds by wavy-glide, TEM observations have shown that dislocations form a cell structure (Mughrabi, Reference Mughrabi1983). At first, thick and woolly cell walls of high dislocation density surround cell-interior regions with considerably lower dislocation densities. At later stages of deformation cell blocks appear which comprise many dislocation cells being separated by differences in orientation of tilt or twist. With further deformation the cell blocks shrink, the cell walls become thin and often form lamellar structures separated by marked differences in orientation (Gil-Sevillano and Aernoudt, Reference Gil Sevillano and Aernoudt1987; Hughes and Nix, Reference Hughes and Nix1989; Hughes and Hansen, Reference Hughes and Hansen1993; Kuhlmann-Wilsdorf, Reference Kuhlmann-Wilsdorf, Nabarro and Duesbery2002). Within the lamellae, however, almost no, or just slightly different orientations between the adjacent subgrains can be observed. A typical TEM micrograph of a copper specimen deformed by a single pass of ECAP at room temperature using a 90° die is shown in Figure 8a (Hellmig et al., Reference Hellmig, Baik, Bowen, Estrin, Juul Jensen, Kim, Seo, Zehetbauer and Valiev2004). The differences in orientation between adjacent regions have been evaluated quantitatively by TEM investigations. A schematic representation of the measured differences in orientation is shown in Figure 8b. The black lines correspond to large differences in orientation ranging up to 25° [see Figure 3(b) in Hellmig et al., Reference Hellmig, Baik, Bowen, Estrin, Juul Jensen, Kim, Seo, Zehetbauer and Valiev2004]. The gray lines correspond to slightly different orientations ranging from 0.2 to about 8° [see Figure 3(a) in Hellmig et al., Reference Hellmig, Baik, Bowen, Estrin, Juul Jensen, Kim, Seo, Zehetbauer and Valiev2004]. The boundaries corresponding to large and slightly different orientations are called geometrically necessary boundaries (GNBs) and incidental dislocation boundaries (IDBs), respectively (Hellmig et al., Reference Hellmig, Baik, Bowen, Estrin, Juul Jensen, Kim, Seo, Zehetbauer and Valiev2004). The size of subgrains with large and slightly different orientations is about 400 or 200 nm, respectively. The X-ray line profile analysis carried out by the MWP method gives about 70 nm for the area-weighted mean crystallite size. This shows that the TEM subgrain size is still much larger than the crystallite size obtained by XLPA, even if the objects with small differences in orientation are taken into account. In the following it is shown that dipolar dislocation walls break down coherent scattering despite there being no difference in orientation between the delineated regions. Since dipolar dislocation walls with almost or perfectly zero differences in orientation are a general feature of plastically deformed materials (Kuhlmann-Wilsdorf, Reference Kuhlmann-Wilsdorf, Nabarro and Duesbery2002), the discrepancy between crystallite size determined by XLPA and TEM is attempted to be explained by the presence of these dipolar dislocation walls.

A schematic dipolar dislocation wall is shown in Figure 9a. For the sake of simplicity, however, not violating generality,

Figure 8. TEM micrograph of a copper specimen deformed by a single pass of ECAP (a). The schematic representation of the measured differences in orientation in (a) is shown in (b). The black lines correspond to large differences in orientation ranging up to 25° while the grey lines correspond to almost zero or small differences in orientation ranging from 0.2° to about 8°.

edge dislocations are considered with the Burgers vectors parallel to the x direction and y perpendicular to the dipolar wall. The dislocation dipoles are arranged periodically with the period s, and are characterised by the two parameters η and δ [see also in Figure 9a]. Denoting the displacement field of a single dislocation by u̱D(x,y), the total displacement field of the dipolar wall is

where n is an integer and s is the periodicity of the dislocations. At y=±∞ the two lattices on the two sides of the dipolar wall are shifted with respect to each other by ṯ in the x direction:

Obviously, ṯ is independent either of η or of x. It can be seen that if δ=0, then ṯ=0. Let u̱D(x,y) be divided into the topological part, u̱T(x,y), and the rest: u̱P(x,y), where

where ḇ is the Burgers vector of the dislocations in the dipolar wall. u̱P(x,y) contains the logarithmic part of the displacement field and is an even function of both x and y.

Figure 9. A schematic dipolar dislocation wall (a). The dislocations are arranged periodically with the period s, and the width and the thickness of the dipoles is η and δ, respectively. The shift, ṯ, of the two lattice halves on the two sides of the dipolar wall is shown in (b). A schematic representation of the structure of a grain interior is shown in (c). The randomly hatched regions are for the subgrain boundaries, in the present case they are assumed to be dipolar dislocation walls. The thick dashed lines represent the large angle grain boundaries. D and d are the grain-and subgrain size, respectively. The lattice-shift relative to the adjacent subgrain lattice in the ith subgrain is ṯi.

Since the limes of u̱(x,y) is singular at y infinity, the derivatives are investigated:

where

Since u̱P is an even function, only u̱T will contribute to ∂ u̱∕∂ δ:

and

Based on Poisson’s rule the summation in Eq. 8. can be replaced by the integral:

where the z=x‐n s‐δ replacement has been used. The integral is equal to π/2 sign(y), thus

The shift, ṯ, of the two lattice halves on the two sides of the dipolar wall is ṯ=(ḇ∕s)δ and is shown schematically in Figure 9b. Due to lattice periodicity, the maximum value of ṯ isṯ max=±ḇ∕2.

Now the scattering of subgrains is calculated where the subgrain boundaries are dipolar dislocation walls and the subgrains are embedded in a grain bordered by large angle grain boundaries, as shown schematically in Figure 9c. The randomly hatched regions are for the subgrain boundaries; in the present case they are assumed to be dipolar dislocation walls. The thick dashed lines represent the large angle grain boundaries. D and d are the grain and subgrain size, respectively. The lattice shift relative to the adjacent subgrain lattice in the ith subgrain is ṯi. Denote the structure factor of the ith subgrain by S i, then the size broadened line profile of the whole grain is

where g̱ is the diffraction vector and only the shape of the line profile is considered. The double sum can be written as

Since ṯi are random, the second term on the right-hand side becomes negligible, and

Equation 13. means that the subgrains scatter out of phase, therefore their intensities add up. In other words, the line profile of the whole grain will be the sum of the line profiles of the subgrains. As a result, size broadening will be determined by the size broadening corresponding to the subgrains, instead of corresponding to the grains. The physical meaning of Eqs. 12 d13. can also be interpreted as follows: size broadening will be determined by the average subgrain-size since the scattering of each subgrain is shifted by a random phase-factor.

The determination of subgrain size or subgrain size-distribution from TEM micrographs is probably an almost impossible task, especially when the dislocation density is high and the subgrain size small. The difficulties encountered when attempting this aim are illustrated by the micrograph and the corresponding schematic line-graph of Figures 3(a) and 3(b) in Hellmig et al. (Reference Hellmig, Baik, Bowen, Estrin, Juul Jensen, Kim, Seo, Zehetbauer and Valiev2004) and shown here as Figures 8a and 8b, respectively. The careful investigation of the

Figure 10. The schematic picture of subgrain or cell structure where dislocations constitute the boundaries of subgrains or cells with slightly different orientations. The figure is similar in its meaning to the schematic illustration in Figure 15.6 of Bolmaro et al. (Reference Bolmaro, Brokmeier, Signorelli, Fourtz, Bertinetti, Mittemeijer and Scardi2004).

micrograph in Figure 8a shows several details which are not indicated in the corresponding schematic line-graph in Figure 8b. It is quite evident that a quantitative evaluation of a TEM micrograph for the sake of determining subgrain size distribution becomes rather subjective, especially when the finer details are attempted to be obtained. The X-ray method might be considered as somewhat more objective, at least for the determination of subgrain∕cell size and size-distribution.

DISCUSSION AND CONCLUSIONS

The scrutiny of the correlation between crystallite size determination either by XLPA or by TEM has shown that the X-ray size is usually either equal to or smaller than the TEM size. In those cases when the crystallites or particles are delineated by well-defined boundaries, as in the case of metallic samples produced by the method of inert gas condensation (Sanders et al., Reference Sanders, Fougere, Thompson, Eastman and Weertman1997), or in the case of loose particles of ceramic materials (Louër et al., Reference Louër, Auffrédic, Langford, Ciosmak and Niepce1983; Gubicza et al., Reference Gubicza, Szépvölgyi, Mohai, Ribárik and Ungár2000a; Scardi and Leoni, Reference Scardi and Leoni2002), the X-ray and TEM data are in good correlation. In the case of bulk ultrafine grained materials formed by SPD methods, however, the X-ray size values are usually smaller than the TEM data, cf. Zhilyaev et al., Reference Zhilyaev, Gubicza, Nurislamova, Révész, Suriñach, Baró and Ungár2003; Gubicza et al., Reference Gubicza, Chinh, Horita and Langdon2004; Zehetbauer et al., Reference Zehetbauer, Kohout, Schafler, Sachslehner and Dubravina2004. The arrangement of dislocations into small-angle grain boundaries provides a simple and straightforward model for subgrain∕cell structure where the TEM grain size is obviously larger than the X-ray subgrain∕cell size, as shown schematically in Figure 15.6 of Bolmaro et al. (Reference Bolmaro, Brokmeier, Signorelli, Fourtz, Bertinetti, Mittemeijer and Scardi2004) and in Figure 10 here. The thorough and systematic measurements of differences in orientation between adjacent subgrains in an ECAP deformed copper specimen (Hellmig et al., Reference Hellmig, Baik, Bowen, Estrin, Juul Jensen, Kim, Seo, Zehetbauer and Valiev2004) have shown, however, that considerable fractions of subgrains are not separated by significant differences in orientation. These TEM investigations indicate that the small angle grain boundary model of subgrain boundaries is definitely not sufficient to explain the apparent discrepancy between TEM and X-ray size values. In the present work it has been shown that when dislocations are arranged in dipolar dislocation-wall configurations the two crystal-halfs on either side of such a wall are shifted with respect to each other parallel to the direction of their Burgers vectors, where this shift varies randomly between zero and ḇ∕2. This random spatial shift causes a random phase shift of the X-rays scattered by the adjacent subgrains. As a result, the intensities of the scattering from adjacent subgrains will be summed up and the line broadening will be determined by the average subgrain size. The two models, i.e., the small-angle grain-boundary model and the dipolar dislocation-wall model of subgrain boundaries, provide together a physically well-established basis for the assumption that size and size distributions determined by X-ray line profile analysis correspond to subgrains or dislocation cells. If, however, the subgrains∕cells and the grains are identical, as might happen in many cases, then the TEM and X-ray size data can be identical. Finally it is noted that neither dipolar dislocation walls nor small angle grain boundaries are so perfect arrays of dislocations as depicted in the schematic drawings in Figures 9 and 10, respectively. The arrays will not be perfectly regular, and the dislocations may be of different type and∕or orientation and∕or sign. For example there may be some dipoles within the small angle grain boundaries, or the dipolar walls may be not straight or flat, and they may also contain different types of dislocations or more dislocations of one sign. The schematic pictures in Figures 9 and 10 intend only to show the net structure and behavior of two different types of boundaries.

ACKNOWLEDGMENT

This work was supported by the Hungarian Scientific Research Fund, OTKA, Grant Nos. F-047057, T-038048, and T-042714.

References

Audebrand, N., Raite, S., and Louër, D. (2003). “The layer crystal structure of [In2(C2O4)3(H2O)3]∙7H2O and microstructure of nanocrystalline In2O3 obtained from thermal decomposition,” Solid State Sci.SSSCFJ 5, 783–794.CrossRefGoogle Scholar
Bakonyi, I., Tóth-Kádár, E., Pogány, L., Cziráki, A., Geröcs, I., Varga-Josepovits, K., Arnold, B., and Wetzig, K. (1996). “Preparation and characterization of dc-plated nanocrystalline nickel electrodeposits,” Surf. Coat. Technol.SCTEEJ 78, 124–136.CrossRefGoogle Scholar
Balzar, D., Audebrand, N., Daymond, M. R., Fitch, A., Hewat, A., Langford, J. I., Le Bail, A., Louër, D., Masson, O., McCowan, C. N., Popa, N. C., Stephens, P. W., and Toby, B. H. (2004). “Size-strain line-broadening analysis of the ceria round-robin sample,” J. Appl. Crystallogr.JACGAR10.1107/S0021889804022551 37, 911–924.CrossRefGoogle Scholar
Bertaut, E. F. (1950). “Raies de Debye-Scherrer et repartition des dimensions des domaines de Bragg dans les poudres polycristallines,” Acta Crystallogr.ACCRA910.1107/S0365110X50000045 3, 14–18.CrossRefGoogle Scholar
Bolmaro, R. E., Brokmeier, H. G., Signorelli, J. W., Fourtz, A., and Bertinetti, M. A. (2004). “Interaction between phases in Co-deforming two-phase materials: The role of dislocation arrangements,” in Diffraction Analysis of the Microstructure of Materials, edited by Mittemeijer, E. J. and Scardi, P. (Springer, Berlin), 391 pp.CrossRefGoogle Scholar
Boulle, A., Legrand, C., Guinebretière, R., Mercurio, J. P., and Dauger, A. (2001). “Planar faults in layered bi-containing perovskites studied by X-ray diffraction line profile analysis,” J. Appl. Crystallogr.JACGAR 34, 699–703.CrossRefGoogle Scholar
Cheary, R. W., Dooryhee, E., Lynch, P., Armstrong, N., and Dligatch, S. (2000). “X-ray diffraction line broadening from thermally deposited gold films,” J. Appl. Crystallogr.JACGAR10.1107/S0021889800009936 33, 1271–1283.CrossRefGoogle Scholar
Dinnebier, R. E., Von Dreele, R., Stephens, P. W., Jelonek, S., and Sieler, J. (1999). “Structure of sodium para-hydroxybenzoate NaO2C–C6H4OH by powder diffraction: application of a phenomenological model of anisotropic peak width,” J. Appl. Crystallogr.JACGAR10.1107/S0021889899005233 32, 761–769.CrossRefGoogle Scholar
Estevez-Rams, E., Leoni, M., Scardi, P., Aragon-Fernandez, B., and Fuess, H. (2003). “On the powder diffraction pattern of crystals with stacking faults,” Philos. Mag.PMHABF 83, 4045–4057.CrossRefGoogle Scholar
Gaál, I. (1984). Proceedings of the Fifth Riso International Symposium on Metallurgy and Material Science, edited by Andersen, N. H. et al. , Riso National Laboratory, Roskilde, Denmark, 249 pp.Google Scholar
Gil Sevillano, J. and Aernoudt, E. (1987). “Low energy dislocation structures in highly deformed materials,” Mater. Sci. Eng.MSCEAA10.1016/0025-5416(87)90441-1 86, 35–51.CrossRefGoogle Scholar
Groma, I. (1998). “X-ray line broadening due to an inhomogeneous dislocation distribution,” Phys. Rev. BPRBMDO10.1103/PhysRevB.57.7535 57, 7535–7542.CrossRefGoogle Scholar
Groma, I., Ungár, T., and Wilkens, M. (1988). “Asymmetric X-ray line broadening of plastically deformed crystals. 1. Theory,” J. Appl. Crystallogr.JACGAR10.1107/S0021889887009178 21, 47–53.CrossRefGoogle Scholar
Gubicza, J., Chinh, N. Q., Horita, Z., and Langdon, T. G. (2004). “Effect of Mg addition on microstructure and mechanical properties of aluminum,” Mater. Sci. Eng., AMSAPE3 387–389, 55–59.CrossRefGoogle Scholar
Gubicza, J., Ribárik, G., Bakonyi, I., and Ungár, T. (2001). “Crystallite-size distribution and dislocation structure in nanocrystalline HfNi5 determined by X-ray diffraction profile analysis,” J. Nanosci. Nanotechnol.JNNOAR10.1166/jnn.2001.039 1, 343–348.CrossRefGoogle ScholarPubMed
Gubicza, J., Szépvölgyi, J., Mohai, I., Ribárik, G., and Ungár, T. (2000a). “The effect of heat-treatment on the grain-size of nanodisperse plasmathermal silicon nitride powder,” J. Mater. Sci.JMTSAS10.1023/A:1004800607605 35, 3711–3717.CrossRefGoogle Scholar
Gubicza, J., Szépvölgyi, J., Mohai, I., Zsoldos, L., and Ungár, T. (2000b). “Particle size distribution and the dislocation density determined by high resolution X-ray diffraction in nanocrystalline silicon nitride powders,” Mater. Sci. Eng. A 280, 263–269.CrossRefGoogle Scholar
Hellmig, R. J., Baik, S. C., Bowen, J. R., Estrin, Y., Juul Jensen, D., Kim, H. S., and Seo, M. H. (2004). “Evolution of mechanical and microstructural properties of ECAP deformed copper,” in Proceedings of the Second International Conference on Nanomaterials by Severe Plastic Deformation: Fundamentals—Processing—Applications, Wien, Austria, 9–13 December 2002, edited by Zehetbauer, M. J. and Valiev, R. Z. (Wiley VCH, Weinheim), 420 pp.Google Scholar
Hinds, W. C. (1982). Aerosol Technology: Properties, Behavior and Measurement of Airbone Particles (Wiley, New York).Google Scholar
Hughes, D. A. and Hansen, N. (1993). “Microstructural evolution in nickel during rolling from intermediate to large strains,” Metall. Trans. AMTTABN 24, 2021–2037.CrossRefGoogle Scholar
Hughes, D. A. and Hansen, N. (2000). “Microstructure and strength of nickel at large strains,” Acta Mater.ACMAFD10.1016/S1359-6454(00)00082-3 48, 2985–3004.CrossRefGoogle Scholar
Hughes, D. A. and Nix, W. D. (1989). “Strain hardening and substructural evolution in Ni–Co solid solutions at large strains,” Mater. Sci. Eng., AMSAPE310.1016/0921-5093(89)90627-8 122, 153–172.CrossRefGoogle Scholar
Ida, T., Shimazaki, S., Hibino, H., and Toraya, H. (2003). “Diffraction peak profiles from spherical crystallites with lognormal size distribution,” J. Appl. Crystallogr.JACGAR 36, 1107–1115.CrossRefGoogle Scholar
Krill, C. E. and Birringer, R. (1998). “Estimating grain-size distributions in nanocrystalline materials from X-ray diffraction profile analysis,” Philos. Mag. APMAADG10.1080/014186198254281 77, 621–640.CrossRefGoogle Scholar
Krivoglaz, M. A. (1996). X-ray and Neutron Diffraction in Nonideal Crystals (Springer, Berlin).CrossRefGoogle Scholar
Kuhlmann-Wilsdorf, D. (2002). “The LES theory of solid plasticity,” in Dislocations in Solids, edited by Nabarro, F. R. N. and Duesbery, M. S. (Elsevier Science, Amsterdam), 211 pp.Google Scholar
Langford, J. I., Boultif, A., Auffrédic, J. P., and Louër, D. (1993). “The use of pattern decomposition to study the combined X-ray diffraction effects of crystallite size and stacking faults in ex-oxalate zinc oxide,” J. Appl. Crystallogr.JACGAR10.1107/S0021889892007684 26, 22–33.CrossRefGoogle Scholar
Langford, J. I. and Louër, D. (1996). “Powder diffraction,” Rep. Prog. Phys.RPPHAG10.1088/0034-4885/59/2/002 59, 131–234.CrossRefGoogle Scholar
Langford, J. I., Louër, D., and Scardi, P. (2000). “Effect of a crystallite size distribution on X-ray diffraction line profiles and whole-powder-pattern fitting,” J. Appl. Crystallogr.JACGAR10.1107/S002188980000460X 33, 964–974.CrossRefGoogle Scholar
Le Bail, A. and Louër, D. (1978). “Smoothing and validity of crystallite-size distributions from X-ray line-profile analysis,” J. Appl. Crystallogr.JACGAR 11, 50–55.CrossRefGoogle Scholar
Leoni, M. and Scardi, P. (2004). “Nanocrystalline domain size distributions from powder diffraction data,” J. Appl. Crystallogr.JACGAR 37, 629–634.CrossRefGoogle Scholar
Levine, L. E. and Thomson, R. (1997). “X-ray scattering by dislocations in crystals. General theory and application to screw dislocations,” Acta Crystallogr., Sect. A: Found. Crystallogr.ACACEQ10.1107/S0108767397005989 53, 590–602.CrossRefGoogle Scholar
Louër, D., Auffrédic, J. P., Langford, J. I., Ciosmak, D., and Niepce, J. C. (1983). “A precise determination of the shape, size and distribution of size of crystallites in zinc oxide by X-ray line-broadening analysis,” J. Appl. Crystallogr.JACGAR10.1107/S0021889883010237 16, 183–191.CrossRefGoogle Scholar
Macherauch, E. (1980). “State-of-the-art and prospects of the X-ray stress analysis. 1,” Metall 34, 443–452.Google Scholar
Marmy, P., Yuzhen, R., and Victoria, M. J. (1991). “The tensile and fatigue properties of type-1.4914 ferritic steel for fusion reactor applications,” J. Nucl. Mater.JNUMAM 179, 697–701.CrossRefGoogle Scholar
Mughrabi, H. (1983). “Dislocation wall and cell structures and long-range internal-stresses in deformed metal crystals,” Acta Metall.AMETAR10.1016/0001-6160(83)90007-X 31, 1367–1379.CrossRefGoogle Scholar
Mughrabi, H., Ungár, T., Kienle, W., and Wilkens, M. (1986). “Long-range internal-stresses and asymmetric X-ray line broadening in tensile deformed [001]-oriented copper single crystals,” Philos. Mag. APMAADG 53, 793–813.CrossRefGoogle Scholar
Noyan, I. C. and Cohen, J. B. (1987). Residual Stress (Springer, New York).CrossRefGoogle Scholar
Révész, A., Lendvai, J., and Ungár, T. (2000). “Melting point depression and microstructure in ball-milled nanocrystalline aluminium powders,” Mater. Sci. ForumMSFOEP 343–3, 326–331.CrossRefGoogle Scholar
Ribárik, G., Ungár, T., and Gubicza, J. (2001). “MWP-fit: A program for multiple whole profile fitting of diffraction profiles by ab-initio theoretical functions,” J. Appl. Crystallogr.JACGAR10.1107/S0021889801011451 34, 669–676.CrossRefGoogle Scholar
Sanders, P. G., Fougere, G. E., Thompson, L. J., Eastman, J. A., and Weertman, J. R. (1997). “Improvements in the synthesis and compaction of nanocrystalline materials,” Nanostruct. Mater.NMAEE710.1016/S0965-9773(97)00167-0 8, 243–252.CrossRefGoogle Scholar
Scardi, P. and Leoni, M. (1999). “Fourier modelling of the anisotropic line broadening of X-ray diffraction profiles due to line and plane lattice defects,” J. Appl. Crystallogr.JACGAR10.1107/S002188989900374X 32, 671–682.CrossRefGoogle Scholar
Scardi, P. and Leoni, M. (2002). “Whole powder pattern modelling,” Acta Crystallogr., Sect. A: Found. Crystallogr.ACACEQ 58, 190–200.CrossRefGoogle ScholarPubMed
Scardi, P., Leoni, M., and Delhez, R. (2004). “Line broadening analysis using integral breadth methods: A critical review,” J. Appl. Crystallogr.JACGAR10.1107/S0021889804004583 37, 381–390.CrossRefGoogle Scholar
Stephens, P. W. (1999). “Phenomenological model of anisotropic peak broadening in powder diffraction,” J. Appl. Crystallogr.JACGAR10.1107/S0021889898006001 32, 281–288.CrossRefGoogle Scholar
Terwilliger, Ch. D. and Chiang, Y. M. (1995). “Size dependent solute segregation and total solubility in ultrafine polycrystals-Ca in TiO2,” Acta Metall. Mater.AMATEB10.1016/0956-7151(94)00231-6 43, 319–328.CrossRefGoogle Scholar
Tóth-Kádár, E., Bakonyi, I., Sólyom, A., Hering, J., Konczos, G., and Pavlyák, F. (1987). “Preparation and characterization of electrodeposited amorphous Ni–P alloys,” Surf. Coat. Technol.SCTEEJ 31, 31–43.CrossRefGoogle Scholar
Treacy, M. M. J., Newsam, J. M., and Deem, M. W. (1991). “A general recursion method for calculating diffracted intensities from crystals containing planar faults,” Proc. R. Soc. London, Ser. APRLAAZ 433, 499–520.Google Scholar
Ungár, T. and Borbély, A. (1996). “The effect of dislocation contrast on x-ray line broadening: A new approach to line profile analysis,” Appl. Phys. Lett.APPLAB10.1063/1.117951 69, 3173–3175.CrossRefGoogle Scholar
Ungár, T., Borbély, A., Goren-Muginstein, G. R., Berger, S., and Rosen, A. R. (1999). “Particle-size, size distribution and dislocations in nanocrystalline tungsten-carbide,” Nanostruct. Mater.NMAEE710.1016/S0965-9773(99)00023-9 11, 103–113.CrossRefGoogle Scholar
Ungár, T., Gubicza, J., Ribárik, G., and Borbély, A. (2001). “Crystallite size distribution and dislocation structure determined by diffraction profile analysis: Principles and practical application to cubic and hexagonal crystals,” J. Appl. Crystallogr.JACGAR10.1107/S0021889801003715 34, 298–310.CrossRefGoogle Scholar
Ungár, T., Martinetto, P., Ribárik, G., Dooryhee, E., Walter, P., and Anne, M. (2002). “Revealing the powdering methods of black makeup in Ancient Egypt by fitting microstructure based Fourier coefficients to the whole x-ray diffraction profiles of galena,” J. Appl. Phys.JAPIAU10.1063/1.1429792 91, 2455–2465.CrossRefGoogle Scholar
Ungár, T. and Tichy, G. (1999). “The effect of dislocation contrast on X-ray line profiles in untextured polycrystals,” Phys. Status Solidi APSSABA10.1002/(SICI)1521-396X(199902)171:2<425::AID-PSSA425>3.0.CO;2-W 171, 425–434.3.0.CO;2-W>CrossRefGoogle Scholar
Ustinov, A. I., Olikhovska, L. O., Budarina, N. M., and Bernard, F. (2004). “Line profile fitting: The case of fcc crystals containing stacking faults,” in Diffraction Analysis of the Microstructure of Materials, edited by Mittemeijer, E. J. and Scardi, P. (Springer, Berlin), 309 pp.Google Scholar
Valiev, R. Z., Kozlov, E. V., Ivanov, Yu. F., Lian, J., Nazarov, A. A., and Baudelet, B. (1994). “Deformation behavior of ultra-fine grained copper,” Acta Metall. Mater.AMATEB10.1016/0956-7151(94)90326-3 42, 2467–2476.CrossRefGoogle Scholar
van Berkum, J. G. M., Vermuelen, A. C., Delhez, R., de Keijser, Th. H., and Mittemeijer, E. J. (1994). “Applicabilities of the Warren-Averbach analysis and an alternative analysis for separation of size and strain broadening,” J. Appl. Crystallogr.JACGAR10.1107/S0021889893010568 27, 345–357.CrossRefGoogle Scholar
Warren, B. E. (1990). X-ray Diffraction (Dover, New York).Google Scholar
Wilkens, M. (1970). Fundamental Aspects of Dislocation Theory (National Bureau of Standards Special Publication, Washington, DC.) Vol. II, No. 317, 1195 pp.Google Scholar
Wilkens, M., Ungár, T., and Mughrabi, H. (1987). “X-ray rocking curve broadening of tensile deformed [001]-oriented copper single crystals,” Phys. Status Solidi APSSABA 104, 157–170.CrossRefGoogle Scholar
Zehetbauer, M. J., Kohout, J., Schafler, E., Sachslehner, F., and Dubravina, A. (2004). “Plastic deformation of nickel under high hydrostatic pressure,” J. Alloys Compd.JALCEU 378, 329–334.CrossRefGoogle Scholar
Zhilyaev, A. P., Gubicza, J., Nurislamova, G., Révész, Á, Suriñach, S., Baró, M. D., and Ungár, T. (2003). “Microstructural Characterization of Ultrafine-Grained Nickel,” Phys. Status Solidi APSSABA10.1002/pssa.200306608 198, 263–271.CrossRefGoogle Scholar
Zhu, Y. T., Huang, J. Y., Gubicza, J., Ungár, T., Wang, Y. M., Ma, E., and Valiev, R. Z. (2003). “Nanostructures in Ti processed by severe plastic deformation,” J. Mater. Res.JMREEE 18, 1908–1917.CrossRefGoogle Scholar
Figure 0

Figure 1. TEM micrograph of silicon nitride ceramic powder synthesized in thermal plasma and crystallized at 1500 °C.

Figure 1

Figure 2. The grain size distribution obtained by TEM (bar diagram), and the crystallite size distribution determined by XLPA (solid line) (the vertical line is an estimated error bar).

Figure 2

Figure 3. TEM micrograph of a grain containing dislocation cells in ultrafine grained titanium formed by ECAP.

Figure 3

Figure 4. The statistical size ranges of different structural features in ECAP processed titanium.

Figure 4

Figure 5. The grain size determined by TEM (dTEM) vs the area-weighted mean crystallite size obtained from XLPA (✩x✪area) for plastically deformed metals and for metallic materials produced by inert-gas condensation or electrodeposition (a). The small grain size region of (a) is replotted in (b) where the different materials are indicated by different symbols: open square—Cu deformed by ECAP (Ungár et al., 2001); closed circle—Ti processed by ECAP (Zhu et al., 2003); cross—Al-3%Mg formed by ECAP (Gubicza et al., 2004); open circle—Ni specimens obtained by different SPD methods (Zhilyaev et al., 2003); open triangle—Cu formed by inert-gas condensation (Sanders et al., 1997); closed square—electrodeposited Ni (Zhilyaev et al., 2003).

Figure 5

Figure 6. The ratio of the grain size determined by TEM and the crystallite size obtained by XLPA vs the dislocation density: open square—Cu formed by inert-gas condensation (Sanders et al., 1997); open circle—Cu deformed by ECAP (Ungár et al., 2001); open triangle—Ni specimens obtained by different SPD methods (Zhilyaev et al., 2003); closed inverted triangle—Ti processed by ECAP (Zhu et al., 2003); cross—pure Al and Al-3%Mg formed by ECAP (Gubicza et al., 2004); closed square—electrodeposited Ni (Zhilyaev et al., 2003).

Figure 6

Figure 7. The dislocation density vs the area-weighted mean crystallite size for different series of plastically deformed materials: open circle—ball milled PbS (Ungár et al., 2002); open square—Cu, Ti, Ni, and Al-3%Mg processed by SPD methods (Ungár et al., 2001; Zhilyaev et al., 2003; Zhu et al., 2003; Gubicza et al., 2004); cross—ball milled Al (Révész et al., 2000).

Figure 7

Figure 8. TEM micrograph of a copper specimen deformed by a single pass of ECAP (a). The schematic representation of the measured differences in orientation in (a) is shown in (b). The black lines correspond to large differences in orientation ranging up to 25° while the grey lines correspond to almost zero or small differences in orientation ranging from 0.2° to about 8°.

Figure 8

Figure 9. A schematic dipolar dislocation wall (a). The dislocations are arranged periodically with the period s, and the width and the thickness of the dipoles is η and δ, respectively. The shift, ṯ, of the two lattice halves on the two sides of the dipolar wall is shown in (b). A schematic representation of the structure of a grain interior is shown in (c). The randomly hatched regions are for the subgrain boundaries, in the present case they are assumed to be dipolar dislocation walls. The thick dashed lines represent the large angle grain boundaries. D and d are the grain-and subgrain size, respectively. The lattice-shift relative to the adjacent subgrain lattice in the ith subgrain is ṯi.

Figure 9

Figure 10. The schematic picture of subgrain or cell structure where dislocations constitute the boundaries of subgrains or cells with slightly different orientations. The figure is similar in its meaning to the schematic illustration in Figure 15.6 of Bolmaro et al. (2004).