2010
DOI: 10.1016/j.msea.2010.08.059
|View full text |Cite
|
Sign up to set email alerts
|

Characterization of the microstructure in random and textured polycrystals and single crystals by diffraction line profile analysis

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
55
1
3

Year Published

2012
2012
2020
2020

Publication Types

Select...
7
1
1

Relationship

0
9

Authors

Journals

citations
Cited by 163 publications
(63 citation statements)
references
References 51 publications
1
55
1
3
Order By: Relevance
“…It was shown that from a set of peaks measured for a number of reflections one can get reliable information about the dislocation type (Kaganer et al, 2006b). The underlaying idea is closely connected to the method of full-profile analysis in powder diffractometry: given a set of profiles for different reflections hkl, the fitting of the whole set enables the determination of the defect parameters (Ribarik & Ungar, 2010;Scardi & Leoni, 2002). The reason is that different defect types produce peak broadening that changes in a different way with hkl and, consequently, that enables one to disentangle the contribution from a distinct defect type.…”
Section: Introductionmentioning
confidence: 99%
“…It was shown that from a set of peaks measured for a number of reflections one can get reliable information about the dislocation type (Kaganer et al, 2006b). The underlaying idea is closely connected to the method of full-profile analysis in powder diffractometry: given a set of profiles for different reflections hkl, the fitting of the whole set enables the determination of the defect parameters (Ribarik & Ungar, 2010;Scardi & Leoni, 2002). The reason is that different defect types produce peak broadening that changes in a different way with hkl and, consequently, that enables one to disentangle the contribution from a distinct defect type.…”
Section: Introductionmentioning
confidence: 99%
“…In the present work, which is the second part of [17], the evolution of lattice strains 21 and dislocation properties during tensile deformation will be presented and discussed in tensile deformation in the two lath packet types will be discussed in relation to the work 27 hardening. The work-hardening mechanism of the lath martensite will be discussed by 28 correlating the dislocation structure with the flow stress in the Taylor equation.…”
mentioning
confidence: 99%
“…(5) it is obvious that we should know the value of Wilkens parameter (M) for the dislocation density calculation [28]. In the deformed materials, this parameter varies in the interval from M = 1 to M = 2 for the dislocation densities from 1 Á 10 10 s m À2 to 1.5 Á 10 11 s m À2 [29,30]. That is why in further calculations we take M = 1.5 for all samples, and C = 0.30 from (5).…”
Section: Discussionmentioning
confidence: 99%