Download presentation

Presentation is loading. Please wait.

1
**Impurity effect on charge and spin density in α-Fe**

– comparison between cellular model, ab initio calculations and Mössbauer spectroscopy data A. Błachowski1, U.D. Wdowik2, K. Ruebenbauer1 1 Mössbauer Spectroscopy Division, Institute of Physics, Pedagogical University, Kraków, Poland 2 Applied Computer Science Division, Institute of Technology,

2
**Impurities dissolved randomly on regular iron sites in BCC iron**

3
**magnetic hyperfine field B (electron spin density on Fe nucleus) and **

Impurities modify magnetic hyperfine field B (electron spin density on Fe nucleus) and isomer shift S (electron charge density on Fe nucleus). Electron charge and spin densities on Fe nucleus are affected by volume effect caused by solution of impurity and by conduction band modification. Aim of this contribution is to separate VOLUME EFFECT and BAND EFFECT due to addition of impurity.

4
1) One can study variation dB/dc of average magnetic hyperfine field B on Fe nucleus versus particular impurity concentration c. Similar variation d/dc of average electron density on Fe nucleus could be conveniently observed via isomer shift variation dS/dc , where S denotes a total shift versus total shift in pure -Fe.

5
Fe100-cPdc Fe100-cMoc

6
References [Be, Cu] I. Vincze and A. T. Aldred, Solid State Communications 17, 639 (1975). [Al] S. M. Dubiel and W. Zinn, Phys. Rev. B 26, 1574 (1982). [Si] S. M. Dubiel and W. Zinn, J. Magn. Magn. Mater. 28, 261 (1982). [P] S. M. Dubiel, Phys. Rev. B 48, 4148 (1993). [Ti] J. Cieślak and S. M. Dubiel, J. Alloys Comp. 350, 17 (2003). [V] S. M. Dubiel and W. Zinn, J. Magn. Magn. Mater. 37, 237 (1983). [Cr] S. M. Dubiel and J. Żukrowski, J. Magn. Magn. Mater. 23, 214 (1981). [Mn, Ni] I. Vincze and I. A. Campbell, J. Phys. F, Metal Phys. 3, 647 (1973). [Co] J. Chojcan, Hyperf. Interact. 156/157, 523 (2004). [Zn] A. Laggoun, A. Hauet, and J. Teillet, Hyperf. Interact. 54, 825 (1990). [Ga] A. Błachowski, K. Ruebenbauer, J. Żukrowski, and J. Przewoźnik, J. Alloys Compd. 455, 47 (2008). [Ge] S. M. Dubiel and W. Zinn, Phys. Rev. B 28, 67 (1983). [As, Sb] I. Vincze and A. T. Aldred, Phys. Rev. B 9, 3845 (1974). [Nb] A. Błachowski, K. Ruebenbauer, and J. Żukrowski, Phys. Status Solidi B 242, 3201 (2005). [Mo] A. Błachowski, K. Ruebenbauer, J. Żukrowski, and J. Przewoźnik, J. Alloys Compd. 482, 23 (2009). [Ru] A. Błachowski, K. Ruebenbauer, and J. Żukrowski, Phys. Rev. B 73, (2006). [Rh] A. Błachowski, K. Ruebenbauer, and J. Żukrowski, J. Alloys Compd. 477, 4 (2009). [Pd] A. Błachowski, K. Ruebenbauer, and J. Żukrowski, Phys. Scr. 70, 368 (2004). [Sn] S. M. Dubiel and W. Znamirowski, Hyperf. Interact. 9, 477 (1981). [W] S. M. Dubiel and W. Zinn, Phys. Rev. B 30, 3783 (1984). [Re] S.M. Dubiel, J. Magn. Magn. Mater. 69, 206 (1987). [Os] A. Błachowski, K. Ruebenbauer, and J. Żukrowski, Nukleonika 49, S67 (2004). [Ir] A. Błachowski, K. Ruebenbauer, and J. Żukrowski, J. Alloys Compd. 464, 13 (2008). [Pt] S. M. Dubiel, Phys. Rev. B 37, 1429 (1988). [Au] A. Błachowski, K. Ruebenbauer, J. Przewoźnik, and J. Żukrowski, J. Alloys Compd. 458, 96 (2008).

7
**BAND EFFECT + VOLUME EFFECT**

Correlation between electron spin density (dB/dc) and electron density (dS/dc) variations for various impurities BAND EFFECT + VOLUME EFFECT Isomer shift S could be transformed into electron density on Fe nucleus Calibration constant

8
**VOLUME EFFECT and BAND EFFECT introduced by impurity? ANSWER **

2) QUESTION How to separate VOLUME EFFECT and BAND EFFECT introduced by impurity? ANSWER VOLUME EFFECT can be calculated for pure -Fe by using ab initio methods (Wien2k). In order to do so one has to calculate magnetic hyperfine field B and electron density on Fe nucleus for pure -Fe varying lattice constant a.

9
**Fe Variation of electron density -0 and**

hyperfine field (contact field) B-B0 versus lattice constant a-a0

10
3) QUESTION How impurities change lattice constant a? ANSWER X-ray diffraction data Lattice constant a versus impurity concentration c Å/at.% Å/at.% Fe100-cOsc Fe100-cAuc

11
**da/dc for all impurities studied**

Ne - number of out of the core electrons donated by impurity

12
**1) 2) 3) 1) + 2) + 3) Mössbauer data ab initio calculations**

- X-ray diffraction data 2) 3) 1) + 2) + 3) Volume correction for electron spin density (hyperfine field) and for electron charge density (isomer shift) Pure BAND MODIFICATION EFFECT i.e. volume effect due to impurity is removed.

13
**Correlation between volume corrected (pure BAND EFFECT) **

electron spin density (dB/dc)b and electron density (dS/dc)b variations for various impurities All d metals fall on single straight line with positive slope. Hence, the band effect is almost the same regardless of principal quantum number of d shell of impurity.

14
**for various impurities: **

Correlation between electron spin density and electron density variations for various impurities: (a) – total; (b) – volume corrected, i.e., pure band effect.

15
**Cellular atomic model (CAM) of Miedema and van der Woude**

- isomer shift of the alloy containing diluted impurity a in the matrix b - electro-chemical potentials of the pure element a and b forming binary alloy - electron densities - CAM parameters [1] A. R. Miedema and F. van der Woude, Physica 100B, 145 (1980) [2] A. R. Miedema, Physica B 182, 1 (1992)

16
**Cellular atomic model (CAM) of Miedema and van der Woude**

Correlation between experimental derivative of the average isomer shift versus impurity concentration c and corresponding derivative within CAM model

17
**Cellular atomic model (CAM) of Miedema and van der Woude**

(b) Correlation between experiment and CAM for the first shell perturbations of isomer shift S1(E) and S1(M) (c) Correlation between ab initio calculated S1(C) and CAM S1(M)

18
**Cellular atomic model (CAM) of Miedema and van der Woude**

B Dispersion mm/(s∙V∙at.%) x102 mm/(s∙at.%) x102 d<S>/dc 0.79 -2.11 0.20 mm/(sV) x102 mm/s x102 S1 exp 3.00 -11.18 2.60 S1 ab initio 4.86 -13.25 1.66

19
**versus distance r from the impurity (co-ordination shell)**

Variation of the electron density (isomer shift S) and hyperfine field B versus distance r from the impurity (co-ordination shell)

20
**Mössbauer spectra for various concentrations of Ru and Os.**

Red lines - perturbations of the charge and spin density obtained from the ab initio calculations.

Similar presentations

OK

1 4.1 Introduction to CASTEP (1) CASTEP is a state-of-the-art quantum mechanics-based program designed specifically for solid-state materials science.

1 4.1 Introduction to CASTEP (1) CASTEP is a state-of-the-art quantum mechanics-based program designed specifically for solid-state materials science.

© 2018 SlidePlayer.com Inc.

All rights reserved.

Ads by Google

Ppt on network topology Ppt on rc coupled amplifier design Free download ppt on world war 1 Ppt on conservation of environment images Eyelid anatomy and physiology ppt on cells Ppt on conservation of nonrenewable resources Free ppt on telephone etiquette Ppt on tcp/ip protocol stack Ppt on types of trees Ppt on art of war game