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Hydrogen Absorbing Materials YOSHIDA Lab. M1 Ryusuke Tominaga.

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Presentation on theme: "Hydrogen Absorbing Materials YOSHIDA Lab. M1 Ryusuke Tominaga."— Presentation transcript:

1 Hydrogen Absorbing Materials YOSHIDA Lab. M1 Ryusuke Tominaga

2 The purpose of research The purpose of my research is through creating high-quality Hydrogen Absorbing Materials, to encourage the prevalence of fuel-cell electric vehicle, and thereby to contribute to the energy and environment concern.

3 fuel-cell electric vehicle 「PUYO」 出典: http://www.nikkei.co.jp/news/main/im20071009AS1D0904609102007.html ( ->) ( ->) environment concern The efficiency of fuel-cell electric vehicle is 2 times more efficient than that of normal vehicle (->energy concern) No emissions of carbon dioxide

4 The structure of Fuel cell

5 What is the Hydrogen Absorbing Materials ? The Hydrogen Absorbing Materials are the materials that can absorb and emit hydrogen. The discover : the Philips Eindhoven institution ( Netherlands)

6 The condition that must be satisfied to be a practical Hydrogen Absorbing system Can the system contain enough fuel for about 480km drive ranges at one time refilling ? Can it release hydrogen at rates fast enough to provide the power and acceleration that drier expect on a freeway ? Can it fill the fuel fast enough at reasonable price ?

7 Specific material ZnO Doping H into T0 Formation energy E f =[E(ZnO:H x )-{E(ZnO)+0.5*x*E(H 2 )}]/x (zincblende) BC: Bond-centered AB: Antibonding T: Tetrahedral H: Hexagonal

8 Condition for calculation Machikaneyama2002 http://sham.phys.sci.osaka-u.ac.jp/~kkr/ Korringa-Kohn-Rostoker (KKR) Green ’ s function method Coherent potential approximation (CPA) Local density approximation (LDA) No lattice relaxationedelt=0.001 Ry, ZnO zincblende structure Experimental lattice constants are used.

9 ZnO

10 同時ドーピング法 ドープするドナーとアクセプター濃度に アンバランつけながら、同時にドープ する方法。 a )溶解度増大効果 b) キャリア活性率増大効果 c )易動度増大効果

11 Specific material ZnO Doping trantion metal into Zn-site Doping H into T0 Formation energy E f =[(E((Zn,X)O:H x )-{E((Zn,X)O)+0.5*x*E(H 2 )}]/x (zincblende) BC: Bond-centered AB: Antibonding T: Tetrahedral H: Hexagonal

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13 Condition for calculation Machikaneyama2002 http://sham.phys.sci.osaka-u.ac.jp/~kkr/ Korringa-Kohn-Rostoker (KKR) Green ’ s function method Coherent potential approximation (CPA) Local density approximation (LDA) No lattice relaxationedelt=0.001 Ry, ZnO zincblende structure Experimental lattice constants are used.

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15 What is the c ause ? LDA error ? Can ZnO be Hydrogen Absorbing Materials ?

16 LDA+SIC ‘ Pseudopotential-like self-interaction correction scheme ’ by Filippetti and Spaldin. We implement the scheme with KKR-CPA code (MACHIKANEYAMA2002 ). Filippetti and Spaldin, PRB 67, 125109 (2003). Akai, PRL 81, 3002 (1998). Orbital independent potential

17 ZnVO Ishida et al., Pysica B 351, 204 (2004). LDA SIC Main peak at E B = 1.8 eV

18 Condition for calculation Machikaneyama2002 http://sham.phys.sci.osaka-u.ac.jp/~kkr/ Korringa-Kohn-Rostoker (KKR) Green ’ s function method Coherent potential approximation (CPA) ( Self-interaction corrected LDA (SIC-LDA) ) No lattice relaxationedelt=0.001 Ry, ZnO zincblende structure Experimental lattice constants are used.

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20 Other material MgH2

21 Sumarry The co-doping method is efficient to ZnO. But the effect is limited. Using SIC-LDA (Self-interaction corrected LDA) Other material ex) MgH2


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