Download e-book for iPad: 3d, 4d and 5d Elements, Alloys and Compounds by H.P.J. Wijn, K. Kanematsu, S. Misawa, M. Shiga, H. Wada

By H.P.J. Wijn, K. Kanematsu, S. Misawa, M. Shiga, H. Wada

ISBN-10: 3540603344

ISBN-13: 9783540603344

Quantity 32 of workforce III is a complement to quantity III/19 and should take care of the magnetic homes of metals, alloys and metal compounds which comprise not less than one transition element.The current subvolume III/32A offers finished and evaluated info on magnetic homes of 3d, 4d and 5d parts, alloys and compounds released often within the prior decade.

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Additional info for 3d, 4d and 5d Elements, Alloys and Compounds (Landolt-Bornstein: Numerical Data and Functional Relationships in Science and Technology - New Series Condensed Matter)

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20. Fe, Co, Ni polycrystalline. Compton profiles at room temperature obtained using circularly polarised X rays with high intensity [87Ml]. The curves for Fe and Ni have been calculated according to [77Wl] and [83Rl], respectively. z-axis 11ki - kr. u. 10-24kg m s-‘. 14 fee Ni [Ref. p. 8 0 I I I I 1 2 3 4 PI- b Fig. 22. fee Ni. E circularly polarised synchrotron radiation [90Tl]. zaxis ]I ki - kr PS ak-3d 2- l1 c? theory l 0 experiment -2 Y -21 SC I I I I I I I I Ti V Cr Mn Fe Co Ni Cu Fig. 23.

15 600 570 565 615 600 I- 630 * 645 K 660 Fig. 8. 999 wt%. Magnetic contribution a,,, to the linear thermal expansion coefficient measured by a neutron back-scattering technique as a function of temperature T. Error bar indicated. The curve is a power-law fit with the constants of Table 2 [88Fl]. 610 620 630 640 K 650 Fig. 9. 999 wt%. Isothermal bulk modulus K in the vicinity of 7’, as derived from changesin the lattice constant (measured by neutron backscattering technique) due to a hydrostatic pressureincrease from I to 100 bar.

Impurity atom Host La Ce Fe Fe co Ni Fe Ni Fe co Ni Fe Fe Ni Fe Ni Fe co Ni Fe co Ni Nd Sm Gd DY ‘1 Er 3, Yb Lu exP H hYP - 370(40) - 410(20) - 300(20) 385(7) 2950(200) 3260(200) 2740(200) 2150(170) 1710(150) -353(l) - 6100(170) - 4650(70) - 7680( 130) - 4760(90) - 1215(75) - 405(10) - 138(10) - 614(17) - 425(18) - 141(35) H4f IIYP 310(30) 3230(210) 3250(210) 3130(210) 2410(180) 1700(150) 29 - 5860(170) -4230(100) - 7200( 150) ‘) - 4680(90) ‘) - 630(110) core H hYP HCeP(“) b - 370(40) - 350(50) 30( 10) - 270(40) - lOO(20) - 3 lO(50) 1lO(10) - 80(30) - 440(70) 160(20) - 340(50) - 120(20) 320(30) - 470(70) 83R2 83R2 83R2 - lO(10) 83R2 - 80(30) 82Kl - 20( 10) 82Kl - 1lO(20) 87Bl - 80(20) 87B 1 - 30(10) 87Bl - 230(50) 87Bl 78Wl - 150(60) ‘) - 40(10) ‘) 78Wl - 550(80) ‘) - lOO(20) ‘) 77N2 150(20) ‘) 30(10) ‘) 77N2 - 600(90) - 30(10) 87Bl 50( 10) - 460(70) 87Bl - 170(20) 87Bl - 614(17) 77K2 - 424( 18) 77K2 - 141(35) 77K2 ‘) Analysis in [87Bl].

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3d, 4d and 5d Elements, Alloys and Compounds (Landolt-Bornstein: Numerical Data and Functional Relationships in Science and Technology - New Series Condensed Matter) by H.P.J. Wijn, K. Kanematsu, S. Misawa, M. Shiga, H. Wada


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