Americium and Curium Chemistry and Technology: Papers from a by Dr. Glenn T. Seaborg (auth.), Norman M. Edelstein, James D.

By Dr. Glenn T. Seaborg (auth.), Norman M. Edelstein, James D. Navratil, Wallace W. Schulz (eds.)

The papers incorporated during this quantity have been provided on the symposium on "Americium and Curium Chemistry and expertise" on the overseas Chemical Congress of Pacific Basin Societies in Honolulu, Hawaii, December 16-21, 1984. This symposium venerated 40 years of study on americium and curium. therefore, the papers integrated during this quantity commence with ancient views at the discovery of americium and curium and the early characterization in their chemical homes, after which hide quite a lot of topics, resembling thermodynamic homes, digital constitution, nuclear reactions, analytic chemistry, excessive strain section transitions, and technological points. hence, this quantity is a evaluation of the chemistry of americium and curium, and offers a point of view at the present learn on those parts 40 years after their discovery. The editors want to thank the members during this symposium for his or her contributions. it's a excitement to recognize the help of Ms. Barbara Moriguchi in dealing with the executive facets of the symposium and of the construction of this quantity. April 2, 1985 Norman M. Edelstein fabrics and Molecular study department Lawrence Berkeley Laboratory collage of California Berkeley, California 94720, U.S.A. James D. Navratil Rockwell foreign Rocky apartments Plant P.O. field 464 Golden, Colorado 80402-0464, U.S.A. Wallace W. Schulz Rockwell Hanford P.O. field 800 Richland, Washington 99352, U.S.A.

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89 Mm thickness. Up to 20K, the resistivity varies with temperature as T2 • 8 , at higher temperatures deviations from the linear law were found similar to those in uranium and neptunium (Fig. 3). The resistivity of curium metal shows a sudden decrease of the slope around 60K (which is related to the magnetic transition around 52K) , and at higher temperatures a behaviour similar to that of a lanthanide metal is seen. 160 Tu 140 a-Pu 120 Np c: 100 6 >- I- > l- (/) (/) 80 Am 60 UJ a:: Figure 3. Electrical resistivity of actinide metals.

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