Efeitos do tratamento térmico na obtenção da fase 2223 em amostras de BSCCO com e sem substituição

Pós-graduação em Ciência dos Materiais - FEIS

Palynologie und Sedimentologie der Interglazialprofile Döttingen, Bonstorf, Munster und Bilshausen

Palynologie und Sedimentologie der Interglazialprofile Döttingen, Bonstorf, Munster und Bilshausen Zusammenfassung In der vorliegenden Dissertation wurden vier dem Holstein-Interglazial zugehörige Bohrkerne sowie ein rhumezeitlicher Bohrkern palynologisch und sedimentologisch bearbeitet. Die holsteinzeitlichen Bohrkerne stammen aus Kieselgurlagerstätten der Lüneburger Heide (Bonstorf und Munster) und aus einem Trockenmaar (Döttingen) in der Eifel. Der rhumezeitliche Kern stammt aus der Typlokalität Bilshausen im Harzvorland. Neben Prozentwertdiagrammen werden Pollendichte- und wenn möglich Polleninfluxwerte vorgestellt, die insbesondere für die Lokalitäten Hetendorf/Bonstorf und Munster/Breloh bisher nicht verfügbar waren. Mit dem Profil Döttingen konnte erstmals eine sowohl vollständige als auch nicht innerhalb des klassischen Aufkommens holsteinzeitlicher Fundstellen im norddeutschen Tiefland positionierte Holsteinsequenz aus dem deutschen Mittelgebirge dokumentiert werden. Das erhaltene Pollendiagramm bestätigt die aus den norddeutschen Profilen bekannte holsteintypische Vegetationsabfolge, durch die das Holstein gegenüber anderen Interglazialen wie Holozän, Eem oder Rhume palynologisch definiert ist. Neben der grundsätzlichen Übereinstimmung der Pollensequenz unterscheidet sich das Profil Döttingen aber deutlich im prozentualen Aufkommen der beteiligten Taxa von den norddeutschen Profilen. So wird eine hohe Alnus-Präsenz als Merkmal deutscher Holsteinprofile bestätigt, jedoch ist die, in den norddeutschen Lokalitäten durchhaltend hohe oder dominante Beteiligung von Pinus im deutschen Mittelgebirge nicht vorhanden und muss daher auf die Standortbedingungen Norddeutschlands zurückgeführt werden. Abies dagegen ist im Holstein der Mittelgebirge wesentlich präsenter als im norddeutschen Flachland. Im Profil Döttingen wurden insgesamt 10 Tephralagen gefunden. Auf eine dieser Tephren folgt ein „Birken-Kiefern-Gräser Vorstoß“, der palynostratigraphisch dem älteren „Birken-Kiefern Vorstoß“ in Munster/Breloh entspricht. Als eine Typologie des Holstein kann das in den Profilen Döttingen und Munster bestätigte intraholsteinzeitliche Carpinus-Minimum verstanden werden. An Hand sedimentologischer und palynologischer Befunde aus dem Bohrkern MU 2 muss die Existenz zweier, in der Literatur postulierter, postholsteinzeitlicher, „Nachschwankungen“ in Munster/Breloh in Frage gestellt, wenn nicht abgelehnt werden. In Kern MU 2 fallen palynostratigraphische Grenzen häufig mit Sandeinschaltungen zusammen. Eine dieser Sandeinschaltungen, nämlich unmittelbar vor dem älteren „Birken-Kiefern-Vorstoß“, korreliert in ihrer stratigraphischen Position mit der den „Birken-Kiefern-Gräser-Vorstoß“ im Profil Döttingen einleitenden Tephralage. Es gelang die Dauer des intraholsteinzeitlichen Carpinus Minimums auf etwa 1500±100 Jahre zu bestimmen und eine interne Zweigliederung zu dokumentieren. Im rhumezeitlichen Kern von Bilshausen (BI 1) konnten zahlreiche Störungen nachgewiesen werden. Insbesondere im Teufenbereich des Bilshausener „Birken-Kiefern-Vorstoßes“ deuten diese auf eine möglicherweise verfälschte Überlieferung. Der palynologisch markante „Lindenfall“ von Bilshausen liegt im Bereich einer isoklinalen Schichtenverfaltung. Die in der Literatur im Horizont des „Lindenfalls“ beschriebene „Bilshausentephra“ wurde nicht gefunden. Warvenzählungen an den Kernen MU 1, MU 2 und BI 1 ermöglichten Pollenzonendauern in Holstein- und Rhume-Interglazial zu bestimmen. Dabei wurde mittels den Warvenzählungen, unter zu Hilfenahme von Literaturdaten und von Schätzwerten eine Dauer für das Holstein-Interglazial sensu stricto (Pollenzonen I-XIV) von 15400-17800 Jahren und für das Rhume-Interglazial von wahrscheinlich 22000 Jahren bis maximal 26000 Jahren ermittelt.

Dynamic stall of small wind systems /

"February 1983."

Minguo wen wu kao gu qi kan hui bian : fu bo wu guan guan kan /

v.1. Anyang fa jue bao gao (1-2 qi) -- v.2. Anyang fa jue bao gao (3-4 qi), Bo wu xue za zhi (1 juan 1 qi) -- v.3. Bo wu xue za zhi (1 juan 2 qi - 2 juan 2 qi) -- v.4. Bo wu xue za zhi (2 juan 3 qi - 2 juan 4 qi), Bo wu za zhi [Beijing] (1-2 qi) -- v.5. Bo wu za zhi [Beijing] (3-7 qi) -- v.6. Bo wu za zhi [Hubei] -- v.7. Bo wu za zhi [Sichuan], Gu quan xue (1-2 qi) -- v.8. Gu quan xue (3-5 qi), Jiangxi wen wu -- v.9. Jin shi hsu hua, Kao gu (1-2 qi) -- v.10. Kao gu (3-4 qi) -- v.11. Kao gu (4-5 qi) -- v.12. Kao gu (6 qi), Quan bi (1 qi) -- v.13. Quan bi (2-10 qi) -- v.14. Quan bi (11-22 qi) -- v.15. Quan bi (23-32 qi), Zhongguo kao gu xue bao (2 qi) -- v.16. Zhongguo kao gu xue bao (3-4 qi) -- v.17. Zhongguo kao gu xue bao (4 qi), Guo li li shi bo wu guan cong kan -- v.18. Guo li Shenyang bo wu guan chou bei wei yuan hui hui kan, Hebei di yi bo wu yuan ban yue kan (1-75 qi) -- v.19. Hebei di yi bo wu yuan ban yue kan (76-126 qi), Henan bo wu guan guan kan (1-3 ji) -- v.20. Henan bo wu guan guan kan (4-8 ji) -- v.21. Henan bo wu guan guan kan (9-12 ji) -- v.22. Henan bo wu guan guan kan (13-15 ji), Sichuan bo wu guan guan kan, Xihu bo wu guan guan kan (1 qi) -- v. 23. Xihu bo wu guan guan kan (2-4 qi) -- v.24. Zhongguo bo wu guan xie hui hui bao.

De yue yi cong shu chu ke /

Block print.

The geometry of Bi nanolines on Si(0 0 1)

A study of the Bi nanoline geometry on Si(0 0 1) has been performed using a combination of ab initio theoretical technique and scanning tunnelling microscopy (STM). Our calculations demonstrate decisively that the recently proposed Haiku geometry is a lower energy configuration than any of the previously proposed line geometries. Furthermore, we have made comparisons between STM constant-current topographs of the lines and Tersoff–Haman STM simulations. Although the Haiku and the Miki geometries both reproduce the main features of the constant-current topographs, the simulated STM images of the Miki geometry have a dark stripe between the dimer rows that does not correspond well with experiment.

Structure evolution and phase change in Ag-5.1 at.% Bi alloy during mechanical alloying

In this paper we explore the enhancement of solubility in a mechanically driven immiscible system experimentally using a mixture of Ag and Bi powders corresponding to a composition of Ag-5.1 at.% Bi. Increase in solubility can be correlated with the combination of sizes of both Ag and Bi at the nanometric scale. It is shown that complete solid solution of Ag-5.1 at.% Bi forms when the respective sizes of :Bi and Ag exceed 13 and 8 nm respectively. We have carried out a thermodynamic analysis of the size- and strain-dependent free energy landscape and compared the results to the initial mixture of microsized particles to rationalize the evolution of Ag solid solution. The agreement indicates that the emerging driving force for the formation of solid solution is primarily due to size reduction rather than the enhanced kinetics of mass transport due to mechanical driving. (c) 2011 Published by Elsevier Ltd. on behalf of Acta Materialia Inc.

Molecular structure and reactions of 1,1 '-bi(acenaphthen-1-ylidene)-2,2 '-dione

The molecular structure of 1,1'-bi(acenaphthen-1-ylidene)-2,2'-dione 1, a potential building-block for the synthesis of fullerene fragments, has been investigated by X-ray crystallography and semi-empirical (AM1 and PM3) calculations. There is a good agreement between the calculated and crystal structure which is essentially planar and has E-configuration. In the solid state, molecules of 1 pack in an interesting manner as corrugated sheets sustained by a network of C-H ... O hydrogen bonds and resulting in the formation of tetrameric loops. While steric factors limit the reactivity of the carbonyl groups in 1, the ene double bond of the ene-dione moiety present in it exhibits propensity toward [4 + 2]-cycloadditions to furnish novel and highly compressed polycycles 8-10.

Solubilities of Pb+2, Bi+3, Sb+3 and Cu+1 sulphides in (NaCl KCl Na2S) melts

Solubilities of common metal sulfides have been determined in the (NaCl+KCl) eutectic melt with and without Na2S. A novel gas-phase equilibrium technique has been used for PbS, Bi2S3, and So2S3, and an improved liquid phase equilibrium technique for Cu2S, which eliminates the errors due to physical entrapment of the sulfide phase and segregation on quenching, enabling precise measurements to be made. Solubilities in the (NaCl+KCl) eutectic melt were determined as a function of temperature in the rante 700° to 950°C, and were found to be small. The partial molar heats of mixing of the sulfides in the eutectic melt have been calculated from the solubility measurements, to be 13.3, 31.4, 37.1, and 49.0 kcal for PbSs), Sb2S2(l), and Cu2S(s), respectively. Sodium sulfide addition was observed to enhance these solubilities, the effect being largest for Cu2S followed by Sb2S3, Bi2S3, and PbS. This effect is explained qualitatively. It was observed that PbS and Sb2S3 obey Henry's law up to saturation in (NaCl+KCl+Na2S) melts.

Role of Bi3+ ions for Er3+ ions efficient 1.54 mu m light emission in Er/Bi codoped SiO2 thin film prepared by sol-gel method

Er/Bi codoped SiO2 thin films were prepared by sol-gel method and spin-on technology with subsequent annealing process. The bismuth silicate crystal phase appeared at low annealing temperature while vanished as annealing temperature exceeded 1000 degrees C, characterized by X-ray diffraction, and Rutherford backscattering measurements well explained the structure change of the films, which was due to the decrease of bismuth concentration. Fine structures of the Er3+-related 1.54 mu m light emission (line width less than 7 nm) at room temperature was observed by photoluminescence (PL) measurement. The PL intensity at 1.54 gm reached maximum at 800 degrees C and decreased dramatically at 1000 degrees C. The PL dependent annealing temperature was studied and suggested a clear link with bismuth silicate phase. Excitation spectrum measurements further reveal the role of Bi3+ ions for Er3+ ions near infrared light emission. Through sol-gel method and thermal treatment, Bi3+ ions can provide a perfect environment for Er3+ ion light emission by forming Er-Bi-Si-O complex. Furthermore, energy transfer from Bi3+ ions to Er3+ ions is evidenced and found to be a more efficient way for Er3+ ions near infrared emission. This makes the Bi3+ ions doped material a promising application for future erbium-doped waveguide amplifier and infrared LED

Synthesis and applications of 3-[6-(hydroxymethyl)pyridin-2-yl]-1,1 '-bi-2-naphthols or 3,3 '-bis[6-(hydroxymethyl)pyridin-2-yl]-1,1 '-bi-2-naphthols

A series of new 1,1'-bi-2-naphthol (BINOL) derived ligands, 3-[6-(hydroxymethyl)pyridin-2-yl]-BINOLs or 3,3'-bis[6(hydroxymethyl)pyridin-2-yl]-BINOLs, bearing one or two chiral pyridinylmetlianols attached to a binaphthyl skeleton, have been synthesized using the Suzuki cross-coupling reaction. The resulting compounds have been used as ligands in the enantioselective addition of diethylzinc to aldehydes; the products were obtained with up to 96% ee.

Synthesis and properties of optically active aromatic polyimides derived from optically pure 1,1'-bi-2-naphthol

A series of new optically active aromatic polyimides containing axially dissymmetric 1,1'-binaphthalene-2,2-diyl units were prepared from optically pure (R)-(+)-or (S)-(-)-2,2'-bis(3,4-dicarboxyphenoxy)-1,1'-binaphthalene dianhydrides and various aromatic diamines via a conventional two-step procedure that included ring-opening polycondensation and chemical cyclodehydration. The optically pure isomer of dianhydride was prepared by a nucleophilic substitution of optically pure (R)-(+)or (S)-(-)1,1'-bi-2-naphthol with 4-nitrophthalonitrile in aprotic polar solvent and subsequent hydrolysis of the resultant tetranitrile derivatives, followed by the dehydration of the corresponding tetracarboxylic acids to obtain the dianhydrides. These polymers were readily soluble in common organic solvents such as N,N-dimethylacetamide, N-methyl-2-pyrrolidone, and m-cresol, etc., and have glass transition temperatures of 251-296 degrees C, and 5% weight loss occurs not lower than 480 degrees C. The specific rotations of the optically active polyimides ranged from +196 degrees to +263 degrees, and the optical stability and chiroptical properties of them were also studied. (C) 1997 John Wiley & Sons, Inc.