Singular terms of helicity amplitudes at one loop in QCD and the soft limit of the cross sections of multi-parton processes

We describe a general method that enables us to obtain all the singular terms of helicity amplitudes of n-parton processes at one loop. The algorithm uses helicity amplitudes at tree level and simple color algebra. We illustrate the method by calculating the singular part of the one-loop helicity amplitudes of all 2 → 3 parton subprocesses. The results are used to derive the soft gluon limit of the cross sections of all 2 → 4 parton scattering subprocesses which provide a useful initial condition for the angular ordering approximation to coherent multiple soft gluon emission, incorporated in existing Monte Carlo simulation programs.     

Globally Linked Pairs of Vertices in Equivalent Realizations of Graphs

A two-dimensional framework (G,p) is a graph G = (V,E) together with a map p: V → ℝ². We view (G,p) as a straight line realization of G in ℝ². Two realizations of G are equivalent if the corresponding edges in the two frameworks have the same length. A pair of vertices {u,v} is globally linked in G if %and for all equivalent frameworks (G,q), the distance between the points corresponding to u and v is the same in all pairs of equivalent generic realizations of G. The graph G is globally rigid if all of its pairs of vertices are globally linked. We extend the characterization of globally rigid graphs given by the first two authors [13] by characterizing globally linked pairs in M-connected graphs, an important family of rigid graphs. As a byproduct we simplify the proof of a result of Connelly [6] which is a key step in the characterization of globally rigid graphs. We also determine the number of distinct realizations of an M-connected graph, each of which is equivalent to a given generic realization. Bounds on this number for minimally rigid graphs were obtained by Borcea and Streinu in [3].     

Synthesis of cephalosporins carrying isoxazolyl acetamido and related side chains

Starting from 3,5-dimethylisoxazole the carboxylic acids I and V, the amino acids VIII (L-) and IX (D-), and the ureido acids X (L-) and XI (D-) were prepared, which were used for the synthesis of the new cephalosporins XVIIb, XXa-c (L-), and XXIb (D-). Thein vitro antibacterial activity of these semi-synthetic antibiotics was studied. The resorption of XVIIb was investigated in mice.Research Group for Antibiotics of the Hungarian Academy of Sciences, H-4010 Debrecen, P.O. Box 70, Hungary. Published in Khimiya Geterotsiklicheskikh Soedinenii, No. 11, pp. 1524–1535, November, 1998.     

Disturbing effect of CaCl2 used for drying in the measurement of 226Ra in water

A frequently used method in determining the radium concentration of water is the radon emanation method. When radon gas is transferred to the Lucas-cell usually CaCl₂ is used to remove the water traces. When we measured the background of the system using ultra clear distilled water the results were astonishing. The detailed investigation has shown that the unwanted radon originated from the CaCl₂, contained about 1000 Bq/kg of ²²⁶Ra. Depending on the time interval between two measurement, the radon deriving from the CaCl₂ disturbed the measurements.     

The first example of a nitrile hydratase model complex that reversibly binds nitriles

Nitrile hydratase (NHase) is an iron-containing metalloenzyme that converts nitriles to amides. The mechanism by which this biochemical reaction occurs is unknown. One mechanism that has been proposed involves nucleophilic attack of an Fe-bound nitrile by water (or hydroxide). Reported herein is a five-coordinate model compound ([Fe(III)(S(2)(Me2)N(3)(Et,Pr))](+)) containing Fe(III) in an environment resembling that of NHase, which reversibly binds a variety of nitriles, alcohols, amines, and thiocyanate. XAS shows that five-coordinate [Fe(III)(S(2)(Me2)N(3)(Et,Pr))](+) reacts with both methanol and acetonitrile to afford a six-coordinate solvent-bound complex. Competitive binding studies demonstrate that MeCN preferentially binds over ROH, suggesting that nitriles would be capable of displacing the H(2)O coordinated to the iron site of NHase. Thermodynamic parameters were determined for acetonitrile (DeltaH = -6.2(+/-0.2) kcal/mol, DeltaS = -29.4(+/-0.8) eu), benzonitrile (-4.2(+/-0.6) kcal/mol, DeltaS = -18(+/-3) eu), and pyridine (DeltaH = -8(+/-1) kcal/mol, DeltaS = -41(+/-6) eu) binding to [Fe(III)(S(2)(Me2)N(3)(Et,Pr))](+) using variable-temperature electronic absorption spectroscopy. Ligand exchange kinetics were examined for acetonitrile, iso-propylnitrile, benzonitrile, and 4-tert-butylpyridine using (13)C NMR line-broadening analysis, at a variety of temperatures. Activation parameters for ligand exchange were determined to be DeltaH(+ +) = 7.1(+/-0.8) kcal/mol, DeltaS(+ +) = -10(+/-1) eu (acetonitrile), DeltaH(+ +) = 5.4(+/-0.6) kcal/mol, DeltaS(+ +) = -17(+/-2) eu (iso-propionitrile), DeltaH(+ +) = 4.9(+/-0.8) kcal/mol, DeltaS(+ +) = -20(+/-3) eu (benzonitrile), and DeltaH(+ +) = 4.7(+/-1.4) kcal/mol DeltaS(+ +) = -18(+/-2) eu (4-tert-butylpyridine). The thermodynamic parameters for pyridine binding to a related complex, [Fe(III)(S(2)(Me2)N(3)(Pr,Pr))](+) (DeltaH = -5.9(+/-0.8) kcal/mol, DeltaS = -24(+/-3) eu), are also reported, as well as kinetic parameters for 4-tert-butylpyridine exchange (DeltaH(+ +) = 3.1(+/-0.8) kcal/mol, DeltaS(+ +) = -25(+/-3) eu). These data show for the first time that, when it is contained in a ligand environment similar to that of NHase, Fe(III) is capable of forming a stable complex with nitriles. Also, the rates of ligand exchange demonstrate that low-spin Fe(III) in this ligand environment is more labile than expected. Furthermore, comparison of [Fe(III)(S(2)(Me2)N(3)(Et,Pr))](+) and [Fe(III)(S(2)(Me2)N(3)(Pr,Pr))](+) demonstrates how minor distortions induced by ligand constraints can dramatically alter the reactivity of a metal complex.     

Etude dilatométrique de la cristallisation et de la transformation polymorphe du polybutène — 1 isotactique

Résumé On étudie par dilatométrie la cinétique de cristallisation et de la transformation III de trois échantillons de polybutène-1 isotactique. On montre que la cristallisation de l'échantillon fondu est initiée par des germes hétérogènes, dont le nombre varie d'un échantillon à l'autre. La vitesse de cristallisation varie linéairement avec l'inverse du degré de surfusion (T ^–1), sa variation thermique étant indépendante de l'échantillon. On met en évidence l'importance de la cristallisation secondaire, qui suit le processus autocatalytique. D'autre part, la transformation III, après refroidissement, est initiée par des germes apparaissant sporadiquement dans les fibrilles lamellaires de la texture sphérulitique, et elle se propage le long de celles-ci. D'une manière générale la vitesse de transformation isotherme dépend de l'histoire thermique: on examine ici l'influence de la température de cristallisation primitive et celle d'une trempe préalable aux basses températures. Cette dernière engendre un grand nombre de germes, dont la fraction qui résiste à une élévation de température, accélère la transformation. On discute, enfin, les trois volumes de référence déterminant la cristallinité des échantillons dans les deux formes. On propose une nouvelle échelle de cristallinité, dont la cohérence est confirmée par l'invariance des valuers des coefficients de dilatation des deux formes de cristaux, déduites de la dilatation des échantillons obtenus après trempe ou cristallisation isotherme à haute température.

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Summary Kinetics of crystallization and transformation III are investigated dilatometrically with three isotactic Polybutene-1 samples. Primary autocatalytic crystallization from the supercooled melt is initiated by a heterogeneous nucleation process, the number of nucle being determined by the previous temperature of the melt. The rate of crystallization depends linearly on the reciprocal of the degree of supercooling (T ^–1) and its thermal variation is identical for the three samples investigated. The importance of the secondary cristallization, which follows the primary process, is emphasized. On the other hand, the transformation III, which occurs after cooling the semicristalline sample in the room temperature range, is initiated by nuclei appearing sporadically in the lamellar ribbons of the spherulitic texture and they grow linearly along these ribbons. In general the isothermal rate of transformation depends on the previous thermal history of the sample: the influence of the cristallization temperature and that of quenching to low temperatures are systematically investigated. Such a quenching prior to transformation generates a great number of nuclei, a fraction of which persiste even at higher temperatures and increases the rate of transformation. Reference volumes, which determine the cristallinity of PB-1 in its two forms, are discussed. A new cristallinity scale is proposed, the coherence of which is confirmed by the constant values of the expansion coefficients of the two cristalline forms, calculated from the actuel thermal expansion of the semicristalline material, the cristallinity of which varied in a large range.

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Zusammenfassung Es wird an drei isotaktischen Polybuten-1-Proben die Kinetik der Kristallisation und der Transformation von II nach I untersucht. Eine primäre autokatalytische Kristallisation aus der unterkühlten Schmelze wird durch einen heterogenen Keimbildungs-Prozeß initiiert. Die Zahl der Keime ist durch die vorausgehende Temperatur der Schmelze bedingt. Die Geschwindigkeit der Kristallisation hängt linear vom reziproken Wert der Unterkühlung ab (T ^–1) und die thermische Variation ist identisch für alle drei untersuchten Proben. Die Wichtigkeit der Sekundär-Kristallisation, die dem primären Prozeß folgt, wird betont. Andererseits wird die Transformation von II nach I, die nach Abkühlen der halb-kristallinen Probe auf Raumtemperatur eintritt, durch Keime initiiert, die verstreut in den laminaren Rippen der sphärulithischen Textur erscheinen. Sie wachsen linear längs der Rippen. Im allgemeinen hängt die isotherme Geschwindigkeit der Transformation von der thermischen Vorgeschichte der Probe ab. Der Einfluß der Kristallisations-Temperatur und der des Abschreckens zu tiefen Temperaturen werden systematisch untersucht. Ein Abschrecken vor der Transformation erzeugt eine große Zahl von Keimen, von denen ein Bruchteil auch bei höheren Temperaturen fortbesteht und die Transformations-Geschwindigkeit so erhöht. Referenz-Volumina, die die Kristallinität von PB-1 bestimmen, werden diskutiert in ihren zwei Formen. Eine neue Kristallinitäts-Skala wird vorgeschlagen, deren Zutreffen durch die konstanten Werte der Ausdehnungs-Koeffizienten der zwei Kristall-Formen, berechnet aus dem tatsächlichen Ausdehnungsverhaltens des semikristallinen Materials, dessen Kristallanteil in einem großen Bereich variierte, gesichert wird.

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Avec 12 figures en 14 détails et 8 tableaux

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Beursier del'OTAN pendant l'année 1966.     

Propriétés des copolymères biséquencés polyoxyéthylène-polystyrène

Résumé On a préparé des monocristaux de copolymères biséquencés polyoxyéthylène-polystyrène (POE-PS) à partir de leurs solutions diluées, qui peuvent contenir jusqu'à 55% de PS. Les principales formes de ces cristaux et leurs variantes morphologiques, observées sous microscope optique, sont décrites et rattachées à la maille cristallographique du POE. On présente aussi quelques exemples de monocristaux obtenus par ensemencement, dans lesquels les différentes formes se succèdent par filiation; on discute les transitions des formes et leur dépendance vis à vis des conditions de cristallisation.La cristallisation de ces copolymères provoque généralement un fractionnement en composition, car la proportion de PS dans les cristaux est limitée. On propose deux modèles de structure différents, dans lesquels une ou deux couches cristallines de POE en configuration repliée sont recouvertes par le PS amorphe. Le processus de fractionnement est interprété à partir de ces deux structures en admettant une extension critique pour les séquences de PS, dont l'une des extrémités est ancrée sur la surface des repliements du POE.

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Summary Single crystals of copolymers, composed of one Poly(ethylene-oxide), (POE), and one Polystyrene (PS) block, (which may contain 55% of PS, by weight), have been prepared from dilute solutions. The principal crystal habits and their morphological variations, as observed with an optical microscope, are described and related to the unit cell of POE. Single crystals grown from various types of seeds, in which different external habits succeed one another, are also shown. Transitions of crystal habits and their dependence on crystallisation conditions are discussed in some detail.Generally, crystallisation of these copolymers produces some fractionation with respect to composition, for only a limited fraction of the initial PS can enter into the crystal. Two different crystal structures are proposed in which a single, or a double crystalline layer of folded POE is covered by amorphous PS. The fractionation process is interpreted on the basis of these two structural models, assuming a critical extension of the PS blocks anchored at one end to the fold surface of PEO.

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Zusammenfassung Einkristalle von Copolymeren aus einem Polyäthylenoxyd (PEO) und Polystyrol (PS)-Block, die gewichtsmäßig 55% PS enthalten können, wurden aus verdünnten Lösungen präpariert. Der grundsätzliche Charakter der Kristalle und ihre morphologischen Variationen, wie es in einem optischen Mikroskop beobachtet wird, ist beschrieben und mit der Elementarzelle PEO in Beziehung gebracht. Einkristalle, entstanden aus verschiedenen Typen von Kristallkeimen, in welchen verschiedene äußere Formen auftreten, die aufeinanderfolgen, werden gezeigt. Die übrigen Kristallformen und ihre Abhängigkeit von den Kristallisationsbedingungen werden im einzelnen diskutiert.Im allgemeinen verursacht die Kristallisation dieser Copolymeren gewisse Fraktionierung hinsichtlich der Zusammensetzung, da nur eine begrenzte Menge des ursprünglichen Polystyrols in den Kristall eintreten kann. Zwei verschiedene Kristall-Strukturen werden vorgeschlagen, in denen bzw. eine oder zwei Schichten von gefaltetem PEO mit amorphem Polystyrol bedeckt ist. Der Fraktionierungsprozeß wird auf Grund dieser zwei Struktur-Modelle interpretiert, die eine kritische Größe der PS-Blöcke, verankert an einem Ende der gefalteten Oberfläche von PEO, annehmen.