Arqueología del paisaje e historia agraria: algunas cuestiones de método

1996

Applications of Molecular Modeling in the Study of Small Molecules (N2, O2, Rare Gas) Interactions with Complex Molecular Systems Like Zeolites and M…

1996

E-Cadherin, ein neuer, unabhängiger Prognoseparameter beim Magenkarzinom

1996

Das transmembranose Glykoprotein E-Cadherin ist in normalen Epithelien und in Tumorzellen fur die Zell-Zell-Haftung verantwortlich. In Magenkarzinomen wird E-Cadherin, dessen Gen auch als Metastasierungs- oder Invasionssuppressorgen bezeichnet wird, je nach Differenzierungsgrad unterschiedlich exprimiert. Bei einer Reihe von malignen Tumoren wie dem Mamma-, Kolon- oder Nierenkarzinom konnte eine reduzierte E-Cadherin-Expression mit einer schlechteren Prognose korreliert werden. Zum Magenkarzinom liegen derzeit nur zwei Studien an nur geringen Fallzahlen vor, die auf einen negativen prognostischen Einflus der reduzierten E-Cadherin-Expression hinweisen [4, 5].

Biproportion et offre dominante (A propos de l'article d'André Torre ‘Sur la signification théorique du modèle d'offre multisectoriel')

1996

One replies here to partisans of the reject of the supply-driven model in input-output analysis and especially to A. Torre (Revue Economique, 5, 44, 951-970). First of all, demand-driven hypothesis (Leontief) and supply-driven hypothesis (Ghosh) are symmetrical and incompatible, what forbidden to reject the second to the motive that it depends on the first. Secondly, the results earlier obtained for France of 1970 to 1985 from the method of the biproportionnal filter show that there is so much instability in the long term in the columns than in the rows of the flow matrix. Thirdly, the assimilation of the usage of allocation coefficients to the adoption of the supply-side model is excessive.

"Table 3" of "Total cross-section measurement for the three double pion production channels on the proton"

1996

No description provided.

"Table 4" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Transverse momentum PTOUT w.r.t. the Shericity axis. For the first table Sphericity axis definition is from seen charged particles corrected to final state particles. For the second table Sphericity axis definition is from seen charged plus neutral particles corrected to final state charged plus neutral particles.

"Table 14" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Oblateness distribution. Corrected to final state particles.

"Table 18" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

C-Parameter distribution. Corrected to final state particles.

"Table 19" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

D-Parameter distribution. Corrected to final state particles.

"Table 2" of "Total cross-section measurement for the three double pion production channels on the proton"

1996

No description provided.

"Table 55" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

XP distribution for SIGMA(1385)+ production.. Data read from plot.

"Table 44" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

XP distribution for K*(892)+- production.. Data read from plot.

"Table 30" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Differential 3-jet rate for the JADE Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.

Medalla a títol pòstum al professor Manuel Sanchís Guarner

1996

Acte acadèmic de concessió, a títol pòstum, de la Medalla de la Universitat de València al professor Manuel Sanchís Guarner. La laudatio va ser llegida per Antoni Ferrando Francès, catedràtic de Filologia Catalana i director del Institut Interuniversitari de Filologia Valenciana.

"Table 35" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Charged particle multiplicity compiled from current LEP I data.

"Table 21" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Light-Hemisphere-Mass distribution. Corrected to final state particles.

"Table 31" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Differential 4-jet rate for the Durham Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.

"Table 2" of "Search for promptly produced heavy quarkonium states in hadronic Z decays"

1996

No description provided.

"Table 3" of "Measurement of inclusive K*(892)0, Phi(1020) and K*2(1430)0 production in hadronic Z decays."

1996

SIG in (1/SIG) is the total hadronic cross section. The statistical and systematic erros are combined quadratically. For 0.05

"Table 1" of "Search for promptly produced heavy quarkonium states in hadronic Z decays"

1996

The analysis of hadrons (from X) provides to distinguish of the various decay modes of Z-boson (see text).

"Table 2" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

"Table 12" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Thrust Major distribution. Corrected to final state particles.

"Table 26" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Difference of the Hemisphere Broadening, BDIFF. Corrected to final state particles.

"Table 1" of "Determination of sin**2 theta(w)(eff) using jet charge measurements in hadronic Z decays"

1996

The first sytematic error is due to the experimental uncertainties, whilst the second is due to the uncertainties in the quark charge separations.

"Table 2" of "First measurement of f2-prime (1525) production in Z0 hadronic decays"

1996

No description provided.

"Table 46" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

XP distribution for RHO0 production.. Data read from plot.

"Table 2" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Transverse momentum PTOUT w.r.t. the Thrust axis. For the first table Thrust axis definition is from seen charged particles corrected to final state particles. For the second table Thrust axis definition is from seen charged plus neutral particles corrected to final state charged plus neutral particles.

"Table 20" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Heavy-Hemisphere-Mass distribution. Corrected to final state particles.

"Table 1" of "Observation of orbitally excited B mesons"

1996

No description provided.

"Table 1" of "Total cross-section measurement for the three double pion production channels on the proton"

1996

No description provided.

"Table 10" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

"Table 43" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

XP distribution for K*(892)0 production.. Data read from plot.

"Table 36" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Compilation of multiplicities of pseudoscalar mesons from current LEP I data.

"Table 7" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Scaled momentum distribution, XP. Corrected to final state charged particles.

"Table 1" of "Transverse momentum of J / psi produced in oxygen uranium collisions at 200-GeV per nucleon."

1996

Two parametrization of the D(SIG)/D(PT) are used: first is : PT*exp(-SLOPE*PT**CONST(C=PT)) and second is : PT*exp(-2*MT/CONST(C=MT)).

"Table 2" of "Measurement of the forward - backward asymmetry of e+ e- ---> Z ---> b anti-b using prompt leptons and a lifetime tag"

1996

No description provided.