Clowninnen: Portrait einer Berufsgruppe /// Arbeitspapiere / Institut für Ethnologie und Afrikastudien ; 76

Clowninnen. Portrait einer Berufsgruppe Eine neue Berufsgruppe etabliert sich: Die Clownin! Seit den 1980er Jahren treten vermehrt Frauen als Clownin in die europäische Öffentlichkeit. Sie erobern zunehmend weitere gesellschaftliche Bereiche, treten aus dem Zirkus heraus, hinein in die wirtschaftliche, religiöse, medizinische, pädagogische und soziale Sphäre. Die Erweiterung der Arbeitsfelder beinhaltet differenzierte Aktionsmöglichkeiten für die Clownin und prägt die Beziehung zu den Zuschauern, die vom Einzelkontakt z.B. im Altenheim über Seminargruppen bis hin zu hunderten von Personen bei Bühnenstücken reichen. Die Zugangswege zur Clownsarbeit sind individuell, wobei sich die früher typisch familiäre Bindung in Zirkus- und anderen Künstlerfamilien nicht mehr finden lässt. Das Clown-Sein begreifen die Frauen als einen Prozess, der vor allem durch Persönlichkeitsarbeit und Lebenserfahrung geprägt ist. Bestimmte Aspekte des Clowns erschließen sich erst im und durch das Clownsspiel, wobei immer wieder Grenzen auf persönlicher und gesellschaftlicher Ebene aufgebrochen werden. Kernstück der Studie bilden zehn qualitative Interviews mit Frauen aus Deutschland und der Schweiz, die beruflich als Clownin in unterschiedlichen Arbeitsfeldern tätig sind. Ergänzend beobachtete die Autorin Auftritte in verschiedenen Arbeitsbereichen und führte eine Befragung an 16 Clownsschulen durch. Ziel dieser Studie ist es, Ausbildungswege, Arbeitsfelder und Arbeitsweisen dieser neuen Berufsgruppe aus emischer Sicht darzulegen. Vertiefend wird das Selbstverständnis der Clowninnen vorgestellt. Welche Ziele verfolgen die Frauen in ihrer Arbeit und wo sehen sie die Grenzen des Clowns? Welche Bedeutung messen sie der Spiritualität und dem Tod zu? Wie gestaltet sich das Wechselspiel zwischen Privatperson und Clownin? In mehreren Portraits und in vergleichenden Darstellungen finden sich Antworten auf diese Fragen, bei denen die Frauen durch vielfältige Zitate immer wieder selber zu Wort kommen.

Misura del flusso triangolare v3 di adroni identificati in collisioni Pb-Pb a √s_NN = 2.76 TeV con l'esperimento ALICE a LHC

In questo lavoro di tesi è presentata la misura con il rivelatore ALICE del flusso triangolare, v3, di pioni, kaoni e protoni prodotti in collisioni PbPb a LHC. Il confronto di v3 con le previsioni di modelli idrodinamici permette di vincolare maggiormente le assunzioni sulle condizioni iniziali del sistema presenti nei diversi modelli ed estrarre una stima maggiormente precisa delle proprietà del mezzo come la viscosità. La misura è effettuata nella regione di pseudorapidità centrale sui dati raccolti da ALICE nel 2010 e 2011 e utilizza una tecnica di identificazione basata sia sulla misura della perdita di energia specifica, con la camera a proiezione temporale (TPC), sia la misura della velocità con il sistema a tempo di volo (TOF). La combinazione di entrambe le tecniche permette di separare le diverse specie in un intervallo esteso di impulsi con elevata efficienza e purezza. Per la misura del piano di reazione è stato utilizzato il rivelatore VZERO che misura la molteplicità delle particelle cariche in una regione di pseudorapidità disgiunta da quella in cui è misurato v3. La misura ottenuta è confrontata con le previsioni di modelli idrodinamici attualmente più utilizzati.

Intense therapy in patients with locally advanced esophageal cancer beyond hope for surgical cure: a prospective, multicenter phase II trial of the Swiss Group for Clinical Cancer Research (SAKK 76/02)

There is no standard treatment for patients with locally advanced esophageal carcinoma without systemic metastasis in whom surgery is no longer considered a reasonable option.

Investigation of border disease and bovine virus diarrhoea in sheep from 76 mixed cattle and sheep farms in eastern Switzerland

The purpose of this study was to examine the occurrence of sheep persistently infected with Border disease virus (BDV) on 76 mixed cattle and sheep farms and whether seroconversion to BDV infection occurred in cattle of these farms. Seroprevalence of BDV and bovine viral disease virus (BVDV) infection in sheep was also investigated. Quantitative RT-PCR for pestivirus detection and an ELISA to detect pestivirus antibodies were used in 2'384 and 2'291 ovine blood samples, respectively. Another 27 seropositive sheep from ten flocks underwent serum neutralization testing to differentiate between BDV and BVDV antibodies. A BDV titre that was at least four times higher than the BVDV titre was interpreted as the result of BDV infection. Titres against BVDV were interpreted in an analogous fashion. All examined sheep were pestivirus-negative, 310 sheep were seropositive, 119 had an indeterminate titre and 1'862 were seronegative. The flock seroprevalence ranged from 0.0 to 73.9 %. Three of the 27 flocks that underwent serum neutralization testing were interpreted as BDV-infected because of 6 sheep with higher BDV titres, and 6 flocks were interpreted as BVDV-infected because of 14 sheep with higher BVDV titres.

Measurement of the distributions of event-by-event flow harmonics in lead-lead collisions at = 2.76 TeV with the ATLAS detector at the LHC

The distributions of event-by-event harmonic flow coefficients v_n for n=2-4 are measured in sqrt(s_NN)=2.76 TeV Pb+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using charged particles with transverse momentum pT> 0.5 GeV and in the pseudorapidity range |eta|<2.5 in a dataset of approximately 7 ub^-1 recorded in 2010. The shapes of the v_n distributions are described by a two-dimensional Gaussian function for the underlying flow vector in central collisions for v_2 and over most of the measured centrality range for v_3 and v_4. Significant deviations from this function are observed for v_2 in mid-central and peripheral collisions, and a small deviation is observed for v_3 in mid-central collisions. It is shown that the commonly used multi-particle cumulants are insensitive to the deviations for v_2. The v_n distributions are also measured independently for charged particles with 0.51 GeV. When these distributions are rescaled to the same mean values, the adjusted shapes are found to be nearly the same for these two pT ranges. The v_n distributions are compared with the eccentricity distributions from two models for the initial collision geometry: a Glauber model and a model that includes corrections to the initial geometry due to gluon saturation effects. Both models fail to describe the experimental data consistently over most of the measured centrality range.

Measurement of the jet radius and transverse momentum dependence of inclusive jet suppression in lead-lead collisions at sqrtsNN=2.76 TeV with the AT detector

Measurements of inclusive jet suppression in heavy ion collisions at the LHC provide direct sensitivity to the physics of jet quenching. In a sample of lead-lead collisions at root S-NN = 2.76 TeV corresponding to an integrated luminosity of approximately 7 mu b(-1), ATLAS has measured jets with a calorimeter system over the pseudorapidity interval vertical bar eta vertical bar < 2.1 and over the transverse momentum range 38 < pT <210 GeV. Jets were reconstructed using the anti-k(t) algorithm with values for the distance parameter that determines the nominal jet radius of R = 0.2, 0.3, 0.4 and 0.5. The centrality dependence of the jet yield is characterized by the jet "central-to-peripheral ratio," R-CP. Jet production is found to be suppressed by approximately a factor of two in the 10% most central collisions relative to peripheral collisions. R-CP varies smoothly with centrality as characterized by the number of participating nucleons. The observed suppression is only weakly dependent on jet radius and transverse momentum. These results provide the first direct measurement of inclusive jet suppression in heavy ion collisions and complement previous measurements of dijet transverse energy imbalance at the LHC.

Measurement of the Azimuthal Angle Dependence of Inclusive Jet Yields in Pb+Pb Collisions at sqrts_NN= 2.76 TeV with the ATLAS detector

Measurements of the variation of inclusive jet suppression as a function of relative azimuthal angle, Delta phi, with respect to the elliptic event plane provide insight into the path-length dependence of jet quenching. ATLAS has measured the Delta phi dependence of jet yields in 0.14 nb(-1) of root s(NN) = 2.76 TeV Pb + Pb collisions at the LHC for jet transverse momenta p(T) > 45 GeV in different collision centrality bins using an underlying event subtraction procedure that accounts for elliptic flow. The variation of the jet yield with Delta phi was characterized by the parameter, nu(jet)(2), and the ratio of out-of-plane (Delta phi similar to pi/2) to in-plane (Delta phi similar to 0) yields. Nonzero nu(jet)(2) values were measured in all centrality bins for p(T) < 160 GeV. The jet yields are observed to vary by as much as 20% between in-plane and out-of-plane directions.

Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector

The inclusive jet cross-section has been measured in proton-proton collisions at root s = 2.76 TeV in a dataset corresponding to an integrated luminosity of 0.20 pb(-1) collected with the ATLAS detector at the Large Hadron Collider in 2011. Jets are identified using the anti-k(t) algorithm with two radius parameters of 0.4 and 0.6. The inclusive jet double-differential cross-section is presented as a function of the jet transverse momentum p(T) and jet rapidity y, covering a range of 20 <= p(T) < 430 GeV and vertical bar y vertical bar < 4.4. The ratio of the cross-section to the inclusive jet cross-section measurement at root s = 7 TeV, published by the ATLAS Collaboration, is calculated as a function of both transverse momentum and the dimensionless quantity x(T) = 2p(T)/root s, in bins of jet rapidity. The systematic uncertainties on the ratios are significantly reduced due to the cancellation of correlated uncertainties in the two measurements. Results are compared to the prediction from next-to-leading order perturbative QCD calculations corrected for non-perturbative effects, and next-to-leading order Monte Carlo simulation. Furthermore, the ATLAS jet cross-section measurements at root s = 2.76 TeV and root s = 7 TeV are analysed within a framework of next-to-leading order perturbative QCD calculations to determine parton distribution functions of the proton, taking into account the correlations between the measurements.