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If we see a film, we experience the passing time in two ways. On the one hand, it is conveyed as the time in which the film action takes place – felt as “lived” time. On the other hand, via camera travels and movements of objects vertically to the picture plane, time is perceived – in a much more indirect way – as a vehicle for representation of spatial depth. It is this link between space and time where the method of “time tilting” introduced here sets in. When a film scene is “time-tilted”, one of the spatial dimensions (here the horizontal direction of the picture plane) is interchanged with the time dimension: In a first step, the pictures of the scene are digitalized. Then, the thus gained pixels of all pictures of the scene are arranged into a three-dimensional data field. Finally, a new series of pictures is read out, along one of the two former picture axes, which is then shown as a scene of moving pictures. The resulting film will present optical phenomena which are, on the one hand, aesthetically appealing and, on the other hand, informative for film analysis. First examples demonstrate how the procedure operates on basic movements in space as well as on camera travels in space.
Bei der Vorführung eines Films wirkt die ablaufende Zeit auf den Zuschauer in zweierlei Weise. Zum einen als die Zeit, in der die Filmhandlung stattfindet und die als gelebte Zeit empfunden wird. Zum anderen, sehr viel indirekter, als Vehikel zur Darstellung von Raumtiefe durch Kamerafahrten und Objektbewegungen senkrecht zur Bildebene. An dieser Verknüpfung von Raum und Zeit setzt die hier vorgestellte Methode „Zeitkippen“ an. Beim Zeitkippen einer Filmszene wird eine der Raumdimensionen (hier die Horizontale der Bildebene) mit der Zeitachse vertauscht: Im ersten Schritt digitalisiert man die Szene. Dann fügt man die Bildpunkte (Pixel) aller Szenen bilder in ein dreidimensionales Datenfeld. Schließlich liest man entlang einer der beiden ehemaligen Bildfeldachsen eine neue Bildserie aus, die man als Bewegtbild-Szene vorführt. Dabei entstehen einerseits ästhetisch ansprechende und andererseits filmanalytisch auf schlussreiche optische Phänomene. Erste Beispiele zeigen, wie sich das Verfahren auf grundlegende Bewegungen im Raum sowie Kamerafahrten im Raum auswirkt.
S. 1 Camera obscura (vom Höhlenmenschen zum Realismus der Aufklärung) S. 2 Laterna magica (von der Zauberlaterne zum Beamer) S. 3 Photographie (vom Unikat zum Massenmedium) S. 4 Stereographie (von Großvaters Aktfoto zur 3D-Virtualität) S. 6 Phasenbilder (von Bewegungsphasen zur Kinematographie) S. 7 Film (von den Lumieres zur Video-DVD) S. 8 Weltbild (das Raum-Zeit-Kontinuum als 4D-Bild)
Vortrag gehalten bei der 34. Jahrestagung des Fachverbandes Medien und Technik im Bildungsbereich (MTB) am 25. September 2003 in Göttingen: "Sehr verehrte Damen und Herren, „Video goes online“ ist ganz allgemein etwas, das auch ohne unser Zutun passieren wird. Wie weit und wie schnell es in die praktische Lehre eindringen wird, wage ich angesichts des heutigen Einsatzes sehr viel älterer Medientechnologien im deutschen Hochschulunterricht nicht abzuschätzen. Damit wäre ich eigentlich am Ende meines Vortrags. Dennoch möchte ich sie mit einigen Gedanken konfrontieren, die um die Frage kreisen: Gibt es für einen künftigen, Internet basierten Einsatz hinreichend geeignete Videos und wie müssen die beschaffen sein?.."
The ALICE Zero Degree Calorimeter system (ZDC) is composed of two identical sets of calorimeters, placed at opposite sides with respect to the interaction point, 114 meters away from it, complemented by two small forward electromagnetic calorimeters (ZEM). Each set of detectors consists of a neutron (ZN) and a proton (ZP) ZDC. They are placed at zero degrees with respect to the LHC axis and allow to detect particles emitted close to beam direction, in particular neutrons and protons emerging from hadronic heavy-ion collisions (spectator nucleons) and those emitted from electromagnetic processes. For neutrons emitted by these two processes, the ZN calorimeters have nearly 100% acceptance.
During the √sNN = 2.76 TeV Pb-Pb data-taking, the ALICE Collaboration studied forward neutron emission with a dedicated trigger, requiring a minimum energy deposition in at least one of the two ZN. By exploiting also the information of the two ZEM calorimeters it has been possible to separate the contributions of electromagnetic and hadronic processes and to study single neutron vs. multiple neutron emission.
The measured cross sections of single and mutual electromagnetic dissociation of Pb nuclei at √sNN = 2.76 TeV, with neutron emission, are σsingle EMD = 187:4 ± 0.2 (stat.)−11.2+13.2 (syst.) b and σmutual EMD = 5.7 ± 0.1 (stat.) ±0.4 (syst.) b, respectively [1]. This is the first measurement of electromagnetic dissociation of 208Pb nuclei at the LHC energies, allowing a test of electromagnetic dissociation theory in a new energy regime. The experimental results are compared to the predictions from a relativistic electromagnetic dissociation model.
The transverse momentum distributions of the strange and double-strange hyperon resonances (Σ(1385)±, Ξ(1530)0) produced in p–Pb collisions at sNN−−−√=5.02 TeV were measured in the rapidity range −0.5<yCMS<0 for event classes corresponding to different charged-particle multiplicity densities, ⟨dNch/dηlab⟩. The mean transverse momentum values are presented as a function of ⟨dNch/dηlab⟩, as well as a function of the particle masses and compared with previous results on hyperon production. The integrated yield ratios of excited to ground-state hyperons are constant as a function of ⟨dNch/dηlab⟩. The equivalent ratios to pions exhibit an increase with ⟨dNch/dηlab⟩, depending on their strangeness content.
The transverse momentum distributions of the strange and double-strange hyperon resonances (Σ(1385)±, Ξ(1530)0) produced in p-Pb collisions at sNN−−−√=5.02 TeV were measured in the rapidity range −0.5<yCMS<0 for event classes corresponding to different charged-particle multiplicity densities, ⟨dNch/dηlab⟩. The mean transverse momentum values are presented as a function of ⟨dNch/dηlab⟩, as well as a function of the particle masses and compared with previous results on hyperon production. The integrated yield ratios of excited to ground-state hyperons are constant as a function of ⟨dNch/dηlab⟩. The equivalent ratios to pions exhibit an increase with ⟨dNch/dηlab⟩, depending on their strangeness content.
The transverse momentum distributions of the strange and double-strange hyperon resonances (Σ(1385)±, Ξ(1530)0) produced in p-Pb collisions at sNN−−−√=5.02 TeV were measured in the rapidity range −0.5<yCMS<0 for event classes corresponding to different charged-particle multiplicity densities, ⟨dNch/dηlab⟩. The mean transverse momentum values are presented as a function of ⟨dNch/dηlab⟩, as well as a function of the particle masses and compared with previous results on hyperon production. The integrated yield ratios of excited to ground-state hyperons are constant as a function of ⟨dNch/dηlab⟩. The equivalent ratios to pions exhibit an increase with ⟨dNch/dηlab⟩, depending on their strangeness content.
The transverse momentum distributions of the strange and double-strange hyperon resonances (Σ(1385)±,Ξ(1530)0) produced in p–Pb collisions at √sNN = 5.02 TeV were measured in the rapidity range −0.5<yCMS<0 for event classes corresponding to different charged-particle multiplicity densities, ⟨dNch/dηlab⟩. The mean transverse momentum values are presented as a function of ⟨dNch/dηlab⟩, as well as a function of the particle masses and compared with previous results on hyperon production. The integrated yield ratios of excited to ground-state hyperons are constant as a function of ⟨dNch/dηlab⟩. The equivalent ratios to pions exhibit an increase with ⟨dNch/dηlab⟩, depending on their strangeness content.