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An example of such series of MDM’s for the OD 69 K Pb-BSCCO sample measured at room temperature is available at the following address: www.ifw-dresden.de/iff/11/spec/areas/cuprat/bmb(Formula presented)wave.avi. In this “movie” the binding energy is represented on the time axis, as the constant energy surface moves down and up through the electronic states. All of the MDM’s contained in the movie are self-normalized and the binding energy interval covered is (Formula presented) to 200 meV
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An example of such series of MDM’s for the OD 69 K Pb-BSCCO sample measured at room temperature is available at the following address: www.ifw-dresden.de/iff/11/spec/areas/cuprat/bmb(Formula presented)wave.avi. In this “movie” the binding energy is represented on the time axis, as the constant energy surface moves down and up through the electronic states. All of the MDM’s contained in the movie are self-normalized and the binding energy interval covered is (Formula presented) to 200 meV.
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Strictly speaking, an exactly vertical line will not correspond to a single k value. The intensity at higher binding energy in a single EDC is given by electrons which have lower absolute values of momentum than those originating from zero binding energy that follows directly from the relation between (Formula presented) and the photoelectron kinetic energy. This assigns a finite momentum window to every EDC. The size of this window is sometimes comparable with momentum resolution and therefore should be taken into account when, for instance, integrated intensity is concerned
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Strictly speaking, an exactly vertical line will not correspond to a single k value. The intensity at higher binding energy in a single EDC is given by electrons which have lower absolute values of momentum than those originating from zero binding energy that follows directly from the relation between (Formula presented) and the photoelectron kinetic energy. This assigns a finite momentum window to every EDC. The size of this window is sometimes comparable with momentum resolution and therefore should be taken into account when, for instance, integrated intensity is concerned.
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It has been shown, however, that a more detailed analysis can still distinguish between the true FS crossings and “false” ones (see Ref. 14).
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Asensio, M.C.5
Tajima, S.6
Gu, G.D.7
Koshizuka, N.8
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47
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85038298333
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The FS maps shown in Fig. 66 show the FS arc around the nodal direction with unprecedented clarity. This fact is due to (i) an intensity enhancement coming from the symmetry selection rules, as in this case the E vector of the ca. 40% linearly polarized component of the He I radiation was aligned perpendicular to the (Formula presented) direction and (ii) the high overall angular resolution for measurement in this direction leading to the large signal to background ratio seen in Fig. 11
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The FS maps shown in Fig. 66 show the FS arc around the nodal direction with unprecedented clarity. This fact is due to (i) an intensity enhancement coming from the symmetry selection rules, as in this case the E vector of the ca. 40% linearly polarized component of the He I radiation was aligned perpendicular to the (Formula presented) direction and (ii) the high overall angular resolution for measurement in this direction leading to the large signal to background ratio seen in Fig. 11.
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48
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85038274487
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MDM normalization using a signal that varies quickly in k space will give unphysical results. This would occur if the normalization signal was a “scaled down version” of the original (Formula presented)-MDM, as could easily be the case taking the intensity above (Formula presented) for finite temperatures
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MDM normalization using a signal that varies quickly in k space will give unphysical results. This would occur if the normalization signal was a “scaled down version” of the original (Formula presented)-MDM, as could easily be the case taking the intensity above (Formula presented) for finite temperatures.
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