By Hall E. H.

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**Additional resources for An Electron Theory of Electric Conduction in Metals**

**Example text**

Kawazoe, T. Yatsui, W. Nomura, K. Kobayashi, K. Akahane, N. Yamamoto, T. Inoue, F. Peper, K. Leibnitz, M. Hoga, Y.

This corresponds to an authentic device D and an authentic reader R. Differences of the reader R are equivalent to differences of Z ; for instance, when Z is shifted by distance Z = −1/100 the angular spectrum is given by the dotted curve in Fig. 8b. Similarly, when Z = 1/100, the angular spectrum is given by the dashed curve in Fig. 8b. As shown by the changes of the curve in Fig. 8b, the slight difference with respect to Z results in a different output signal from the system. In order to quantitatively evaluate the Z -dependence, the correlation coefficient of the angular spectrum is calculated as a function of Z as summarized in Fig.

Iii) Deposition is inhibited at a position where the block sees clusters at both the left- and right-hand sides and when the total size of both clusters is larger than Bth2 . (iv) In other cases, deposition at the position succeeds 30 nm-deep groove was formed in the substrate. Also, the substrate was illuminated with light linearly polarized perpendicularly to the direction of the groove during the RF sputtering. Thanks to the well-defined edge of the groove, a strong optical near-field was generated in its vicinity.