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NORMAN M. R. et al., Nature, 392 (1998) 157; DING H. et al., Nature, 382 (1996) 51; SHEN Z.-X. et al., Phys. Rev. Lett., 70 (1993) 1533.
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Norman, M.R.1
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NORMAN M. R. et al., Nature, 392 (1998) 157; DING H. et al., Nature, 382 (1996) 51; SHEN Z.-X. et al., Phys. Rev. Lett., 70 (1993) 1533.
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Ding, H.1
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NORMAN M. R. et al., Nature, 392 (1998) 157; DING H. et al., Nature, 382 (1996) 51; SHEN Z.-X. et al., Phys. Rev. Lett., 70 (1993) 1533.
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Shen, Z.-X.1
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CORSON J. et al., Nature, 398 (1999) 221.
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Miyakawa, N.1
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16
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0001958138
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note
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0) value is determined when the gap-like structure in tunneling spectra disappears.
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17
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0001756619
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note
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c resemble the spectra shown in fig. 2. It is not easy to make any conclusions concerning the physical meaning of this correlation which can be paraphrased as follows: tunneling spectra which look similar to the spectra shown in fig. 2 are observed as rule in more "metallic" samples.
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18
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0001830519
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edited by H. MAEDA and K. TOGANO (Marsel Dekker Inc., New York)
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HASEGAWA T., NANTOH M., OGINO M. and KITAZAWA K., in Bismuth-Based High-Temperature Superconductors, edited by H. MAEDA and K. TOGANO (Marsel Dekker Inc., New York) 1996, pp. 75-92.
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(1996)
Bismuth-Based High-Temperature Superconductors
, pp. 75-92
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Hasegawa, T.1
Nantoh, M.2
Ogino, M.3
Kitazawa, K.4
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21
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0001953429
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note
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It is difficult to indicate if the presence of this hump is meaningful or not. However, it is clear that the amplitude of this hump is much weaker than the amplitude of the hump which disappears at 110-115 K.
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24
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0001756623
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Proceedings of MOS-99 conference, Stockholm 28 July - 2 August 1999, (also cond-mat/9908052)
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MOURACHKINE A., Proceedings of MOS-99 Conference, Stockholm 28 July - 2 August 1999, to be published in J. Low Temp. Phys. (also cond-mat/9908052).
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J. Low Temp. Phys.
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Mourachkine, A.1
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25
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0001950671
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note
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However, no presence of the Bi2223 phase has been detected in our Bi2212 samples by EDAX measurements.
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