-
15
-
-
0035907835
-
-
(formula presented) beyond 60 T is evaluated by a fit to (formula presented) at different temperatures. This evaluation is insensitive to the detailed functional form of the fit
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T. Shibauchi, Phys. Rev. Lett.86, 5763 (2001). (formula presented) beyond 60 T is evaluated by a fit to (formula presented) at different temperatures. This evaluation is insensitive to the detailed functional form of the fit.
-
(2001)
Phys. Rev. Lett.
, vol.86
, pp. 5763
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-
Shibauchi, T.1
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16
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-
0000174103
-
-
The origin of the peak in (formula presented) (and the negative magnetoresistance above) comes from the, -axis dissipation being a parallel two-channel tunneling process: (i) (formula presented) of Cooper pairs and (ii) (formula presented) of quasiparticles, i.e., (formula presented) With increasing field the Josephson contribution decreases while the quasiparticle one increases
-
N. Morozov, Phys. Rev. Lett.84, 1784 (2000). The origin of the peak in (formula presented) (and the negative magnetoresistance above) comes from the c-axis dissipation being a parallel two-channel tunneling process: (i) (formula presented) of Cooper pairs and (ii) (formula presented) of quasiparticles, i.e., (formula presented) With increasing field the Josephson contribution decreases while the quasiparticle one increases.
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 1784
-
-
Morozov, N.1
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20
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-
0033706273
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-
The true normal state resistivity (formula presented) was mapped via tunneling spectroscopy of micron-size mesa-shaped BSCCO structures at high-bias (above the gap energy) voltages by, It was found to be, -linear even below (formula presented)
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The true normal state resistivity (formula presented) was mapped via tunneling spectroscopy of micron-size mesa-shaped BSCCO structures at high-bias (above the gap energy) voltages by V M. Krasnov, Phys. Rev. Lett.84, 5860 (2000). It was found to be T-linear even below (formula presented)
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(2000)
Phys. Rev. Lett.
, vol.84
, pp. 5860
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-
Krasnov, V.M.1
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21
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-
0030146242
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-
BSCCO, (formula presented) at the first-order melting transition at high temperatures is over (formula presented) times smaller than that in the normal state
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K. Kadowaki, Physica C263, 164 (1996). In BSCCO, (formula presented) at the first-order melting transition at high temperatures is over (formula presented) times smaller than that in the normal state.
-
(1996)
Physica C
, vol.263
, pp. 164
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-
Kadowaki, K.1
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23
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-
4243964989
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-
The systematic dependence of (formula presented) on, gives (formula presented) at (formula presented)
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T. Watanabe, T. Fujii, and A. Matsuda, Phys. Rev. Lett.79, 2113 (1997). The systematic dependence of (formula presented) on p gives (formula presented) at (formula presented)
-
(1997)
Phys. Rev. Lett.
, vol.79
, pp. 2113
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-
Watanabe, T.1
Fujii, T.2
Matsuda, A.3
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30
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-
0001504077
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-
The measured effective viscocity (formula presented) in BSCCO in the flux-flow regime is about 10 times smaller than the estimated Bardeen-Stephen value
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L N. Bulaevskii, Phys. Rev. B50, 3507 (1994). The measured effective viscocity (formula presented) in BSCCO in the flux-flow regime is about 10 times smaller than the estimated Bardeen-Stephen value.
-
(1994)
Phys. Rev. B
, vol.50
, pp. 3507
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-
Bulaevskii, L.N.1
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