0:00:03 | superconducting versus a conducting electronic ground state in generality specific double wall carbon and l |
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0:00:09 | two s the authors of this paper doctor team chang and professor pinching or from |
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0:00:14 | the department of physics hong kong university of science and technology |
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0:00:22 | after the discovery of super conductivity and carbon and l two systems theoretical analysis show |
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0:00:28 | in quasi one-dimensional see entities electron film on interaction can offer to potential ground state |
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0:00:34 | super conductivity empires distorted from a conducting state |
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0:00:38 | then all the interaction between electrons becomes the deciding factor and screening of coulomb interaction |
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0:00:45 | is crucial for the appearance of super conductivity and cindy's the super conductivity behaviors usually |
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0:00:51 | a currency into bundles |
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0:00:53 | a single wall c n t is known to be some a conducting and zero |
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0:00:57 | temperature |
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0:00:58 | an interesting question is how about a single metallic double wall carbon and l two |
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0:01:03 | here we consider two of them the three any state and five zero fifteen zero |
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0:01:11 | respectively |
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0:01:13 | the inner tubes with strong electron phone on interaction to provide possibilities of electron for |
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0:01:19 | non related processes and the other tools are metallic so as to provide screening of |
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0:01:24 | coulomb interaction in the inner two |
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0:01:30 | interaction between electrons can have two components |
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0:01:34 | one is the attractive form on mediated coupling |
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0:01:37 | the other is the repulsive coulomb interaction |
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0:01:40 | we estimate the magnitude of the first one from the density function of theory and |
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0:01:44 | the second one is estimated with and without screening of the outer shell for comparison |
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0:01:50 | then we perform second order but normalisation group analysis to identify the system behaviors including |
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0:01:56 | process and the zero temperature ground state |
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0:02:00 | with a single c m t the electric lines spread over on the space |
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0:02:05 | this is the bare climb coupling without screening |
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0:02:08 | however if there is an outer metallic shell the coulomb interaction will be screen and |
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0:02:13 | its strength can be estimated with the random phase approximation |
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0:02:17 | it is about one to two order of magnitude smaller than their potential |
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0:02:27 | with for normalisation group analysis for single wall three and five zero z entities we |
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0:02:34 | get spirals distorted from a conducting ground state in agreement with all the prior theoretical |
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0:02:40 | predictions |
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0:02:41 | in the plots moving from zero to minus infinity along x-axis represents the crawling process |
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0:02:47 | approaching zero temperature |
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0:02:49 | the y-axis denotes the amplitude of different order parameters |
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0:02:54 | black lines to know charge density wave and red lines denote single super conductivity |
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0:03:00 | the charge density wave order is seem to diverge much faster than the superconducting order |
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0:03:05 | in both single wall see entities |
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0:03:11 | when the inner tubes are embedded in d w c entities results are quite different |
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0:03:16 | in both systems |
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0:03:18 | single super conductivity order exceeds charge density weight order in the closing process and this |
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0:03:24 | indicates that zero temperature ground state is superconducting |
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0:03:28 | the crossover temperature of three eight a t w c m t is extremely low |
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0:03:34 | while four five zero and fifteen zero is relatively higher |
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0:03:39 | this may be attributed to the difference in the electron film on coupling strength of |
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0:03:43 | the two systems |
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0:03:45 | the screening due to one or two greatly modifies the ground state |
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0:03:49 | this is the main result of our paper |
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0:03:57 | screening due to the outer shell of d w c m t sufficiently reduces column |
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0:04:01 | interaction between electrons |
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0:04:04 | the results g analysis shows two systems have superconducting ground state |
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0:04:09 | and broaden implication of our result is that most of the metallic d w c |
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0:04:13 | entities can become superconducting at low temperatures in agreement with the experiment |
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