0:00:02 | this is a very abstract for the obstacle formation of heavy the electronic ways i |
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0:00:07 | particles instrument in three within into oxygen seven |
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0:00:12 | the by layer resonate strong team three rethinking to oxygen seven often abbreviated a strong |
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0:00:19 | team three to seven is a quasar a two-dimensional natural with the familiar ground state |
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0:00:24 | it's a large electronic specific heat indicates an unusually high mass enhancement |
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0:00:29 | and then applied magnetic field strong team three to seven on the case multiple nets |
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0:00:34 | of magnetic phase transitions |
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0:00:36 | and shows consonant critical behavior as well as an exotic kinematic state |
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0:00:40 | where the transport properties break the four fold rotational send symmetry of the lattice |
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0:00:46 | actually there is much theoretical interest instrument in three to seven |
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0:00:50 | mix models developed in recent years to explained in treating phase diagram a strong team |
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0:00:55 | three to seven involve heavy coincide particles that to find a mysterious low energy scale |
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0:01:02 | in our article we present and go over so fainter that run spectroscopy experiments to |
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0:01:07 | visualize the low energy electronic structure a strong team three to seven in momentum space |
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0:01:13 | we discovered coexistence of lines and very heavy bands |
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0:01:17 | yielding an uncanny resemblance to contour type every funny on systems |
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0:01:23 | in order to test the relevance of that data for the exotic physics displayed by |
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0:01:27 | strong team three to seven in applied field we to detailed measurements not only along |
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0:01:32 | one direction but as a function of k x k y |
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0:01:36 | and energy to deliver a complete three-dimensional data set of the spectral weight sk an |
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0:01:41 | amiga |
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0:01:43 | is the last a parametrized the complex pan structures transient three to seven and importantly |
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0:01:50 | using this parameterization we can extract the phone quite five possible densities states which a |
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0:01:55 | deeper the it was a p right below the phoneme level |
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0:01:59 | using a simple model |
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0:02:00 | we show that the strongly p density of states found in the experiments can explain |
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0:02:05 | the non trivial attempted dependence of the electronic specific heat reported previously |
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0:02:11 | assuming a symposium inspecting in applied field we find that data that the quality of |
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0:02:16 | leave reproduces the strong enhancement of the electronic specific heat which was observed experimentally |
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0:02:22 | much has been related to quantum criticality |
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0:02:26 | the main focus of our goal is to provide insight into how the heavy bands |
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0:02:30 | underlying the physics a strong team three to seven a formant we find and describe |
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0:02:34 | several of s |
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0:02:36 | the presence of three need to generate t two g u one salisbury indian on |
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0:02:41 | together with binary a spacing and back holding a funny services sheets to choose structural |
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0:02:46 | distortion needs to a large number of bands near the chemical potential |
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0:02:50 | the sizable spin orbit interaction in the wreath indian forty shell which could is a |
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0:02:55 | little mixing in small hybridization gaps then gives weekly dispersing bands of mixed were able |
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0:03:00 | to character |
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0:03:01 | an extended areas of k space |
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0:03:04 | we further find a very strong |
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0:03:06 | and all sentiment independent re normalization of these bands juju electron correlation affects |
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0:03:12 | data indicate that legal electron correlations course the strong masking huntsman to the pronounced kay |
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0:03:18 | space and i stopped repeat instrument in three to seven and we expect that this |
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0:03:23 | effect is a general relevance to multi-band systems with over two mixing along the funny |
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0:03:28 | services such as many times |
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0:03:30 | and different forty transition metal oxide |
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