0:00:06 | three dimensional topological insulator is a fundamentally new phase electronic matter that is captured a |
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0:00:12 | lot of interest and the condensed matter physics community over the past two or three |
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0:00:15 | years |
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0:00:16 | fundamental interest and three topological slayers |
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0:00:19 | lies in the fact that exhibit a rare type behaviour called topological order |
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0:00:24 | which describes organized movement of electrons the crystal |
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0:00:27 | a consequence of this is that their surface electronics spectrums qualitatively distinct from any ordinary |
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0:00:33 | material |
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0:00:34 | in such a way is to allow us to select constant flow would not be |
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0:00:37 | tracked by impurities |
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0:00:40 | first experimental discovery but really talk much translator was making apply this that in and |
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0:00:45 | money i think he has sounds group of princeton university falling really prediction by charles |
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0:00:51 | cans collaborators at the university of pennsylvania |
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0:00:54 | the prediction was based on the idea that pure and the money which is a |
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0:00:57 | metal would become a topological insulator taken this newly formed into an insulator |
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0:01:03 | outgoing edge when you would there's no |
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0:01:05 | was predicted to perform this the defamation |
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0:01:08 | to test for the topological slater phase the has a group search for the distinguishing |
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0:01:13 | features of the serb select runs is a window into the box topological properties |
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0:01:18 | in a general insulated with been or be coupling there can be seen or insert |
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0:01:22 | states that standard log energy get is shown in this diagram |
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0:01:26 | for an ordinary insulator these of the state always discourse such that they form even |
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0:01:31 | number for me services |
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0:01:34 | topological insulator however the number of surface form is services are |
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0:01:38 | if even right count |
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0:01:40 | is a topological distinction and it is clear that this method can only relies on |
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0:01:44 | the material in a console |
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0:01:48 | in this paper we address the question of whether they're experimental signatures the topological order |
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0:01:53 | even in pure and to money |
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0:01:55 | because it's money metallic surface take only relies on being able to separate surface reebok |
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0:02:00 | states that the from the energy |
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0:02:02 | the technique we need to do this is an angle result photo emission spectroscopy |
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0:02:07 | the basic principles that photons intentional crystal bands money and excite electrons into the backing |
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0:02:13 | by measuring the energy momentum these further we electrons the energy momentum dispersion inside the |
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0:02:19 | crystal can be deduced |
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0:02:21 | two measures then these energy and momentum analyzed electrons an accelerated towards the heavy scattering |
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0:02:27 | target |
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0:02:28 | where they will be preferential e scattered left to right based on there's interaction going |
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0:02:33 | to standard scattering |
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0:02:35 | the distinguishing properties of statistics are that there's and colourised and have no dispersion one |
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0:02:41 | a direction normal to the surface |
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0:02:43 | a typical for emission spectrum of an someone you shown here along momentum cut denoted |
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0:02:47 | by the red line |
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0:02:49 | if we look at how the state that for me energy change against bearing on |
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0:02:53 | another one surface normal direction we find it only for right branches around zero momentum |
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0:02:57 | show no dispersion |
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0:03:00 | also find that these four ranges are still polarised proving that there indeed surfaced |
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0:03:05 | there are two possible ways these service states comes first which reflect whether enter non-use |
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0:03:10 | topological or not |
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0:03:11 | if the word topological and the surface states as first in the sense shown in |
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0:03:15 | the upper panel informant had a like for me services it on the right |
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0:03:20 | if you were not topological the surface data disposition below and instead form a concentric |
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0:03:25 | circular from is this |
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0:03:27 | the dispersion certain states overall momentum space |
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0:03:31 | we experimentally find that the from step is exhibited had a light all g which |
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0:03:35 | confirms that and twenty the d topological |
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0:03:38 | our here shows that even in metal there can be signatures a topological order |
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0:03:43 | it also confirmed that topological properties of is intentionally three topological and sliders the right |
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0:03:49 | from the electronic structure event |
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0:03:52 | in future this procedure can be generally applied to search for her materials a topological |
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0:03:56 | insulator |
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