0:00:07 | or |
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0:00:10 | i representation initially we sure where a person and where you can tell you about |
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0:00:16 | a quarter was also power michael however |
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0:00:23 | the paper is control of conditional one i think i do the clearance |
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0:00:31 | our experiment is less crime interference between indistinguishable pass |
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0:00:36 | to demonstrate ground state one |
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0:00:39 | we have data with this electronic interview little structure to available at that time each |
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0:00:44 | with three d models splits at levels with energy splitting dot e |
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0:00:49 | we start in a single zero ground state in |
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0:00:53 | by one or like we can try transition to and that was your state right |
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0:01:00 | after characteristic a time |
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0:01:02 | that indicate that are the grass to mandible and a simple song |
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0:01:07 | conservation of momentum allows to indicate that is |
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0:01:10 | and want to be here are those people's plusminus one states |
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0:01:16 | using coordination measurements a new method works on |
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0:01:19 | you can build rather than which electronically to an angle |
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0:01:24 | however are correlation interests cannot tell us which individual little electronic and it's a superposition |
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0:01:31 | unit was minus one states |
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0:01:34 | conditional on the detection of appropriate |
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0:01:38 | and seventy absorption of another over time from the right is or |
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0:01:41 | that is part of the superposition involves frequency proportional to energy splitting |
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0:01:47 | which is the opposite sign for each state in the superposition |
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0:01:53 | problems portion of the time from the try |
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0:01:55 | the superposition is coherently cited |
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0:01:57 | and stress first right now |
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0:02:00 | finally the atom to separate |
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0:02:03 | you single iteration measurements you'd order out of photons which hero indicate that and that |
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0:02:08 | equals your state |
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0:02:10 | the probability of this occurring equal to this where users you amplitude |
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0:02:15 | would you can be induced interference between arts assigned a solutions of the components of |
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0:02:21 | the relative position |
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0:02:23 | our data reflects the probability measure that conditional on the detection of first which pair |
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0:02:30 | of the relative position |
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0:02:32 | the data exhibits quantity into which gives as a measure of the coherence in the |
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0:02:37 | ground state position |
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0:02:40 | andreas number one at a more of our experimental and how women feedback mechanism to |
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0:02:46 | preserve coherence in the ground station |
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0:02:50 | this interference correspondingly that chris us introduce a can be experimentally realise using for example |
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0:02:58 | we have any five times which we can obtain |
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0:03:02 | to anatomically i and working i will explain a little bit more about the experimental |
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0:03:09 | part |
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0:03:11 | so we practise religion doesn't come nearly individually a pitch in little boxes run time |
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0:03:18 | i and so we use an alternate approach |
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0:03:22 | what we actually is the device that produces that these are |
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0:03:27 | and with an arrangement of lisa's a nine year old we only use quite intimate |
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0:03:33 | contact e |
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0:03:34 | we just analyzer small problem this task it but doesn't make the left and right |
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0:03:39 | many atoms that time and the outgoing what would be a scatter masks and i |
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0:03:43 | s |
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0:03:45 | so that we rely on a clever sure that uses something called not compactly and |
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0:03:50 | i'll go values just basically information to two years facing each other |
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0:03:56 | and when you shine light on the one last time for many times and a |
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0:04:02 | dash |
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0:04:03 | with this configuration we can wait for a single but in this brochure the on |
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0:04:10 | that selecting the interaction between the driver but constantly at the gap also serve to |
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0:04:15 | final the one that the atoms of this makes it much easier to master in |
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0:04:20 | a systematic way |
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0:04:21 | the driver's on israeli for instance interaction with the atom is characterized by the release |
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0:04:26 | of the segments are for the |
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0:04:29 | as long as the cavity we filter out the polarised right but on polarised and |
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0:04:34 | time step derive a limited but |
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0:04:38 | this process is iterated thousands of times second for different items and the interference can |
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0:04:43 | be as their statistical this during an appearance that indicates over time due to environmental |
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0:04:47 | and that is what we can't control |
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0:04:51 | so what we actually not doing with our experiment is we use one of our |
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0:04:56 | detectors to do some feedback on our experiments where we chernoff momentarily are directly so |
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0:05:04 | this has the effect of increased amplitude on the interference pattern you saw before |
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0:05:11 | a two factors to a which translates to are superposition living longer in the in |
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0:05:18 | protected against something covariance processes |
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0:05:21 | ultimately what we wanna do with our experiment is trying to preserve the superposition as |
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0:05:27 | long as possible |
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0:05:29 | many people especially in the information area are interested in using a function positions |
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0:05:39 | two |
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0:05:41 | that story information they wanna map some information store in light for example in to |
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0:05:48 | a |
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0:05:50 | into the electronic energy level of and then extract that back and forth hans and |
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0:05:57 | then built in this week one networks and other devices |
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0:06:03 | our goal for this experiment was simply to keep the superposition i alive this long |
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0:06:09 | as possible with a fast very simple feedback |
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