0:00:03 | although i material are |
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0:00:05 | one of the authors of disordered rhythm also phase coherence and acquires i two d |
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0:00:08 | call that obsessed |
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0:00:10 | we present evidence the disorder can drive phase fluctuations in two d systems |
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0:00:14 | results the may help explain the super conducted insulator phase transition in disorder two d |
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0:00:18 | super conductors |
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0:00:20 | although this covered in nineteen eighty seven the underlying mechanism that explains their super conductivity |
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0:00:24 | is still open here |
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0:00:27 | i temperature copper oxide super conductors are made of stacks of weakly coupled planes of |
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0:00:31 | atoms and the physics of this order to use systems seems to play a large |
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0:00:34 | role in determining the material properties |
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0:00:37 | we model the point of the super conductor with two parallel search for shape the |
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0:00:41 | time examples are well controlled |
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0:00:43 | all trickle gas |
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0:00:44 | we show that the phase coherence of the plane spanish as faster than the fraction |
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0:00:48 | of coherent atoms as we increase disorders |
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0:00:50 | this reveals the disorder drive strong phase fluctuations in tv systems |
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0:00:55 | these phase fluctuations in turn are expected to drive a transition from a high temperature |
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0:00:59 | superconducting state to a normal state |
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0:01:01 | but are harder to see in these materials |
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0:01:05 | our experiment begins with an optically track three d pose einstein contents a rib idiom |
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0:01:10 | eighty seven times |
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0:01:11 | which we split into two i'm couple because i two d planes using intersecting laser |
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0:01:16 | being |
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0:01:17 | this order is introduced by optical spectral |
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0:01:20 | which causes the atoms to be repelled regions of higher intensity |
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0:01:23 | we're just disorders right by controlling intensity of the spectral be |
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0:01:29 | to make measurements with suddenly turn off the confinement and the disorder |
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0:01:33 | planes expand rapidly overlapping informing interference pattern seen absorption images |
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0:01:38 | the visibility of these interference fringes |
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0:01:41 | tells us the phase coherence of our clan |
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0:01:43 | perpendicular to the interference pattern we observe the momentum of the atoms |
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0:01:47 | and the two component distribution |
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0:01:49 | with the incoherent formal atoms forming a broad background and which a coherent adam so |
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0:01:54 | in the centre |
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0:01:55 | we much about the temperature of our plans from the with the remote distribution as |
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0:01:59 | well as a fraction of coherent at |
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0:02:02 | we can adjust the initial phase based density of the atoms before adding the disorder |
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0:02:06 | analogous to controlling the temperature |
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0:02:08 | you know sell |
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0:02:10 | this allows us to produce cue based i |
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0:02:13 | with this order shrink along why |
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0:02:16 | in face-to-face density along x |
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0:02:18 | one phase diagram shows range visibility and the other shows go a higher fraction |
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0:02:22 | without disorder |
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0:02:24 | this fraction closely tracks the visibility of the interference |
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0:02:27 | however as we increase the disorders right this is no longer true as can be |
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0:02:32 | observed in the upper right corner |
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0:02:33 | of the phase diagrams |
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0:02:35 | where the coherent retraction phase diagram |
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0:02:37 | is much darker than the visibility based |
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0:02:40 | we can further quantify this by integrating the phase diagrams |
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0:02:44 | along the phase based density s |
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0:02:47 | clearly |
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0:02:47 | these two quantities that tracking each other high disorders |
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0:02:52 | although we don't see if a transition in a relatively small finite system |
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0:02:56 | our results show that disorder generically dries phase fluctuations in quality systems |
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0:03:01 | is phase fluctuations i thought to be a mechanism behind the superconducting phase transition in |
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0:03:06 | high temperature super conductors and this is the first direct observation of disorder causing these |
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0:03:10 | phase fluctuations |
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