0:00:02 | bright iambs at the use of energy a professor in the department of physics of |
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0:00:06 | the indian institute of technology con for these are my collaborators mister work we show |
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0:00:10 | admissible with someone that might be these students and prosody achieved among right from the |
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0:00:15 | university of tokyo |
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0:00:16 | the relatively low density ordered vortex so that a sensible conduct that smells into a |
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0:00:20 | higher density disordered vortex liquid phase under the influence of an ensemble fluctuations |
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0:00:26 | shown below is a schematic representation of the behavior of the sheer elastic more like |
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0:00:30 | of the vortex like that of the function of increasing magnetic |
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0:00:34 | what x melting is the expected whenever the vortex lattices are namely when the elastic |
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0:00:39 | more like is low at low and high magnetic at low magnetic field theoretically a |
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0:00:44 | transformation from the vortex liquid two solid phase is expected you to the and hunting |
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0:00:49 | stiffness of the lattice due to increasing in the vortex interactions with increasing magnetic field |
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0:00:54 | in the present study we have investigated the nature of the low we walked experience |
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0:00:59 | i feel mending is an already well studied phenomena |
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0:01:02 | using the high sensitivity magnet optical imaging setup a lot the tidy contour we measure |
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0:01:08 | the local magnetic field distribution inside this upon the though |
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0:01:12 | shown here is a schematic of the local field distribution of process above conducted you |
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0:01:16 | but the presence of what this is the |
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0:01:18 | the local magnetic field is proportional to the density of porpoises in this apartment |
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0:01:24 | we measure the local magnetic field distribution inside the material by measuring the intensity of |
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0:01:31 | the parity rotated linearly polarised light |
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0:01:34 | you know what experiment we have attempted to measure the changes in the vortex tensity |
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0:01:39 | you to face transformations in the vortex state at low magnetic |
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0:01:44 | these are differential magnet optical images captured at fifty calibre in which represent the changes |
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0:01:49 | in the local magnetic field produced in response to the next on a field modulation |
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0:01:54 | of one gauss which is applied at each of the measuring applied magnetic |
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0:02:00 | nor the bright white regions in these images corresponds to what actually with bottles where |
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0:02:05 | there is a comparatively larger change in the local magnetic field or vortex tensity |
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0:02:10 | our initial investigations show an initial low field vortex liquid phase which sustains larger changes |
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0:02:17 | in the vortex tensity settling down into a vortex solid phase at heart magnetic field |
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0:02:24 | with sustained smaller changes in the vortex tensity furthermore |
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0:02:28 | new creation of the vortex solid phase is characterized by the disappearance of shielding cartons |
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0:02:33 | within the vortex solid regions ad is noted with then circled region and also with |
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0:02:39 | the saddle |
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0:02:41 | based on such studies we have identified the vortex liquid the solid melting line experimentally |
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0:02:48 | this experimentally determined based on the shen boundary is also matching well with the theoretically |
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0:02:54 | predicted melting line at low magnetic field in be infeasible conductors |
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0:03:00 | around this mending phrase boundary we have also identified a le de marco existence but |
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0:03:05 | the vortex solid and liquid phases coexist |
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0:03:08 | using our magnet optical imaging technique we spatially it is all the information on relaxation |
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0:03:14 | of them in a magnet isolation at different locations in the sample which we used |
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0:03:19 | to reduce the pinning landscape across the sample |
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0:03:22 | the variation in pinning across different regions of the sample are represented by the coloured |
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0:03:27 | bar the present beside the coloured image of the sample |
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0:03:31 | we find that the location of the low in vortex liquid the solid based on |
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0:03:35 | that and boundary shifts but radiation in training |
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0:03:40 | which is well described by the effectively in the men but increasing with the pinning |
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0:03:45 | strand thank you |
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