0:00:03 | i mean i will have something about the latest submission to usual |
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0:00:09 | but pressure remotes and saw that structure a promising candidate continues very effective information |
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0:00:16 | the speech along coherence times in many of them can be degraded micron size |
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0:00:22 | and this paper we propose and analyze to make an given in table scraps operations |
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0:00:28 | on a localised pressure |
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0:00:31 | inter annotator |
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0:00:33 | transmit and state between the every week but |
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0:00:37 | all these operations control instantly modulating driving laser intensity |
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0:00:43 | let us now briefly review the van on optical spring effect |
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0:00:47 | just as the basis for scheme |
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0:00:49 | in addition unlighted training and it smoothly changing the position of them are also because |
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0:00:56 | it is resting frequency which affect the lives intensity circulating inside the cavity |
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0:01:02 | the not so it's radiation pressure imposed on the matter which is proportional to like |
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0:01:07 | intensity |
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0:01:09 | thus |
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0:01:10 | for depends on the position of the marrow |
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0:01:13 | under certain conditions as well as can be expressed as the remote of a conservative |
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0:01:18 | potential |
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0:01:21 | the assume that the motion of the narrow can be more the santa monica last |
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0:01:26 | night |
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0:01:27 | we can easily incorporated this into the potential picture adding inharmonic potentially to the radiation |
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0:01:33 | pressure country |
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0:01:35 | the most of them there is not affected what and which are just the harmonic |
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0:01:41 | and radiation pressure |
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0:01:44 | detecting potential you just a little the meeting in which can be robust |
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0:01:49 | to describe someone relations are on the minimum we thank the potential to second order |
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0:01:55 | and we combine money okay however the slope of this parameter is better than the |
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0:02:01 | original one meaning that the narrow pieces that the sprinkle |
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0:02:06 | on a global that's that the interaction with my view students to spring constant of |
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0:02:11 | the matter |
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0:02:12 | this phenomenon is called optical spring |
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0:02:16 | now we have to what right model that all how well the same article |
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0:02:21 | their deltas bring a fast as descending all does that our model |
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0:02:28 | and you see this and uses that x coupling between the model |
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0:02:32 | this coupling is effective if the models are in reference |
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0:02:36 | we are interested in frequency selective operations that we have models of different frequency leading |
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0:02:43 | to an inefficient currently |
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0:02:45 | however the system will try to make it works well today the coupling entire |
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0:02:50 | the parametrically this is the ad detection can become effect |
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0:02:55 | in order to this can be done by modulating the driving like intensity |
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0:03:00 | so that modulate the optical spring effect |
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0:03:04 | for different modulation frequencies |
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0:03:06 | if they are all the interaction cameras |
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0:03:11 | yes schematic diagram of the wrestlers region while everyone operation |
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0:03:16 | they are plotted against the data modulation frequency |
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0:03:19 | and the driving for |
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0:03:22 | a model is inside the right column |
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0:03:25 | the green clones corresponding time-domain creation |
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0:03:32 | for two relays intensity dissipation programs operations |
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0:03:38 | for medium intensity dissipation is overcome and resonance regions |
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0:03:44 | i think the like the modulation frequency operations can be selected |
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0:03:51 | while too high intensity the cold overlap and selectivity is lost |
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0:03:57 | in our paper we extend the sensors for scalable the mechanical architecture |
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