| 0:00:07 | hello this is a video articulation submission db |
|---|
| 0:00:11 | so here we |
|---|
| 0:00:12 | images and marcus at ash stephen clark myself tom ridge |
|---|
| 0:00:20 | well start by describing the kinds of stops in my present is |
|---|
| 0:00:23 | is it possible realisation that any crystal geometry |
|---|
| 0:00:27 | when detecting the crystal whole more questions in a set of buttons can coherently sounding |
|---|
| 0:00:31 | sites |
|---|
| 0:00:33 | we can use nonlinearities by local coupling each resonance with a to the system is |
|---|
| 0:00:37 | described by james comes interaction |
|---|
| 0:00:40 | a common in hamilton for the total system here since the change coming something |
|---|
| 0:00:44 | and we note there are several a promising technology stimuli something notably those nations that |
|---|
| 0:00:49 | q t |
|---|
| 0:00:51 | present in a race tracks a lot of attention recently hundred platforms realising strongly colour |
|---|
| 0:00:56 | many by state applied |
|---|
| 0:00:57 | because of the possibilities use them as content similar to interesting facts |
|---|
| 0:01:02 | on the person persons wishing idealise large was also raised |
|---|
| 0:01:06 | but resonator losses in future experiments like to use |
|---|
| 0:01:10 | the first very small |
|---|
| 0:01:12 | and now require external pumping sort become losses |
|---|
| 0:01:16 | so that in my |
|---|
| 0:01:17 | the purpose of our work is twofold |
|---|
| 0:01:19 | on the one hand we investigate how to describe resonator is but physically accurately |
|---|
| 0:01:24 | and the other ones one dissipated this is expected in the future small-scale rise |
|---|
| 0:01:30 | so that's part of our work involves looking at accurately model which is |
|---|
| 0:01:34 | the chain coming haven't model was introduced about |
|---|
| 0:01:36 | if the full description of the rise coupled to double system |
|---|
| 0:01:39 | it's actually citations a joint adam for example are |
|---|
| 0:01:44 | but sometimes the purely prosodic breaks habit |
|---|
| 0:01:46 | which arises naturally incorporate optical lattice setups |
|---|
| 0:01:49 | is used to approximate the dynamics of resonators |
|---|
| 0:01:52 | so its importance new information is approximation about thing to do |
|---|
| 0:01:56 | only taking the full description with the novel aspect not captured by the perceptible |
|---|
| 0:02:01 | so in this work we compared experimentally accessible observable also present in race describer models |
|---|
| 0:02:06 | and that is |
|---|
| 0:02:08 | we need a meaningful way that between |
|---|
| 0:02:10 | we chose to match the one i can structure |
|---|
| 0:02:12 | i details in this matter |
|---|
| 0:02:15 | we don't do not compare spectral correlation functions with small or medium sized arrays and |
|---|
| 0:02:20 | the reader perceptive or jamestown subscription |
|---|
| 0:02:23 | i don't i solution experimentally realistic parameters but coupling one straight road panel in general |
|---|
| 0:02:28 | very important differences between the two models |
|---|
| 0:02:31 | mostly on account of the additional atomic degree of freedom that the full description possesses |
|---|
| 0:02:36 | note the second time dissipate near future experiments were raised we need ways to simulate |
|---|
| 0:02:42 | large and medium sized arrays |
|---|
| 0:02:44 | to solve these databases |
|---|
| 0:02:46 | we use the combination of the matrix per state representation to describe your one trajectories |
|---|
| 0:02:53 | we can this combination is very efficient as we can average are many independent realizations |
|---|
| 0:02:58 | we can also every time steps |
|---|
| 0:03:00 | and in many cases also provide insights |
|---|
| 0:03:04 | so this numerical has been investigated with the two recently proposed anybody effects could be |
|---|
| 0:03:09 | observed in a rise and that probably described in its comes have a model |
|---|
| 0:03:13 | participants were predicted to occur really tonic systems these numbers of approximation |
|---|
| 0:03:19 | but this design is based on permutation and then given by me and characterized by |
|---|
| 0:03:23 | buttons and a strong on the conditions |
|---|
| 0:03:26 | and we also found increase or duration |
|---|
| 0:03:28 | we should best replication importance become glued together so that's one raises a lot of |
|---|
| 0:03:33 | particles random a theory |
|---|
| 0:03:36 | in both cases we calculate an equivalence when we are described it wasn't |
|---|
| 0:03:41 | are there are several differences in tune abilities p without any case |
|---|
| 0:03:45 | and is reflected general conclusions this work the trend is very resonator weights must be |
|---|
| 0:03:50 | described by jane comments have able to make a physical predictions |
|---|
| 0:03:55 | so initial watching at least two three nine questions |
|---|