| 0:00:03 | how about the video abstract for re combination of facts it soft x ray cluster |
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| 0:00:08 | interactions at |
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| 0:00:10 | z-norm joint press |
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| 0:00:12 | where we introduce an augmented |
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| 0:00:15 | our |
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| 0:00:16 | cluster laser interaction model which is at the mystic quantum classical hybrid model the irradiation |
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| 0:00:23 | was done at resident |
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| 0:00:27 | which |
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| 0:00:28 | predominantly causes z non to have an inner shell electron i know |
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| 0:00:35 | this is later followed by which lead to k |
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| 0:00:38 | which creates higher charged |
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| 0:00:41 | this means that very few |
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| 0:00:43 | audience as seen on are single the ionised when a gases rate we then look |
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| 0:00:49 | at the cluster signal and experimentally it was determined that a large one plus i |
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| 0:00:56 | on signal was detected |
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| 0:00:58 | this must come from re combination |
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| 0:01:02 | so we combination was include interval |
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| 0:01:05 | we did so and compare our recombination model |
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| 0:01:08 | two |
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| 0:01:10 | plasma models well known |
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| 0:01:12 | and found very good agreement between the two |
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| 0:01:16 | incorporating this into one large |
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| 0:01:19 | model for the entire interaction |
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| 0:01:22 | we simulate in three steps the interaction all the way to detected |
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| 0:01:29 | and recreate bowl experimental signals as can be seen in the following year |
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| 0:01:34 | the blue curve represents the experimental results with our results shown in right |
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| 0:01:41 | the multiple peaks |
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| 0:01:43 | in each charge they are due to z-norm isotope distribution |
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| 0:01:48 | we find very good agreement |
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| 0:01:51 | with the big difference being gassed in between are peaks this is largely due to |
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| 0:01:56 | are inclusion of a single size cluster multiple flies clusters would be present in the |
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| 0:02:03 | experimental signal |
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| 0:02:06 | we find |
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| 0:02:07 | also that we can break these signals and look at a single task isotope distribution |
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| 0:02:14 | and see what is the cause of each of these |
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| 0:02:18 | i on charge state |
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| 0:02:20 | so in the following figure we can see |
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| 0:02:23 | what if we just looked at the |
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| 0:02:26 | isotope distribution |
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| 0:02:27 | for the tahoe |
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| 0:02:29 | fifty percent of the latest ripples |
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| 0:02:32 | as shown in blue we find predominately the high charge state or created at the |
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| 0:02:38 | peak of the laser |
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| 0:02:40 | with diminishing amount and lower charge state |
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| 0:02:43 | the green which shows what would happen if we included only the top ninety percent |
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| 0:02:47 | of the laser pulls |
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| 0:02:49 | we find that again we can reproduce most of the high charge state up to |
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| 0:02:55 | around the seven plus |
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| 0:02:57 | but the proportion becomes less and less |
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| 0:03:00 | and to look for re combination with low primarily at the single each chores z |
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| 0:03:06 | not final |
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| 0:03:07 | and we find is the blue and green while having contributions the contributions or very |
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| 0:03:12 | small |
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| 0:03:13 | but only right which is the inclusion of all intensities |
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| 0:03:17 | we see that the difference between the red and green house thus it must be |
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| 0:03:22 | these intensities the very low intensities which represent the wings of the spatial distribution of |
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| 0:03:29 | the les miserables |
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| 0:03:30 | which do not have a plasma strongly happens allow recombination |
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| 0:03:35 | thank you for your attention |
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