0:00:00 | i don't result can also be |
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0:00:08 | in the present study we have no you must be what we also live in |
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0:00:18 | a whole |
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0:00:20 | i still |
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0:00:22 | in addition we got |
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0:00:26 | i can be used and is warranted |
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0:00:32 | e |
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0:00:33 | so the formulation we have started a it is probably should but there is |
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0:00:40 | while this |
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0:00:43 | back at a time where each state |
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0:00:50 | in the stuff |
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0:00:54 | this e |
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0:00:56 | we wonder why it's |
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0:01:00 | we want to investigate whether the present work in yes |
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0:01:06 | i mean |
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0:01:11 | where the implication in the modulation |
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0:01:17 | okay |
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0:01:19 | more than one can but it's |
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0:01:22 | e da information so our initial training |
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0:01:30 | this is a hole in your you know as well at low prices on an |
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0:01:37 | allpass and |
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0:01:39 | each you |
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0:01:42 | we also all |
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0:01:45 | in the present study |
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0:01:47 | for a while we |
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0:01:49 | this he wishes time you see in be a and |
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0:01:58 | only use you well starting point for us but we have just to if you |
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0:02:06 | have |
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0:02:07 | fourier transform infrared scope just to see whether you can interact and the and you |
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0:02:18 | we try again |
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0:02:22 | this one and |
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0:02:24 | and |
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0:02:26 | we not formation but isn't that this might sound or vibration the |
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0:02:34 | and a formation this |
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0:02:36 | now we have been based different physical |
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0:02:42 | as i say |
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0:02:47 | there are still then i said by back |
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0:02:54 | we just one |
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0:02:56 | in |
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0:02:58 | we can say that this is a or b |
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0:03:03 | presence of only one |
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0:03:06 | since these results faster and then slow but at the right i mean we've |
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0:03:17 | no one |
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0:03:20 | and this i |
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0:03:22 | as well as well but also |
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0:03:27 | wore a key step only five |
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0:03:33 | but it was o b condition |
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0:03:37 | i |
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0:03:38 | i |
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0:03:41 | a reference for |
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0:03:43 | in one but i don't by this would be used in the for each in |
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0:03:51 | i |
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