0:00:04 | this to be used giving a short introduction to the paper examining the ionisation process |
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0:00:08 | going on during elimination of nitrogen vacancy defect indictment |
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0:00:12 | indeed effect and diamond is a single foot an amateur it gives that's fluorescence emission |
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0:00:17 | which can be detected the confocal microscope at room temperature |
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0:00:21 | indeed effect contains an election spin and a new peers been yet occurrence been can |
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0:00:26 | be initialize and read out optically |
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0:00:29 | these properties especially the long coherence times makes the envy defect a candidate for the |
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0:00:34 | application of a quantum register |
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0:00:37 | furthermore it has been demonstrated that the envied effect can serve as a magnetic and |
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0:00:41 | electric field sensor |
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0:00:44 | all these applications are based on the negatively charged envied effect |
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0:00:48 | but there is also another charge state of envy |
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0:00:50 | if one electron is removed we get the neutrally charged and we center |
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0:00:54 | this chart state is actually a part of the process but hidden |
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0:00:59 | by illumination with highly the power the charts data switching at a very fast rate |
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0:01:07 | these ionisation and recombination processes can be slow down by changing the excitation wavelength and |
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0:01:13 | lowering the intensity |
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0:01:16 | the time traits shows the blinking between chart states on a time scale of seconds |
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0:01:22 | that's have a closer look on the time trace |
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0:01:25 | we have single burst that can be assigned to a chart state |
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0:01:29 | that i've ever since level we are in the new minus state the low fluorescence |
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0:01:33 | level belongs to the n b zero state |
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0:01:37 | the time the envy defect resides in the any minus and then be zero state |
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0:01:41 | can be determined by analysing the time tries |
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0:01:45 | furthermore defer sense level gives us direct information about and b minus absorption |
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0:01:51 | the probability to be in your mind as they can be determined but it opens |
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0:01:55 | as shown in the formula |
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0:01:58 | we examine to dependence of these processes on the excitation wavelength and power |
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0:02:05 | in the graph you can see d n b minus probability plotted versus the excitation |
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0:02:10 | wavelength |
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0:02:11 | for broad range of excitation wavelengths and maximum and b minus probability of seventy percent |
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0:02:15 | can be observed |
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0:02:19 | in addition to this we succeeded in measuring the intrinsic absorption spectra from be minus |
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0:02:27 | the results help us an understanding how the chart state switching is working |
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0:02:32 | the ionisation from n b minus trained with zero functions as a twofold and process |
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0:02:36 | for a broad range of excitation wavelengths |
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0:02:41 | a first photonic sides and b minus |
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0:02:44 | a second photo lifts the electron into the conduction bent |
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0:02:48 | consequently in be minus has been ionised and we end up in the n b |
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0:02:52 | zero state |
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0:02:54 | recombination works accordingly |
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0:02:57 | a first photo excites and v zero and the second courses to capture of an |
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0:03:02 | electron ending up in the n b minus crone state |
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0:03:07 | if it to foreign process can cause the ionisation with higher for to manage it |
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0:03:11 | should also be possible to ionised in be detected only one photon |
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0:03:15 | this is exactly what we have observed |
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0:03:18 | liu illumination excites an electron from the ground state directly into the conduction band |
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0:03:24 | the recombination process is also possible with one photon |
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0:03:32 | the thing that charge state detection method enabled us to determine the exact energetic localisation |
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0:03:37 | of n b minus crone stayed within the band k |
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0:03:41 | the results of this paper are important for the implementation of high resolution microscopy techniques |
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0:03:46 | that are based on stochastic blinking |
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0:03:49 | multiple in v centres in a diffraction limited area cannot be resolved because they're all |
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0:03:54 | the meeting photons at a time |
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0:03:56 | a switching of charge states allows us to localise envied effects be on t diffraction |
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0:04:00 | blurring |
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0:04:04 | furthermore the charts the detection method can be used to initialize the chart state with |
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0:04:08 | fidelity of almost hundred percent |
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0:04:11 | in the future d measurement of charge state dynamics of envy centres of make it |
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0:04:15 | possible to send surrounding charts concentration since it influences defame eleven endowment |
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