0:00:04 | well can do all video abstract |
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0:00:09 | quantum effects are everywhere l |
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0:00:11 | from a solstice semiconductors to super conductors to chemistry and biology |
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0:00:17 | similarity the field of control is essential for most model technology for example regarding robotics |
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0:00:24 | died in systems micro controllers in chemical engineering |
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0:00:28 | naturally we would also like to extend controlled and then a scale systems and quantum |
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0:00:33 | dynamics in atoms molecules and quantum devices |
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0:00:36 | this can be done by engineering the hamiltonian that governs the evolution of the system |
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0:00:41 | my have the application of optimized extol of electromagnetic fields |
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0:00:47 | many applications of quantum control |
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0:00:49 | in this paper we focus on the implementation of robust quantum gates which ones realized |
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0:00:56 | with pave the way to full scale quantum computers |
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0:01:01 | and major obstacle for the realization of robust quantum gates uncontrollable interactions with the environment |
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0:01:07 | that lead to d coherence eliminating the system's not classical properties |
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0:01:13 | different types of environment in the markovian grapheme system back correlations tk fast so that |
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0:01:19 | the environment has effectively no memory of past interactions with the system |
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0:01:24 | many physical processes of this nature for example the spontaneous emission of falling tones and |
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0:01:30 | phone and what collusion of the facing atomic labels |
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0:01:33 | on the other hand it correlations between the system and that all significant on the |
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0:01:39 | times you know which the system impulse |
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0:01:41 | then the environment is non-markovian |
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0:01:44 | typically the case for small structured environments such as one almost is computed surrounded by |
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0:01:50 | weakly coupled noise q s found solid state systems |
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0:01:54 | both types of environment all important in practice leading us to the key question we |
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0:02:00 | study in this paper |
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0:02:03 | how to the differences between these environments affect our ability to coherently controls the dynamics |
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0:02:09 | specifically we address in the implementation of quantum gates in different environments using optimal control |
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0:02:15 | it's really filters finite time resolution they minimize kate errors using an iterative algorithm |
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0:02:21 | in each iteration the fields are updated four times at once as shell using a |
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0:02:25 | quasi newton message was extracted at gradient which is more efficient than the popular quote |
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0:02:30 | of method |
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0:02:32 | the performance of the algorithm is analyzed in terms of the minimum gate errors obtained |
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0:02:36 | in the convergence behavior |
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0:02:38 | a simple problems little variability is observed for more challenging task however frequent wrapping long |
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0:02:44 | tails a diminishing returns make sensible termination conditions and repeated runs essential |
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0:02:50 | to quantify the likelihood of success of a typical run and the time required on |
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0:02:54 | average to find a suitable field |
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0:02:57 | new notions of success rate and sixty four introduce |
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0:03:00 | density plots show then utilized to study the effects of parameters that risky operation times |
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0:03:06 | and initial field of these performance indicators |
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0:03:10 | we also consider how feels optimize in the closed system setting perform open systems |
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0:03:15 | in the non market in case of fields can be substantially improved by explicitly considering |
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0:03:20 | the environment |
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0:03:21 | well almost no improvement in the markovian case |
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0:03:25 | how does the controls work |
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0:03:27 | in the non-markovian case plots a trajectory plot shows that the improved performance controls |
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0:03:33 | is mainly due to suppression of indirect no skip the expectation that result from the |
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0:03:38 | closed system optimal the others are applied |
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0:03:41 | however certainly factors such as feel they could cause unwanted most cupid excitations that renders |
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0:03:47 | the controls completely ineffective |
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0:03:50 | i can be mitigated by explicitly considering leakage in the optimisation but at the expense |
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0:03:54 | of substantially increase kate operation time to control complexity |
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0:03:58 | as shown this demonstrated limited control robustness an underscore c important the system design and |
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0:04:04 | characterization for control |
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