NatureSir Norman Lockyer Macmillan Journals Limited, 2007 |
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Zadetki 1–3 od 73
Stran 301
... field ( that is , several hundred nanometres ) . Theory has indicated11,12 that the spatial limitation to coherent control can be overcome with the illumination of nanostructures : the spatial near - field distribution was shown to ...
... field ( that is , several hundred nanometres ) . Theory has indicated11,12 that the spatial limitation to coherent control can be overcome with the illumination of nanostructures : the spatial near - field distribution was shown to ...
Stran 303
... field control , we calculated the local electric field for the nanostructure ( Fig . 1 ) and optimized laser pulse shapes ( Figs 2e and f ) used in the experiments . We solve the frequency - dependent Maxwell equations rigorously by ...
... field control , we calculated the local electric field for the nanostructure ( Fig . 1 ) and optimized laser pulse shapes ( Figs 2e and f ) used in the experiments . We solve the frequency - dependent Maxwell equations rigorously by ...
Stran 630
... field was not observed at the intens- ity level chosen . The XUV - generated Ne2 + yield was therefore not affected by the NIR probe for At≪ - t1 but was significantly enhanced by the laser field for At approaching zero and becoming ...
... field was not observed at the intens- ity level chosen . The XUV - generated Ne2 + yield was therefore not affected by the NIR probe for At≪ - t1 but was significantly enhanced by the laser field for At approaching zero and becoming ...
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MAPKmediated bimodal gene expression and adaptive gradient | 46 |
The structure of suspended graphene sheets | 60 |
NATURE ONLINE | 79 |
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