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SEM-CL在量子点异质结方面的应用

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The second half of the 20th century has seen the emergence of semiconductor quantum structures driven by promises of far superior performances in particular regarding light emission. The dimensionality was reduced down to point-like quantum dots (QDs). QDs exhibit intriguing similarities with atoms and tremendous efforts were made to assess their properties.

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阴极荧光分析设备SEM-CL在量子点异质结方面的应用attolightBe Part of the NewCathodoluminescenceRevolution Attolight CL / Applications on Quantum Heterostructures The second hal f of the 2oth century ha s seen the emergence of semiconductor quantum struc-tures driv e n by promises of far s u perior performances in particular reg a rding l ight emission.The dimensionality was reduced down to point -like quantum d o ts (QDs). QDs exhibit intriguing similari t ies with atoms and tremendous efforts were made to assess thei r propert i es The growth of quantum dots e mbedded i n filamentary crystals, known as nanowires (NWs),become relevant g i ven the strong interac t ion between light and NWs. QDs in NWs are par t icular expected to be key e l ements in quantum tech n ologies, such as quantum commun i -cations and c r yptography. However , the reduced dimensionality of both QDs (ar. 5-10 nm)and NWs (ar. 100-200 nm i n diameter) can strongly complicates the measurements of the QDs propertie s . In particular, absolute QD s position and resol u tion between closely lying dots i s hard to assess with full-optical measurement due to dif f rac ti on l imitations. Y an nik F o nt a n a Laboratory of Semiconductor Materials (Fontcuberta Grou p) E PFL Works on: Quantum emitters localized in III-V Nanowires This limit can be overcomed with cathodoluminescence measurements, which makes possible t he investigations on the position of QDs an d the i r appea r ance depending on t he propert i es o f the hos t NW. For our structures, made of GaAs a n d AlG a As, the Attol i ght CL-SEM allows us to work at cryogenic temperature, a necessary condi t ion to observe light emission from the Q D s. Furthermore , t he Attol i ght micro s cope provides the following advantages comp a red to traditional system: - The large numerical aperture ensures a very high signal -to -noise ratio, lead i ng to a shorter exposure of the QDs to t he electron beam and hence red u cing the risk of bleaching a s well a s speed i ng up the experiment. - The h i gher signal allows to use straightforwardly a spec t rometer-CCD detec ti on channel, wit h out the need of photomu l t i pl i er tube, y i elding di r ec t ly fas t hyper -spectral mapping. The wide em i ssion spectral r a nge i s then c a ptured (in our case trom 650 nm to 900 nm). - The spatial resolut i on permits to resolve closely lying dots as wel l as local features such as changes i n the matrix crystal phase. Summing up, an a lysi s done with the Attolight system simply provide i nformation on both the QDs a n d the matr i x that cannot be obta i ned by other means without extreme effort and compromises. 500 nm 500 nm Close-up of two NWs tip. Red now represent emission from the GaAs core (820 nm) o f the wire, when blue regions mark the QDs emission (670 nm). Dots a t l ess than 500 nm can be easily resolved. Mapping of the QDs location with respect to the emitted wavelength. Blue, green and red correspond to 3 wavelengths between 650 and 7o0 nm. Some dots emit are several wavelength, resul t i ng i n composite colors (e.g. yellow)

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