{"id":647,"date":"2018-02-13T17:36:42","date_gmt":"2018-02-13T16:36:42","guid":{"rendered":"http:\/\/www.icmm.csic.es\/luxrerum\/?page_id=647"},"modified":"2018-02-13T17:36:42","modified_gmt":"2018-02-13T16:36:42","slug":"general-microscopy-characterization","status":"publish","type":"page","link":"https:\/\/wp.icmm.csic.es\/luxrerum\/general-microscopy-characterization\/","title":{"rendered":"General microscopy characterization"},"content":{"rendered":"
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Microscopy characterization<\/span><\/h1>\n
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FIGURE 1. SEM
\nimage of a cleft edge of an artificial opal. A triangular arrangement (fcc {111} set of
\nplanes) is observed on the lower part of the image. Square ({100}), rectangular ({110})
\nand triangular ({111}) orderings appear on the upper part of the image.<\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

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It is well know (1), that hard spheres canequally be close packed into a face centred cubic (fcc), a hexagonal close packed (hcp) orany mixture thereof. From gravitational energy considerations, all of them are equally probable. This fact is of crucial importance in PBG technology, since the fcc structure has been shown to present a full gap, provided an appropriate refractive index contrast is achieved. In this sense, a sophisticated method was devised in order to force the colloidal crystallisation in the fcc phase. Only recently, it has been shown both theoretically, by using computer simulations (2), and experimentally (3) that fcc order is the most stable phase. In Fig. 1 one can see a low magnification SEM image of internal facets (observable after cleavage) of an artificial opal made by natural sedimentation as described above. The triangular order corresponding to a crystalline plane belonging to the {111} family (lower part of the image) can be seen. Also, square, rectangular and\u00a0 triangular arrangements of spheres, belonging to {100}, {110} and {111} sets of planes, can be seen at the cleft edge (upper part of the image).<\/p>\n

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FIGURE 2. Computer simulated
\nimage of an fcc order (centre image) along with 4 different SEM images of different
\ncrystalline facets. Upper left: external (111), upper right: internal (111), lower left
\n(110) and lower right (001).<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

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In Fig. 2 one can see a computer
\nsimulation of an fcc order (central image) surrounded by SEM images of actual
\ncrystallographic planes. All these planes can only be present in an fcc stacking thus
\ndemonstrating the statement. The results reported, so far, involve opals in which the
\ninterparticle voids are filled with air. We call those samples “bare opals”.
\nBare as-grown opals are solid but present a low mechanical stability. To improve it, a
\nsintering process can be performed.<\/p>\n

Want to see more pictures?<\/p>\n

1.- C. Kittel. 1968. ‘Introduction to
\nSolid State Physics’, Third Edition, John Wiley.<\/p>\n

2.- L.V. Woodcock. 1997. Nature 385,
\n141.<\/p>\n

3.- H. M\u00edguez, F. Meseguer C. L\u00f3pez, A.
\nMifsud, J. S. Moya, and L. V\u00e1zquez. 1997. Langmuir. 13, 6009.<\/p>\n","protected":false},"excerpt":{"rendered":"

Microscopy characterization FIGURE 1. SEM image of a cleft edge of an artificial opal. A triangular arrangement (fcc {111} set of planes) is observed on the lower part of the image. Square ({100}), rectangular ({110}) and triangular ({111}) orderings appear on the upper part of the image.   It is well know (1), that hard […]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-647","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/pages\/647","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/comments?post=647"}],"version-history":[{"count":0,"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/pages\/647\/revisions"}],"wp:attachment":[{"href":"https:\/\/wp.icmm.csic.es\/luxrerum\/wp-json\/wp\/v2\/media?parent=647"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}