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DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.5281/zenodo.17913776475and) was visible in the surrounding text but could not be confirmed against doi.org as printed.
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For each point in the diagram, we compile statistics from 50 realizations with distinct initial111 particle distributions (Figure S2). Results for other particle numbers (N= 5,7,8) are provided in112 Figures S3– S5. AcrossN, the regime diagrams share the same qualitative structure; differences113 arise mainly in the positions of the boundaries. For ease of comparison, the corresponding114 boundaries for differentNare superimposed as dashed lines in Figure 2(b).115 We first discuss the effect of the evaporation rateU e on the packing structure of colloidal116 clusters, and for simplicity, let us initially consider smooth particles with negligible friction (µ <117 0.05). With varyingCa, we identified three distinct categories of final packing configurations:118 open, closed, and minimal moment packings, as illustrated in Figure 2a. The three regions in the119 regime diagram in Figure 2b are defined based on the occurrence probabilities of open, closed,120 and minimal moment packings. In the minimal moment regime (blue region in Figure 2b), the121 minimal moment packing is obtained with100%probability. In the closed regime (red region in122 Figure 2b), both closed and minimal moment packings can appear. In the open regime (green123 region in Figure 2b), all three types of structures may occur. 124 For large evaporation rates (Ca >0.05; indicated in green in Figure 2b), hydrodynamic forces125 dominate, and capillary attraction is not sufficient to draw colloidal particles into cl
Evidence payload
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"reconstructed_doi": "10.5281/zenodo.17913776475and",
"ref_index": 1,
"resolved_title": null,
"verdict_class": "incontrovertible"
}