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Emphasis is placed on generating long optical path lengths and global focus times.  A trajectory with an optical path length of 18 m is generated within a 68 cm³ volume.  This path length to volume ratio (26.9 cm-²) is large compared to current state of the art multipass cells such as the cylindrical multipass cell (6.6 cm-²) and astigmatic Herriott cell (9 cm-²). This work simplifies the process of designing RACs with long optical path lengths and could lead to broader implementation of these multipass cells.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/collections/Optical_pathlength_and_trajectory_stability_in_rotationally_asymmetric_multipass_cells/3285455","contentUrl":null,"metadataVersion":1,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"api","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":1,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2016-08-12T17:41:24.000Z","registered":"2016-08-12T17:41:25.000Z","published":"2016","updated":"2024-12-15T11:41:32.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.c.3285455","type":"media"}},"references":{"data":[{"id":"10.1364/oe.24.019497","type":"dois"}]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}