{"data":{"id":"10.6084/m9.figshare.c.3285455.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.c.3285455.v1","prefix":"10.6084","suffix":"m9.figshare.c.3285455.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Harden, Galen","nameType":"Personal","givenName":"Galen","familyName":"Harden","affiliation":[],"nameIdentifiers":[]},{"name":"Hoffman, Anthony","nameType":"Personal","givenName":"Anthony","familyName":"Hoffman","affiliation":[],"nameIdentifiers":[]},{"name":"Cortes-Herrera, Luis","nameType":"Personal","givenName":"Luis","familyName":"Cortes-Herrera","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Optical pathlength and trajectory stability in rotationally asymmetric multipass cells"}],"publisher":"Figshare","container":{},"publicationYear":2016,"subjects":[{"subject":"90605 Photodetectors, Optical Sensors and Solar Cells","subjectScheme":"FOR"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2016-08-12","dateType":"Created"},{"date":"2016-08-12","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"GEN","bibtex":"misc","citeproc":"article","schemaOrg":"Collection","resourceType":"Collection","resourceTypeGeneral":"Collection"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1364/oe.24.019497","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.c.3285455","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"CC-BY","rightsUri":"http://creativecommons.org/licenses/by/3.0/us"}],"descriptions":[{"description":"We describe the behavior of optical trajectories in multipass rotationally asymmetric cavities (RACs) using a phase space motivated approach.  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/3285455/1","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":"2016-08-12T17:41:23.000Z","registered":"2016-08-12T17:41:24.000Z","published":"2016","updated":"2024-12-15T11:41:33.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.c.3285455.v1","type":"media"}},"references":{"data":[{"id":"10.1364/oe.24.019497","type":"dois"}]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}