{"@context":"http://iiif.io/api/presentation/3/context.json","id":"https://makingscience.royalsociety.org/items/rr_43_94/referees-report-by-paul-adrein-maurice-dirac-on-a-paper-the-quantum-theory-of-dispersion-in-metallic-conductors-ii-by-r-de-l-kronig/manifest.json","type":"Manifest","label":{"en":["Referee's report by Paul Adrein Maurice Dirac, on a paper 'The quantum theory of dispersion in metallic conductors. — II' by R de L Kronig"]},"requiredStatement":{"label":{"en":["Attribution"]},"value":{"en":["The Royal Society"]}},"rights":"http://creativecommons.org/licenses/by/4.0/legalcode","provider":[{"id":"https://royalsociety.org/","type":"Agent","label":{"en":["The Royal Society"]},"homepage":[{"id":"https://makingscience.royalsociety.org","type":"Text","label":{"en":["The Royal Society - Science in the Making"]},"format":"text/html"}]}],"thumbnail":[{"id":"https://royalsociety-image-public.s3.eu-west-2.amazonaws.com/w400/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.jpeg","type":"Image","format":"image/jpeg"}],"metadata":[{"label":{"en":["Format"]},"value":{"en":["Manuscript"]}},{"label":{"en":["Reference Number"]},"value":{"en":["RR/43/94"]}},{"label":{"en":["Physical description"]},"value":{"en":["Standardised form (type D)"]}},{"label":{"en":["Creator"]},"value":{"en":["Paul Adrien Maurice Dirac"]}}],"items":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.ptif/canvas","type":"Canvas","label":{"en":["Referee's report by Paul Adrein Maurice Dirac, on a paper 'The quantum theory of dispersion in metallic conductors. — II' by R de L Kronig - 1"]},"height":5461,"width":8585,"thumbnail":[{"id":"https://royalsociety-image-public.s3.eu-west-2.amazonaws.com/w128/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.jpeg","type":"Image","format":"image/jpeg","width":128,"height":128}],"items":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.ptif/annotation_page","type":"AnnotationPage","items":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.ptif/annotation","type":"Annotation","motivation":"Painting","body":{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.ptif/info.json","type":"Image","service":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.ptif","type":"ImageService2","profile":"http://iiif.io/api/image/2/level2.json"}],"height":8585,"width":5461},"target":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_001.ptif/canvas"}]}]},{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.ptif/canvas","type":"Canvas","label":{"en":["Referee's report by Paul Adrein Maurice Dirac, on a paper 'The quantum theory of dispersion in metallic conductors. — II' by R de L Kronig - 2"]},"height":8588,"width":5454,"thumbnail":[{"id":"https://royalsociety-image-public.s3.eu-west-2.amazonaws.com/w128/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.jpeg","type":"Image","format":"image/jpeg","width":128,"height":128}],"items":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.ptif/annotation_page","type":"AnnotationPage","items":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.ptif/annotation","type":"Annotation","motivation":"Painting","body":{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.ptif/info.json","type":"Image","service":[{"id":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.ptif","type":"ImageService2","profile":"http://iiif.io/api/image/2/level2.json"}],"height":5454,"width":8588},"target":"https://rs-images.cogapp.cloud/iiif/3/RR%2FRR_43_71_153%2FRR_43_94%2FTIF%2FRR_43_94_002.ptif/canvas"}]}]}]}