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Opt. Soc. Am. A"],"published-print":{"date-parts":[[2020,10,1]]},"abstract":"<jats:p>We call a surface that appears undistorted when viewed in a curved\n\t\t\t\t\tmirror an <jats:italic toggle=\"yes\">eigensurface<\/jats:italic> and the mirror an\n\t\t\t\t\t<jats:italic toggle=\"yes\">eigenmirror<\/jats:italic>. Such pairs are described by\n\t\t\t\t\ta first-order nonlinear partial differential equation of the form <jats:inline-formula>\n      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mn>0<\/mml:mn>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mo>+<\/mml:mo>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mn>1<\/mml:mn>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>u<\/mml:mi>\n\t    <mml:mi>x<\/mml:mi>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mspace width=\"thinmathspace\"\/>\n\t<mml:mo>+<\/mml:mo>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mn>2<\/mml:mn>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>u<\/mml:mi>\n\t    <mml:mi>y<\/mml:mi>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mo>+<\/mml:mo>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mn>3<\/mml:mn>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>u<\/mml:mi>\n\t    <mml:mi>x<\/mml:mi>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>u<\/mml:mi>\n\t    <mml:mi>y<\/mml:mi>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mo>+<\/mml:mo>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mn>4<\/mml:mn>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:msubsup>\n\t  <mml:mi>u<\/mml:mi>\n\t  <mml:mi>x<\/mml:mi>\n\t  <mml:mn>2<\/mml:mn>\n\t<\/mml:msubsup>\n\t<mml:mo>+<\/mml:mo>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mn>5<\/mml:mn>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:msubsup>\n\t  <mml:mi>u<\/mml:mi>\n\t  <mml:mi>y<\/mml:mi>\n\t  <mml:mn>2<\/mml:mn>\n\t<\/mml:msubsup>\n\t<mml:mo>=<\/mml:mo>\n\t<mml:mn>0<\/mml:mn>\n      <\/mml:math>\n    <\/jats:inline-formula>, where <jats:inline-formula>\n      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mi>i<\/mml:mi>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mo>=<\/mml:mo>\n\t<mml:mrow class=\"MJX-TeXAtom-ORD\">\n\t  <mml:msub>\n\t    <mml:mi>a<\/mml:mi>\n\t    <mml:mi>i<\/mml:mi>\n\t  <\/mml:msub>\n\t<\/mml:mrow>\n\t<mml:mo stretchy=\"false\">(<\/mml:mo>\n\t<mml:mi>x<\/mml:mi>\n\t<mml:mo>,<\/mml:mo>\n\t<mml:mi>y<\/mml:mi>\n\t<mml:mo>,<\/mml:mo>\n\t<mml:mi>u<\/mml:mi>\n\t<mml:mo stretchy=\"false\">)<\/mml:mo>\n      <\/mml:math>\n    <\/jats:inline-formula>, which we call the <jats:italic toggle=\"yes\">anti-eikonal equation<\/jats:italic>. We give examples of\n\t\t\t\t\tsymbolic and numerical solutions, including pairs that are\n\t\t\t\t\tgeometrically congruent. Ray tracing simulations are included that\n\t\t\t\t\tvisually confirm the unusual properties of these surfaces.<\/jats:p>","DOI":"10.1364\/josaa.401301","type":"journal-article","created":{"date-parts":[[2020,8,18]],"date-time":"2020-08-18T20:00:21Z","timestamp":1597780821000},"page":"1566","update-policy":"https:\/\/doi.org\/10.1364\/crossmark_policy","source":"Crossref","is-referenced-by-count":1,"title":["Anti-eikonal equation of an eigenmirror"],"prefix":"10.1364","volume":"37","author":[{"given":"R. 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