Journal
JOURNAL OF MODERN OPTICS
Volume 49, Issue 9, Pages 1537-1543Publisher
TAYLOR & FRANCIS LTD
DOI: 10.1080/09500340110107504
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Propagation-invariant azimuthally and radially polarized fields are examined. The orthogonality of these fields in every point of space is used to form propagation-invariant intensity distributions outside the scope of scalar theory. The same principle is then used to form self-imaging electromagnetic fields with non-self-imaging scalar components.
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