{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,2,21]],"date-time":"2025-02-21T01:18:27Z","timestamp":1740100707935,"version":"3.37.3"},"reference-count":10,"publisher":"IEEE","license":[{"start":{"date-parts":[[2022,4,21]],"date-time":"2022-04-21T00:00:00Z","timestamp":1650499200000},"content-version":"stm-asf","delay-in-days":0,"URL":"https:\/\/doi.org\/10.15223\/policy-029"},{"start":{"date-parts":[[2022,4,21]],"date-time":"2022-04-21T00:00:00Z","timestamp":1650499200000},"content-version":"stm-asf","delay-in-days":0,"URL":"https:\/\/doi.org\/10.15223\/policy-037"}],"funder":[{"DOI":"10.13039\/501100000921","name":"European Cooperation in Science and Technology","doi-asserted-by":"publisher","id":[{"id":"10.13039\/501100000921","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":[],"published-print":{"date-parts":[[2022,4,21]]},"DOI":"10.1109\/radioelektronika54537.2022.9764902","type":"proceedings-article","created":{"date-parts":[[2022,5,3]],"date-time":"2022-05-03T20:20:02Z","timestamp":1651609202000},"page":"1-4","source":"Crossref","is-referenced-by-count":0,"title":["Reciprocity of the Turbulent Cascade Model"],"prefix":"10.1109","author":[{"given":"Alzbeta","family":"Kovalova","sequence":"first","affiliation":[{"name":"Brno University of Technology,Department of Radio Electronics,Brno,Czech Republic"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Lucie","family":"Hudcova","sequence":"additional","affiliation":[{"name":"Brno University of Technology,Department of Radio Electronics,Brno,Czech Republic"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"263","reference":[{"key":"ref4","doi-asserted-by":"publisher","DOI":"10.1109\/ICTON.2019.8840526"},{"journal-title":"Optimal Intensity Distribution in a Laser Beam for FSO Communications","year":"2016","author":"barcik","key":"ref3"},{"journal-title":"Quantification Of Turbulence By The Equivalent Temperature Gradient","year":"2021","author":"kovalova","key":"ref10"},{"key":"ref6","doi-asserted-by":"crossref","first-page":"1312","DOI":"10.1109\/PROC.1966.5119","article-title":"Laser beams and resonators","volume":"54","author":"kogelnik","year":"1966","journal-title":"Proceedings of the IEEE"},{"key":"ref5","doi-asserted-by":"publisher","DOI":"10.1109\/RADIOELEK.2018.8376401"},{"journal-title":"Introduction to Matrix Methods in Optics","year":"1994","author":"gerrard","key":"ref8"},{"key":"ref7","article-title":"Matrix Model of the Turbulent Cells Cascade","author":"kovalova","year":"0","journal-title":"Radioengineering"},{"key":"ref2","doi-asserted-by":"publisher","DOI":"10.1109\/CSNDSP.2016.7573975"},{"key":"ref9","first-page":"498","article-title":"The Gladstone - Dale Relationship - Part 1: Derivation of New Constants","author":"mandarino","year":"1976","journal-title":"The Canadian Mineralogist"},{"key":"ref1","doi-asserted-by":"publisher","DOI":"10.1117\/3.412858"}],"event":{"name":"2022 32nd International Conference Radioelektronika (RADIOELEKTRONIKA)","start":{"date-parts":[[2022,4,21]]},"location":"Kosice, Slovakia","end":{"date-parts":[[2022,4,22]]}},"container-title":["2022 32nd International Conference Radioelektronika (RADIOELEKTRONIKA)"],"original-title":[],"link":[{"URL":"http:\/\/xplorestaging.ieee.org\/ielx7\/9764897\/9764898\/09764902.pdf?arnumber=9764902","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2022,7,4]],"date-time":"2022-07-04T20:14:21Z","timestamp":1656965661000},"score":1,"resource":{"primary":{"URL":"https:\/\/ieeexplore.ieee.org\/document\/9764902\/"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2022,4,21]]},"references-count":10,"URL":"https:\/\/doi.org\/10.1109\/radioelektronika54537.2022.9764902","relation":{},"subject":[],"published":{"date-parts":[[2022,4,21]]}}}