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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="ru"><front><journal-meta><journal-id journal-id-type="publisher-id">alternative</journal-id><journal-title-group><journal-title xml:lang="ru">Альтернативная энергетика и экология (ISJAEE)</journal-title><trans-title-group xml:lang="en"><trans-title>Alternative Energy and Ecology (ISJAEE)</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">1608-8298</issn><publisher><publisher-name>Международный издательский дом научной периодики "Спейс</publisher-name></publisher></journal-meta><article-meta><article-id custom-type="elpub" pub-id-type="custom">alternative-31</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>ОПТИЧЕСКИЕ ЯВЛЕНИЯ И УСТРОЙСТВА</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>OPTICAL PHENOMENA AND FACILITIES</subject></subj-group></article-categories><title-group><article-title>LiNbO3 КЛИНООБРАЗНАЯ TГц АНТЕННА, ЧАСТИЧНО ЗАПОЛНЯЮЩАЯ МЕТАЛЛИЧЕСКИЙ ВОЛНОВОД</article-title><trans-title-group xml:lang="en"><trans-title>LiNbO3 TAPERED THz ANTENNA  PARTIALLY FILLING THE METAL WAVEGUIDE</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Никогосян</surname><given-names>А. С.</given-names></name><name name-style="western" xml:lang="en"><surname>Nikoghosyan</surname><given-names>A. S.</given-names></name></name-alternatives><bio xml:lang="ru"><p>канд. физ.-мат. наук, доцент кафедры радиофизики СВЧ и телекоммуникаций</p></bio><bio xml:lang="en"><p>PhD, Associate Professor, Department of Microwave Radiophysics and Telecommunications</p></bio><email xlink:type="simple">nika@ysu.am</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru">Ереванский Государственный университет<country>Армения</country></aff><aff xml:lang="en">Yerevan State University<country>Armenia</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2015</year></pub-date><pub-date pub-type="epub"><day>07</day><month>11</month><year>2015</year></pub-date><volume>0</volume><issue>6</issue><fpage>87</fpage><lpage>91</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Международный издательский дом научной периодики "Спейс, 2015</copyright-statement><copyright-year>2015</copyright-year><copyright-holder xml:lang="ru">Международный издательский дом научной периодики "Спейс</copyright-holder><copyright-holder xml:lang="en">Международный издательский дом научной периодики "Спейс</copyright-holder><license xlink:href="https://www.isjaee.com/jour/about/submissions#copyrightNotice" xlink:type="simple"><license-p>https://www.isjaee.com/jour/about/submissions#copyrightNotice</license-p></license></permissions><self-uri xlink:href="https://www.isjaee.com/jour/article/view/31">https://www.isjaee.com/jour/article/view/31</self-uri><abstract><p>В работе представлены результаты генерации широкополосного ТГц излучения в области 0,1-2 ТГц. Генерация ТГц излучения осуществлена в нелинейном кристалле LiNbO3 клинообразной формы благодаря нелинейному эффекту – оптическому выпрямлению фемтосекундных световых лазерных импульсов. Показано, что временные и частотные характеристики ТГц поля, излученного нелинейным клинообразным кристаллом, частично заполняющим металлический волновод, меняются,  если  кристалл  расположить  в  свободном  пространстве. В  спектре ТГц  импульса  интенсивные  спектральные линии наблюдались на частотах 279 ГГц и 1 ТГц.  </p></abstract><trans-abstract xml:lang="en"><p>Results on generation of ultrabroadband terahertz (THz) radiation in band 0.1-2 THz via optical rectification of femtosecond laser pulses in nonlinear tapered crystal are presented. It is shown that placing the LiNbO3 crystal in the free space and in the hollow waveguide both the time and spectral features of the emitted THz field are changed. Several intense spectral regions (at 279 GHz and 1 ТHz) whose frequency depends on the LiNbO3 size are observed. Excitation of ТHz radiation in the tapered nonlinear crystal antenna, partially filling the metal waveguide with the help of an optical femtosecond laser pulse permits the resolution of problems connected with input/output coupling – mode matching and single mode propagation.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>оптическое  выпрямление</kwd><kwd>фемтосекундный лазер</kwd><kwd>терагерцовое излучениe</kwd><kwd>клинообразная ТГц антенна</kwd><kwd>частично заполненный металлический волновод</kwd></kwd-group><kwd-group xml:lang="en"><kwd>optical rectification</kwd><kwd>femtosecond laser</kwd><kwd>terahertz radiation</kwd><kwd>tapered THz antenna</kwd><kwd>partially filling the metallic wаveguide</kwd></kwd-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Stockman M.I. Nanofocusing of optical energy in tapered plasmonic waveguides // Phys. Rev. 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