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"\u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u062F\u0627\u0626\u0631\u064A \u0641\u064A \u0639\u0644\u0645 \u0627\u0644\u0628\u0635\u0631\u064A\u0627\u062A \u0648\u0627\u0644\u0636\u0648\u0621 \u0647\u0648 \u0623\u0646 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u0645\u0646 \u0645\u0648\u062C\u0629 \u0627\u0644\u0636\u0648\u0621 \u0644\u0627 \u062A\u062A\u063A\u064A\u0631 \u0634\u062F\u062A\u0647 \u0648\u0627\u0646\u0645\u0627 \u064A\u062A\u063A\u064A\u0631 \u0627\u062A\u062C\u0627\u0647\u0647 \u0628\u0634\u0643\u0644 \u062F\u0627\u0626\u0631\u064A. \u0641\u064A \u0627\u0644\u0639\u0644\u0648\u0645 \u0641\u0625\u0646 \u0634\u062F\u0629 \u0648\u0627\u062A\u062C\u0627\u0647 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u062A\u0639\u0631\u0641 \u0628\u0645\u0627 \u064A\u0637\u0644\u0642 \u0639\u0644\u064A\u0647 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u0627\u0644\u0645\u062A\u062C\u0647\u064A (\u0628\u0627\u0644\u0625\u0646\u062C\u0644\u064A\u0632\u064A\u0629:electric field vector). \u0641\u064A \u062D\u0627\u0644\u0629 \u0627\u0644\u0645\u0648\u062C\u0629 \u0627\u0644\u0643\u0647\u0631\u0648\u0645\u063A\u0646\u0627\u0637\u064A\u0633\u064A\u0629 \u0627\u0644\u0636\u0648\u0626\u064A\u0629 \u0627\u0644\u0645\u0633\u062A\u0642\u0637\u0628\u0629 \u062F\u0627\u0626\u0631\u064A\u0627 \u0643\u0645\u0627 \u0641\u064A \u0627\u0644\u0635\u0648\u0631\u0629 \u0641\u0625\u0646 \u0646\u0647\u0627\u064A\u0629 \u0627\u0644\u0645\u062A\u062C\u0647 \u0644\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u062A\u0635\u0641 \u062F\u0627\u0626\u0631\u0629 \u0641\u064A \u0643\u0644 \u0646\u0642\u0637\u0629 \u0641\u0636\u0627\u0626\u064A\u0629 (\u0645\u062A\u062C\u0647\u064A\u0629). \u0641\u064A \u062D\u0627\u0644\u0629 \u062A\u0648\u0642\u064A\u0641 \u0627\u0644\u0635\u0648\u0631\u0629 \u0627\u0644\u0645\u062A\u062D\u0631\u0643\u0629 \u0632\u0645\u0646\u064A\u0627\u064B\u060C \u0641\u064A\u0635\u0641 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u0627\u0644\u0645\u062A\u062C\u0647\u064A \u0634\u0643\u0644 \u062D\u0644\u0632\u0648\u0646\u064A\u0627 \u0639\u0644\u0649 \u0627\u0645\u062A\u062F\u0627\u062F \u0627\u0646\u062A\u0634\u0627\u0631 \u0627\u0644\u0645\u0648\u062C\u0629 \u0627\u0644\u0636\u0648\u0626\u064A\u0629.\u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u062F\u0627\u0626\u0631\u064A \u0647\u0648 \u062D\u0627\u0644\u0629 \u062E\u0627\u0635\u0629 \u0645\u0646 \u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u0628\u064A\u0636\u0627\u0648\u064A. \u0627\u0644\u062D\u0627\u0644\u0629 \u0627\u0644\u062B\u0627\u0646\u064A\u0629 \u0647\u064A \u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u062E\u0637\u064A \u0628\u062D\u064A\u062B \u064A\u0645\u0643\u0646 \u062A\u062E\u064A\u0644\u0647 \u0628\u0627\u0633\u062A\u0642\u0637\u0627\u0628\u064A\u0646 \u062F\u0627\u0626\u0631\u064A\u064A\u0646 \u0645\u0646\u0639\u0643\u0633\u064A \u0627\u0644\u0627\u062A\u062C\u0627\u0647 \u0641\u064A \u0627\u0644\u062F\u0648\u0631\u0627\u0646\u060C \u0628\u062D\u064A\u062B \u064A\u062F\u0648\u0631 \u062C\u0632\u0621 \u0645\u0639 \u0639\u0642\u0627\u0631\u0628 \u0627\u0644\u0633\u0627\u0639\u0629 \u0648\u0627\u0644\u0622\u062E\u0631 \u0628\u0639\u0643\u0633\u0647\u0627."@ar . . . . . . . . . . "\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u062F\u0627\u0626\u0631\u064A"@ar . . . . . . . . . . . . . . . . . . . . . . "Zirkularpolarisation"@de . "40875"^^ . . . . . . . . "Left-handed/counterclockwise circularly polarized light displayed with and without the use of components. This would be considered right-handed/clockwise circularly polarized if defined from the point of view of the source rather than the receiver."@en . "Polaritzaci\u00F3 circular"@ca . . . "In electrodynamics, circular polarization of an electromagnetic wave is a polarization state in which, at each point, the electromagnetic field of the wave has a constant magnitude and is rotating at a constant rate in a plane perpendicular to the direction of the wave. The phenomenon of polarization arises as a consequence of the fact that light behaves as a two-dimensional transverse wave. Circular polarization occurs when the two orthogonal electric field component vectors are of equal magnitude and are out of phase by exactly 90\u00B0, or one-quarter wavelength."@en . . "left"@en . . . . . . "\u0412 \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u0434\u0438\u043D\u0430\u043C\u0438\u043A\u0435 \u043A\u0440\u0443\u0433\u043E\u0432\u0430\u044F \u043F\u043E\u043B\u044F\u0440\u0438\u0437\u0430\u0446\u0438\u044F \u0438\u043B\u0438 \u0438\u043D\u0430\u0447\u0435 \u0446\u0438\u0440\u043A\u0443\u043B\u044F\u0440\u043D\u0430\u044F \u043F\u043E\u043B\u044F\u0440\u0438\u0437\u0430\u0446\u0438\u044F \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0438\u0442\u043D\u043E\u0433\u043E \u0438\u0437\u043B\u0443\u0447\u0435\u043D\u0438\u044F \u2014 \u044D\u0442\u043E \u043E\u0434\u043D\u043E \u0438\u0437 \u0441\u043E\u0441\u0442\u043E\u044F\u043D\u0438\u0439 \u043F\u043E\u043B\u044F\u0440\u0438\u0437\u0430\u0446\u0438\u0438, \u043F\u0440\u0438 \u043A\u043E\u0442\u043E\u0440\u043E\u0439 \u0432\u0435\u043A\u0442\u043E\u0440 \u044D\u043B\u0435\u043A\u0442\u0440\u0438\u0447\u0435\u0441\u043A\u043E\u0433\u043E \u043F\u043E\u043B\u044F E \u0432 \u043A\u0430\u0436\u0434\u043E\u0439 \u0442\u043E\u0447\u043A\u0435 \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0438\u0442\u043D\u043E\u0433\u043E \u043F\u043E\u043B\u044F \u0432\u043E\u043B\u043D\u044B \u0438\u043C\u0435\u0435\u0442 \u043F\u043E\u0441\u0442\u043E\u044F\u043D\u043D\u0443\u044E \u0432\u0435\u043B\u0438\u0447\u0438\u043D\u0443, \u043D\u043E \u0435\u0433\u043E \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u0438\u0435 \u0432\u0440\u0430\u0449\u0430\u0435\u0442\u0441\u044F \u0441 \u043F\u043E\u0441\u0442\u043E\u044F\u043D\u043D\u043E\u0439 \u0441\u043A\u043E\u0440\u043E\u0441\u0442\u044C\u044E \u0432 \u043F\u043B\u043E\u0441\u043A\u043E\u0441\u0442\u0438, \u043F\u0435\u0440\u043F\u0435\u043D\u0434\u0438\u043A\u0443\u043B\u044F\u0440\u043D\u043E\u0439 \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u0438\u044E \u0440\u0430\u0441\u043F\u0440\u043E\u0441\u0442\u0440\u0430\u043D\u0435\u043D\u0438\u044F \u0432\u043E\u043B\u043D\u044B."@ru . . . "38313"^^ . . . . . . . . . . . . . . . "Circular.Polarization.Circularly.Polarized.Light_With.Components_Right.Handed.svg"@en . . . . . . . "In electrodynamics, circular polarization of an electromagnetic wave is a polarization state in which, at each point, the electromagnetic field of the wave has a constant magnitude and is rotating at a constant rate in a plane perpendicular to the direction of the wave. In electrodynamics, the strength and direction of an electric field is defined by its electric field vector. In the case of a circularly polarized wave, as seen in the accompanying animation, the tip of the electric field vector, at a given point in space, relates to the phase of the light as it travels through time and space. At any instant of time, the electric field vector of the wave indicates a point on a helix oriented along the direction of propagation. A circularly polarized wave can rotate in one of two possible senses: clockwise or right-handed circular polarization (RHCP) in which the electric field vector rotates in a right-hand sense with respect to the direction of propagation, and counter-clockwise or left-handed circular polarization (LHCP) in which the vector rotates in a left-hand sense. Circular polarization is a limiting case of elliptical polarization. The other special case is the easier-to-understand linear polarization. All three terms were coined by Augustin-Jean Fresnel, in a memoir read to the French Academy of Sciences on 9 December 1822. Fresnel had first described the case of circular polarization, without yet naming it, in 1821. The phenomenon of polarization arises as a consequence of the fact that light behaves as a two-dimensional transverse wave. Circular polarization occurs when the two orthogonal electric field component vectors are of equal magnitude and are out of phase by exactly 90\u00B0, or one-quarter wavelength."@en . "La polarisation circulaire d'un rayonnement \u00E9lectromagn\u00E9tique est une polarisation o\u00F9 la norme du vecteur du champ \u00E9lectrique ne change pas alors que son orientation change selon un mouvement de rotation. En \u00E9lectrodynamique la norme et la direction d'un champ \u00E9lectrique sont repr\u00E9sent\u00E9s par un vecteur comme on peut le voir dans l'animation ci-contre. Dans le cas d'une onde polaris\u00E9e circulairement, les vecteurs d'un champ \u00E9lectrique, \u00E0 un point donn\u00E9 dans l'espace, d\u00E9crivent un cercle en fonction du temps. Si l'on observe l'onde \u00E0 un moment donn\u00E9, le vecteur du champ \u00E9lectrique de l'onde d\u00E9crit un mouvement h\u00E9lico\u00EFdal le long de la direction de propagation. La polarisation circulaire est un cas particulier de la (en), tout comme la (en). Le ph\u00E9nom\u00E8ne de polarisation se pr\u00E9sente comme une cons\u00E9quence du fait que la lumi\u00E8re se comporte comme une onde transversale \u00E0 deux dimensions."@fr . . . . . . . "En electrodin\u00E1mica, la polarizaci\u00F3n circular\u200B de una onda electromagn\u00E9tica es una polarizaci\u00F3n en la que el campo el\u00E9ctrico de la onda de paso no cambia la fuerza, sino solo de direcci\u00F3n de una manera rotativa. En electrodin\u00E1mica, la fuerza y la direcci\u00F3n de un campo el\u00E9ctrico, se define por lo que se llama un . En el caso de una onda polarizada circularmente, como se ve en la animaci\u00F3n de acompa\u00F1amiento, la punta del campo el\u00E9ctrico vector, en un punto dado en el espacio, describe un c\u00EDrculo a medida que avanza el tiempo. Si la onda se congela en el tiempo, el campo de vector el\u00E9ctrico de la onda describe una h\u00E9lice a lo largo de la direcci\u00F3n de propagaci\u00F3n. La polarizaci\u00F3n circular es un de la condici\u00F3n m\u00E1s general de polarizaci\u00F3n el\u00EDptica. El otro es el m\u00E1s f\u00E1cil de entender, la polarizaci\u00F3n lineal. El fen\u00F3meno de la polarizaci\u00F3n surge como consecuencia del hecho de que la luz se comporta como una onda transversal de dos dimensiones."@es . . . . . "Right-handed/clockwise circularly polarized light displayed with and without the use of components. This would be considered left-handed/counterclockwise circularly polarized if defined from the point of view of the source rather than the receiver. Refer to the below [[#Left.2Fright handedness conventions"@en . . "\u041A\u0440\u0443\u0433\u043E\u0432\u0430\u044F \u043F\u043E\u043B\u044F\u0440\u0438\u0437\u0430\u0446\u0438\u044F"@ru . . . . . . . . . . . . . "Polarisation circulaire"@fr . . "Polarizaci\u00F3n circular"@es . . . . . . . . . "La polarisation circulaire d'un rayonnement \u00E9lectromagn\u00E9tique est une polarisation o\u00F9 la norme du vecteur du champ \u00E9lectrique ne change pas alors que son orientation change selon un mouvement de rotation. La polarisation circulaire est un cas particulier de la (en), tout comme la (en). Le ph\u00E9nom\u00E8ne de polarisation se pr\u00E9sente comme une cons\u00E9quence du fait que la lumi\u00E8re se comporte comme une onde transversale \u00E0 deux dimensions."@fr . "440"^^ . . . . . . . . . . "Circular.Polarization.Circularly.Polarized.Light_Without.Components_Right.Handed.svg"@en . "1123720334"^^ . "Circular.Polarization.Circularly.Polarized.Light_Without.Components_Left.Handed.svg"@en . . . . "En electrodin\u00E1mica, la polarizaci\u00F3n circular\u200B de una onda electromagn\u00E9tica es una polarizaci\u00F3n en la que el campo el\u00E9ctrico de la onda de paso no cambia la fuerza, sino solo de direcci\u00F3n de una manera rotativa. La polarizaci\u00F3n circular es un de la condici\u00F3n m\u00E1s general de polarizaci\u00F3n el\u00EDptica. El otro es el m\u00E1s f\u00E1cil de entender, la polarizaci\u00F3n lineal. El fen\u00F3meno de la polarizaci\u00F3n surge como consecuencia del hecho de que la luz se comporta como una onda transversal de dos dimensiones."@es . . . "Circular.Polarization.Circularly.Polarized.Light_With.Components_Left.Handed.svg"@en . "Circular polarization"@en . . . . . . . . . . . . . . . . . . . "\u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u062F\u0627\u0626\u0631\u064A \u0641\u064A \u0639\u0644\u0645 \u0627\u0644\u0628\u0635\u0631\u064A\u0627\u062A \u0648\u0627\u0644\u0636\u0648\u0621 \u0647\u0648 \u0623\u0646 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u0645\u0646 \u0645\u0648\u062C\u0629 \u0627\u0644\u0636\u0648\u0621 \u0644\u0627 \u062A\u062A\u063A\u064A\u0631 \u0634\u062F\u062A\u0647 \u0648\u0627\u0646\u0645\u0627 \u064A\u062A\u063A\u064A\u0631 \u0627\u062A\u062C\u0627\u0647\u0647 \u0628\u0634\u0643\u0644 \u062F\u0627\u0626\u0631\u064A. \u0641\u064A \u0627\u0644\u0639\u0644\u0648\u0645 \u0641\u0625\u0646 \u0634\u062F\u0629 \u0648\u0627\u062A\u062C\u0627\u0647 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u062A\u0639\u0631\u0641 \u0628\u0645\u0627 \u064A\u0637\u0644\u0642 \u0639\u0644\u064A\u0647 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u0627\u0644\u0645\u062A\u062C\u0647\u064A (\u0628\u0627\u0644\u0625\u0646\u062C\u0644\u064A\u0632\u064A\u0629:electric field vector). \u0641\u064A \u062D\u0627\u0644\u0629 \u0627\u0644\u0645\u0648\u062C\u0629 \u0627\u0644\u0643\u0647\u0631\u0648\u0645\u063A\u0646\u0627\u0637\u064A\u0633\u064A\u0629 \u0627\u0644\u0636\u0648\u0626\u064A\u0629 \u0627\u0644\u0645\u0633\u062A\u0642\u0637\u0628\u0629 \u062F\u0627\u0626\u0631\u064A\u0627 \u0643\u0645\u0627 \u0641\u064A \u0627\u0644\u0635\u0648\u0631\u0629 \u0641\u0625\u0646 \u0646\u0647\u0627\u064A\u0629 \u0627\u0644\u0645\u062A\u062C\u0647 \u0644\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u062A\u0635\u0641 \u062F\u0627\u0626\u0631\u0629 \u0641\u064A \u0643\u0644 \u0646\u0642\u0637\u0629 \u0641\u0636\u0627\u0626\u064A\u0629 (\u0645\u062A\u062C\u0647\u064A\u0629). \u0641\u064A \u062D\u0627\u0644\u0629 \u062A\u0648\u0642\u064A\u0641 \u0627\u0644\u0635\u0648\u0631\u0629 \u0627\u0644\u0645\u062A\u062D\u0631\u0643\u0629 \u0632\u0645\u0646\u064A\u0627\u064B\u060C \u0641\u064A\u0635\u0641 \u0627\u0644\u062D\u0642\u0644 \u0627\u0644\u0643\u0647\u0631\u0628\u0627\u0626\u064A \u0627\u0644\u0645\u062A\u062C\u0647\u064A \u0634\u0643\u0644 \u062D\u0644\u0632\u0648\u0646\u064A\u0627 \u0639\u0644\u0649 \u0627\u0645\u062A\u062F\u0627\u062F \u0627\u0646\u062A\u0634\u0627\u0631 \u0627\u0644\u0645\u0648\u062C\u0629 \u0627\u0644\u0636\u0648\u0626\u064A\u0629.\u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u062F\u0627\u0626\u0631\u064A \u0647\u0648 \u062D\u0627\u0644\u0629 \u062E\u0627\u0635\u0629 \u0645\u0646 \u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u0628\u064A\u0636\u0627\u0648\u064A. \u0627\u0644\u062D\u0627\u0644\u0629 \u0627\u0644\u062B\u0627\u0646\u064A\u0629 \u0647\u064A \u0627\u0644\u0627\u0633\u062A\u0642\u0637\u0627\u0628 \u0627\u0644\u062E\u0637\u064A \u0628\u062D\u064A\u062B \u064A\u0645\u0643\u0646 \u062A\u062E\u064A\u0644\u0647 \u0628\u0627\u0633\u062A\u0642\u0637\u0627\u0628\u064A\u0646 \u062F\u0627\u0626\u0631\u064A\u064A\u0646 \u0645\u0646\u0639\u0643\u0633\u064A \u0627\u0644\u0627\u062A\u062C\u0627\u0647 \u0641\u064A \u0627\u0644\u062F\u0648\u0631\u0627\u0646\u060C \u0628\u062D\u064A\u062B \u064A\u062F\u0648\u0631 \u062C\u0632\u0621 \u0645\u0639 \u0639\u0642\u0627\u0631\u0628 \u0627\u0644\u0633\u0627\u0639\u0629 \u0648\u0627\u0644\u0622\u062E\u0631 \u0628\u0639\u0643\u0633\u0647\u0627."@ar . . . . . . "vertical"@en . . . . . . . . . "right"@en .