. "\uC774\uB860\uBB3C\uB9AC\uD559\uC5D0\uC11C \uD53C\uC5D0\uB974\uCE20-\uD30C\uC6B8\uB9AC \uC791\uC6A9(Fierz-Pauli\u4F5C\u7528, \uC601\uC5B4: Fierz\u2013Pauli action) \uB610\uB294 \uC120\uD615\uD654 \uC911\uB825(\u7DDA\u578B\u5316\u91CD\u529B, \uC601\uC5B4: linearized gravity)\uC740 \uC2A4\uD540 2\uC758 \uBB34\uC9C8\uB7C9 \uC790\uC720 \uC785\uC790\uB97C \uB098\uD0C0\uB0B4\uB294 \uC791\uC6A9\uC774\uB2E4. \uC774\uB294 \uC77C\uBC18 \uC0C1\uB300\uC131\uC774\uB860 \uBC0F \uB2E4\uB978 \uC911\uB825 \uC774\uB860\uB4E4\uC758 \uC120\uD615\uD654 \uADF9\uD55C\uC5D0 \uD574\uB2F9\uD55C\uB2E4."@ko . . "\u0420\u0456\u0432\u043D\u044F\u043D\u043D\u044F \u0415\u0439\u043D\u0448\u0442\u0435\u0439\u043D\u0430, \u0432\u0438\u0432\u0435\u0434\u0435\u043D\u0435 \u0456\u0437 \u043F\u0440\u0438\u043D\u0446\u0438\u043F\u0456\u0432 \u0437\u0430\u0433\u0430\u043B\u044C\u043D\u043E\u0457 \u0442\u0435\u043E\u0440\u0456\u0457 \u0432\u0456\u0434\u043D\u043E\u0441\u043D\u043E\u0441\u0442\u0456: \u0454 \u043D\u0435\u043B\u0456\u043D\u0456\u0439\u043D\u0438\u043C \u0434\u0438\u0444\u0435\u0440\u0435\u043D\u0446\u0456\u0430\u043B\u044C\u043D\u0438\u043C \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F\u043C \u0434\u0440\u0443\u0433\u043E\u0433\u043E \u043F\u043E\u0440\u044F\u0434\u043A\u0443 \u0449\u043E\u0434\u043E \u043D\u0435\u0432\u0456\u0434\u043E\u043C\u0438\u0445 \u043A\u043E\u043C\u043F\u043E\u043D\u0435\u043D\u0442 \u043C\u0435\u0442\u0440\u0438\u0447\u043D\u043E\u0433\u043E \u0442\u0435\u043D\u0437\u043E\u0440\u0430 . \u0406\u0441\u043D\u0443\u0454 \u043F\u0440\u0430\u043A\u0442\u0438\u0447\u043D\u0438\u0439 \u0456\u043D\u0442\u0435\u0440\u0435\u0441 \u0432\u0438\u043F\u0430\u0434\u043E\u043A \u043D\u0430\u0441\u0442\u0456\u043B\u044C\u043A\u0438 \u0441\u043B\u0430\u0431\u043A\u043E\u0433\u043E \u0433\u0440\u0430\u0432\u0456\u0442\u0430\u0446\u0456\u0439\u043D\u043E\u0433\u043E \u043F\u043E\u043B\u044F, \u0449\u043E\u0431 \u043D\u0435\u043B\u0456\u043D\u0456\u0439\u043D\u043E\u0441\u0442\u044F\u043C\u0438 \u043C\u043E\u0436\u043D\u0430 \u0431\u0443\u043B\u043E \u0437\u043D\u0435\u0445\u0442\u0443\u0432\u0430\u0442\u0438 \u0456 \u043E\u0434\u0435\u0440\u0436\u0430\u0442\u0438 \u043D\u0430\u0431\u043B\u0438\u0436\u0435\u043D\u0435 \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F, \u044F\u043A\u0435 \u0431\u043B\u0438\u0437\u044C\u043A\u0435 \u0434\u043E \u043A\u043B\u0430\u0441\u0438\u0447\u043D\u043E\u0433\u043E \u0437\u0430\u043A\u043E\u043D\u0443 \u0412\u0441\u0435\u0441\u0432\u0456\u0442\u043D\u044C\u043E\u0433\u043E \u0442\u044F\u0436\u0456\u043D\u043D\u044F, \u0430\u043B\u0435 \u0437 \u0440\u0435\u043B\u044F\u0442\u0438\u0432\u0456\u0441\u0442\u0441\u044C\u043A\u0438\u043C\u0438 \u043F\u043E\u043F\u0440\u0430\u0432\u043A\u0430\u043C\u0438. \u0426\u0435 \u043D\u0430\u0431\u043B\u0438\u0436\u0435\u043D\u0435 \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F \u043C\u043E\u0436\u043D\u0430 \u0437\u0430\u0441\u0442\u043E\u0441\u043E\u0432\u0443\u0432\u0430\u0442\u0438 \u0432 \u043C\u0435\u0436\u0430\u0445 \u0421\u043E\u043D\u044F\u0447\u043D\u043E\u0457 \u0441\u0438\u0441\u0442\u0435\u043C\u0438 \u0456 \u043D\u0430\u0432\u0456\u0442\u044C \u043F\u0440\u0438 \u0440\u043E\u0437\u0433\u043B\u044F\u0434\u0456 \u0433\u0430\u043B\u0430\u043A\u0442\u0438\u043A \u2014 \u0430\u0434\u0436\u0435 \u0442\u0438\u043F\u043E\u0432\u0456 \u0448\u0432\u0438\u0434\u043A\u043E\u0441\u0442\u0456 \u0437\u0456\u0440\u043E\u043A \u0432 \u0433\u0430\u043B\u0430\u043A\u0442\u0438\u043A\u0430\u0445 \u0431\u0456\u043B\u044C\u0448 \u043D\u0456\u0436 \u0443 \u0442\u0438\u0441\u044F\u0447\u0443 \u0440\u0430\u0437\u0456\u0432 \u043C\u0435\u043D\u0448\u0456 \u0437\u0430 \u0448\u0432\u0438\u0434\u043A\u0456\u0441\u0442\u044C \u0441\u0432\u0456\u0442\u043B\u0430. \u0404 \u0449\u0435 \u043E\u0434\u043D\u0430 \u043F\u0440\u0438\u0447\u0438\u043D\u0430 \u0440\u043E\u0437\u0433\u043B\u044F\u043D\u0443\u0442\u0438 \u043B\u0456\u043D\u0435\u0430\u0440\u0438\u0437\u043E\u0432\u0430\u043D\u0435 \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F (1) - \u0437\u043D\u0430\u0439\u0442\u0438 \u043A\u043E\u043D\u0441\u0442\u0430\u043D\u0442\u0443 \u043F\u0440\u0438 \u0442\u0435\u043D\u0437\u043E\u0440\u0456 \u0435\u043D\u0435\u0440\u0433\u0456\u0457-\u0456\u043C\u043F\u0443\u043B\u044C\u0441\u0443, \u044F\u043A\u0430 \u0437\u0430\u043B\u0438\u0448\u0438\u043B\u0430\u0441\u044F \u043D\u0435\u0432\u0456\u0434\u043E\u043C\u043E\u044E \u043F\u0440\u0438 \u0432\u0438\u0432\u043E\u0434\u0456 \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F \u0415\u0439\u043D\u0448\u0442\u0435\u0439\u043D\u0430 (1)."@uk . "\u7DDA\u6027\u5316\u91CD\u529B\uFF08\u82F1\u8A9E\uFF1ALinearized gravity\uFF09\u662F\u5EE3\u7FA9\u76F8\u5C0D\u8AD6\u4E2D\u4E00\u500B\u8FD1\u4F3C\u65B9\u6848\uFF0C\u5176\u5FFD\u7565\u6642\u7A7A\u5EA6\u898F\u5F35\u91CF\u7684\u975E\u7DDA\u6027\u8CA2\u737B\u3002\u9019\u4F7F\u5F97\u8A31\u591A\u7814\u7A76\u554F\u984C\u5F97\u4EE5\u7C21\u5316\u3002"@zh . . . . "1051357129"^^ . . . . . "A aproxima\u00E7\u00E3o para campos gravitacionais fracos inclui encontrar solu\u00E7\u00F5es aproximadas das equa\u00E7\u00F5es de campo de Einstein da relatividade geral. A relatividade geral \u00E9 reduzida \u00E0 relatividade restrita na aus\u00EAncia de campos gravitacionais, o que n\u00E3o ocorre na pr\u00E1tica pois o universo inteiro \u00E9 considerado permeado por campo gravitacional. Assim sendo, podemos dizer que a relatividade geral pode ser aproximada da relatividade restrita na presen\u00E7a de campos gravitacionais fracos. Essa aproxima\u00E7\u00E3o assume grande import\u00E2ncia em f\u00EDsica, em diversos campos de sua aplica\u00E7\u00E3o, dado que campos gravitacionais em muitos sistemas f\u00EDsicos estudados s\u00E3o realmente fracos, como na maior parte de nosso sistema solar, onde a imensa maioria de nossas medi\u00E7\u00F5es s\u00E3o feitas."@pt . . . . "A aproxima\u00E7\u00E3o para campos gravitacionais fracos inclui encontrar solu\u00E7\u00F5es aproximadas das equa\u00E7\u00F5es de campo de Einstein da relatividade geral. A relatividade geral \u00E9 reduzida \u00E0 relatividade restrita na aus\u00EAncia de campos gravitacionais, o que n\u00E3o ocorre na pr\u00E1tica pois o universo inteiro \u00E9 considerado permeado por campo gravitacional. Assim sendo, podemos dizer que a relatividade geral pode ser aproximada da relatividade restrita na presen\u00E7a de campos gravitacionais fracos. Essa aproxima\u00E7\u00E3o assume grande import\u00E2ncia em f\u00EDsica, em diversos campos de sua aplica\u00E7\u00E3o, dado que campos gravitacionais em muitos sistemas f\u00EDsicos estudados s\u00E3o realmente fracos, como na maior parte de nosso sistema solar, onde a imensa maioria de nossas medi\u00E7\u00F5es s\u00E3o feitas."@pt . . . . . . . . . . . . "Approssimazione per i campi gravitazionali deboli"@it . "La aproximaci\u00F3n para campos gravitatorios d\u00E9biles comprende la b\u00FAsqueda de soluciones aproximadas de las ecuaciones del campo de Einstein de la teor\u00EDa general de la relatividad."@es . . "\u0420\u0456\u0432\u043D\u044F\u043D\u043D\u044F \u0415\u0439\u043D\u0448\u0442\u0435\u0439\u043D\u0430, \u0432\u0438\u0432\u0435\u0434\u0435\u043D\u0435 \u0456\u0437 \u043F\u0440\u0438\u043D\u0446\u0438\u043F\u0456\u0432 \u0437\u0430\u0433\u0430\u043B\u044C\u043D\u043E\u0457 \u0442\u0435\u043E\u0440\u0456\u0457 \u0432\u0456\u0434\u043D\u043E\u0441\u043D\u043E\u0441\u0442\u0456: \u0454 \u043D\u0435\u043B\u0456\u043D\u0456\u0439\u043D\u0438\u043C \u0434\u0438\u0444\u0435\u0440\u0435\u043D\u0446\u0456\u0430\u043B\u044C\u043D\u0438\u043C \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F\u043C \u0434\u0440\u0443\u0433\u043E\u0433\u043E \u043F\u043E\u0440\u044F\u0434\u043A\u0443 \u0449\u043E\u0434\u043E \u043D\u0435\u0432\u0456\u0434\u043E\u043C\u0438\u0445 \u043A\u043E\u043C\u043F\u043E\u043D\u0435\u043D\u0442 \u043C\u0435\u0442\u0440\u0438\u0447\u043D\u043E\u0433\u043E \u0442\u0435\u043D\u0437\u043E\u0440\u0430 . \u0406\u0441\u043D\u0443\u0454 \u043F\u0440\u0430\u043A\u0442\u0438\u0447\u043D\u0438\u0439 \u0456\u043D\u0442\u0435\u0440\u0435\u0441 \u0432\u0438\u043F\u0430\u0434\u043E\u043A \u043D\u0430\u0441\u0442\u0456\u043B\u044C\u043A\u0438 \u0441\u043B\u0430\u0431\u043A\u043E\u0433\u043E \u0433\u0440\u0430\u0432\u0456\u0442\u0430\u0446\u0456\u0439\u043D\u043E\u0433\u043E \u043F\u043E\u043B\u044F, \u0449\u043E\u0431 \u043D\u0435\u043B\u0456\u043D\u0456\u0439\u043D\u043E\u0441\u0442\u044F\u043C\u0438 \u043C\u043E\u0436\u043D\u0430 \u0431\u0443\u043B\u043E \u0437\u043D\u0435\u0445\u0442\u0443\u0432\u0430\u0442\u0438 \u0456 \u043E\u0434\u0435\u0440\u0436\u0430\u0442\u0438 \u043D\u0430\u0431\u043B\u0438\u0436\u0435\u043D\u0435 \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F, \u044F\u043A\u0435 \u0431\u043B\u0438\u0437\u044C\u043A\u0435 \u0434\u043E \u043A\u043B\u0430\u0441\u0438\u0447\u043D\u043E\u0433\u043E \u0437\u0430\u043A\u043E\u043D\u0443 \u0412\u0441\u0435\u0441\u0432\u0456\u0442\u043D\u044C\u043E\u0433\u043E \u0442\u044F\u0436\u0456\u043D\u043D\u044F, \u0430\u043B\u0435 \u0437 \u0440\u0435\u043B\u044F\u0442\u0438\u0432\u0456\u0441\u0442\u0441\u044C\u043A\u0438\u043C\u0438 \u043F\u043E\u043F\u0440\u0430\u0432\u043A\u0430\u043C\u0438. \u0426\u0435 \u043D\u0430\u0431\u043B\u0438\u0436\u0435\u043D\u0435 \u0440\u0456\u0432\u043D\u044F\u043D\u043D\u044F \u043C\u043E\u0436\u043D\u0430 \u0437\u0430\u0441\u0442\u043E\u0441\u043E\u0432\u0443\u0432\u0430\u0442\u0438 \u0432 \u043C\u0435\u0436\u0430\u0445 \u0421\u043E\u043D\u044F\u0447\u043D\u043E\u0457 \u0441\u0438\u0441\u0442\u0435\u043C\u0438 \u0456 \u043D\u0430\u0432\u0456\u0442\u044C \u043F\u0440\u0438 \u0440\u043E\u0437\u0433\u043B\u044F\u0434\u0456 \u0433\u0430\u043B\u0430\u043A\u0442\u0438\u043A \u2014 \u0430\u0434\u0436\u0435 \u0442\u0438\u043F\u043E\u0432\u0456 \u0448\u0432\u0438\u0434\u043A\u043E\u0441\u0442\u0456 \u0437\u0456\u0440\u043E\u043A \u0432 \u0433\u0430\u043B\u0430\u043A\u0442\u0438\u043A\u0430\u0445 \u0431\u0456\u043B\u044C\u0448 \u043D\u0456\u0436 \u0443 \u0442\u0438\u0441\u044F\u0447\u0443 \u0440\u0430\u0437\u0456\u0432 \u043C\u0435\u043D\u0448\u0456 \u0437\u0430 \u0448\u0432\u0438\u0434\u043A\u0456\u0441\u0442\u044C \u0441\u0432\u0456\u0442\u043B\u0430."@uk . . . "La aproximaci\u00F3n para campos gravitatorios d\u00E9biles comprende la b\u00FAsqueda de soluciones aproximadas de las ecuaciones del campo de Einstein de la teor\u00EDa general de la relatividad."@es . . . . . . . . "\u7DDA\u6027\u5316\u91CD\u529B\uFF08\u82F1\u8A9E\uFF1ALinearized gravity\uFF09\u662F\u5EE3\u7FA9\u76F8\u5C0D\u8AD6\u4E2D\u4E00\u500B\u8FD1\u4F3C\u65B9\u6848\uFF0C\u5176\u5FFD\u7565\u6642\u7A7A\u5EA6\u898F\u5F35\u91CF\u7684\u975E\u7DDA\u6027\u8CA2\u737B\u3002\u9019\u4F7F\u5F97\u8A31\u591A\u7814\u7A76\u554F\u984C\u5F97\u4EE5\u7C21\u5316\u3002"@zh . . . . . . . "\u0421\u043B\u0430\u0431\u043A\u0435 \u0433\u0440\u0430\u0432\u0456\u0442\u0430\u0446\u0456\u0439\u043D\u0435 \u043F\u043E\u043B\u0435"@uk . . . . "\uD53C\uC5D0\uB974\uCE20-\uD30C\uC6B8\uB9AC \uC791\uC6A9"@ko . . "2865024"^^ . . . "L'approximation des champs faibles en relativit\u00E9 g\u00E9n\u00E9rale est utilis\u00E9e pour d\u00E9crire les champs gravitationnels loin de la source de la gravit\u00E9. Elle permet de retrouver les lois de la gravitation de Newton."@fr . . . . . . "Eremu grabitatorio ahulen hurbilketa"@eu . . . . "Eremu grabitatorio ahuletarako hurbilketan, gutxi gora-beherako soluzioak bilatzen dira erlatibitate orokorraren teoriako Einsteinen eremu-ekuazioetarako. Erlatibitate orokorraren teorian, grabitate linealizatua espazio-denboraren geometria deskribatzeko tentsore metrikoan aplikatzeari deritzo. Ondorioz, grabitate linearizatuaren bidez, grabitazio-eremuak ahulak direneko grabitatearen efektuak modu eraginkor batean modelatu daitezke. Grabitate linearizatuaren erabilera ezinbestekoa da grabitazio-uhin eta eremu ahuleko grabitazio-leiarren azterketarako."@eu . "Approximation des champs faibles"@fr . "\uC774\uB860\uBB3C\uB9AC\uD559\uC5D0\uC11C \uD53C\uC5D0\uB974\uCE20-\uD30C\uC6B8\uB9AC \uC791\uC6A9(Fierz-Pauli\u4F5C\u7528, \uC601\uC5B4: Fierz\u2013Pauli action) \uB610\uB294 \uC120\uD615\uD654 \uC911\uB825(\u7DDA\u578B\u5316\u91CD\u529B, \uC601\uC5B4: linearized gravity)\uC740 \uC2A4\uD540 2\uC758 \uBB34\uC9C8\uB7C9 \uC790\uC720 \uC785\uC790\uB97C \uB098\uD0C0\uB0B4\uB294 \uC791\uC6A9\uC774\uB2E4. \uC774\uB294 \uC77C\uBC18 \uC0C1\uB300\uC131\uC774\uB860 \uBC0F \uB2E4\uB978 \uC911\uB825 \uC774\uB860\uB4E4\uC758 \uC120\uD615\uD654 \uADF9\uD55C\uC5D0 \uD574\uB2F9\uD55C\uB2E4."@ko . . . . . "L'approximation des champs faibles en relativit\u00E9 g\u00E9n\u00E9rale est utilis\u00E9e pour d\u00E9crire les champs gravitationnels loin de la source de la gravit\u00E9. Elle permet de retrouver les lois de la gravitation de Newton."@fr . "L'approssimazione per i campi gravitazionali deboli o gravit\u00E0 linearizzata o linearizzazione delle equazioni di Einstein \u00E8 uno schema di approssimazione nella relativit\u00E0 generale in cui vengono ignorati i contributi non lineari della metrica dello spazio-tempo. Ci\u00F2 permette di semplificare lo studio di molti problemi."@it . . . "Aproxima\u00E7\u00E3o para campos gravitacionais fracos"@pt . . "L'approssimazione per i campi gravitazionali deboli o gravit\u00E0 linearizzata o linearizzazione delle equazioni di Einstein \u00E8 uno schema di approssimazione nella relativit\u00E0 generale in cui vengono ignorati i contributi non lineari della metrica dello spazio-tempo. Ci\u00F2 permette di semplificare lo studio di molti problemi."@it . "Linearized gravity"@en . . "\u7DDA\u6027\u5316\u91CD\u529B"@zh . "Aproximaci\u00F3n para campos gravitatorios d\u00E9biles"@es . . . "Eremu grabitatorio ahuletarako hurbilketan, gutxi gora-beherako soluzioak bilatzen dira erlatibitate orokorraren teoriako Einsteinen eremu-ekuazioetarako. Erlatibitate orokorraren teorian, grabitate linealizatua espazio-denboraren geometria deskribatzeko tentsore metrikoan aplikatzeari deritzo. Ondorioz, grabitate linearizatuaren bidez, grabitazio-eremuak ahulak direneko grabitatearen efektuak modu eraginkor batean modelatu daitezke. Grabitate linearizatuaren erabilera ezinbestekoa da grabitazio-uhin eta eremu ahuleko grabitazio-leiarren azterketarako."@eu . "In the theory of general relativity, linearized gravity is the application of perturbation theory to the metric tensor that describes the geometry of spacetime. As a consequence, linearized gravity is an effective method for modeling the effects of gravity when the gravitational field is weak. The usage of linearized gravity is integral to the study of gravitational waves and weak-field gravitational lensing."@en . . . . "10641"^^ . "In the theory of general relativity, linearized gravity is the application of perturbation theory to the metric tensor that describes the geometry of spacetime. As a consequence, linearized gravity is an effective method for modeling the effects of gravity when the gravitational field is weak. The usage of linearized gravity is integral to the study of gravitational waves and weak-field gravitational lensing."@en .