銆�銆�寰尝鍌虫劅鍣ㄤ富瑕佺敱寰尝鎸暕鍣ㄥ拰寰尝澶╃窔绲勬垚銆傚井娉㈡尟钑╁櫒鏄敘鐢熷井娉㈢殑瑁濈疆銆傛鎴愬井娉㈡尟钑╁櫒鐨勫櫒浠舵湁閫熻绠�銆佺鎺х鎴栨煇浜涘浐楂斿厓浠躲�傜敱寰尝鎸暕鍣ㄧ敘鐢熺殑鎸暕淇¤櫉闇�鐢ㄦ尝灏庣鍌宠几锛屽苟閫氶亷澶╃窔鐧�(f膩)灏勫嚭鍘汇�傜偤浜嗕娇鐧�(f膩)灏勭殑寰尝鍏锋湁涓�鑷寸殑鏂瑰悜鎬�锛屽ぉ绶氭噳鍏锋湁鐗规畩鐨勬閫犲拰褰㈢媭銆�
鏂规硶
闂滀簬璜ф尟寮忓井娉㈠偝鎰熷櫒鐨勫熀鏈師鐞嗘杩板涓嬶細涓�鍊嬩粙璩～鍏呰鎸厰鐨勮鎸牷鐜囧拰鍝佽唱鍥犲瓙鍜屽～鍏呬粙璩殑浠嬮浕甯告暩涔嬮枔鐨勯棞绯诲寮忓瓙锛�1锛夛紝灏嶄竴鑸殑鍟忛鎴戝�戦兘閲囩敤Harrington鎻愬嚭鐨勭悊璜栨柟娉曚締姹傝В?锛孎(xi脿n)鍦ㄨ�冩叜涓�鍊嬬湡绌虹殑鑵旈珨锛屼护鍏惰鎸牷鐜囧拰鍏朵腑鐨勯浕纾佸牬鍒嗗垾鐐� 蠅0 E0 H0 , 鐩告噳鍦�锛屽亣瑷従(xi脿n)鍦ㄨ厰楂旇濉厖浜嗕粙闆诲父鏁哥偤蔚=蔚0+螖蔚鐨勪粙璩�銆�
璜ф尟闋荤巼鐨勮┎璁婇噺濡備笅寮忓瓙鎵�绀猴細
鍏朵腑蠅, E, H 鏄叾璜ф尟闋荤巼鍜屽皪鎳夌殑闆荤鍫村垎甯�銆傚京鏁稿舰寮忕殑璜ф尟闋荤巼鐢卞鏁搁儴鍒喯塕 鍜屽寘鍚搧璩洜瀛怮 鐨勮櫅閮ㄥ叐閮ㄥ垎绲勬垚銆�
鍏朵腑鐨勫搧璩洜瀛愬彲浠ュ鎴�
鍦ㄥ紡瀛�(3)涓� W 鏄竴娈垫檪闁撳収璜ф尟鑵旈噷瀛樺劜鐨勫钩鍧囪兘閲忥紝Pd 鏄柈浣嶆檪闁撴悕鑰楃殑鑳介噺銆�
涓婇潰鐨勫紡瀛愯〃鏄庯紝鍋囧鎴戝�戝凡鐭ヤ簡寰呮脯鏉愭枡鐨勮鎸牷鐜囅塕鍜屽搧璩洜瀛怮 灏卞彲浠ユ眰寰楀緟娓潗鏂欑殑寰╀粙闆诲父鏁搞��
Fig. 1 - Example of the results of the fitting algorithm applied to the measured da
鍦�1灞曠ず浜嗕竴鍊嬭鎸厰鐨勫吀鍨嬫脯瑭︽洸绶�锛屽湒涓郸鍑轰簡璜ф尟闋荤巼f0鍜�3dB 甯跺 BW=1/Q 銆�
娓│鏉愭枡鐨勫京浠嬮浕甯告暩 蔚=蔚'-j蔚'' 鍖呮嫭浠ヤ笅骞惧�嬫椹燂細
a. 娓噺浠嬭唱濉厖璜ф尟鑵旂殑s21鍙冩暩銆�
b. 瑷堢畻璜ф尟闋荤巼鍜�3dB甯跺銆�
c. 鏍规摎鍏紡锛�1锛夎▓绠楀緟娓潗鏂欑殑寰╀粙闆诲父鏁�銆�
鐐轰簡鐛插緱杓冮珮绮惧害鐨勮鎸牷鐜囧拰3dB甯跺锛屾噳瑭查噰鐢ㄨ純绐勭殑闋荤巼姝ラ暦锛岄�欐ǎ鏈冨緱鍒板緢澶氶牷鐜囬噰妯�锛岄�欏皪浜庡鏅傛脯閲忕殑閫熷害鏄笉鍒╃殑銆俆o circumvent this difficulty, the resonant response is fitted in a least square sense to the Lorentzian curve (4):
缍韩闆诲瓙閫�锛岄浕瀛愮煡璀橈紝涓�鏌ョ櫨閫�锛�
宸叉敹閷勮姊�153979鍊�
