resonant wavelength 中文意思是什麼

resonant wavelength 解釋
共振波長
  • resonant : adj. 共振的;能共鳴的;反響的,有回聲的。adv. -ly
  • wavelength : 【無線電】波長。
  1. E., the carrier frequency of a gaussian beam deviates from the resonant frequency of a fabry - perot etalon ), variations of the peak intensity, the position of the peak intensity and the dwdm systems, has received considerable attention. in this work, after taking into account the wavelength - depended reflectivity distribution profile of a fiber bragg grating, the oscillation wavelength # _ ( 1 ) of long external cavity fiber bragg grat

    與共振情況(即高斯光束的載波頻率與法布里一拍羅濾波器的諧振頻率一致)相比,非共振條件(即高斯光束的載波頻率與法布里一拍羅濾波器的諧振頻率存在偏差)一透射光束的峰值強度、峰值強度所對應的位置、以及光斑的大小隨入射角的變化都發生了顯著的改變。
  2. The wavelength of pump light in white light mode is 400nm. 2. the excitonic tunneling from cdznse qw to cdse quantum dots under resonant excitation was investigated using femtosecond pump - probe technology on the cdznse quantum well / cdse quantum dots structure

    用飛秒脈沖泵浦-探測方法研究了cdse量子點znse cdznse量子阱結構在對cdznse量子阱的激子共振激發條件下激子在量子阱與量子點之間的隧穿。
  3. In part three, the normal raman and resonant raman scattering spectra of single - walled carbon nanotubes are measured at 457. 5nm and 632. 8nm laser excitation wavelength. by theoretical analysis, the diameter distributions of swnts were obtained, style and configuration parameter were speculated furtherly

    研究了在兩種不同激發波長下的單壁碳納米管的拉曼光譜,用457 . 5nm和632 . 8nrn兩種不同的激發光分別測得了單壁碳納米管的正常拉曼光譜和共振拉曼光譜。
  4. 4 ) the tuning characteristics of doubly - resonant optical parametric oscillator propo ) output by changing crystal ' s temperature, opo ' s cavity length and pump frequency respectively are theoretically analyzed and experimental obtained the wavelength of the opo output can be tuned from 2038nm to 2227nm by the crystal ' s temperature changed of 5. 3, from 2044nm to 2219nm by the cavity length changed of 514nm, and 375mhz by the pump frequency continuously tuned 750mhz

    當晶體溫度變化5 . 3時,得到2038nm - 2227nm可調諧下轉換光輸出;當opo的腔長相對于簡並點腔長變化514nm時,得到2044nm - 2219nm可調諧下轉換光輸出:當泵浦光頻率連續的改變了750mhz時,下轉換光的頻率相應連續調諧375mhz 。理論擬合與實驗結果基本一致。
  5. ( 3 ). the flattening arithmetic of an edfa was presented based on the inter - correlative function between the gain spectrum function of the edfa and that of the reserve transmission spectrum of the lpfg. for optimal matching between the two spectra, the flattening arithmetic calculates the variation of the resonant amplitude and wavelength of the lpfg

    Iii .提出了一種動態增益均衡的平坦演算法,這種演算法的本質就是利用摻鉺光纖放大器增益譜函數和新型長周期光纖光柵的透射譜反轉譜函數的相關性,給出新型長周期光纖光柵諧振峰幅度和位置的調節量,使改變后的新型長周期光纖光柵的反轉譜線能和edfa的增益輸出譜線進行最佳匹配。
  6. 4. we design the experiment of acvity - ring - down to measure reflectivity of the mirrors of coil and df laser with high reflectivity respectively at wavelength 1. 315 m and 3. 8 m, and perform the experiment of measuring reflectivity of coil laser resonant mirrors. the experimental result is discussed in detail

    設計並建立了用光腔衰蕩法測量氧碘激光器(波長為1 . 315 m )和氟化氘激光器(波長為3 . 8 m )高反射腔鏡的實驗平臺;測量了氧碘激光器振蕩腔鏡的反射率,並對實驗結果做了詳細的誤差分析。
  7. In particularly, the relation of the thickness of the metal layer and the surface plasma resonant wavelength and the relation of the incident angle and the surface plasma resonant wavelength based on the theory and experiments

    特別的從理論和實驗兩個方面研究了金屬膜層厚度與表面等離子體波傳感器的共振波長的關系和入射角與表面等離子體波傳感器的共振波長的關系。
  8. The tunable optical characteristics of the novel lpfgs are recognized during the study of their optical characteristics : ( 1 ). the relationship between the resonant amplitude and the applied curvature radius in the bend - sensitive orientation of the novel lpfgs is linear, ( 2 ). the relationship between the resonant amplitude and the applied transverse load in the wavelength - insensitive orientation of the novel lpfgs is linear, ( 3 ). the relationship between the resonant wavelength shift of the novel lpfgs and the applied temperature is linear

    在對新型長周期光纖光柵光學特性的研究中,我們發現了新型長周期光纖光柵的一些獨特的可調諧性:新型長周期光纖光柵的諧振峰幅度和彎曲敏感方向所受的彎曲率呈線性關系;新型長周期光纖光柵在波長不敏感方向其諧振峰幅度和它所受的橫向壓力呈線性關系;長周期光纖光柵的諧振峰中心波長隨溫度的變化呈線性關系。
  9. The method of dynamic gain equalization based on the temperature and bending characteristics of the novel lpfg was demonstrated. another method based on the temperature and transverse load characteristics was also demonstrated. the resonant amplitude and wavelength of the lpfg were adjusted by applying bend or transverse load and temperature to the lpfg, respectively

    Ii .利用新型長周期光纖光柵進行了edfa的動態增益均衡,根據新型長周期光纖光柵的可調諧性,提出了一種基於新型長周期光纖光柵的溫度及彎曲特性的動態增益均衡器,並介紹了另外一種基於溫度及橫向壓力特性的動態增益均衡器。
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