激光增益開關 的英文怎麼說

中文拼音 [guāngzēngkāiguān]
激光增益開關 英文
laser gain switching
  • : Ⅰ動詞1 (水因受到阻礙或震蕩而向上涌) swash; surge; dash 2 (冷水突然刺激身體使得病) fall ill fr...
  • : Ⅰ名詞1 (照耀在物體上、使人能看見物體的一種物質) light; ray 2 (景物) scenery 3 (光彩; 榮譽) ...
  • : Ⅰ名詞1 (好處) benefit; profit; advantage 2 (姓氏) a surname Ⅱ形容詞(有益的) beneficialⅢ動詞...
  • : Ⅰ動詞1 (使開著的物體合攏) close; shut 2 (圈起來) shut in; lock up 3 (倒閉; 歇業) close down...
  • 激光 : [物理學] laser 激光靶 laser target; 激光報警器 laser avoidance device; 激光玻璃纖維 laser fibre; ...
  1. In chapter 3, we studied the effect of gaussian transverse profile for the driving and laser fields on lasing without population inversion ( lwi ) in a closed v - type system and an open v - type system. moreover, we discussed also the effect of the unsaturated gain coefficient, the cavity - damping rate, the ratio of the atomic injection rates and atomic exit rate on the corresponding systems. in chapter 4, we mainly discussed the effect of doppler broadening on the gain, dispersion and the frequency up - conversion of the open v - type lwi system and compared the differences and the same between the open system and the corresponding closed system

    發現: ( 1 )在考慮doppler展寬的情況下,通過選取合適的實驗室條件(比如合適的原子環境溫度等)可得到合適doppler展寬值,從而使系統獲得最佳; ( 2 )要想實現系統的頻率上轉換,同時又要獲得足夠強的無反轉,則系統頻率轉換比不能選取的太大; ( 3 )對于放系統,比較小的粒子注入速率比與退出速率對產生無反轉是有利碩士學位論文摘要的: ( 4 )由於dopp1oy展寬的存在,當探測場與驅動場的傳播方向相反時,在探測場失諧的某一段區域產生振蕩,且振蕩的振幅、頻率失諧范圍的大小與dopper展寬的取值有
  2. The cr + : yag crystal has been operated differently as passive q - switching and mode - locking medium by researchers at home and abroad. chapter 2 : researching the q - switching performance of cr4 + : yag crystals with the rate equations

    Cr ~ ( 4 + ) yag晶體優良的物化性能,使它作為被動調q介質已實現了不同種類的調q和鎖模運轉。
  3. With the theoretical and experimental methods, the characters of cr4 + : yag are studied from cr4 + : yag as passive q - switching in nd : yag laser, intracavity frequency - doubling of q - switching laser and dual - wavelength laser, which is based on cr4 + : yag ' s operations of saturable absorption and laser gaining medium. chapter 1 : introducing the cr4 + : yag ' s optical function, the general research situation and the main idea of this thesis

    本論文基於cr ~ ( 4 + ) yag晶體既可以作為nd yag器的被動調q、又可以作為介質的特點,採用理論和實驗相結合的研究方法,詳細而具體的研究了cr ~ ( 4 + ) yag晶體被動調q 、調q倍頻和雙波長輸出的特性。
  4. Secondly, basing on the theory of on - off gain of small signal, the raman gain coefficient for frequency shift between 0. 5 and 20 thz of standard sigle mode optical fiber is measured by pump - probe method through a super luminescent diode ( sld ) as a broadband small signal probe source. thirdly, numerical simulation analysis of gain characteristic of raman fiber amplifier for c band wdm signal light is made according to the raman gain coefficient of the fiber measured before through target and four rank runge - kutta method. at the invariability of wavelength and maximum power of each of two pumps, schematic of powers of two pumps for best flatness on c band wdm optical gain was found out, at the same time, the factors of resulting in gain saturation is analyzed, too

    本文首先應用經典的電磁理論對拉曼纖放大器的工作機制進行了分析,然後,根據小信號理論推導出的求出了纖拉曼系數的表達式,採用泵浦-探測波的方法,利用超輻射二極體( superluminescentdiode簡稱sld )作為探測源,測量了所用標準單模纖頻移為0 . 5 - 20thz的拉曼系數,之後根據所測得的纖的拉曼系數譜對應用該類纖構成的放大c波段wdm信號的拉曼纖放大器的特性採用打靶法和四階龍格- - -庫塔進行了數值計算,在給定了兩個泵浦源的波長和最大功率后,找出了反向泵浦情況下使c波段wdm最平坦的兩個泵浦的各自最佳功率,同時也分析了導致信號飽和的原因。
  5. In this thesis, we used the q - switched nd : yag laser pulse focused by lens to pump the cr ~ ( 4 + ) : mg _ 2sio _ 4 crystal, with the pump laser pulse duration and energy of 30ns and 50 mj separately, and got the laser pulse with center wavelength, pulse duration and energy of 1. 22 m, 8. 2 ns and 10 mj on the best work condition. on the base of zhangguowei s approximation about gain - switching and the parameter of cr ~ ( 4 + ) : mg _ 2sio _ 4 crystal, we calculated the time characteristics of cr ~ ( 4 + ) : mg _ 2sio _ 4 laser pulse with rate equation by numerical method, obtained the conclusion that the laser pulse duration is only related to the pump energy and cavity length : the larger the pump energy is, the narrower the pulse duration is ; the longer the cavity is, the wider the

    本論文採用調qnd : yag脈沖通過透鏡聚焦后縱向抽運cr ~ ( 4 + ) : mg _ 2sio _ 4晶體,抽運脈沖寬度為30ns 、能量為50mj ,在較佳工作條件下得到了中心波長為1 . 22 m 、脈寬為8 . 2ns 、能量為10mj的脈沖;並在張國威分析時間特性的近似法基礎上,結合實際的cr ~ ( 4 + ) : mg _ 2sio _ 4器的相參數,從速率方程出發,用數值計算的方法更為精確的模擬了cr ~ ( 4 + ) : mg _ 2sio _ 4器輸出脈沖的時間特性,得出了脈寬只與抽運能量、腔長有的結論,即抽運能量愈大,脈寬越窄;腔長越長,脈寬則愈寬。
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