cavity mirror 中文意思是什麼

cavity mirror 解釋
諧振腔反射鏡
  • cavity : n. 1. 【解剖學】穴,窩,盂,腔,空腔;【醫學】(空)洞。2. 【物理學】模槽;氣蝕區;空腔諧振器;【原子能】(反應堆中的)小室,暗盒。
  • mirror : n. 1. 鏡;反射鏡。2. 反映;借鑒;榜樣。vt. 映,反射;反映。
  1. Two - dichroic - mirror cavity yb3 - doped double - clad fiber laser

    雙包層光纖激光器
  2. Semiconductor saturable absorber mirror mode - locked optically pumped vertical - external - cavity surface - emitting semiconductor lasers

    半導體可飽和吸收鏡鎖模光抽運垂直外腔面發射半導體激光器
  3. We firstly summarize the development of yb - doped fiber lasers, pumping methods and the applications of high - power fiber lasers. 2. considering the scattering loss, we deduce the relationships between laser performances of yb - doped double - clad fiber laser and parameters of laser cavity from the steady state rate equations, numerically analysis the changes of laser performances, such as laser power with the parameters of laser cavity, including output mirror reflectivity, optimum length of double clad fiber

    研究主要內容包括如下幾個方面:一、首先對摻鐿光纖及摻鐿光纖激光器的發展狀況、包層泵浦技術和高功率光纖激光器的應用等進行了綜述;二、在前人對高功率雙包層光纖激光器的理論基礎上,在考慮了光纖散射損耗因子的情況對光纖激光器理論進行了推導,給出了準解析解,進一步完善了理論分析。
  4. In this paper, micro - cavity semiconductor laser ( mcsl ) with pillar vertical - cavity surface - emitting structure ( vcsel ) which has potential applications in optical communication and optical interconnect is theoretically analyzed, the calculation model that used to discuss the modal performance of rectangular columnar and cylinder vcsel with oxidized aperture is established by using vector field model. the numerical simulations in the case of cylinder structure show oscillating wavelength and threshold gain against inside and outside radius of laser, the layer refractive index and pair number of bragg mirror, thickness, position and oxidized material ' s refractive index of oxidized aperture, in detail. more practically, considering dos shell of laser as non - perfect one, or supposing that dos shell is separated from the laser, we can obtain more significative results

    本工作以矢量場模型出發,對具有誘人應用前景的柱形垂直腔面發射結構( vcsel )的微腔半導體激光器( mcsl )進行了理論分析,建立了用於分析方柱形和圓柱形結構具有氧化孔徑層的激光器的模式特性的理論模型;對圓柱形結構情況進行了數值模擬,得到了振蕩波長、閾值增益隨激光器內外半徑、 bragg反射鏡層折射率、周期數以及氧化孔徑層厚度、位置和氧化物折射率的詳細變化規律;為使理論計算更接近實際,將外加金屬包殼視為非理想導體,或將金屬包殼與激光器結構隔開,分別對這兩種情況下的結果進行了討論。
  5. 3. the thermal - mechanical and lasering properties of cr * : lisaf crystal were carefully studied. especially the up - conversion and the esa effect. all of these were given fully considered when design the three - mirror folded cavity tunable lisaf laser which was pumped by a accousto - optical active q - switched nd : yvo4 lbo intra - cavity frequency doubling 671nm laser

    在對cr ~ ( 3 - ) : lisaf晶體的熱機械特性和激光特性詳細研究的基礎上,通過對折疊腔理論進行簡要介紹並由穩區計算,設計了三鏡折疊腔可調諧cr ~ ( 3 - ) : lisaf激光器。
  6. Then some cavity quantum electro - dynamic ( cqed ) effects are studied by experiment. the photoluminescence ( pl ) intensity enhancement at resonance wavelength and suppression at off - resonance wavelength, emission spectrum narrowing as well as emission intensity redistribution in space are observed in the microcavity device fabricated with distributed bragg reflector ( dbr ) and silver mirror as well as that done with two silver mirrors

    分別在帶有dbr結構的平面微腔及全金屬鏡構成的平面微腔中觀察到了諧振模式處的輻射增強及非諧振模式處的輻射抑制,發射譜線窄化以及輻射強度空間分佈重組等腔量子電動力學現象。
  7. Based on these foundations, we give a perfect scheme of the bbo opos : single pass amplification coefficient of the opg under different pump intensity is calculated ; collinear type - i and type - ii phase matching tuning curve pumped by the q switch nd : yag various harmonics as well as noncollinear type - i tuning curve are calculated in details ; the effect of the walkoff for the nonlinear effect coefficient and the group velocity matching are analyzed ; the acceptance angle in parametric process is calculated ; the numerical threshold of the bbo opo is calculated ; the process of the saturation and depletion of the pump beam are analyzed ; the relationship of the conversion efficiency and reflectance of output mirror are discussed ; various linewidth controlling methods are discussed ; the improvement of the beam quality applying the unstable cavity is discussed ; and the crystal bbo design is considered

    在此基礎上,給出了一整套bbo - opo激光參數設計方案:計算了不同泵浦強度下的參量放大倍數;詳細計算了在nd : yag調q激光器各次諧波泵浦條件下的共線類和類相位匹配的調諧曲線,以及非共線類相位匹配調諧曲線;分析了走離角對非線性系數和群速匹配的影響;計算了參量過程的允許角;計算了bbo - opo的理論閾值條件;分析了飽和與泵浦光束的消耗過程;給出了轉換效率與超過泵浦閾值的倍數的關系;討論了轉換效率與輸出鏡反射率的關系;討論了線寬控制的各種方法;研究了利用非穩腔改善光束質量的方法;考慮了bbo晶體的設計。
  8. Theoretical and experimental research of three - mirror - cavity self - locked ti : sapphire laser with low pump power

    低抽運三鏡腔自鎖模摻鈦藍寶石激光器的理論與實驗研究
  9. This design has combined a degnan and hall case iii coupling configuration and u - folded cavity, that is, the mirror - waveguide space is folded and there is only one ceramic waveguide in the whole cavity

    採用了輸出鏡類耦合方式+ u型折疊腔的設計方案,即僅含單根陶瓷方波導的「輸出鏡?波導」耦合空間的折疊。
  10. From the theoretical calculation and the experimental results, we makehe conclusion that the last cavity setup is most suitable for the wavelength tuning. we calculated the stable regions and the peak power on the sesam, at the same time, ave the beam size on the sesam and on the crystal. we achieved the q - switchedutput with a three - mirror folded - cavity after optimizing it

    計算了v型腔和五鏡腔的穩區、晶體和sesam上光斑半徑、 sesam上的峰值功率密度,對腔的參數進行了優化,並做了sesam被動調q和鎖模的激光實驗,實現了v型腔調q 、五鏡腔調q的激光輸出。
  11. With the cavity of output from zero - order diffractive beam, tunable range of about 70nm from 543 - 610nm had been achieved, and the highest slope efficiency of 17 % was obtained at 583nm wavelength. while using the cavity of output from a coupling mirror, tunable range of over 30nm from 553 - 585nm was obtained, and the

    在腔鏡耦合輸出的可調諧激光器實驗中,輸出調諧范圍超過30nm ,此結果與報道的p567固態染料調諧范圍相近;在光柵零級輸出實驗中,激光輸出調諧范圍近70nm ,此結果在已知報道的p567固態染料激光調諧范圍中是最寬的。
  12. Proof deformable mirror face solution at cavity mirror in four - pass amplifier system

    四程放大系統腔鏡位置變形鏡的面形解
  13. The resonant box effect is the most important. in chapter five, we use the experimental setup constructed and the cavity decay time method to measure the total loss of a passive resonant cavity, and analyse the experimental data in very detail. we conclude that, in present experimental conditions it is the uniformity and stability of laser mirror to confine the precision and repeatability of experimental results

    第五章在建立起了連續光波時間衰減法測量裝置的基礎上,進行了無源諧振腔總損耗的測量,仔細分析了實驗過程中的誤差因素,並指出在目前的實驗條件下限制測量精度和重復性的主要原因是激光鏡片的均勻性和穩定性不理想。
  14. The optical characteristics of metal silver film used as the reflective mirror of microcavity are calculated by characteristic matrix method and it is shown that the thickness of metal mirror affects not only the reflectivity but also the penetration depth and thus the cavity mode. this conclusion is confirmed by experiment

    通過特徵矩陣法計算了金屬薄膜在光學微腔中的性質,得到了金屬膜厚度不僅影響腔的品質因子,而且隨金屬膜厚度增加,由反射相移引起的等效穿透深度增加的結果,並在實驗上進行了驗證。
  15. Study of cavity mirror alignment in multi - pass amplifier

    多程放大腔鏡準直研究
  16. The cavity mirror can also be designed according to an objective function. the second part ( the 5th chapter ) is to introduce the concept of low diffraction beam and to illustrate the principle and method how to realize it. a low diffraction beam is obtained by reconstructing the existing optical resonator of a co2 laser using a special diffraction phase plate

    第二部分(第五章)提出了低衍射光束的概念,簡述了實現低衍射光束原理和方法;通過腔內放置衍射元件的方法實現了低衍射光束的輸出;並對這種光束進行了理論和實驗研究,理論模型結果和實驗結果很好地吻合。
  17. It makes use of the mirror reflection boundary condition. the calculation result shows that the terse technique can save much calculation tune ( more than 30 % ). in fact, its result is more accurate, because it does n ' t take any approximation in the cavity region

    本文還對內含空腔系統的計算通過引入鏡面反射邊界條件而作了簡化處理,實際計算表明,簡化處理大幅度節省了計算時間,達30以上,而且其計算結果更為準確,因為它在計算過程中對空腔所在區域並未採取任何近似。
  18. Four - mirror ring cavity and six - mirror ring cavity has its advantages and shortcomings, respectively

    四鏡環形諧振腔和六鏡環形?振腔有各自的優點和不足。
  19. Laser system ' s stable condition and frequency function are gained by virtue of theoretical model of a three - mirror f - p cavity and semiconductor laser, and then the mathematical model of common self - mixing interference effect is established

    由三鏡f - p腔理論和半導體激光器性質得到系統的穩態條件和輸出光頻率的求解方程,從而建立了自混合干涉的數值模型。
  20. The former has compact structure ;, little cavity loss, higher coupling efficiency, and higher superposition efficiency. but there is no enough room for other devices. the latter overcome this problem, but the diffraction loss and mirror loss is increased

    六鏡環形諧振腔可以確保角度很小,但總腔長較長,腔內衍射及腔鏡吸收和不完全反射造成的損耗較大,同樣很難得到穩定的雙波長激光輸出。
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