激發譜線 的英文怎麼說

中文拼音 [xiàn]
激發譜線 英文
exciting line
  • : 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...
  • : 名詞(頭發) hair
  • : Ⅰ名詞[書面語]1 (按類別或系統編成的書或冊子等) table; chart; register 2 (指導練習的格式或圖形)...
  • : 名詞1 (用絲、棉、金屬等製成的細長的東西) thread; string; wire 2 [數學] (一個點任意移動所構成的...
  • 激發 : 1 (使奮發) arouse; stimulate; set off; stir up 2 [物理學] excitation; exciting; incitement; inc...
  1. Using the multi - configuration dirac - fock method ( mcdf ), we studied the characteristic of the decay processes of the 4d core excited states of csiv, the low - lying excitation structure of super - heavy element bohrium ( z = 107 ) and the x - ray spectra of the 3d - 4f transitions of highly charged xenon ions in details in this work, by including the electron correlation and the relaxation effects systematically

    本論文運用mcdf方法,通過系統考慮電子相關效應和馳豫效應,分別研究了cs離子的4d內殼層態衰變動力學特性,超重元素bh ( z = 107 )的低態結構以及高離化態氙離子的3d - 4f躍遷產生的x射的結構等問題。
  2. A spectral line is emitted when an atom proceeds from an excited state to a lower state.

    當原子從一個受態進入另一個較低的狀態時,就射一條
  3. The electronic temperature, intensities of all lines and continuous spectra gradually increased with the increment of laser energy, and they got to maximum at different laser energy. our results of copper and aluminum show that there are possibly different thresholds of laser energy to electronic temperature and intensities of emission spectra of laser ablated plasma. at the different environmental gas pressure, spatial emission intensity distribution is explained by the competition among " heat reservoir effect ", " confined effect " and " s hadow effect "

    認為cu等離子體羽的光機制是由電子與粒子的碰撞傳能、電子與離子的復合形成的;隨光能量的增加, cu等離子體特徵輻射(分立) 、連續背景輻射(連續) 、電子溫度都出現最大值;結合對al的實驗結果說明:光燒蝕金屬產生的等離子體,其特徵輻射、連續輻射、電子溫度可能都存在一定的能量閾值;背景氣壓對光燒蝕等離子體的影響,其機理可以認為是「熱庫效應」 、 「約束效應」及「陰影效應」相互競爭的綜合結果。
  4. ( 2 ) the emission spectra of laser ablation metal copper plasma were measured. the detailed mechanism of plume emission of cu plasma was qualitatively explained using a simple model based on excitation of atom and ion in plume arising from inelastic collision between the elemental species and electron with high kinetic energy. under the local thermal equilibrium model, the electronic temperature of copper plasma was deduced to be in the 104 scale by its emission lines

    ( 2 ) cu等離子體光:在420 570nm波長范圍內觀測了光燒蝕cu等離子體的光和各在等離子體中的空間分佈;比較了光能量對cu等離子體射光、電子溫度的影響;用局部熱力學平衡( lte )近似,測得cu等離子體的電子溫度為104k數量級;在不同背景氣壓下,觀測了光燒蝕cu等離子體光的空間分佈。
  5. The absorption of this radiation in various lines followed by cascade transitions to lower levels might ultimately produce an anomalously high population for the excited levels of these molecules.

    在各處對這種輻射的吸收以及接著向低能級的級聯躍遷最終可能使這些分子的能級產生異常高的粒子數。
  6. Observation of the on - off sequencing of characteristic spectral lines from tracer materials arranged in layers in, or surface patterns on, planar or spherical targets can provide a record of radial or lateral energy transport processes in laser - generated plasmas

    測量光聚變靶產生的軟x射時間變化連續的形狀,可以知道許多x射產生過程的詳細動態記錄,這有助於理解實驗的熱學條件。觀察軌跡特徵的閉合序列,能提供關于光等離子體能量和滯后能量的傳輸過程記錄。
  7. With the rapid development of optical fiber communication technology, low - cost and high quality near infrared laser and light emitted diode working at room temperature become widely available. the emit wavelength from these light resource is not only consistent with the three low - decay windows of fiber optics, but also with many wide - frequency or recombination absorption spectrum of environmental and industrial gases

    光纖通信技術的展使相對低價、工作于常溫、高質量的近紅外光器和光二極體可廣泛獲得,這些光光源的射波長與光纖的三個低損耗窗口相一致,也與許多環境和工業氣體的泛頻或復合吸收相一致。
  8. If the focal point of the len shifts around the surface of the sample, the mass ablation, the temperature of the plasma and the spectral intensity appear asymmetric and their maximum occur at the location which is about 0. 4mm under the surface of the sample. ( 2 ) to the plasma of the aluminum alloy sample, when the operating voltage is 1600v, the height from the observed location of the plasma to the surface of the sample is 2mm and the argon pressure is 660 torr, the spectral intensity have the maximum values

    ( 2 )對于標準鋁樣品,在光器工作電壓為1600v 、等離子體觀測高度為2mm 、氬氣壓力為660乇時,其強度最強;以al 308 . 22nm 、 al 309 . 27nm兩條為分析現隨著環境氣壓的增大,自吸效應明顯增強,當環境氣壓達到600 - 700乇時,幾乎產生自蝕。
  9. By the study of the whole decay curves of 10 hours, the influence of each step is summarized, and the best stoichiometry and preparation techniques are acquired. the crystal structure of sral2o4 eu2 +, dy3 + is monoclinic system, which is a high efficiency luminescence crystal structure. the emission spectrum and the excitation spectrum of sral2o4 eu2 +, dy3 + powder are measured

    此外,通過x射衍射確定了所制備的sral _ 2o _ 4 : eu , dy長余輝材料晶體為單斜晶系結構,並測量其射光,初步討論了sral _ 2o _ 4 : eu , dy長余輝蓄能材料可能的光機理。
  10. Using the multi - cloud model to fit the ha - spectra data of the april 27, 1981 post flare loop, we obtained the spacial distributions of the four physical parameters in the space of the post flare loop : the line - of - sight velocity v the excitation temperature tex, the micro - turbulence velocity vt and the column number density of the hydrogen atoms at the second level along the line - of - sight direction fields n2

    我們利用多雲模型處理了1981年4月27日太陽西邊緣耀斑后環的三個時段的h光掃描資料。通過對1000餘條對稱和不對稱的計算,我們得到了該耀斑后環各個時段在空間上的視向速度場,溫度場,視向上處于第二能態的氫原子柱密度場以及湍流速度場。
  11. Xrd patterns, excitation spectra, emission spectra, photo - stimulated emission spectra, photo - stimulated emission decay curves and thermo - luminescence spectra have been measured on the samples

    對樣品進行了x射衍射分析( xrd ) 、射光、光光光、光光衰減和熱釋光測定。
  12. The energy level structures of the 4d core excited configuration 4d 5s25p5, final radiative configuration 4d105s25p4 and final auger configurations 4d105s25p3 and 4d105s15p4 of csv ion and all possible decay dynamics processes related to these configurations are all determined by mcdf method. we also compared the present results of radiative transition, oscillator strength and the line width with the results obtained by experimental spectra and the quasi - relativistic configuration interaction method and got a good agreement. we also make prediction for some dominant features of the auger electron spectrum emitted by the auger decay process of the 4d95s25p6 core excited states

    論文第三章中詳細的介紹了cs離子的4d內殼層電子組態4d ~ 95s ~ 25p ~ 5 、輻射末態4d ~ ( 10 ) 5s ~ 25p ~ 4及auger末態4d ~ ( 10 ) 5s ~ 25p ~ 3和4d ~ ( 10 ) 5s5p ~ 4的能級結構及各種可能的輻射和auger衰變過程,獲得了與已有的實驗結果和相關的半經驗準相對論組態相互作用計算結果相符的輻射躍遷能、振子強度以及寬,預言了4d ~ 95s ~ 25p ~ 5態的以auger衰變為主的auger電子的特性。
  13. It is convenient for x - ray tube excited source to detect multi - component on site due to the advantages of high excitation flux, easy protection, and characteristic x - ray and continuous bremsstrahlung spectrum included in its exciting spectra

    X光管源具有活性強、易於防護等優點,產生的包括特徵x射和連續的軔致射,方便現場測定多元素。
  14. By use of g. d. shen ' s tunneling cascade theory we have fabricated high performance and high power tunneling cascade ingaas / gaas / algaas 950nm / 990nm double wavelength strained quantum well lasers on the basis of former tunneling cascade high power lasers and high brightness light emitting diodes. the lasers " two peak wavelength are 95 ? nm and 990 ? nm. el spectrum ' s fwhm is 3nm

    在以往隧道級聯大功率應變量子阱光器及高亮度光管的理論研究與實驗的基礎之上,採用沈光地教授提出的隧道級聯思想,成功研製出基於ingaas gaas algaas材料的高性能大功率隧道級聯950nm及990nm雙波長應變量子阱光器,射波長分別為952 2nm和990 2nm , el寬度約3nm ,未鍍膜器件單面最大輸出光功率可達2w以上,閾值電流最低達120ma 。
  15. Its principle can be outlined as follows : the accelerator produces a beam of fast ions which directs through the foil, because of collisions with the foil atoms the fast ions may undergo further ionization, and they often emerge from the foil in excited electronic states

    其原理如下:加速器產生的高能離子束與碳箔相碰撞而失去電子,同時剩餘電子被到高態,在隨后的退過程中,通過研究這些可以得到原子的能級結構。
  16. In order to understand the origin of lead in air, proton microprobe was used to measure pm10 environmental monitoring samples of wusong district, shanghai city, and lead pollution origin of this district was studied with micro - pixe spectrum " fingerprint " combined with pattern recognition technique

    摘要為?解空氣中鉛的來源,用質子微探針測量了上海市吳淞地區空氣pm10環境監測樣品,用微束質子單顆粒x射「指紋」結合模式識別技術研究了該地區鉛污染的來源。
  17. The optimal length of crystal was achieved for the characteristics of quasi - three - level. three types of crystal were compared, we select lbo as the main frequency doubler. meanwhile, the other strong spectrum were restrained by suitable coating

    光晶體的準三能級特性出,充分考慮增益與損耗之間的矛盾,選擇出最佳晶體長度;對三種倍頻晶體進行了比較,選擇出lbo作為主要倍頻晶體;對膜系進行了必要的分析,在維持946nm振蕩的同時,充分考慮了其它的抑制。
  18. The experiment populated the excitation state of 64cu via 64ni ( p, ny ) 64cu * reaction and the lifetime of low - lying excitation state of 64cu were determined via the delayed coincidence method between pulse proton beam and de - excitation y rays detected by ge ( li ) detector

    Sns )與ge ( l )探測器測量退y射延遲符合的方法,由時間tof峰的中值移動的方法來確定態壽命。
  19. At the same time, we show that under a proper nitrogen doping concentration, due to the " concentration quenching " effect, the full spectrum of the nn3 center ( i. e., its zero phonon line and various phonon replicas ) is revealed without the interference from the spectra of other higher energy centers ( especially nn4 - nn6 )

    Gapi . xn :的在低組分下由尖銳的nn 。及其聲子伴組成,隨著組分x的提高,這些尖銳的的逐漸展寬,並向低能端移動,在這個過程中,子的能量傳輸起著重要作用
  20. The optimized experimental conditions are determined and the densities of some elements in the mental alloy standard samples are measured. the experimental results shows that the spectral intensity of the plasma enhances significantly with the increase of the operating voltage and the power density. ( 1 ) to the steel ally sample, the emission intensities of the spectra reach to the maximum values when the laser operating voltage is 1600v and the argon pressure is 600 torr. under the same pressure, the spectral intensity of the plasma in the argon atmosphere is stronger than that in the air. when the argon pressure is 320 to rr, the signal - noise ration is about 5 times than that which the argon pressure is 700 torr, but the temperature of plasma is less about 1000k

    ( 1 )對于光標鋼準樣品,當光器工作電壓為1600v 、氬氣壓力為600乇時,強度達到最大,並且在相同壓強下,氬氣中的等離子體與空氣中的等離子體相比,其輻射強度明顯增強;氬氣壓力為320乇時的信背比約為600乇條件下的5倍,而等離子體溫度卻下降了近1000k ,即等離子體溫度隨環境氣壓的增大而增大;當光束的焦斑在樣品表面上下移動時,光誘導量、等離子體的溫度、強度都呈不對稱性分佈,其最大值對應的焦斑位置都位於樣品表面之下0 . 4mm左右。
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