Zero two profile pic的問題,透過圖書和論文來找解法和答案更準確安心。 我們找到下列線上看、影評和彩蛋懶人包

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國立中央大學 電機工程學系 許晉瑋所指導 温智閔的 超高速單載子傳輸光偵測器和其在超寬頻帶的波導耦合式兆赫茲光子傳輸器之應用 (2017),提出Zero two profile pic關鍵因素是什麼,來自於光偵測器、波導、光子傳輸器、超高速。

而第二篇論文國立清華大學 先進光源科技學位學程 柳克強、劉偉強所指導 魏子喻的 軸向耦合結構熱陰極射頻電子槍之設計與分析 (2012),提出因為有 電子槍、軸向耦合、射頻、熱陰極、光注射器、加速器的重點而找出了 Zero two profile pic的解答。

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超高速單載子傳輸光偵測器和其在超寬頻帶的波導耦合式兆赫茲光子傳輸器之應用

為了解決Zero two profile pic的問題,作者温智閔 這樣論述:

在此篇論文中,我們成功的實現幾種能操作於兆赫茲頻率(THz)之單載子光偵測器(uni-traveling-carrier photodiodes, UTC-PD).首先,其中之一為近彈道單載子光偵測器(Near-ballistic uni-traveling-carrier photodiode, NBUTC-PD),藉由P型電場控制層(P-type charge layer)調整電場分佈維持電子在最高飄移速度(overshot drift-velocity)以達到高速頻寬表現. 此元件在兆赫茲頻率操作下之最佳偏壓通常位在-2V。然而,在此高偏壓操作下,高功率輸出時亦承受更高機率的熱失效(T

hermal failure)。為了解決此問題,我們提出另一種創新的設計N-UTC-PD,藉由在收集層插入N型電場控制層(N-type charge layer)重新最佳化電場分佈進一步加強抑制空間電荷屏蔽效應(Space charge screening effect, SCS)。此結構即使在較低的電場即-1V偏壓操作下,電子在跨越收集層時依然維持最高飄移速度(overshot drift-velocity)。總結來說,對新結構N-UTC-PD來說,它仍然具有優異的高頻寬表現(~315GHz),但它在功率輸出表現上會有些許衰減(-3dBm@280GHz)。而對NBUTC-PD來說,雖然它有較

佳的輸出功率(-1.8dBm)及頻寬表現(~325GHz),但設計上需要更有效的散熱方式來避免熱失效。 然而,為了獲得超高速頻寬操作,設計上會使用較薄之吸收層,此類光偵測器會極大的犧牲響應度(Responsivity)進而造成光的吸收效率嚴重降低。為了解決此問題,我們藉由改良磊晶結構來獲取較高的響應度表現。最新設計的另一種GaAs0.5Sb0.5/In0.53Ga0.47As II型混合吸收層之單載子光偵測器。此3μm直徑主動區元件經由覆晶鍵結封裝後從量測結果可得知,與現有相關長波長(1.3–1.55μm)之光偵測器研究相比,亦具有適度合理之響應度值0.11A/W (NBUTC-PD:0

.08A/W, N-UTC-PD:0.09A/W), O-E頻寬操作可高達0.33THz。 最後,我們成功實現此結構之光偵測器在正弦波封包(Sinusoidal envelope)產生之射頻頻率(Radio frequency, RF) 0.32 THz及63% 調製深度之光訊號操作下,在 −1 V偏壓擁有13mA之飽和電流及-3dBm毫米波功率輸出。透過使用此種光偵測器,我們也成功實現具有新穎前端波導耦合(Waveguide, WR6)設計之超寬頻、整合型光子傳輸器( Photonic transmitter);並藉由創新設計之高增益雙邊山脊型號角天線(Dual-ridge horn ant

enna)及設計平面電路波導激發,此傳輸器頻率操作可達紀錄之0.1至0.3THz帶寬,在無線傳輸過程中維持0.24THz 頻率操作下,接收端亦偵測高達31.6 W之毫米波輸出功率

軸向耦合結構熱陰極射頻電子槍之設計與分析

為了解決Zero two profile pic的問題,作者魏子喻 這樣論述:

Abstract Thermionic-cathode radio-frequency electron gun (RF gun) has been a compact electron source of accelerators for more than two decades. In an RF gun, electrons pulled out from the cathode by the high gradient field setup in its microwave cavity are rapidly accelerated to relativistic ene

rgy such that space charge effects are less significant. Motivated by the need of a high quality electron source for the NSRRC ultrashort beam facility, we studied a 2998 MHz, 1/2+1/2+1 cell, thermionic cathode RF gun with on-axis coupled structure (OCS RF gun). OCS RF gun features simplicity of fre

quency tuning during fabrication due to its axial symmetry. We started with circuit analysis that provides a reliable model through the investigation. Microwave properties and electron beam characteristics of designed OCS RF gun has been evaluated by 2D simulations of SUPERFISH and PARMELA as well a

s 3D simulations of HFSS and CST-PS. Operating parameters are optimized to obtain a 2.5 MeV electron beam with quasi-linear energy chirp that allows aggressive bunch compression in the RF linac located downstream after proper beam selection. We have also investigated power distribution of back-strea

med electrons that eventually lost onto the surface of thermionic cathode. A prototype of the designed OCS RF gun structure has been fabricated for low power microwave test. Measured frequencies and longitudinal electric field profile of the cavity structure agree well with the results predicted in

the simulation studies.