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Subpicosecond jitter in picosecond electron bunches

机译:皮秒电子束中的亚皮秒抖动

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摘要

We have simulated and measured 60-120 fs time jitter of photoelectron pulses emitted by a nitride photocathode at 100 GHz rate as in order to evaluate the resolution performance of a previously proposed photonic analog to digital converter. Recently, there has been an increasing demand for high speed analog-to-digital converters (ADCs) for microwave bandwidth signals. State of the art electronic ADCs have reached 10 Gigasamples/second (GS/s), 6-12 bit performance [P. W. Juodawlkis, J. C. Twichell, G. E. Betts, J. J. Hargreaves, R. D. Younger, J. L. Wasserman, F. J. O'Donnell, K. G. Ray, and R. C. Williamson, IEEE Microwave Theory Tech. 49, 1840 (2001)]. We have previously introduced a photoelectronic ADC implementation with measured performance of 3 bits at 100 GS/s [K. Ioakeimidi, R. Leheny, S. Gradinaru, K. Ma, R. Aldana, J. Clendenin, J. S Harris, R. F. W. Pease, IEEE Trans. Microwave Theory Tech. (to be published); Conference on Lasers and Electro-Optics, Baltimore MD, 1-6 June 2003]. The basic operating principle of the ADC is based on a miniaturized cathode ray tube where a bunch of photoemitted electrons passing through an electric deflection system is directed to a specific detector whence a digital code word emanates. The electron bunch samples the analog deflecting voltage that is then quantized according to the position of the detector receiving the bunch. The fundamental limit of the number of distinguishable voltage levels is the ratio of the deflecting voltage to the energy spread due to diffraction of the electron beam, This allows for up to 12 bits at 100 GS/s [R. F. Pease, K. loakeimidi, R. Aldana, and R. Leheny, J. Vac. Sci. Technol. B 21, 2826 (2003)]. At a more practical level, the bit resolution is primarily limited by the uncertainty in the emission of each electron bunch (temporal jitter). For 100 fs time uncertainty 5 bits of resolution are attainable with the nitride cathode for a 50 GHz bandwidth analog signal.
机译:为了评估先前提出的光子模数转换器的分辨率性能,我们已经模拟并测量了氮化物光电阴极以100 GHz速率发射的60-120 fs时间抖动的氮化物光电阴极。近年来,对用于微波带宽信号的高速模数转换器(ADC)的需求不断增长。最新的电子ADC已达到10 Gigasamples /秒(GS / s),6-12位性能[P. W.Juodawlkis,J.C.Twichell,G.E.Betts,J.J.Hargreaves,R.D.Younger,J.L.Wasserman,F.J.O'Donnell,K.G.Ray和R.C.Williamson,IEEE微波理论技术。 49,1840(2001)]。我们之前已经介绍了一种光电ADC的实现,在100 GS / s [K]时可测量3位性能。 Ioakeimidi,R.Leheny,S.Gradinaru,K.Ma,R.Aldana,J.Clendenin,J.S Harris,R.F.W.Pease,IEEE Trans。微波理论技术。 (待发布);激光和光电会议,马里兰州巴尔的摩,2003年6月1-6日]。 ADC的基本工作原理基于小型化的阴极射线管,通过电子偏转系统将一束通过电子偏转系统的光电子发射到特定的检测器,从而发出数字代码字。电子束对模拟偏转电压进行采样,然后根据接收电子束的检测器的位置对其进行量化。可区分的电压电平数的基本极限是偏转电压与由于电子束衍射而产生的能量散布之比。这允许在100 GS / s [R]时最多12位。 F. Pease,K。loakeimidi,R。Aldana和R. Leheny,J。Vac。科学技术。 B 21,2826(2003)。在更实际的水平上,位分辨率主要受到每个电子束发射不确定性的限制(时间抖动)。对于100 fs的时间不确定性,氮化物阴极对于50 GHz带宽的模拟信号可获得5位分辨率。

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