1988
DOI: 10.1109/3.115
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Picosecond optical sampling of GaAs integrated circuits

Abstract: We present a novel printed monopole antenna for ultrawideband applications. The proposed antenna consists of a square radiating patch and a ground plane with cross-shaped slot and conductor-backed plane, which provides a wide usable fractional bandwidth of more than 130% (3.06-12.87 GHz). By cutting a modified cross-shaped slot with variable dimensions on the ground plane and also by inserting cross-shaped conductor-backed plane, additional resonances are excited and hence much wider impedance bandwidth can be… Show more

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Cited by 363 publications
(57 citation statements)
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“…In the 1980s, Dave Bloom at Stanford made pioneering contributions to the synchronization of actively modelocked picosecond lasers to a microwave frequency reference [105,106], which he then applied to electro-optic sampling of GaAs integrated circuits [45]. I did my Ph.D. work in his group and explored to extend this synchronization technique to femtosecond fiber Raman soliton lasers [107,108] to improve the time resolution in electro-optic sampling, which turned out not to work due to the poor noise properties of these lasers [109].…”
Section: Frequency Comb Stabilizationmentioning
confidence: 99%
See 1 more Smart Citation
“…In the 1980s, Dave Bloom at Stanford made pioneering contributions to the synchronization of actively modelocked picosecond lasers to a microwave frequency reference [105,106], which he then applied to electro-optic sampling of GaAs integrated circuits [45]. I did my Ph.D. work in his group and explored to extend this synchronization technique to femtosecond fiber Raman soliton lasers [107,108] to improve the time resolution in electro-optic sampling, which turned out not to work due to the poor noise properties of these lasers [109].…”
Section: Frequency Comb Stabilizationmentioning
confidence: 99%
“…I was made aware of this paper during my Ph.D. thesis work in Stanford (1985Stanford ( -1989 during which my Ph.D. advisor Prof. Dave Bloom sent me to Prof. Anthony Siegman, one of the pioneers in active modelocking theories [42,43], to find out why we cannot passively modelock Nd:glass lasers. At that time we used 30 to 100 ps pulses from flashlamppumped Nd:YAG and Nd:YLF lasers which we had to externally compress into the few picosecond regime [44] for electro-optic sampling applications [45]. We needed even shorter pulses, which we achieved with a double-stage pulse compressor-rather tricky to use, to say the least.…”
Section: Q-switching Instabilitiesmentioning
confidence: 99%
“…The semiconductor mode-locked laser has been the subject of extensive research for over a decade [38]- [44]. The motivation for research on semiconductor mode-locked lasers derives from the potential applications as a source of ultra short pulses for electro-optic sampling systems [45,46], optical clock distribution [47,48], and as a source for high speed data communication systems [49].…”
Section: Construction Of the Semiconductor Mode-locked Lasermentioning
confidence: 99%
“…There are numerous applications for multi-GHz laser sources in science and technology such as optical clocking [1], photonic switching [2] or high-speed electro-optic sampling [3], just to mention a few. Multi-GHz mode-locked lasers emitting in the 1.5 µm spectral range are particularly interesting for fiber-optical telecommunication applications as they operate in the window of minimal glass absorption, which enables long-haul data transfer.…”
Section: Introductionmentioning
confidence: 99%