scholarly journals Repetition rate performance for frequency mixing of four simultaneous QPSK signals based on a SOA-MZI photonic sampling mixer

2021 ◽  
Vol 60 (11) ◽  
Author(s):  
Hassan Termos ◽  
Ali Mansour ◽  
Abbass Nasser
1985 ◽  
Author(s):  
Gabriella Vietri ◽  
Renato Marchetti ◽  
Eugenio Penco ◽  
Gianemilio Salvetti

1980 ◽  
Vol 23 (4) ◽  
pp. 894-908 ◽  
Author(s):  
William R. Tiffany

Paragraphs with controlled phonetic structures were matched to similarly structured diadochokinetic (Maximum Repetition Rate) tasks in an effort to devise a more valid measurement for (1) assessing possible relationships between diadochokinesis and speech rate, and (2) evaluating the effects on articulation rates of such structural variables as number of consonants in a syllable, and alternating versus simple syllable repetitions. Highly stable results were obtained, suggesting the possibility of a sharp neurophysiological or biomechanical barrier which varies markedly among presumably normal speakers. Maximum repetition rates were poor predictors of normal reading rate performance. On the other hand, normal reading rates were found to be approximately the same as the maximum repetition rates—about 13.5 phones per second. The inference is that normal speech is not, as commonly supposed, obviously slower than maximum rates of syllable articulation, for equivalent syllables. The major source of variation in syllable rate measures was simply the number of phones in a syllable. The effects of articulatory place and manner appeared relatively trivial by comparison.


1990 ◽  
Vol 29 (Part 1, No. 6) ◽  
pp. 1108-1111 ◽  
Author(s):  
Shigeyuki Takagi ◽  
Noboru Okamoto ◽  
Saburo Sato ◽  
Tatsumi Goto

2019 ◽  
Author(s):  
Le Wang ◽  
Devon Jakob ◽  
Haomin Wang ◽  
Alexis Apostolos ◽  
Marcos M. Pires ◽  
...  

<div>Infrared chemical microscopy through mechanical probing of light-matter interactions by atomic force microscopy (AFM) bypasses the diffraction limit. One increasingly popular technique is photo-induced force microscopy (PiFM), which utilizes the mechanical heterodyne signal detection between cantilever mechanical resonant oscillations and the photo induced force from light-matter interaction. So far, photo induced force microscopy has been operated in only one heterodyne configuration. In this article, we generalize heterodyne configurations of photoinduced force microscopy by introducing two new schemes: harmonic heterodyne detection and sequential heterodyne detection. In harmonic heterodyne detection, the laser repetition rate matches integer fractions of the difference between the two mechanical resonant modes of the AFM cantilever. The high harmonic of the beating from the photothermal expansion mixes with the AFM cantilever oscillation to provide PiFM signal. In sequential heterodyne detection, the combination of the repetition rate of laser pulses and polarization modulation frequency matches the difference between two AFM mechanical modes, leading to detectable PiFM signals. These two generalized heterodyne configurations for photo induced force microscopy deliver new avenues for chemical imaging and broadband spectroscopy at ~10 nm spatial resolution. They are suitable for a wide range of heterogeneous materials across various disciplines: from structured polymer film, polaritonic boron nitride materials, to isolated bacterial peptidoglycan cell walls. The generalized heterodyne configurations introduce flexibility for the implementation of PiFM and related tapping mode AFM-IR, and provide possibilities for additional modulation channel in PiFM for targeted signal extraction with nanoscale spatial resolution.</div>


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