2012
DOI: 10.1088/1742-6596/359/1/012002
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Toward highly stable Terahertz Coherent Synchrotron Radiation at the synchrotron SOLEIL

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Cited by 5 publications
(4 citation statements)
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“…The flux of this emission between 250 and 750 GHz (about 0.4 to 1.2 mm wavelength) is advantageous for performing broad band interferometric spectroscopy measurements (here about nine hours). For high resolution measurements, (here •30 MHz resolution) the signal-to-noise has been optimized through minimizing the source instabilities [14,16,17]. These optimal conditions allowing for an intense emission over a wide frequency range are found for a momentum compaction factor: α = α 0 /25 (with α 0 the nominal compaction factor) , corresponding to a theoretical bunch length at zero current of around 3 ps (1 mm), and a current per bunch of 70µA.…”
Section: Methodsmentioning
confidence: 99%
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“…The flux of this emission between 250 and 750 GHz (about 0.4 to 1.2 mm wavelength) is advantageous for performing broad band interferometric spectroscopy measurements (here about nine hours). For high resolution measurements, (here •30 MHz resolution) the signal-to-noise has been optimized through minimizing the source instabilities [14,16,17]. These optimal conditions allowing for an intense emission over a wide frequency range are found for a momentum compaction factor: α = α 0 /25 (with α 0 the nominal compaction factor) , corresponding to a theoretical bunch length at zero current of around 3 ps (1 mm), and a current per bunch of 70µA.…”
Section: Methodsmentioning
confidence: 99%
“…The synchrotron provides a source of infrared radiation that combines the advantages of a high brilliance and a wide spectral coverage [10 and reference therein]. To enhance its intensity in the THz range, a number of synchrotron radiation facilities around the world have studied the production of Coherent Synchrotron Radiation (CSR) obtained by reducing the bunch length so that it becomes comparable to the emitted wavelength [11][12][13][14][15][16][17]. Although this operation mode allows a large flux enhancement in the THz range (•10 10 4 ), the interaction of the electrons with their own electromagnetic field causes a microstructure (microbunching) in the electron bunch, resulting in bursts of THz radiation and with accompanying source instabilities [14].…”
mentioning
confidence: 99%
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“…More than fifteen years have passed since it was proven that CSR is a suitable source for diffraction-limited Fourier transform spectroscopy [8] and the first successful scientific experiment using THz radiation from short electron bunches was performed [9]. The low α technology is now becoming available at several storage rings worldwide (e.g., [10][11][12][13][14][15]) and this powerful broadband source allows for many scientific experiments [16] including THz-electron paramagnetic resonance (EPR) [17] and high-resolution spectroscopy with THz frequency combs [18]. Currently, storage rings offer to users the low α mode at reduced currents stored.…”
Section: Introductionmentioning
confidence: 99%