Far Infrared Coherent Synchrotron Edge Radiation at ANKA

A synchrotron radiation source emits coherent infrared (IR) radiation when the electron bunch length is comparable to the wavelength of the emitted radiation (see for example [1, 2]). To generate coherent radiation in the far IR (THz) region, a 'low alpha mode' has been devised at the ANKA...

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Hauptverfasser: Muller, A.-S., Birkel, I., Gasharova, B., Huttel, E., Kubat, R., Mathis, Y.-L., Moss, D.A., Mexner, W., Rossmanith, R., Wuensch, M., Wesolowski, P., Perez, F., Pont, M., Hirschmugl, C.J.
Format: Tagungsbericht
Sprache:eng
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Zusammenfassung:A synchrotron radiation source emits coherent infrared (IR) radiation when the electron bunch length is comparable to the wavelength of the emitted radiation (see for example [1, 2]). To generate coherent radiation in the far IR (THz) region, a 'low alpha mode' has been devised at the ANKA storage ring operating at 1.3 GeV. The corresponding lattice has a significantly reduced momentum compaction factor. The spectral dependence of the emitted radiation is recorded at the ANKA-IR beam line, where the synchrotron light is produced in the fringe field of a bending magnet [3]. This edge radiation has the advantage of being more collimated than constant field radiation. This allows the observation of frequencies down to 1 cm -1 through a modest vertical aperture, which would not be possible with classical constant field emission due to the increasing beam divergence with decreasing frequency. The onset of coherent emission is found at a synchrotron frequency of about 10 kHz. At 5 kHz, an intensity enhancement of up to 5 orders of magnitude, with respect to the incoherent emission, is observed in the spectral range between 1 and 65 cm -1 .
ISSN:1944-4680
2152-9582
DOI:10.1109/PAC.2005.1591164