000 | 03295nlm1a2200493 4500 | ||
---|---|---|---|
001 | 663945 | ||
005 | 20231030041913.0 | ||
035 | _a(RuTPU)RU\TPU\network\35115 | ||
090 | _a663945 | ||
100 | _a20210319a2020 k y0engy50 ba | ||
101 | 0 | _aeng | |
102 | _aUS | ||
135 | _adrcn ---uucaa | ||
181 | 0 | _ai | |
182 | 0 | _ab | |
200 | 1 |
_aNoninvasive bunch length measurements exploiting Cherenkov diffraction radiation _fA. Curcio, M. Bergamaschi, R. Corsini [et al.] |
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203 |
_aText _celectronic |
||
300 | _aTitle screen | ||
320 | _a[References: 40 tit.] | ||
330 | _aWe present the observation and the detailed investigation of coherent Cherenkov diffraction radiation (CChDR) in terms of spectral-angular characteristics. Electromagnetic simulations have been performed to optimize the design of a prismatic dielectric radiator and the performance of a detection system with the aim of providing longitudinal beam diagnostics. Successful experimental validations have been organized on the CLEAR and the CLARA facilities based at CERN and Daresbury laboratory respectively. With ps to sub-ps long electron bunches, the emitted radiation spectra extend up to the THz frequency range. Bunch length measurements based on CChDR have been compared to longitudinal bunch profiles obtained using a radio frequency deflecting cavity or coherent transition radiation (CTR). The retrieval of the temporal profile of both Gaussian and non-Gaussian bunches has also been demonstrated. The proposed detection scheme paves the way to a new kind of beam instrumentation, simple and compact for monitoring short bunches of charged particles, particularly well-adapted to novel accelerator technologies, such as dielectric and plasma accelerators. Finally, CChDR could be used for generating intense THz radiation pulses at the MW level in existing radiation facilities, providing broader opportunities for the user community. | ||
461 | _tPhysical Review Accelerators and Beams | ||
463 |
_tVol. 23, iss. 2 _v[022802, 13 p.] _d2020 |
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610 | 1 | _aэлектронный ресурс | |
610 | 1 | _aтруды учёных ТПУ | |
610 | 1 | _aпучки | |
610 | 1 | _aизлучение | |
610 | 1 | _aсгустки | |
610 | 1 | _aэлектромагнитное моделирование | |
701 | 1 |
_aCurcio _bA. _gAlessandro |
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701 | 1 |
_aBergamaschi _bM. |
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701 | 1 |
_aCorsini _bR. _gRoberto |
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701 | 1 |
_aFarabolini _bW. _gWilfrid |
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701 | 1 |
_aGamba _bD. _gDavide |
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701 | 1 |
_aGarolfi _bL. |
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701 | 1 |
_aKieffer _bR. |
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701 | 1 |
_aFedorov _bK. V. _gKirill Valerjevich |
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701 | 1 |
_aKarataev _bP. V. _gPavel Vladimirovich |
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701 | 1 |
_aLekomtsev _bK. V. _gKonstantin |
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701 | 1 |
_aSaveliev _bYu. M. _gYuri |
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701 | 1 |
_aPotylitsyn _bA. P. _cRussian physicist _cProfessor of the TPU _f1945- _gAlexander Petrovich _2stltpush _3(RuTPU)RU\TPU\pers\26306 |
|
712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИсследовательская школа физики высокоэнергетических процессов _c(2017- ) _h8118 _2stltpush _3(RuTPU)RU\TPU\col\23551 |
801 | 2 |
_aRU _b63413507 _c20210319 _gRCR |
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856 | 4 | _uhttps://doi.org/10.1103/PhysRevAccelBeams.23.022802 | |
942 | _cCF |