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Steffen B, Gerth C, Caselle M, Felber M, Kozak T, Makowski DR, Mavrič U, Mielczarek A, Peier P, Przygoda K, Rota L. Compact single-shot electro-optic detection system for THz pulses with femtosecond time resolution at MHz repetition rates. Rev Sci Instrum 2020; 91:045123. [PMID: 32357714 DOI: 10.1063/1.5142833] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/17/2019] [Accepted: 04/08/2020] [Indexed: 05/23/2023]
Abstract
Electro-optical detection has proven to be a valuable technique to study temporal profiles of THz pulses with pulse durations down to femtoseconds. As the Coulomb field around a relativistic electron bunch resembles the current profile, electro-optical detection can be exploited for non-invasive bunch length measurements at accelerators. We have developed a very compact and robust electro-optical detection system based on spectral decoding for single-shot longitudinal bunch profile monitoring at the European X-ray Free Electron Laser (XFEL) for electron bunch lengths down to 200 fs (rms). Apart from the GaP crystal and the corresponding laser optics at the electron beamline, all components are housed in 19 in. chassis for rack mount and remote operation inside the accelerator tunnel. An advanced laser synchronization scheme based on radio-frequency down-conversion has been developed for locking a custom-made Yb-fiber laser to the radio-frequency of the European XFEL accelerator. In order to cope with the high bunch repetition rate of the superconducting accelerator, a novel linear array detector has been employed for spectral measurements of the Yb-fiber laser pulses at frame rates of up to 2.26 MHz. In this paper, we describe all sub-systems of the electro-optical detection system as well as the measurement procedure in detail and discuss the first measurement results of longitudinal bunch profiles of around 400 fs (rms) with an arrival-time jitter of 35 fs (rms).
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Affiliation(s)
- B Steffen
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - Ch Gerth
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - M Caselle
- IPE, Karlsruhe Institute of Technology (KIT), 76344 Eggenstein-Leopoldshafen, Germany
| | - M Felber
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - T Kozak
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - D R Makowski
- DMCS, Łódź University of Technology (TUL), 90-924 Łódź, Poland
| | - U Mavrič
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - A Mielczarek
- DMCS, Łódź University of Technology (TUL), 90-924 Łódź, Poland
| | - P Peier
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - K Przygoda
- MSK, Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
| | - L Rota
- IPE, Karlsruhe Institute of Technology (KIT), 76344 Eggenstein-Leopoldshafen, Germany
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Juranić PN, Stepanov A, Ischebeck R, Schlott V, Pradervand C, Patthey L, Radović M, Gorgisyan I, Rivkin L, Hauri CP, Monoszlai B, Ivanov R, Peier P, Liu J, Togashi T, Owada S, Ogawa K, Katayama T, Yabashi M, Abela R. High-precision x-ray FEL pulse arrival time measurements at SACLA by a THz streak camera with Xe clusters. Opt Express 2014; 22:30004-12. [PMID: 25606930 DOI: 10.1364/oe.22.030004] [Citation(s) in RCA: 13] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/19/2023]
Abstract
The accurate measurement of the arrival time of a hard X-ray free electron laser (FEL) pulse with respect to a laser is of utmost importance for pump-probe experiments proposed or carried out at FEL facilities around the world. This manuscript presents the latest device to meet this challenge, a THz streak camera using Xe gas clusters, capable of pulse arrival time measurements with an estimated accuracy of several femtoseconds. An experiment performed at SACLA demonstrates the performance of the device at photon energies between 5 and 10 keV with variable photon beam parameters.
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