000607055 001__ 607055
000607055 005__ 20250723171739.0
000607055 020__ $$a 9781510669987
000607055 0247_ $$2doi$$a10.1117/12.3003195
000607055 0247_ $$2openalex$$aopenalex:W4392693270
000607055 037__ $$aPUBDB-2024-01754
000607055 041__ $$aEnglish
000607055 082__ $$a620
000607055 1001_ $$0P:(DE-H253)PIP1097267$$aRentschler, Christian$$b0$$eCorresponding author
000607055 1112_ $$aSPIE Photonics West LASE$$cSan Francisco$$d2024-01-29 - 2024-01-31$$wUnited States
000607055 245__ $$aParameter dependencies in multicycle THz generation with tunable high-energy pulse trains in large-aperture crystals
000607055 260__ $$aBellingham, Wash.$$bSPIE$$c2024
000607055 29510 $$aNonlinear Frequency Generation and Conversion: Materials and Devices XXIII
000607055 300__ $$a10
000607055 3367_ $$2ORCID$$aCONFERENCE_PAPER
000607055 3367_ $$033$$2EndNote$$aConference Paper
000607055 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$mjournal
000607055 3367_ $$2BibTeX$$aINPROCEEDINGS
000607055 3367_ $$2DRIVER$$aconferenceObject
000607055 3367_ $$2DataCite$$aOutput Types/Conference Paper
000607055 3367_ $$0PUB:(DE-HGF)8$$2PUB:(DE-HGF)$$aContribution to a conference proceedings$$bcontrib$$mcontrib$$s1715939750_2376937
000607055 3367_ $$0PUB:(DE-HGF)7$$2PUB:(DE-HGF)$$aContribution to a book$$mcontb
000607055 520__ $$aEfficiencies of nonlinear optical-to-terahertz (THz) conversion below one percent remain a limiting factor for applications of multicycle THz radiation like THz-driven acceleration and inspired the use of multi-line pump spectra. To overcome the difficulty of phase stabilization of multiple narrowband sources required by the multi-line approach, we exploit its temporal analog, i.e., regular pulse trains with THz repetition rate, in which the THz waves generated by rectifying the individual pulses add coherently. The optical setup producing the pulse trains consists of motorized interferometers and enables precise control over the pulse train parameters like pulse spacing and amplitude. It is operated with a laser providing 400 fs pulses and energies of up to 110 mJ, which is the highest yet attempted for a pulse-train-type experiment. Opposed to earlier work, pulse division is done after amplification making the system more flexible in terms of tuning the pulse number. We present initial results of an experimental campaign of multicycle THz generation in custom periodically poled crystals with large apertures up to 10x20 mm2. The available pump energy allows filling these apertures at high fluences, promising increased THz yields. We investigate the dependence of the conversion efficiency on the single pulse duration and aim to find the optimum pulse number for different crystal lengths to determine the efficiency limitations in a regime avoiding laser-induced damage. Since crystal length and pulse number define the bandwidth of the THz pulses, this work demonstrates a path to an optimized THz source tunable to different requirements of applications.
000607055 536__ $$0G:(DE-HGF)POF4-631$$a631 - Matter – Dynamics, Mechanisms and Control (POF4-631)$$cPOF4-631$$fPOF IV$$x0
000607055 536__ $$0G:(EU-Grant)609920$$aAXSIS - Frontiers in Attosecond X-ray Science: Imaging and Spectroscopy (609920)$$c609920$$fERC-2013-SyG$$x1
000607055 588__ $$aDataset connected to CrossRef Conference
000607055 693__ $$0EXP:(DE-H253)AXSIS-20200101$$1EXP:(DE-H253)SINBAD-20200101$$5EXP:(DE-H253)AXSIS-20200101$$aSINBAD$$eAXSIS: Frontiers in Attosecond X-ray Science, Imaging and Spectroscopy$$x0
000607055 7001_ $$0P:(DE-H253)PIP1026174$$aMatlis, Nicholas$$b1$$udesy
000607055 7001_ $$0P:(DE-H253)PIP1032520$$aDemirbas, Umit$$b2
000607055 7001_ $$0P:(DE-H253)PIP1094307$$aZhang, Zhelin$$b3
000607055 7001_ $$0P:(DE-H253)PIP1014672$$aPergament, Mikhail$$b4$$udesy
000607055 7001_ $$0P:(DE-HGF)0$$aZukauskas, Andrius$$b5
000607055 7001_ $$0P:(DE-HGF)0$$aCanalias, Carlota$$b6
000607055 7001_ $$0P:(DE-HGF)0$$aIshizuki, Hideki$$b7
000607055 7001_ $$0P:(DE-HGF)0$$aPasiskevicius, Valdas$$b8
000607055 7001_ $$0P:(DE-HGF)0$$aLaurell, Fredrik$$b9
000607055 7001_ $$0P:(DE-HGF)0$$aTaira, Takunori$$b10
000607055 7001_ $$0P:(DE-H253)PIP1013198$$aKärtner, Franz$$b11$$udesy
000607055 7001_ $$0P:(DE-HGF)0$$aSchunemann, Peter G.$$b12$$eEditor
000607055 77318 $$2Crossref$$3proceedings-article$$a10.1117/12.3003195$$bSPIE$$d2024-03-12$$p44$$tNonlinear Frequency Generation and Conversion: Materials and Devices XXIII$$y2024
000607055 773__ $$0PERI:(DE-600)2398361-9$$a10.1117/12.3003195$$p44$$tProceedings of SPIE$$v12869$$x0038-7355$$y2024
000607055 8564_ $$uhttps://www.spiedigitallibrary.org/conference-proceedings-of-spie/12869/128690M/Parameter-dependencies-in-multicycle-THz-generation-with-tunable-high-energy/10.1117/12.3003195.full
000607055 8564_ $$uhttps://bib-pubdb1.desy.de/record/607055/files/Rentschler-et-al_Parameter%20dependencies%20in%20multicycle%20THz%20generation%20with%20tunable%20high-energy%20pulse%20trains%20in%20large-aperture%20crystals.pdf$$yRestricted
000607055 8564_ $$uhttps://bib-pubdb1.desy.de/record/607055/files/Rentschler-et-al_Parameter%20dependencies%20in%20multicycle%20THz%20generation%20with%20tunable%20high-energy%20pulse%20trains%20in%20large-aperture%20crystals.pdf?subformat=pdfa$$xpdfa$$yRestricted
000607055 909CO $$ooai:bib-pubdb1.desy.de:607055$$pec_fundedresources$$pVDB$$popenaire
000607055 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1097267$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000607055 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1097267$$aCentre for Free-Electron Laser Science$$b0$$kCFEL
000607055 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1026174$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
000607055 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1026174$$aCentre for Free-Electron Laser Science$$b1$$kCFEL
000607055 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1032520$$aExternal Institute$$b2$$kExtern
000607055 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1094307$$aExternal Institute$$b3$$kExtern
000607055 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1014672$$aDeutsches Elektronen-Synchrotron$$b4$$kDESY
000607055 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1014672$$aCentre for Free-Electron Laser Science$$b4$$kCFEL
000607055 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1013198$$aDeutsches Elektronen-Synchrotron$$b11$$kDESY
000607055 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1013198$$aCentre for Free-Electron Laser Science$$b11$$kCFEL
000607055 9101_ $$0I:(DE-588)1043621512$$6P:(DE-H253)PIP1013198$$aEuropean XFEL$$b11$$kXFEL.EU
000607055 9131_ $$0G:(DE-HGF)POF4-631$$1G:(DE-HGF)POF4-630$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lVon Materie zu Materialien und Leben$$vMatter – Dynamics, Mechanisms and Control$$x0
000607055 9141_ $$y2024
000607055 915__ $$0StatID:(DE-HGF)0430$$2StatID$$aNational-Konsortium$$d2025-01-01$$wger
000607055 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2025-01-01
000607055 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline$$d2025-01-01
000607055 9201_ $$0I:(DE-H253)FS-CFEL-2-20120731$$kFS-CFEL-2$$lUltrafast Lasers & X-rays Division$$x0
000607055 980__ $$acontrib
000607055 980__ $$aVDB
000607055 980__ $$ajournal
000607055 980__ $$acontb
000607055 980__ $$aI:(DE-H253)FS-CFEL-2-20120731
000607055 980__ $$aUNRESTRICTED
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.27.027273
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/nphoton.2013.184
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/ncomms9486
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.2357551
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1063/1.2959846
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.optcom.2010.10.092
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OL.40.005762
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OL.42.002118
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/s41467-019-10657-4
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.398268
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OL.413410
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/s41598-022-20622-9
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OL.448457
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/s42005-020-00421-2
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.475604
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OL.41.003806
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.24.025582
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.27.019254
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1002/lpor.v14.11
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.503480
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.14.002263
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OE.20.020002
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1007/s10762-015-0165-5
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1364/OME.1.000201
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1109/3.748831
000607055 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/scientificamerican0464-38