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virtual diagnostics, where learned surrogate models provide information about the state of an accelerator that would oth- erwise be difficult or even impossible to acquire using a physicaldiagnosticasinourcase. Theprovidedinformation cangiveusefuldataaboutexperimentsandhelpoperators tune the accelerator. Previous work ...
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7bd06d1d-734e-4b4d-9236-e5435ca09a7f
dimensionalLPSattheEuXFELfromRFsettingsandthe CRISP spectrum. In consideration of the limited amount of LPSmeasurementsavailable,wedecidedtobasethetraining of such model on simulated data. METHODS AND RESULTS Dataset Generation In order to effectively train a surrogate model, large scale simulated data is required. For...
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392ae252-b782-45ff-827a-dbccafeeebdb
scenariointhefirstbunchcompressor. Thelasttwoparame- ters,theL1andL2chirps,controlthecompressionstrengths inthesecondandthirdchicanesections. Preliminarystudies were conducted in the past [ 9,10], where the RF settings where adjusted with relatively small variations based on the nominal design. The aim of this project ...
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a511dc1b-5e7b-4d8b-a456-c4a677a0c262
Figure 1: Schematiclayoutof the EuXFEL. Table 1: The RF Parameter Input Features and the Values Ranges Used in Simulations for the Dataset Generation Parameter (unit) lower upper bound bound Injector chirp ( 1/𝑚) -10 -7 Injector curvature ( 1/𝑚2) -100 +300 Injector cubic coefficient ( 1/𝑚3) 0 30000 L1 chirp ( 1/𝑚) ...
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e25bece1-ba7e-4bea-984a-c7b6d0f2be8d
ular framework for beam dynamics simulations allowing for particle tracking, optics functions calculations, matching of Twissparametersinamagneticlatticebyoptimizingasetof variables. The Ocelot model of physical processes includes collectiveeffectsasspacecharge,coherentsynchrotronra- diation, wakefields and more. Figur...
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b06c4574-b871-4ff9-960b-7cf1dbfa4a6a
model that is trained on data from a start-to-end beam dy- namicssimulationtocombinescalarandspectralinforma- tion in order to infer either the current profile or the two- dimensional LPS. To this end, we construct a model that receives two inputs: a 5D vector of RF settings and a 240-D THz formfactor sampled from 0.7 ...
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ahigh-resolution(300×300)imageofthephasespace. To ensure physical units, the network includes a secondary out- put head that predicts the energy and spatial scales (ranges) of the distribution. The model is trained in a supervised setup to minimise the difference between the reconstructed andthegroundtruthLPSimages. Th...
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be partially attributed to the inductive bias of the chosen convolutionalarchitecture. The network’slayersinherently prioritizethereconstructionofcontinuous,low-frequency features,whichare more stableduring the gradient descent process. Also the loss function might be responsible for smearing the intensity over a certa...
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Figure 3: Three examplesfrom the validationset comparing ground truth and reconstructed 2D LPS images. Operational Applications The developed model serves a dual-purpose for machine operations. Asa virtualdiagnostic ,ittakesreal-timeread- backsofRFsettingsandmeasuredCRISPspectratoprovide operators with an instantaneous...
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machine. CONCLUSIONS AND OUTLOOK In this paper, we demonstrated the first steps toward a machine-learning-based virtual diagnostic for the longitu- dinal phase space at the European XFEL. By leveraging the Ocelot simulation toolkit, we generated a comprehen- sive dataset validated against experimental injector mea- sur...
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variational autoencoders to sharpen the reconstructed im- ages and recover the slice details. The corrected model willthenbeintegratedintotheEuXFELcontrolsystemviaaded- icated graphical user interface, enabling livecomparisons between predicted and measured beam properties during facility operation. This work lays the ...
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Maxwell computational resources operated at DESY. REFERENCES [1]E. Volobuev et al., “Transverse deflecting structure XFEL TDS INJ”, J. Phys.: Conf. Ser. , vol. 747, p. 012083, Sep. 2016. doi:1/zero.alt4.1/zero.alt488/1742-6596/747/1//zero.alt412/zero.alt483 [2]S.Wesch,B.Schmidt,C.Behrens,H.Delsim-Hashemi,andP. Schmüser...
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vol.23, no. 11, p. 112801, Nov.2020. doi:1/zero.alt4.11/zero.alt43/PhysRevAccelBeams.23.1128/zero.alt4117th International Particle Accelerator Conference, Deauville, France JACoW Publishing ISBN: 978-3-95450-252-3 ISSN: 2673-5350 doi: 10.18429/JACoW-IPAC2026-WEP6156 2894 MC6.T33: Online Modelling and Software ToolsWEP6...
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[4]S. Tomin, W. Decking, N. Golubeva, A. I. Novokshonov, T. Wohlenberg, and I. Zagorodnov, “Longitudinal Phase Space Diagnostics with Corrugated Structure at the Euro- peanXFEL”,in Proc.IPAC’22 ,Bangkok,Thailand,pp.275– 278, Jul. 2022. doi:1/zero.alt4.18429/JACoW-IPAC2/zero.alt422-MOPOPT/zero.alt42/zero.alt4 [5]P. Dijk...
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doi:1/zero.alt4.1/zero.alt416/j.nima.2/zero.alt421.165111 [7]C.Emma,A.Edelen,M.J.Hogan,B.O’Shea,G.White,and V. Yakimenko, “Machine learning-based longitudinal phase spacepredictionofparticleaccelerators”, Phys.Rev.Accel. Beams, vol.21, no. 11, p. 112802, Nov.2018. doi:1/zero.alt4.11/zero.alt43/PhysRevAccelBeams.21.1128...
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4467,Sep. 2023. doi:1/zero.alt4.18429/JACoW-IPAC2/zero.alt423-THPL/zero.alt419 [10]S. T. Z. Zhu and J. Kaiser, “Application of machine learning inlongitudinalphasespacepredictionattheeuropeanXFEL”, inProc. FEL2022 , Trieste, pp. 391–394, Aug. 2022. doi:1/zero.alt4.18429/JACoW-FEL2/zero.alt422-WEP12 [11]S. Tomin, I. Aga...
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A, vol. 768, pp. 151–156, 2014. doi:1/zero.alt4.1/zero.alt416/j.nima.2/zero.alt414./zero.alt49./zero.alt457 [13]D. P. Kingma and J. Ba, “Adam: a method for stochastic optimization”, 2017, doi:1/zero.alt4.4855/zero.alt4/arXiv.1412.698/zero.alt4 ,17th International Particle Accelerator Conference, Deauville, France JACoW...
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GLOBAL START-TO-END OPTIMIZATION WITH BAYESIAN OPTIMIZATION∗ B. Veglia†, B. Beutner, S. Tomin, S. D. Walker Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany Abstract Controlling the beam longitudinal phase space (LPS) dis- tributioniscrucialforadvancedfree-electronlaseroperation modes. AttheEuropeanXFEL,thistask...
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measured longitudinal phase space profiles. INTRODUCTION Precisecontroloverthelongitudinalphasespace(LPS) distribution of electron bunches is fundamental to the op- eration of modern X-ray free-electron lasers (FELs). At facilities such as the European XFEL (EuXFEL), advanced operating modes—including the generation of...
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efficiently, minimizing the number of expensive ”black-box” evaluations required to reach an optimal solution. Recent advancesinmachinelearningandglobaloptimizationoffera pathforward. Bayesianoptimization(BO)[ 1,2]hasemerged as a particularlyeffectivetool for accelerator physics [ 3,4], characterized byitssample effici...
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ing first on the task of model calibration. We show that byautomatingthetuningofRFparameterswithinstart-to- endsimulations,theBOframeworkcanefficientlyreconcile ∗Worksupported bythe EuXFEL R&D program. †bianca.veglia@desy.dephysicsmodelswithexperimentalmeasurements, ensuring thatsimulation-basedpredictionsaccuratelyref...
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7dbd8698-5466-46e3-bbef-cd3c0cfa1cb7
where the beam compression was varied by scanning the Linac L1 chirp from -12.4 to −4.4m−1in 9 steps. The chirp is defined as−𝑘𝑉sin𝜑 𝐸0+𝑉cos𝜑, where𝜑and𝑉are the voltageand phase of Linac L1, 𝐸0= 130 MeV is the initial energy of thebeambeforeL1, and 𝑘 = 2𝜋𝑓/𝑐 ,𝑓 =1.3GHz. Details abouttheEuropeanXFELthreest...
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Voltage in L1 ± 5 MeV Phase in L1 ± 0.3 deg Voltage in L2 ± 15 MeV Phase in L2 ± 0.5 deg WeimplementedaBOframeworktotuneOCELOTsimu- lations[9–11]byidentifyingtheoptimalparametersrequired to reproduce the observed beam characteristics. The opti- mizationparametersincludedtheRFsettingsfortheinjector andlinacsL1andL2. The...
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Mean Square Error (RMSE) between the reference and sim- ulated current profiles. To ensure a robust comparison, a cross-correlation function aligns the two curves by identify- ing the temporal shift that maximizes their overlap.17th International Particle Accelerator Conference, Deauville, France JACoW Publishing ISBN:...
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Figure 1: Comparison of optimized simulations vs current profiles measured with the CRISP spectrometer. Each plot corresponds to a different value of the chirp in L1. Table1detailstheoptimizedRFparametersandtheirtun- ing ranges, defined relative to the initial machine read-outs at the time of the experiment: at the inj...
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showed similar agreement (and closely resemble the curves shown in the plot corresponding to L1 chirp = -7.4). Minor discrepanciescanbeattributedtothefactthatmeasurements weretakenwiththelaserheaterdeactivated. Theresulting microbunching instabilities are not currently modeled in the OCELOT tracking simulations, leadin...
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a7ab0185-4e0a-4ff5-8b9c-6124f22c48f8
hardX-rayself-seeding(HXRSS)[ 12]whicharehighlysen- sitive to the electron beam’s longitudinal distribution [ 13]. Figure2shows the performance of the BO when optimiz- ing for different reference profiles. We observed that theconvergenceoftheoptimizerishighlysensitivetotheinitial parametersandthechoiceofhyperparameters...
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experimental CRISP measurements by identifying small butsignificantoffsetsinRFparameters. Furthermore,the frameworkprovedcapableof”reverse-engineering”machine configurationstomatchspecific,user-definedlongitudinal current profiles, including Gaussian, flat-top, and triangular distributions. Looking forward, we intend t...
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discrepancies,newmeasurement campaigns areplanned in whichthemicrobunchinginstability(MBI)willbefullysup- pressed using the laser heater. This will facilitate a more direct comparison with numerical models and provide a17th International Particle Accelerator Conference, Deauville, France JACoW Publishing ISBN: 978-3-95...
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(a) Gaussian (b) Flat top (c) Left triangle (d) Right triangle Figure2: Examplesofsimulationsoptimizedtofitreference profiles.clearer understanding of the underlying longitudinal dynam- ics. ACKNOWLEDGEMENTS The authors are thankful for the support through the Maxwell computational resources operated at DESY. REFERENCE...
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[3]R. Roussel et al., “Bayesian Optimization Algorithms for AcceleratorPhysics”, Phys.Rev.Accel.Beams ,vol.27,no.8, p. 084801, 2024. doi:1/zero.alt4.11/zero.alt43/PhysRevAccelBeams.27./zero.alt4848/zero.alt41 [4]F.Jietal.,“Multi-objectiveBayesianactivelearningforMeV- ultrafastelectrondiffraction”, NatureCommun. ,vol.15...
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Rev. Accel. Beams , vol. 22, no. 2, p. 024401, Feb. 2019. doi:1/zero.alt4.11/zero.alt43/PhysRevAccelBeams.22./zero.alt4244/zero.alt41 [7]S.Wesch,B.Schmidt,C.Behrens,H.Delsim-Hashemi,andP. Schmüser, “A multi-channel THz and infrared spectrometer for femtosecond electron bunch diagnostics by single-shot spectroscopy of c...
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[9]S. Tomin, I. Agapov, M. Dohlus, and I. Zagorodnov, “OCELOT as a Framework for Beam Dynamics Simulations ofX-RaySources”,in Proc.IPAC’17 ,Copenhagen,Denmark, May 2017, pp. 2642–2645. doi:1/zero.alt4.18429/JACoW-IPAC2/zero.alt417-WEPAB/zero.alt431 [10]I. Agapov, G. Geloni, S. Tomin, and I. Zagorodnov, “OCELOT: A softw...
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[11]I.Zagorodnov,S.Tomin,Y.Chen,andF.Brinker,“Experi- mental validation of collective effects modeling at injector section of X-ray free-electron laser”, Nucl. Instrum. Methods Phys. Res., Sect. A , vol. 995, p. 165111, 2021. doi:1/zero.alt4.1/zero.alt416/j.nima.2/zero.alt421.165111 [12]S.Liuetal.,“Updatesonthehardx-ra...
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c7546eff-a50d-40df-a2fc-b3cc427113a0
ISBN: 978-3-95450-252-3 ISSN: 2673-5350 doi: 10.18429/JACoW-IPAC2026-WEP6157 MC6.T33: Online Modelling and Software Tools 2899WEP: Poster session WEP6157 Content from this work may be used under the terms of the CC BY 4.0 licence (© 2026). Any distribution of this work must maintain attribution to the author(s), title ...
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265552ad-ca3b-42d8-a445-2a2ce5f9f4ef
TURNING LOGBOOK DATA INTO OPERATIONAL INSIGHT WITH A NEW STATISTICS SERVICE AT GSI AND FAIR H. Stemmler∗, A. Bloch-Späth, M. Stein, O. Geithner, S. Reimann GSI Helmholtz Centre for Heavy Ion Research, Darmstadt, Germany Abstract Itiscommonpracticeduringacceleratoroperationtocon- tinuouslydocumentallrelevantmachinestate...
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2f459d25-06e1-4dcf-8352-04d5e4404937
search(FAIR)as its operations graduallycommence in the upcoming beamtimes. This service is built as twolayers: a backend layer using the Micronaut framework, which com- municates with the database to retrieve logbook entries and calculatestatistics,andafrontendlayerusingtheAngular framework,whichhandlesuserrequestsandp...
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b9b7f4d2-279a-4515-9b13-cdb424ae3b48
allteams,whichallowsforthemaintenanceofefficientcom- municationbetweencomplex,interactingareassuchasbeam diagnosticsandphysics,technicalinfrastructure,andcontrol systems. At GSI, shift crew operators use OLOG [ 2], an electronic logbook tool developed in-house to continuously record events that may influence beam deliv...
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2e3e01ef-df03-4c3b-a8b0-63c54c0946d4
performanceassessmentatGSIhasrecentlybeenintroduced in Ref. [3]. Resultsare presented in Ref.[ 4]. In addition, documentation becomes increasingly impor- tantasfacilitiesexpand. Withthegradualdevelopmentof the Facility for Antiproton and Ion Research (FAIR) [ 5], the complexity and scale of accelerator operations will ...
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7c0abbce-0c43-456a-b81e-2e0f3a5b86ca
logbook. Upuntilitslastversion,theOLOGwebapplication includedafeatureforgeneratingstatisticalsummaries. Users were able to export tables containing calculated statistics basedonthelogbookentriesstoredinthedatabase. Theseta- bleswouldprovideinformationabouteventsasdocumented bytheoperators. However,concatenationofstatis...
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7b0f3b7a-57e2-468c-99ed-bb06cc323cbb
systemisdesignedtoallowuserstorequestspecificstatistics for a chosen time range and immediately receive both the calculated results and the underlying data. Onceastatisticisselected,theservicerunsthroughsev- eral steps to first retrieve the necessary entries from the OLOG database. Next, the system processes the data a...
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6e6dacce-fb27-4c20-82a0-16df8bdb7ce6
Requirements Asidefromensuringaccurateandreli- ablestatisticalcalculation,thedesignofthenewserviceis guided by three main objectives. First,thesystemmustbeeasytouse. Thewebinterface mustremainintuitiveandrequireminimaltraining,enabling both technical and non-technical users to extract statistics with minimal effort.17t...
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73c24671-0134-4e28-8e6e-b032203123b4
Figure 1: User interfaceof OLOG, the electronic logbook system used at GSI and FAIR to document operational data. Second, loading and computation times must remain low despite large data volumes, ensuring results are generated within seconds. Third,the systemshould producehigh-qualitygraphical outputs. Clear and custom...
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datastructures. Thislimitsthehistoricalrangeofpossible analyses. Additionally, much of the data in the OLOG system is documented manually by operators. While this allows for detaileddescriptionsofevents,italsointroducespotentialin- consistencies, as naming conventions or classification meth- ods may have changed over t...
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work is widely used for building responsive and dynamic webapplications. It providesa robustenvironmentforhan- dlinguserinteractions,andisalreadybeingusedindevel- opment of many other web applications at GSI. Figure2: StaticAngularcomponenthandlingstatisticand timerangeselectionwiththedisplayofselectedtimeranges stampe...
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f9cb925f-6d89-46ed-aa28-77bb03e07453
section. Upon receiving a response from the backend layer, thefrontendgeneratesgraphicalrepresentationsusingthe D3[11] package from the data. Figure 3shows the graphic generated by D3 for the selected statistic and time range specified in Fig. 2. Every graph is configured to display the corresponding statistic as accur...
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ISBN: 978-3-95450-252-3 ISSN: 2673-5350 doi: 10.18429/JACoW-IPAC2026-WEP6158 MC6.T33: Online Modelling and Software Tools 2901WEP: Poster session WEP6158 Content from this work may be used under the terms of the CC BY 4.0 licence (© 2026). Any distribution of this work must maintain attribution to the author(s), title ...
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Figure 3: D3 generated SVG graphic of chosen statistic and time range as specified in Fig. 2. As the backend layer receives requests from the frontend specifyingtheselectedstatisticandthedesiredtimerange, the service then retrieves the corresponding logbook entries fromtheOLOGdatabase. Thebackendthenprocessesthe data e...
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at first sight. As such, the response objects are converted into JSON files, that have the relevant information at first or second level, while the raw data the statistic was calculated from is then provided in deeper levels to the finest detail. Data All calculations are based on event entries manually doc- umentedinO...
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error as some entries are made during hectic in-shift mo- ments. Duringweeklymeetings,eventsdocumentedsince the previous meeting are reviewed and potentially revised to better reflect the reported incident in light of hindsight. This reduces errors and inaccuracies but does not guarantee complete correctness. RESULTS I...
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f8165828-99dc-4549-9ac5-629a34df9a1e
usefulness as a diagnostic resource. Anothernotableresultisthesystem’sperformance. De- spite retrieving thousands of logbook entries spanning over tenyears,theserviceachievesloadingtimesofonlyafew seconds. This gives confidence that expanding the database and the service with further development of FAIR won’t have a bi...
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18f12649-198c-45f4-b465-4277f178dd06
at GSI. By combining automated data retrieval, statistical analysis,andgraphicalvisualization,thesystemsignificantly improves the accessibility and usability of operational data. The service also demonstrates strong performance and scal- ability, enabling the analysis of large datasets with minimal waiting time. Future...
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www.gsi.de/en/start/news [2]P.Schuett etal.,“TheGSIOperationLogbookOLog”,pre- sentedatthe7thInt.WorkshoponAccel.Oper.(WAO’10), Daejeon,Korea,Apr.2010, https://www-conf.kek.jp/ wao/WAO2/zero.alt41/zero.alt4/PDF/O-17.pdf [3]O. Geithner et al., “Introduction of key performance indi- cators for the GSI accelerator facility...
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Taiwan, Jun. 2025, pp. 2495–2498. doi:1/zero.alt4.18429/JACoW-IPAC2/zero.alt425-THBN217th International Particle Accelerator Conference, Deauville, France JACoW Publishing ISBN: 978-3-95450-252-3 ISSN: 2673-5350 doi: 10.18429/JACoW-IPAC2026-WEP6158 2902 MC6.T33: Online Modelling and Software ToolsWEP6158 WEP: Poster se...
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[6]M. Vossberg, K. Berkl, S. Reimann, P. Schuett, R. J. Stein- hagen, and G. Stephan, “FAIR Control Centre (FCC) - Con- cepts and Interim Options for the Existing GSI Main Control Room”,in Proc.8thInt.Part.Accel.Conf.(IPAC’17) ,Copen- hagen, Denmark, May 2017, pp. 1791–1794. doi:1/zero.alt4.18429/JACoW-IPAC2/zero.alt41...
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[9]Angular, https://angular.dev/ [10]Micronaut, https://micronaut.io/ [11]D3,https://d3js.org/ [12]P. Duval, R. Bacher, H. Ehrlichmann, D. Haupt, M. Lom- perski, and J. Bobnar, “Automating Operation Statistics at PETRA-3”,in Proc.16thInt. Conf. Accel.LargeExp. Phys. ControlSyst.(ICALEPCS’17) , Barcelona, Spain, Oct. 20...
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INOVESALIB: A MODULAR VLASOV-FOKKER-PLANCK SOLVER FRAMEWORK F. Donoso∗, M. Brosi, E. Bründermann, M. Frank, S. Funkner, J. Gethmann, A.-S. Müller, P. Schreiber, Karlsruhe Institute of Technology, Karlsruhe, Germany Abstract The numerical solution of the Vlasov–Fokker–Planck (VFP) equation is a well-established method t...
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providesaPythonwrapperforseamlessintegrationintouser workflows. Inovesalib decouples the solver core from appli- cationlogicandoffersapluginarchitecturethatallowsusers to implement custom algorithms without modifying the un- derlyingsolver. TheredesignedstructureturnsInovesafrom a standalone application into a flexible...
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throughwakefields[1],orequivalently,throughthebeam couplingimpedance. Theseinteractionsgiverisetophenom- enasuchascoherentsynchrotronradiation(CSR)andmicro- bunchinginstabilities,whichcansignificantlydegradebeam quality, reduce beam lifetime, and limit the performance of synchrotronradiationfacilities[2,3]. Specificall...
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∗felipe.donoso@kit.eduTosolvethisequationefficientlyinpractice,Inovesawas developed as a runtime-efficient VFPE solver for desktop- classhardware. Theoriginalcodebase,developedbySchön- feldtat KIT[5],combinedadiscretized longitudinalphase space model with optimized numerical operators and paral- lelization, making syst...
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chronous phase shift at KARA, connecting the solver to an experimentally accessible machine observable. In a related study,Funkneret al.[8]developedanon-destructivelongitu- dinal phase space density tomography method, qualitatively validating their reconstructed dynamics against Inovesa sim- ulations driven by KARA mac...
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et al. [11] utilized Inovesa as a primary VFP solver in a cross-code comparison between SOLEIL and KARA. Most recently,Brosiet al.[12]applieditatMAXIVtoinvestigate microwave instabilities under varying intra-beam scatter- ing (IBS) conditions, finding good qualitative agreement between simulation and experiment. These ...
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how these effects depend on bunch length conditions in low momentum compaction operation [14]. Wanget al.[15] usedInovesaastheCSRsimulationenvironmentforaccel- erateddeepreinforcementlearningaimedatfastfeedback17th International Particle Accelerator Conference, Deauville, France JACoW Publishing ISBN: 978-3-95450-252-3...
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of beam dynamics at KARA, showing that Inovesa can also serveasasimulationbackendforlowlatencycontrolsystem development. The original Inovesa software was primarily organized as an application, which is suitable for batch runs and command-linestudiesbutrestrictivewhenthesolvermust be embedded into other software. Moder...
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and algorithms via plugin loading. In practical terms, the samephysicalproblemcannowbesolvedthroughacompact C++API,dynamicallyloadedalgorithmimplementations, or Python bindings, making the solver easier to integrate, extend, and maintain. ARCHITECTURE Inovesalibisorganizedasamodularscientificsoftware frameworkbuiltarou...
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pattern that preserves the validated Inovesa numerical work- flow while exposing it through a compact object interface for external applications, analysis pipelines, and Python- basedworkflows. Inthisway,theestablishedsolverkernel is reorganized into a form with explicit and reusable state management, runtime control, ...
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runtime, so that controller-driven parameter changes can updatetheaffectednumericalmapswithoutrebuildingthe full solver instance.Parameter models Inovesalibintroducesanexplicitparametermodellayer that separates simulation parameter configuration from solverexecution. Inthissoftwarecontext,amodelisnotthe physicaldynamic...
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eter schema and the parameter values. Here, the schema denotesthemetadatathatdescribestheavailableparameters, suchastheirnames,mutability,units,grouping,andvalue types. Themethod describeAttributes() publishesthis schema, whereas the actual parameter values remain stored in the concrete model instance and are accessed ...
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whichprovidestheminimalpolymorphicinterfaceusedto attachoutput-sidecomponentstothesolver. Thisseparation preventssimulationcodefrombeingentangledwithfileI/O, visualization, benchmarking, or communication back-ends, andmakesitpossibletocombineseveraloutputpathways with the same solver run. Severalobserverfamiliesarealre...
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purposeisnottoconsumeoutput,buttomodifythemodelor trigger solver updates while the simulation is running. This is particularly relevant for interactive steering, parameter scanswithfeedback,andfuturehardware-orientedoronline applications. The main controller currently implemented in Inovesalib is the ZMQ model control....
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schema, and applies accepted updates during iteration. These changes can selectively refresh the RF, drift, Fokker- Planck, or wake operators, depending on which parameters havebeenmodified. Thisarchitecturekeepsruntimesteer- ingoutside thenumericalcore whilepreserving consistency between the model state and the active...
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can optionally develop plugins to introduce entirely new types of algorithms, such as novel numerical schemes, data- driven methods, or alternative physics models, expanding the library’s capabilities without ever modifying the core codebase. Thisdesignfollowsthestrategypattern: atruntime,the framework selects and inst...
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ing how models, solvers, observers, and related components interact in typical workflows. C++ The first example illustrates the high-level usage path, where an Inovesa instance is created from a configured model, observers and controllers are attached, and the simu- lation is executed. This reflects the most direct app...
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at construction time through SolverVFP , emphasizing howtheexecutionstrategyischosenindependentlyfrommodel and observers. Listing 2: Algorithm-oriented workflow with explicit strat- egy selection. #include"inovesalib/Inovesalib.h" intmain() { inovesalib::InovesaModel param_model; vector<inovesalib::ObserverBase*> obser...
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attached, and the simulation is executed. The snippet below shows a practical workflow. Listing 3: Minimal Python example. importinovesalibasinl param_model = inl.model("InovesaLegacy") param_model.grid_size = 256 param_model.beam_current = 8.5e-4 solver = inl.Inovesa(param_model) observer = inl.InovesaLegacyObserver()...
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physics studies while enabling new forms of integration throughacompactuserinterfaceandapluginmechanism for developers. Ongoing work focuses on a differentiable VFPsolverthatsupportsbothforwardsimulationandgra- dient propagation for inverse problems and optimization workflows. Access to the Inovesalib codebase is avail...
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REFERENCES [1]M. Dohlus and R. Wanzenberg, “An introduction to wake fields and impedances”,CERN Yellow Rep. School Proc., vol. 3, p. 15, 2017.doi:10.23730/CYRSP-2017-003.15 [2]M. Brosi, “Overview of the micro-bunching instability in electron storage rings and evolving diagnostics”, inProc. IPAC’21, Campinas, SP, Brazil...
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Stanford, CA, USA, Rep. SLAC-PUB-8404, 2000. doi:10.2172/753322 [5]P. Schönfeldt, M. Brosi, M. Schwarz, J. L. Steinmann, and A.-S. Müller, “Parallelized Vlasov–Fokker–Planck solver for desktop personal computers”,Phys. Rev. Accel. Beams, vol. 20, no. 3, p. 030704, 2017. doi:10.1103/PhysRevAccelBeams.20.030704 [6]J. L. ...
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tomography”,Sci. Rep., vol. 13, no. 1, p. 4618, 2023. doi:10.1038/s41598-023-31196-5 [9]M. Brosiet al., “Studies of the micro-bunching instability inthepresenceofadampingwiggler”,J. Phys.: Conf. Ser., vol. 1067, p. 062017, 2018. doi:10.1088/1742-6596/1067/6/062017[10]T. Boltzet al., “Perturbation of synchrotron motion ...
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Taipei, Taiwan, pp. 2207–2210, Jun. 2025. doi:10.18429/JACoW-IPAC2025-WEPM099 [13]S. Maieret al., “Simulation of the effect of corrugated struc- tures on the longitudinal beam dynamics at KARA”, inProc. IPAC’22, Bangkok, Thailand, pp. 2241–2244, Jun. 2022. doi:10.18429/JACoW-IPAC2022-WEPOMS006 [14]S. Maieret al., “Simu...
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of ultra-short electron bunch profiles for the generation of coherent THz radiation”, Ph.D. thesis, Karlsruhe Institute of Technology, Karlsruhe, Germany, 2018. doi:10.5445/IR/1000084466 [17]F.Donosoet al.,“Longitudinalphasespacedensitytomog- raphy constrained by the Vlasov–Fokker–Planck equation”, inProc. IPAC’24, Nas...
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ISBN: 978-3-95450-252-3 ISSN: 2673-5350 doi: 10.18429/JACoW-IPAC2026-WEP6163 MC6.T33: Online Modelling and Software Tools 2907WEP: Poster session WEP6163 Content from this work may be used under the terms of the CC BY 4.0 licence (© 2026). Any distribution of this work must maintain attribution to the author(s), title ...
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PROVIDING REPRODUCIBILITY AND ACCESSIBILITY OF RESEARCH SOFTWARE DEVELOPMENT FOR ACCELERATOR PHYSICS AT KARA F. Donoso∗, E. Bründermann, M. Frank, S. Funkner, J. Gethmann, S. Masoumi, A.-S. Müller Karlsruhe Institute of Technology, Karlsruhe, Germany Abstract Modernacceleratorfacilitiesgenerateheterogeneousdata fromdia...
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971ce173-deea-47d2-8044-436e87cdebad
C++andPythonthatinterfaceswiththeKadi4Mat(Kadi) virtual research environment. BenchTune records metadata for each algorithm run, compiler information, parameters, metrics and stores it in Kadi as portable, traceable research artifacts. Aproject-viewplugininKadivisualizestheevo- lution of a research project, linking cod...
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0e739a90-6a51-41a9-9bd1-2251b4d71b92
isacceleratorresearchattheKarlsruheResearchAccelerator (KARA),usingitasatestfacilityforstudieswithelectron beams, beam diagnostics, and related developments such as magnet systems. KARAservesasacriticaltestbedfornoveldiagnostics, beamdynamicsstudies,and advancedlightsourceapplica- tions,generatinglargeandheterogeneouss...
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andprocesseddataisalreadytreatedasacentralconcernand is addressed according to established FAIR principles [ 1]. At IBPT, this process has recently been strengthened by the ∗felipe.donoso@kit.eduadoption of Kadi4Mat [ 2] (Kadi), a virtual research envi- ronment that supports the structured organization of data, metadat...
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in long-term repositories such as Zenodo, the provenance of individual software executions is rarely preserved as a research object in its own right [ 7]. Such execution-level provenanceextendsbeyondthesourcecodeandincludesthe scientificliteraturemotivatingtheimplementation,metadata describingtheexecutionenvironment,co...
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this, a scientist attempting to reproduce the results at a later stage may still fail. The code in the repository may have changed since the plots were originally produced, the ex- act runtime parameters mayneverhavebeen documented, and the computation itself may have relied on a specific compiler version, build config...
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e532987f-796e-43c0-a653-3f7926adf06b
software execution, runtime environment, and configuration has not been properly persisted [ 8]. Softwareprovenanceisparticularlyimportant inacceler- atorphysics,wheremanybeampropertiescannot bemea- sureddirectlybutmustbereconstructedfromheterogeneous diagnosticdata. Manyquantitiesofscientificinterestareob- tainedonlyt...
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7c57133b-e980-48bf-bf8c-9d796a2410cb
Figure1: OverviewoftheKARAresearchstack,illustrating thepipelinefrominitialsensordataandmetadataacquisition to the persistence of algorithm execution RUNs and their visualization via the Kadi Project View. isreconstructedthroughcode,thescientificsoftwareoften evolves iteratively alongside the research questions. Sim- u...
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27b2ee11-a733-4ac4-a7dd-3d8b049d0afd
The work presented in this paper addresses this gap by extendingprovenancetrackingbeyondtraditionaldataand metadata records to individual software execution instances, hereafterdenotedasRUNs. Inthisnotation,RUNreferstoa research object representing one execution of research soft- ware. Our approach persists both the re...
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Tune,whichsendsrunmetadatadirectlytoKadi,and Kadi ProjectView ,avisualmanagementextensionfororganizing and exploring these relationships. Byintegratingthesetools,weprovideaframeworkthat isintendedtomakeresearchsoftwareatKARAastraceable and reproducible as the physical experiments themselves. KARA RESEARCH STACK During ...
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Facility (LSDF), or temporarily saved on local researcher workstations. Inthisheterogeneousenvironment,dataandmetadataare notautomaticallytransferredtoKadi. Instead,researchers decide which artifacts should be persisted in the local Kadi instance,whichisitselfconnectedtotheLSDFinfrastruc- ture. For experimental dataset...
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tion, simulation, and benchmarking, and therefore forms an essential part of the scientific workflow [ 8]. Tocapturetheprovenanceofthesecomputationalsteps, the metadata and outputs produced during individual RUNs of research software are transferred to Kadi through the BenchTunelibrary. Inthisway,eachrunbecomesatraceab...
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Project View plugin developed for Kadi, these relationships can be explored visually, allowing researchers to analyze, preserve, and communicate the evolution of a project in a more intuitive and structured way. BENCHTUNE: RUNs TELEMETRY BenchTune is a telemetry and reporting layer for C++ and Python that captures syst...
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effort. Onceenabled,itautomaticallygathersmetadatafrom the execution environment, including kernel, storage, CPU, compiler, virtualization, distribution, memory, executable information, and user-defined parameter values provided by thecodeitself. Thisallowseachexecutiontobedocumented17th International Particle Accelera...
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Figure 2: Kadi project viewcanvasexample. /vskip2mm asatraceablerunenrichedwithrelevantcomputationalcon- text. Thefollowingcode snippet showsan exampleof Bench- Tune usage in a C++ program. Listing 1: BenchTuneC++ use example. #include <BenchTuneManager.hpp> using namespace BenchTune; BenchTuneConfig cfg; cfg.name = "R...
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benchtune->add("model/parameter", model->parameter); benchtune->add("magic_number", 42); // Write file and sent to kadi (if kadi available) benchtune->close(); KADI PROJECT VIEW Kadi Project View extends the Kadi environment with an interactive visual workspace in which researchers can organize records, collections, an...
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making the evolution of datasets, record versions, and their interconnections easier to inspect and communicate. Beyond visualization, Kadi Project View also introduces analysis-oriented functionality directly into the project can- vas. Records can be enriched with attached analysis tools that expose relevant metadata ...
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class research artifacts within Kadi, through BenchTune and Kadi Project View, advances the implementation of FAIR4RSprinciplesat KARA. Toservethe broader scien- tificcommunity,futureworkwilldeeplyintegratetheProject ViewintotheKadiecosystemandexpandBenchTunetosup- port additional programming languages. ACKNOWLEDGEMENT...
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