0000000000988332

AUTHOR

Sampsa Vihonen

showing 11 related works from this author

Study of scintillation light collection, production and propagation in a 4 tonne dual-phase LArTPC

2020

The $3 \times 1 \times 1$ m$^3$ demonstrator is a dual phase liquid argon time projection chamber that has recorded cosmic rays events in 2017 at CERN. The light signal in these detectors is crucial to provide precise timing capabilities. The performances of the photon detection system, composed of five PMTs, are discussed. The collected scintillation and electroluminescence light created by passing particles has been studied in various detector conditions. In particular, the scintillation light production and propagation processes have been analyzed and compared to simulations, improving the understanding of some liquid argon properties.

photon: propagationPhotomultiplierCERN LabPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorstutkimuslaitteetPerformance of High Energy Physics DetectorPhase (waves)FOS: Physical sciencesCosmic rayNoble liquid detectors (scintillation ionization double-phase)Scintillator01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Optics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentationphysics.ins-detMathematical Physicsscintillation counterPhysicsScintillationTime projection chamberphotomultiplier010308 nuclear & particles physicsbusiness.industryhep-exDetectorScintillators scintillation and light emission processes (solid gas and liquid scintillators)Instrumentation and Detectors (physics.ins-det)time projection chamber: liquid argonNoble liquid detectors (scintillation ionization double-phase); Performance of High Energy Physics Detectors; Photon detectors for UV visible and IR photons (vacuum) (photomulti-pliers HPDs others); Scintillators scintillation and light emission processes (solid gas and liquidscintillators)Photon detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others)FIS/01 - FISICA SPERIMENTALEilmaisimetScintillation counterbusinesskosminen säteilyperformanceParticle Physics - Experiment
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EFFECTS OF BSMS ON θ23 DETERMINATION

2019

Particle Physics at the Silver Jubilee of Lomonosov Conferences
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Determination of the θ23 octant in long baseline neutrino experiments within and beyond the standard model

2018

The recent data indicate that the neutrino mixing angle $\theta_{23}$ deviates from the maximal-mixing value of 45$^\circ$, showing two nearly degenerate solutions, one in the lower octant (LO) ($\theta_{23}45^\circ$). We investigate, using numerical simulations, the prospects for determining the octant of $\theta_{23}$ in the future long baseline oscillation experiments. We present our results as contour plots on the ($\theta_{23}-45^\circ$, $\delta$)--plane, where $\delta$ is the $CP$ phase, showing the true values of $\theta_{23}$ for which the octant can be experimentally determined at 3$\,\sigma$, 2$\,\sigma$ and 1$\,\sigma$ confidence level. In particular, we study the impact of the p…

PhysicsParticle physicsneutrino oscillationsta114010308 nuclear & particles physicsPhysics beyond the Standard ModelneutrinosMonte Carlo methodsOctant (solid geometry)01 natural sciencesHigh Energy Physics - Phenomenologysterile neutrinos0103 physical sciencesCP violationNeutrinoNuclear Experiment010306 general physicsNeutrino oscillationneutrino detectorsPhysical Review
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Simulations of CERN to Pyhasalmi Neutrino Experiments with GLoBES

2014

Pitkän kantaman neutriino-oskillaatiotutkimus on siirtymässä uuteen aikaan tehokkaampien neutriinosuihkujen myötä. Viimeisimmät analyysit erilaisien neutriinokokeiden mittaustuloksista ovat rajanneet kolmen neutriinon järjestelmän oskillaatioita kuvaavan PMNS - matriisin parametriarvioita entistäkin tarkemmiksi, ja jopa θ13 > 0 -tulos on ensi kertaa todennettu reaktoridatasta. Kehitteillä olevien neutriinosuihkujen tavoitteena on saavuttaa tulevaisuudessa usean GeV:n energian mahdollistaen aiemmin ratkaisemattomien kysymysten kuten massahierarkiaongelman ja mahdollisen CP-symmetriarikon tutki- misen. Tässä tutkielmassa keskitytään LAGUNA-LBNO -hankkeessa esitettyjen LENA ja GLACIER -detekto…

neutriinotfysiikkalaskennallinen fysiikka
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Determination of the $\theta_{23}$ octant in LBNO

2014

According to the recent results of the neutrino oscillation experiment MINOS, the neutrino mixing angle $\theta_{23}$ may not be maximal ($45^{\circ}$). Two nearly degenerate solutions are possible, one in the lower octant (LO) where $\theta_{23}45^{\circ}$. Long baseline experiments measuring the $\nu_{\mu}\rightarrow\nu_{e}$ are capable of resolving this degeneracy. In this work we study the potential of the planned European LBNO experiment to distinguish between the LO and HO solutions.

PhysicsParticle physicsNeutrino Detectors and TelescopesNuclear and High Energy Physicsta114010308 nuclear & particles physicsOscillationDegenerate energy levelsHigh Energy Physics::PhenomenologyOctant (solid geometry)01 natural sciencesHigh Energy Physics - ExperimentOscillationHigh Energy Physics - PhenomenologyMINOS0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationDegeneracy (mathematics)Mixing (physics)
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A 4 tonne demonstrator for large-scale dual-phase liquid argon time projection chambers

2018

A 10 kilo-tonne dual-phase liquid argon TPC is one of the detector options considered for the Deep Underground Neutrino Experiment (DUNE). The detector technology relies on amplification of the ionisation charge in ultra-pure argon vapour and offers several advantages compared to the traditional single-phase liquid argon TPCs. A 4.2 tonne dual-phase liquid argon TPC prototype, the largest of its kind, with an active volume of \three has been constructed and operated at CERN. In this paper we describe in detail the experimental setup and detector components as well as report on the operation experience. We also present the first results on the achieved charge amplification, prompt scintillat…

Physics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorshiukkasfysiikka01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNeutrino detectorHigh Energy Physics - Experiment (hep-ex)Ionization[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Neutrino detectorsDetectors and Experimental TechniquesNuclear ExperimentInstrumentationphysics.ins-detMathematical Physicsgas: admixtureLarge Hadron ColliderDetectorneutriinotInstrumentation and Detectors (physics.ins-det)experimental equipmentneutrino: detectorNeutrino detectorTime projection chamberilmaisimettime projection chambersLarge scale cryogenic liquid detectors [8]photon: yieldParticle Physics - ExperimentperformanceMaterials scienceCERN LabTime projection chambersParticle tracking detectors (Gaseous detectors)ionization: yieldparticle tracking detectors (gaseous detectors)tutkimuslaitteetFOS: Physical scienceschemistry.chemical_elementNeutrino detectors; Particle tracking detectors (Gaseous detectors); Time projection chambersOptics0103 physical sciencesDeep Underground Neutrino Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsScintillationArgon010308 nuclear & particles physicsbusiness.industryhep-extime projection chamber: liquid argonchemistrymuon: cosmic radiationHigh Energy Physics::ExperimentbusinessTonneneutrino detectors
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Effects of triplet Higgs bosons in long baseline neutrino experiments

2018

The triplet scalars $(\Delta=\Delta^{++},\Delta^{+},\Delta^{0})$, utilized in the so-called Type-II seesaw model to explain the lightness of neutrinos, would generate nonstandard interactions (NSI) for neutrino propagating in matter. We investigate the prospects to probe these interactions in long baseline neutrino oscillation experiments. We analyze the upper bounds that the proposed DUNE experiment might set on the nonstandard parameters and numerically derive upper bounds, as function of the lightest neutrino mass, on the ratio the mass $M_\Delta$ of the triplet scalars and strength $|\lambda_\phi|$ of the coupling $\phi\phi\Delta$ of the triplet $\Delta$ and conventional Higgs doublet $…

Particle physicsVIOLATIONPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical scienceshiukkasfysiikkaComputer Science::Digital Libraries114 Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)effective field theory0103 physical sciences010306 general physicsNeutrino oscillationBosonPhysicsLEFT-RIGHT SYMMETRYneutrino oscillationsPARITYta114010308 nuclear & particles physicsHiggsin bosoniHigh Energy Physics::PhenomenologyneutriinotParity (physics)Coupling (probability)extensions of Higgs sectorHigh Energy Physics - PhenomenologyHiggsin bosonitHiggs bosonDOUBLY-CHARGED HIGGSHigh Energy Physics::ExperimentNeutrinoLepton
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Constraining the nonstandard interaction parameters in long baseline neutrino experiments

2016

In this article we investigate the prospects for probing the strength of the possible non-standard neutrino interactions (NSI) in long baseline neutrino oscillation experiments. We find that these experiments are sensitive to NSI couplings down to the level of 0.01-0.1 depending on the oscillation channel and the baseline length, as well as on the detector's fiducial mass. We also investigate the interference of the leptonic CP angle $\delta_{CP}$ with the constraining of the NSI couplings. It is found that the interference is strong in the case of the $\nu_{e}\leftrightarrow\nu_{\mu}$ and $\nu_{e}\leftrightarrow\nu_{\tau}$ transitions but not significant in other transitions. In our numeri…

Particle physicsPhysics beyond the Standard ModelFOS: Physical sciences114 Physical sciences01 natural sciencesOSCILLATION EXPERIMENTSNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)EXPERIMENT-SIMULATOR0103 physical sciencesneutrino oscillationStatistical analysisSensitivity (control systems)010306 general physicsNeutrino oscillationlong baseline experimentsPhysicsta114010308 nuclear & particles physicsOscillationHigh Energy Physics::Phenomenologynonstandard neutrino interactionsneutriino-oskillaatioHigh Energy Physics - PhenomenologyCP violationHigh Energy Physics::ExperimentATMOSPHERIC NEUTRINOSNeutrinoPhysical Review D
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Searching for neutrino oscillation parameters in long baseline experiments

2016

Vihonen, Sampsa "Searching for neutrino oscillation parameters in long baseline experiments" in Proceedings, Magellan Workshop: Connecting Neutrino Physics and Astronomy / Dahmke, Stefan K.G., Meyer, Mikko, Vanhoefer, Laura (eds.), Deutsches Elektronen-Synchrotron, DESY : 2016 ; Magellan Workshop, 2016-03-17 - 2016-03-18, Hamburg Magellan Workshop, Hamburg, Germany, 17 Mar 2016 - 18 Mar 2016 ; DESY-PROC 65-70(2016). doi:10.3204/DESY-PROC-2016-05/8

High Energy Physics - Phenomenologyneutrino oscillationsHigh Energy Physics - Phenomenology (hep-ph)Physics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::Phenomenologylong baseline neutrino experimentsFOS: Physical sciencesHigh Energy Physics::Experiment
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Determination of the θ23 octant in long baseline neutrino experiments within and beyond the standard model

2018

The recent data indicate that the neutrino mixing angle θ 23 deviates from the maximal-mixing value of 45°, showing two nearly degenerate solutions, one in the lower octant (LO) ( θ 23 4 5 ° ). We investigate, using numerical simulations, the prospects for determining the octant of θ 23 in the future long baseline oscillation experiments. We present our results as contour plots on the ( θ 23 − 4 5 ° , δ )–plane, where δ is the C P phase, showing the true values of θ 23 for which the octant can be experimentally determined at 3 σ , 2 σ and 1 σ confidence level. In particular, we study the impact of the possible nonunitarity of neutrino mixing on the experimental determination of θ 23 in thos…

Monte Carlo -menetelmätneutrino oscillationssterile neutrinosneutriinotneutrino detectors
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Optimizing the θ23 octant search in long baseline neutrino experiments

2017

Determination of the θ 23 octant will be an important goal for the next generation of neutrino oscillation experiments, as it will show whether the true value of θ 23 lies in the high octant, θ 23 > 45°, or in the low octant, θ 23 < 45°. In this work we investigate the prospects of studying the θ 23 octant in future long baseline neutrino experiments. Using the GLoBES software, we study the sensitivity to θ 23 octant in terms of baseline length and beam sharing and use the LBNO setup as our benchmark. We also show the interference on the octant determination that arises from the unconstrained CP violation angle δ CP. In our results, we show the impact of matter effects on the octant determi…

neutriinotneutrino oscillation experimentsmixing angle
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