about
The murchison widefield array 21 cm power spectrum analysis methodologyPattern recognition and PID for COMPASS RICH-1Collins and Sivers asymmetries in muonproduction of pions and kaons off transversely polarised protonsQ27021140Interplay among transversity induced asymmetries in hadron leptoproductionCryogenic Si detectors for ultra radiation hardness in SLHC environmentCharge collection efficiency of irradiated silicon detector operated at cryogenic temperaturesA Superconducting Magnet UCN Trap for Precise Neutron Lifetime Measurements.A magnetically shielded room with ultra low residual field and gradient.A positron emission tomograph based on LSO-APD modules with a sampling ADC read-out system for a students' advanced laboratory course.Evidence for Isospin Violation and Measurement of CP Asymmetries in B→K^{*}(892)γ.Energy Scan of the e^{+}e^{-}→h_{b}(nP)π^{+}π^{-} (n=1, 2) Cross Sections and Evidence for ϒ(11020) Decays into Charged Bottomoniumlike States.Observation of the Decay B_{s}^{0}→K^{0}K[over ¯]^{0}.Observation of a New Narrow Axial-Vector Meson a1(1420).Lepton-Flavor-Dependent Angular Analysis of B→K^{*}ℓ^{+}ℓ^{-}.Measurement of the charged-pion polarizability.Observation of D^{0}→ρ^{0}γ and Search for CP Violation in Radiative Charm Decays.Measurement of the τ Lepton Polarization and R(D^{*}) in the Decay B[over ¯]→D^{*}τ^{-}ν[over ¯]_{τ}.Observation of excited Ωc charmed baryons in e+e− collisionsThe puzzle of neutron lifetimeConcepts of UCN sources for the FRM-IITechnical design report for the P̄ ANDA (AntiProton Annihilations at Darmstadt) Straw Tube TrackerExperimental access to Transition Distribution Amplitudes with the P̄ANDA experiment at FAIRDevelopment of cryogenic Si detectors by CERN RD39 Collaboration for ultra radiation hardness in SLHC environmentLow-temperature tracking detectorsRecent results from the CERN RD39 Collaboration on super-radiation hard cryogenic silicon detectors for LHC and LHC upgradeThe effect of charge collection recovery in silicon p–n junction detectors irradiated by different particlesRadiation hardness of cryogenic silicon detectorsSilicon detectors irradiated “in situ” at cryogenic temperaturesCharge collection efficiency of an irradiated cryogenic double-p silicon detectorCryogenic technology for tracking detectorsReview on the development of cryogenic silicon detectorsFirst limits on the 21 cm power spectrum during the Epoch of X-ray heatingEmpirical covariance modeling for 21 cm power spectrum estimation: A method demonstration and new limits from early Murchison Widefield Array 128-tile dataπ0decay process ofCΛ12andBΛ11hypernucleiΛ 4 H formation from K− absorption at rest on4He,7Li,9Be,12C,16O and40Ca targetsformation from K− absorption at rest on4He,7Li,9Be,12C,16O and40Ca targetsA measurement of the π0 decay of Λ 12 C and Λ 11 B hypernucleihypernucleiFormation ofHΛ4hypernuclei fromK−absorption at rest on light nucleiMeasurement of time-dependent CP asymmetries in B0→KS0ηγ decaysObservation of $$\Xi _{c}(2930)^0$$Ξc(2930)0 and updated measurement of $$B^{-} \rightarrow K^{-} \Lambda _{c}^{+} \bar{\Lambda }_{c}^{-}$$B-→K-Λc+Λ¯c- at Belle
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Q27011594-FFFC5935-2CA6-4A37-AC6C-0814F95FCD2EQ27020348-2FF9885A-9668-4B44-A8FC-A9429F7B42A9Q27020894-607D6924-2F6C-4A17-A230-4BCBEE6F471CQ27021140-1329786C-E789-4FE5-BD8A-6D21491CAFFFQ27021294-1FA5E9C1-983A-438C-87E0-D8112D3036F5Q29038278-B20FE69C-C554-466B-9945-72A2861F8B4BQ29040025-8FF79897-6495-4A32-9E5F-A0BF04798BBAQ36857193-FB263A1A-989B-4B2A-BE42-F1DDA57C55E0Q39149771-244B0665-C98C-4FE9-9A91-712A3CEEDB70Q40004007-3B8B6AEC-10AC-4127-9792-CFB9FA0C230CQ50012540-E71C09E1-F413-43BF-ADAC-D75FBCC2E737Q50571336-1B955223-F05E-46F9-9012-A2BD82538FDCQ50651393-2C004D6F-539D-45FF-B6C2-9B38A107D3A0Q50859185-81997F55-5543-4F8C-8CD4-B3CED88595A2Q50935462-2A4F9EA2-A500-4917-B1CA-700D2B3D3332Q50954145-7FEAC875-1184-41CC-BD9D-711CDA27AE2EQ51000011-CE0356E7-BEA1-484E-9913-F0956060D167Q53233311-93CD0F60-EE2A-46E4-B41D-5C03ED42151AQ55950579-1E65B8AD-124B-4C5A-8CBD-3131B8186038Q56621186-5C339BBD-25FC-4F5B-9D09-36E0F194F107Q56637693-36A52774-F1A8-4DFE-8E94-68502F60F78AQ56947584-2A592A34-B6F1-4FDA-8082-A7870301B182Q57539479-4F649A5D-DDCE-4443-873D-AAFFE0C6DDB6Q57723961-BEA35FAD-EB8F-4A4B-BFFF-B450A333B3B2Q57724046-F7198ECB-50AD-4F0B-8168-689A3D8D8CFEQ57724050-B2E683D1-ECCC-4D1F-B0B0-8A245CB41238Q57724063-C71EAA8F-8AEE-49A8-A780-5237D8076914Q57724077-4F2974FB-9ED2-4DCF-902D-8EF36EAF7228Q57724078-6AF3CB71-EF92-447E-B7EB-182912B2B101Q57724085-7A81DC90-9C13-480F-9FAE-55C6CD8D3306Q57724087-37D8CFB4-957C-476E-B59C-02D4B5AB2C2AQ57724089-BC84A8D0-8B74-42CD-88E1-06BB8E483F80Q57807582-2D1BD7EE-ED7E-48EE-99FA-606C6464C7C3Q57817272-E8820C66-1863-44BD-AEE6-59817CF6E849Q57841058-C533532A-FE6F-4A93-8747-6918D11A835BQ57841076-809B0535-EA32-415F-A2AB-4BECD80ABC96Q57841077-332E1279-D3C7-4409-B0D7-4A49141B8631Q57841082-CB23E4EE-D627-4BB4-95EA-0E2DD7B8D629Q58030798-E7FA4B65-872C-44B7-9C6C-1D67F6CDFF25Q58030801-2D1451F7-1E81-4684-9F55-67E9A387DBE3
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description
onderzoeker
@nl
researcher ORCID id 0000-0002-8813-0437
@en
name
S. Paul
@nl
Stephan Paul
@en
Stephan Paul
@es
type
label
S. Paul
@nl
Stephan Paul
@en
Stephan Paul
@es
altLabel
S. Paul
@en
prefLabel
S. Paul
@nl
Stephan Paul
@en
Stephan Paul
@es
P108
P106
P21
P2456
196/9942-2
P31
P496
0000-0002-8813-0437