A. C. König
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View article: Analyzing variability and possible trends in NDVI for urban water management: A remote-sensing approach for long term monitoring of green infrastructure
Analyzing variability and possible trends in NDVI for urban water management: A remote-sensing approach for long term monitoring of green infrastructure Open
The changing climate creates challenges for green spaces everywhere. A special case is presented by the urban tree, which has several harsh environmental conditions to deal with, i.e. compacted soil, polluted rainwater, etc. Climate adapta…
View article: FELIX-MROD, a FELIX-based data acquisition system for the ATLAS Muon Drift Tubes
FELIX-MROD, a FELIX-based data acquisition system for the ATLAS Muon Drift Tubes Open
The ATLAS Muon Drift Tube (MDT) ReadOut Drivers (MROD), 204 VME modules that are an essential part of the readout chain of the 1,150 MDT chambers, have been in operation for more than 15 years and are expected to remain in operation until …
View article: Subgroup A : nuclear model codes report to the Sixteenth Meeting of the WPEC
Subgroup A : nuclear model codes report to the Sixteenth Meeting of the WPEC Open
The Subgroup A activities focus on the development of nuclear reaction models and codes, used in evaluation work for nuclear reactions from the unresolved energy region up to the pion threshold production limit, and for target nuclides fro…
View article: Erratum 2: Search for the HH → bb¯¯bb¯¯process via vector-boson fusion production using proton-proton collisions at √s eV with the ATLAS detector
Erratum 2: Search for the HH → bb¯¯bb¯¯process via vector-boson fusion production using proton-proton collisions at √s eV with the ATLAS detector Open
Contains fulltext : 234123.pdf (Publisher’s version ) (Open Access)
View article: Measurements of the Higgs boson inclusive and differential fiducial cross sections in the 4$\ell$ decay channel at $\sqrt{s}$ = 13 TeV
Measurements of the Higgs boson inclusive and differential fiducial cross sections in the 4$\ell$ decay channel at $\sqrt{s}$ = 13 TeV Open
Inclusive and differential fiducial cross sections of the Higgs boson are measured in the $H \to ZZ \to 4l$ ($l$ = $e$;$\mu$) decay channel. The results are based on proton-proton collision data produced at the Large Hadron Collider at a c…
View article: Search for supersymmetry in final states with two same-sign or three leptons and jets using 36 fb(-1) of √s = 13 TeV pp collision data with the ATLAS detector (vol 09, 084, 2017)
Search for supersymmetry in final states with two same-sign or three leptons and jets using 36 fb(-1) of √s = 13 TeV pp collision data with the ATLAS detector (vol 09, 084, 2017) Open
Contains fulltext : 207596.pdf (Publisher’s version ) (Open Access)
View article: Search for the X (5568) State Decaying into B[superscript 0][subscript s] π[superscript ±] in Proton-Proton Collisions at √ s = 8 TeV
Search for the X (5568) State Decaying into B[superscript 0][subscript s] π[superscript ±] in Proton-Proton Collisions at √ s = 8 TeV Open
A search for resonancelike structures in the B[subscript s][superscript 0] π[superscript ±] invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at √s =8 TeV, corresponding to a…
View article: Measurement of quarkonium production cross sections in pp collisions at √s =13 TeV
Measurement of quarkonium production cross sections in pp collisions at √s =13 TeV Open
SEIDI, CPAN, PCTI and FEDER (Spain); Individuals have received support from the Marie-Curie program and the European Research Council and Horizon 2020 Grant, contract No. 675440 (European Union); the Programa Severo Ochoa del Principado de…
View article: Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton–proton collisions at √s =13 TeV
Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton–proton collisions at √s =13 TeV Open
A search for the production of Higgs boson pairs in proton–proton collisions at a centre-of-mass energy of 13 TeV is presented, using a data sample corresponding to an integrated luminosity of 35.9 fb$^{-1}$ collected with the CMS detector…
View article: Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV
Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV Open
In the original paper, figure 10 was incorrect. The correct figure is shown below.
\nAdditionally, the unparticle entries in table 3, as well as figure 4 and 5 were labelled with
\nincorrect values of ΛU. The entries correctly correspond t…
View article: Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at $$\sqrt{s}= 13\,\text{TeV} $$ s = 13 TeV
Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at $$\sqrt{s}= 13\,\text{TeV} $$ s = 13 TeV Open
A search is presented for an excess of events with heavy-flavor quark pairs ( ${t}\overline{{t}} $ and ${b} \overline{{b}} $ ) and a large imbalance in transverse momentum in data from proton–proton collisions at a center-of-mass energy of…
View article: Erratum to: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV
Erratum to: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV Open
In the original paper, figure 10 was incorrect. The correct figure is shown above.
View article: Exclusive and semi-exclusive pi+pi- production in proton-proton collisions at sqrt(s) = 7 TeV
Exclusive and semi-exclusive pi+pi- production in proton-proton collisions at sqrt(s) = 7 TeV Open
A measurement is presented of the exclusive and semi-exclusive production of charged pion pairs in proton-proton collisions, pp to p(p*) + pi+pi- + p(p*) here the pi+pi- pair is emitted at central rapidities, and the scattered protons stay…