Search results for "1420"

showing 4 items of 4 documents

New national and regional Annex I Habitat records: from #60 to #82

2023

New Italian data on the distribution of the Annex I Habitats are reported in this contribution. Specifically, 8 new occurrences in Natura 2000 sites are presented and 49 new cells are added in the EEA 10 km × 10 km reference grid. The new data refer to the Italian administrative regions of Campania, Calabria, Marche, Piedmont, Sardinia, Sicily, Tuscany and Umbria. Relevés and figures are provided as Supplementary material respectively 1 and 2.

2250*1240 1310 1420 2250* 3130 3220 3260 3270 3280 4090 6110* 6430 7210* 8210 91AA* 91B0 91E0* 92A0 92D0 933091AA*92D01310142091B03270328032607210*933031308210124032206430Settore BIO/03 - Botanica Ambientale E Applicata409091E0*6110*92A0
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Gravitational depolarization of ultracold neutrons : comparison with data

2015

We compare the expected effects of so-called gravitationally enhanced depolarization of ultracold neutrons to measurements carried out in a spin-precession chamber exposed to a variety of vertical magnetic-field gradients. In particular, we have investigated the dependence upon these field gradients of spin depolarization rates and also of shifts in the measured neutron Larmor precession frequency. We find excellent qualitative agreement, with gravitationally enhanced depolarization accounting for several previously unexplained features in the data.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsField (physics)FOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsGravitationHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]NeutronDetectors and Experimental Techniques010306 general physicsQCLarmor precessionPhysics010308 nuclear & particles physics1420DhDepolarizationInstrumentation and Detectors (physics.ins-det)Magnetic field gradient1130Ernumbers: 1340Em0755GeElectric dipole momentPhysics::Space PhysicsUltracold neutronsAtomic physics
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"Decay Phase-Space Volume of Partial Waves" of "Light isovector resonances in $\pi^- p \to \pi^-\pi^-\pi^+ p$ at 190 GeV/${\it c}$"

2018

Decay phase-space volume $I_{aa}$ for the 14 selected partial waves as a function of $m_{3\pi}$, normalized such that $I_{aa}(m_{3\pi} = 2.5~\text{GeV}/c^2) = 1$. The wave index $a$ represents the quantum numbers that uniquely define the partial wave. The quantum numbers are given by the shorthand notation $J^{PC} M^\varepsilon [$isobar$] \pi L$. We use this notation to label the decay phase-space volume in the column headers. The labels are identical to the ones used in the column headers of the table of the transition amplitudes. $I_{aa}$ is calculated using Monte Carlo integration techniques for fixed $m_{3\pi}$ values, which are given in the first column, in the range from 0.5 to 2.5 Ge…

PI- P --> PI2(2005)- PLight-Meson SpectroscopyIsobar ModelPI- P --> PI- F2(1270) PAmplitude AnalysisPI- P --> PI1(1600)- PDiffractivePI- P --> A1(1420)- PPI- P --> A1(1260)- PPI- P --> A2(1320)- PPI- P --> A1(1640)- PPI- P --> A4(2040)- PPI- P --> PI- RHO0 PPI- P --> PI- F0(980) PPI- P --> PI- PI- PI+ PPI- P --> PI2(1670)- PPI- P --> A2(1700)- PExclusivePI- P --> PI(1800)- PPI- P --> PI2(1880)- PPion-Proton Scattering
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"Transition Amplitudes" of "Light isovector resonances in $\pi^- p \to \pi^-\pi^-\pi^+ p$ at 190 GeV/${\it c}$"

2018

Real and imaginary parts of the normalized transition amplitudes $\mathcal{T}_a$ of the 14 selected partial waves in the 1100 $(m_{3\pi}, t')$ cells (see Eq. (12) in the paper). The wave index $a$ represents the quantum numbers that uniquely define the partial wave. The quantum numbers are given by the shorthand notation $J^{PC} M^\varepsilon [$isobar$] \pi L$. We use this notation to label the transition amplitudes in the column headers. The $m_{3\pi}$ values that are given in the first column correspond to the bin centers. Each of the 100 $m_{3\pi}$ bins is 20 MeV/$c^2$ wide. Since the 11 $t'$ bins are non-equidistant, the lower and upper bounds of each $t'$ bin are given in the column he…

PI- P --> PI2(2005)- PLight-Meson SpectroscopyIsobar ModelPI- P --> PI- F2(1270) PAmplitude AnalysisPI- P --> PI1(1600)- PDiffractivePartial-Wave AmplitudePI- P --> A1(1420)- PPI- P --> A1(1260)- PPI- P --> A2(1320)- PPI- P --> A1(1640)- PPI- P --> A4(2040)- PPI- P --> PI- RHO0 PPI- P --> PI- F0(980) PPI- P --> PI- PI- PI+ PPI- P --> PI2(1670)- PPI- P --> A2(1700)- PExclusive19.0PI- P --> PI(1800)- PPI- P --> PI2(1880)- PPion-Proton ScatteringAMP
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