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At least 1,045 records · Page 58

Precise Modeling of a Complex Solenoidal Magnetic Field Using a Combination of Analytic Functions and a PINN

We demonstrate an iterative approach to modeling a sparsely measured magnetic field in a large-bore solenoid. This approach uses a hybrid of traditional and machine learning techniques. The traditional technique is a linear least-squares fit using a series solution to Laplace's equation, while the machine learning technique involves the training of a physics-informed neural network (PINN) on the least-squares fit residuals. We use a newly defined activation function "DELTAsnake," a modification to the snake activation function proposed by Ziyin et al. that allows for stronger curvature and non-monotonicity. The combined model approximately obeys Maxwell's equations to a level sufficient for producing high quality physics simulations and analysis. Our approach is applied to a highly realistic calculation of the expected magnetic field in the Mu2e experiment's Detector Solenoid which includes a simple model for the expected statistical measurement uncertainties. Using ten toy measurement simulations, we demonstrate the capabilities of our model in comparison to the least-squares method alone; the least-squares method alone results in a reduced chi-squared statistic of ${2.15 \pm 0.01}$, while our approach improves the reduced chi-square to ${1.034 \pm 0.005}$. Furthermore, for an average toy simulation, we show that the range of the RMS of the three field component residuals reduces from ${0.07-0.37}$ Gauss to ${0.05-0.07}$ Gauss. We find that this novel method is robust against a realistic systematic uncertainty deriving from Hall probe calibration bias and can be used to significantly reduce the number of measurements required to achieve an accurate model.

Kampa, Cole [Caltech] (ORCID:0000000192972920)↗

Reaching For New Physics With MeV-scale Reconstruction In The MicroBooNE LArTPC Neutrino Detector

Large neutrino liquid argon time projection chamber (LArTPC) experiments can broaden their physics reach by reconstructing MeV-Scale energy depositions, or blips, in their data. We demonstrate new calorimetric and particle discrimination capabilities at the MeV scale using reconstructed blips in MicroBooNE LArTPC data at Fermilab. A concentration of low-energy ($<$3 MeV) blips is observed around fiberglass mechanical support struts along the TPC edges, with spectral features consistent with the Compton edge of the 2.614 MeV $^{208}$Tl decay $\gamma$ ray. With these features we perform the electron energy scale calibration to few-percent precision and yield the specific activity of $^{208}$Tl in the struts, $(11.7 \pm 0.2 \text{(stat)} \pm 2.8 \text{(syst)})$ Bq/kg. Using cosmogenic blips above 3 MeV, we demonstrate the ability of large LArTPCs to discriminate low-energy proton and electron depositions. An enriched low-energy proton sample selected with this technique is smaller in data than in dedicated CORSIKA simulations, pointing to possible mismodeling in CORSIKA incident cosmic fluxes or Geant4 particle transport. These methods are applied to MicroBooNE's inclusive single-photon search, which reported a 2.2$\sigma$ excess below 600 MeV in shower energy for events with no reconstructed protons. By identifying and classifying blips near single-photon events selected by the WireCell reconstruction framework, a more comprehensive labeling of nearby hadronic activity is established: blips upstream of the shower axis indicate previously unidentified final-state protons, while elevated blip counts at wide angles signal final-state neutrons. Taken together with MiniBooNE's long-standing low-energy excess (LEE) and MicroBooNE electron-like and sterile neutrino searches disfavored as possible explanations of the MiniBooNE anomaly, this analysis motivates an expanded exploration of the single-photon channel in Fermilab's short-baseline LArTPC program. This thesis documents the current status of this enhanced analysis, which will form a key part of MicroBooNE's final low-energy-excess results.

Andrade Aldana, Diego Armando [IIT, Chicago (main)↗

Materials Data on PmF3 by Materials Project

PmF3 is alpha bismuth trifluoride structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Pm3+ is bonded to twelve F1- atoms to form a mixture of edge, corner, and face-sharing PmF12 cuboctahedra. There are eight shorter (2.50 Å) and four longer (2.66 Å) Pm–F bond lengths. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded to four equivalent Pm3+ atoms to form a mixture of distorted edge and corner-sharing FPm4 tetrahedra. In the second F1- site, F1- is bonded in a distorted square co-planar geometry to four equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on PmH3 by Materials Project

PmH3 is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pm3+ is bonded in a distorted body-centered cubic geometry to fourteen H1- atoms. There are eight shorter (2.32 Å) and six longer (2.68 Å) Pm–H bond lengths. There are two inequivalent H1- sites. In the first H1- site, H1- is bonded to four equivalent Pm3+ atoms to form HPm4 tetrahedra that share corners with twelve equivalent HPm6 octahedra, corners with sixteen equivalent HPm4 tetrahedra, edges with six equivalent HPm4 tetrahedra, and faces with four equivalent HPm6 octahedra. The corner-sharing octahedral tilt angles are 55°. In the second H1- site, H1- is bonded to six equivalent Pm3+ atoms to form HPm6 octahedra that share corners with six equivalent HPm6 octahedra, corners with twenty-four equivalent HPm4 tetrahedra, edges with twelve equivalent HPm6 octahedra, and faces with eight equivalent HPm4 tetrahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗

Materials Data on PmInPt2 by Materials Project

PmPt2In is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pm3+ is bonded in a body-centered cubic geometry to eight equivalent Pt2- atoms. All Pm–Pt bond lengths are 3.00 Å. Pt2- is bonded in a body-centered cubic geometry to four equivalent Pm3+ and four equivalent In1+ atoms. All Pt–In bond lengths are 3.00 Å. In1+ is bonded in a body-centered cubic geometry to eight equivalent Pt2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on NaPmTe2 by Materials Project

NaPmTe2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Na1+ is bonded in a body-centered cubic geometry to eight equivalent Te2- atoms. All Na–Te bond lengths are 3.37 Å. Pm3+ is bonded in a body-centered cubic geometry to eight equivalent Te2- atoms. All Pm–Te bond lengths are 3.37 Å. Te2- is bonded in a body-centered cubic geometry to four equivalent Na1+ and four equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on PmTlTe2 by Materials Project

PmTlTe2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pm3+ is bonded in a body-centered cubic geometry to eight equivalent Te2- atoms. All Pm–Te bond lengths are 3.43 Å. Tl1+ is bonded in a body-centered cubic geometry to eight equivalent Te2- atoms. All Tl–Te bond lengths are 3.43 Å. Te2- is bonded in a body-centered cubic geometry to four equivalent Pm3+ and four equivalent Tl1+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on PmB3 by Materials Project

PmB3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pm3+ is bonded in a 12-coordinate geometry to twelve equivalent B1- atoms. There are six shorter (2.78 Å) and six longer (2.85 Å) Pm–B bond lengths. B1- is bonded in a 10-coordinate geometry to four equivalent Pm3+ and six equivalent B1- atoms. There is two shorter (1.79 Å) and four longer (2.01 Å) B–B bond length.

36 MATERIALS SCIENCE↗

Materials Data on PmAu3 by Materials Project

PmAu3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pm3+ is bonded to twelve equivalent Au1- atoms to form a mixture of corner and face-sharing PmAu12 cuboctahedra. There are six shorter (3.12 Å) and six longer (3.22 Å) Pm–Au bond lengths. Au1- is bonded in a distorted rectangular see-saw-like geometry to four equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on PmBr3 by Materials Project

PmBr3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two PmBr3 ribbons oriented in the (0, 0, 1) direction. Pm3+ is bonded to six equivalent Br1- atoms to form distorted face-sharing PmBr6 pentagonal pyramids. All Pm–Br bond lengths are 2.90 Å. Br1- is bonded in an L-shaped geometry to two equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on PmCl3 by Materials Project

PmCl3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two PmCl3 ribbons oriented in the (0, 0, 1) direction. Pm3+ is bonded to six equivalent Cl1- atoms to form distorted face-sharing PmCl6 pentagonal pyramids. All Pm–Cl bond lengths are 2.75 Å. Cl1- is bonded in an L-shaped geometry to two equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on PmI3 by Materials Project

PmI3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two PmI3 ribbons oriented in the (0, 0, 1) direction. Pm3+ is bonded to six equivalent I1- atoms to form distorted face-sharing PmI6 pentagonal pyramids. All Pm–I bond lengths are 3.13 Å. I1- is bonded in an L-shaped geometry to two equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pm2O3 by Materials Project

Pm2O3 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. Pm3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Pm–O bond distances ranging from 2.30–2.67 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Pm3+ atoms to form OPm4 tetrahedra that share corners with six equivalent OPm6 octahedra, corners with six equivalent OPm4 tetrahedra, edges with three equivalent OPm6 octahedra, and edges with three equivalent OPm4 tetrahedra. The corner-sharing octahedra tilt angles range from 18–56°. In the second O2- site, O2- is bonded to six equivalent Pm3+ atoms to form OPm6 octahedra that share corners with twelve equivalent OPm4 tetrahedra, edges with six equivalent OPm6 octahedra, and edges with six equivalent OPm4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on PmN by Materials Project

PmN is Halite, Rock Salt structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pm3+ is bonded to six equivalent N3- atoms to form a mixture of edge and corner-sharing PmN6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pm–N bond lengths are 2.56 Å. N3- is bonded to six equivalent Pm3+ atoms to form a mixture of edge and corner-sharing NPm6 octahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗

Materials Data on PmSe2 by Materials Project

PmSe2 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. Pm3+ is bonded in a 9-coordinate geometry to nine Se+1.50- atoms. There are a spread of Pm–Se bond distances ranging from 3.04–3.13 Å. There are two inequivalent Se+1.50- sites. In the first Se+1.50- site, Se+1.50- is bonded in a 8-coordinate geometry to four equivalent Pm3+ and four equivalent Se+1.50- atoms. All Se–Se bond lengths are 2.93 Å. In the second Se+1.50- site, Se+1.50- is bonded to five equivalent Pm3+ atoms to form a mixture of distorted edge and corner-sharing SePm5 trigonal bipyramids.

36 MATERIALS SCIENCE↗

Materials Data on PmS2 by Materials Project

PmS2 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. Pm3+ is bonded in a 9-coordinate geometry to nine S+1.50- atoms. There are a spread of Pm–S bond distances ranging from 2.89–2.99 Å. There are two inequivalent S+1.50- sites. In the first S+1.50- site, S+1.50- is bonded in a 8-coordinate geometry to four equivalent Pm3+ and four equivalent S+1.50- atoms. All S–S bond lengths are 2.79 Å. In the second S+1.50- site, S+1.50- is bonded to five equivalent Pm3+ atoms to form a mixture of distorted edge and corner-sharing SPm5 trigonal bipyramids.

36 MATERIALS SCIENCE↗

Materials Data on PmAs3 by Materials Project

PmAs3 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Pm3+ is bonded to twelve As1- atoms to form a mixture of corner, edge, and face-sharing PmAs12 cuboctahedra. There are four shorter (2.94 Å) and eight longer (3.26 Å) Pm–As bond lengths. There are two inequivalent As1- sites. In the first As1- site, As1- is bonded in a 8-coordinate geometry to four equivalent Pm3+ and four equivalent As1- atoms. All As–As bond lengths are 2.94 Å. In the second As1- site, As1- is bonded in a square co-planar geometry to four equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pm2MgS4 by Materials Project

MgPm2S4 crystallizes in the tetragonal I-42d space group. The structure is three-dimensional. Mg2+ is bonded in a 4-coordinate geometry to eight equivalent S2- atoms. There are four shorter (2.63 Å) and four longer (3.21 Å) Mg–S bond lengths. Pm3+ is bonded in a 8-coordinate geometry to eight equivalent S2- atoms. There are a spread of Pm–S bond distances ranging from 2.76–3.19 Å. S2- is bonded in a 6-coordinate geometry to two equivalent Mg2+ and four equivalent Pm3+ atoms.

36 MATERIALS SCIENCE↗