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Materials Data on RhN by Materials Project

RhN is Molybdenum Carbide MAX Phase-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Rh3+ is bonded to six equivalent N3- atoms to form a mixture of face, edge, and corner-sharing RhN6 octahedra. The corner-sharing octahedral tilt angles are 48°. All Rh–N bond lengths are 2.18 Å. N3- is bonded to six equivalent Rh3+ atoms to form a mixture of distorted edge and corner-sharing NRh6 pentagonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on RhN by Materials Project

RhN is Halite, Rock Salt structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Rh3+ is bonded to six equivalent N3- atoms to form a mixture of corner and edge-sharing RhN6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rh–N bond lengths are 2.18 Å. N3- is bonded to six equivalent Rh3+ atoms to form a mixture of corner and edge-sharing NRh6 octahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗

Materials Data on RhN by Materials Project

RhN is Tungsten Carbide structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Rh3+ is bonded to six equivalent N3- atoms to form a mixture of distorted edge, corner, and face-sharing RhN6 pentagonal pyramids. All Rh–N bond lengths are 2.21 Å. N3- is bonded to six equivalent Rh3+ atoms to form a mixture of distorted edge, corner, and face-sharing NRh6 pentagonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on RhN by Materials Project

RhN is Zincblende, Sphalerite structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Rh3+ is bonded to four equivalent N3- atoms to form corner-sharing RhN4 tetrahedra. All Rh–N bond lengths are 2.00 Å. N3- is bonded to four equivalent Rh3+ atoms to form corner-sharing NRh4 tetrahedra.

36 MATERIALS SCIENCE↗

Gravity-improved metastability bounds for the Type-I seesaw mechanism

Right-handed neutrinos (RHN) destabilize the electroweak vacuum by increasing its decay rate. In the SM, the latter is dominated by physics at the RG scale at which λ reaches its minimum, ${\mu}_{\ast}^{\textrm{SM}}$ ~10 17 GeV. For large neutrino Yukawa coupling Y ν , RHNs can push μ* beyond the Planck scale, implying that gravitational effects need to be taken into account. In this work, we perform the first comprehensive study of electroweak vacuum metastability in the type-I seesaw mechanism including these effects. Our analysis covers both low- and high-scale seesaw models, with two as well as three RHNs and for multiple values of the Higgs’ non-minimal coupling to gravity. We find that gravitational effects can significantly stabilize the vacuum, leading to weaker metastability bounds. We show that metastability sets the strongest bounds for low-scale seesaws with M N > 1 TeV. For high-scale seesaws, we find upper bounds on the allowed masses for the RHNs, which are relevant for high-scale leptogenesis. We also point out that Tr(${Y}_{\nu}^{\dagger}$Y ν ), which is commonly used to express these metastability bounds, cannot be used for all of parameter space. Instead, we argue that bounds can always be expressed reliably through Tr(${Y}_{\nu}^{\dagger}$Y ν ${Y}_{\nu}^{\dagger}$Y ν ). Lastly, we use this insight to develop a new technique for an easier RG analysis applicable to scenarios with degenerate RHN masses.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Materials Data on PdRh(NO)10 by Materials Project

RhNPdN4(NO2)5 crystallizes in the monoclinic P2_1/m space group. The structure is zero-dimensional and consists of two azanide;palladium molecules, ten nitrous acid molecules, and two RhN clusters. In each RhN cluster, Rh4+ is bonded in a single-bond geometry to one N+1.40+ atom. The Rh–N bond length is 1.66 Å. N+1.40+ is bonded in a single-bond geometry to one Rh4+ atom.

36 MATERIALS SCIENCE↗

Massive right-handed neutrinos in $\bar{B} \to D^* τ\bar X$ decay

We explore signatures of a massive right-handed neutrino (RHN) in angular distributions of $\bar{B} \to D^* (\to D π) τ(\to πν_τ) \bar X$ decays, where $X$ is an invisible state. We assume the new physics is described by the standard model effective field theory extended with an RHN in the MeV-GeV mass range. We calculate for the first time the full differential distributions in terms of the visible final states, including the decay of the $τ$ lepton. We evaluate the sensitivity of various distributions to the new physics operators.

FOS: Physical sciences↗

Right-handed Dirac and Majorana neutrinos at Belle II

We assess the ability of the Belle II experiment to probe the Dirac or Majorana nature of a massive right-handed neutrino (RHN) N in the MeV to GeV mass range. We consider the production and decay of RHNs to proceed via new interactions described by the standard model effective field theory (SMEFT) extended with right-handed neutrino fields (SMNEFT), and not via mass mixing with active neutrinos. We find that Belle II has the potential to discover N if kinematically accessible. We perform detailed simulations of the angular distributions of lepton pairs from the decay of N produced in two-body and three-body decays of B mesons. We show that for m N above 100 MeV, Belle II can distinguish between Dirac and Majorana neutrinos at more than the 5σ CL for most operators, and the combination of the production and decay operators can be identified from the subsequent decay of the heavy neutrino. Also, the production operators can be identified using three-body B meson decay for any m N if the B → DℓN and B → D * ℓN events can be well separated.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗