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(Rb)3Cd is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is zero-dimensional and consists of one cadmium molecule and three rubidium molecules.
(Rb)3Cr is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is zero-dimensional and consists of one chromium molecule and three rubidium molecules.
(Rb)3Cd crystallizes in the tetragonal I4/mmm space group. The structure is zero-dimensional and consists of two cadmium molecules and six rubidium molecules.
RbK2As is Cyanogen Chloride-like structured and crystallizes in the orthorhombic Immm space group. The structure is zero-dimensional and consists of two rubidium molecules and two K2As clusters. In each K2As cluster, K1+ is bonded in a single-bond geometry to one As3- atom. The K–As bond length is 3.16 Å. As3- is bonded in a linear geometry to two equivalent K1+ atoms.
(Rb)2RbPrCl6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight rubidium molecules and one RbPrCl6 framework. In the RbPrCl6 framework, Rb1+ is bonded to six equivalent Cl1- atoms to form RbCl6 octahedra that share corners with six equivalent PrCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–Cl bond lengths are 3.12 Å. Pr3+ is bonded to six equivalent Cl1- atoms to form PrCl6 octahedra that share corners with six equivalent RbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pr–Cl bond lengths are 2.75 Å. Cl1- is bonded in a linear geometry to one Rb1+ and one Pr3+ atom.
(Rb)3Cr crystallizes in the tetragonal I4/mmm space group. The structure is zero-dimensional and consists of two chromium molecules and six rubidium molecules.
(Rb)2AuTaF6 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is zero-dimensional and consists of four gold molecules, eight rubidium molecules, and four TaF6 clusters. In each TaF6 cluster, Ta5+ is bonded in an octahedral geometry to six equivalent F1- atoms. All Ta–F bond lengths are 1.92 Å. F1- is bonded in a single-bond geometry to one Ta5+ atom.
(Rb)2CsDyCl6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight rubidium molecules and one CsDyCl6 framework. In the CsDyCl6 framework, Cs1+ is bonded to six equivalent Cl1- atoms to form CsCl6 octahedra that share corners with six equivalent DyCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Cl bond lengths are 3.26 Å. Dy3+ is bonded to six equivalent Cl1- atoms to form DyCl6 octahedra that share corners with six equivalent CsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Dy–Cl bond lengths are 2.64 Å. Cl1- is bonded in a linear geometry to one Cs1+ and one Dy3+ atom.
RbRb6NaSi8 crystallizes in the cubic Pa-3 space group. The structure is three-dimensional and consists of four rubidium molecules and one Rb6NaSi8 framework. In the Rb6NaSi8 framework, Rb1+ is bonded in a 6-coordinate geometry to six Si1- atoms. There are a spread of Rb–Si bond distances ranging from 3.54–3.82 Å. Na1+ is bonded in a 6-coordinate geometry to six equivalent Si1- atoms. All Na–Si bond lengths are 2.96 Å. There are two inequivalent Si1- sites. In the first Si1- site, Si1- is bonded in a 9-coordinate geometry to six equivalent Rb1+ and three equivalent Si1- atoms. All Si–Si bond lengths are 2.42 Å. In the second Si1- site, Si1- is bonded in a 1-coordinate geometry to four equivalent Rb1+, one Na1+, and three Si1- atoms. Both Si–Si bond lengths are 2.48 Å.
RbCs2Sb is Cyanogen Chloride-like structured and crystallizes in the orthorhombic Immm space group. The structure is zero-dimensional and consists of two antimony;cesium molecules and two rubidium molecules.
(Rb)2CsGaI6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight rubidium molecules and one CsGaI6 framework. In the CsGaI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent GaI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.59 Å. Ga3+ is bonded to six equivalent I1- atoms to form GaI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ga–I bond lengths are 2.81 Å. I1- is bonded in a linear geometry to one Cs1+ and one Ga3+ atom.
(Rb)2RbLaCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight rubidium molecules and one RbLaCl6 framework. In the RbLaCl6 framework, Rb1+ is bonded to six equivalent Cl1- atoms to form RbCl6 octahedra that share corners with six equivalent LaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–Cl bond lengths are 3.13 Å. La3+ is bonded to six equivalent Cl1- atoms to form LaCl6 octahedra that share corners with six equivalent RbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All La–Cl bond lengths are 2.77 Å. Cl1- is bonded in a linear geometry to one Rb1+ and one La3+ atom.
RbFe2AlF2 crystallizes in the tetragonal P4/mbm space group. The structure is two-dimensional and consists of two rubidium molecules and one Fe2AlF2 sheet oriented in the (0, 0, 1) direction. In the Fe2AlF2 sheet, Fe is bonded in a distorted linear geometry to two equivalent Al atoms. Both Fe–Al bond lengths are 2.47 Å. Al is bonded in a linear geometry to four equivalent Fe and two equivalent F atoms. Both Al–F bond lengths are 1.83 Å. F is bonded in a single-bond geometry to one Al atom.
(Rb)2CsYBr6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight rubidium molecules and one CsYBr6 framework. In the CsYBr6 framework, Cs1+ is bonded to six equivalent Br1- atoms to form CsBr6 octahedra that share corners with six equivalent YBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Br bond lengths are 3.41 Å. Y3+ is bonded to six equivalent Br1- atoms to form YBr6 octahedra that share corners with six equivalent CsBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Y–Br bond lengths are 2.80 Å. Br1- is bonded in a linear geometry to one Cs1+ and one Y3+ atom.
(Rb)2CsYCl6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight rubidium molecules and one CsYCl6 framework. In the CsYCl6 framework, Cs1+ is bonded to six equivalent Cl1- atoms to form CsCl6 octahedra that share corners with six equivalent YCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Cl bond lengths are 3.26 Å. Y3+ is bonded to six equivalent Cl1- atoms to form YCl6 octahedra that share corners with six equivalent CsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Y–Cl bond lengths are 2.64 Å. Cl1- is bonded in a linear geometry to one Cs1+ and one Y3+ atom.
(Rb2O2)2N2(O2)2 crystallizes in the orthorhombic Pmma space group. The structure is zero-dimensional and consists of two ammonia molecules, two hydrogen peroxide molecules, and four rubidium hydroxide molecules.
Rb is alpha structured and crystallizes in the cubic I-43m space group. The structure is three-dimensional and consists of two rubidium molecules and one Rb framework. In the Rb framework, there are three inequivalent Rb sites. In the first Rb site, Rb is bonded in a trigonal non-coplanar geometry to three equivalent Rb atoms. All Rb–Rb bond lengths are 4.89 Å. In the second Rb site, Rb is bonded in a 12-coordinate geometry to eight Rb atoms. There are a spread of Rb–Rb bond distances ranging from 4.67–5.11 Å. In the third Rb site, Rb is bonded in a 6-coordinate geometry to eight Rb atoms. There are one shorter (4.49 Å) and two longer (4.66 Å) Rb–Rb bond lengths.
The AWAKE facility uses novel proton beam-driven plasma wakefields to accelerate electron bunches over 10m of Rubidium plasma. Precise monitoring of 2 diverse beam types necessitates an electron beam position monitor (BPM) working in a frequency regime of tens of GHz. A high frequency conical button-style BPM with a working regime of up to 40 GHz has been investigated as a way to discriminate the electromagnetic fields of 19 MeV, 4 ps electron bunches propagating spatially and temporally together with a 400 GeV, 170 ps proton bunch in the AWAKE common beamline. The sensitivity of the HF BPM to the electron beam position is determined under various beam conditions, with both electrons and protons, and integration with a TRIUMF front-end is discussed.