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At least 235 records · Page 13

Cluster Dynamics Simulations of Intra-Granular Fission Gas Bubble Size and Pressure Evolution in UO 2

Fission gases such as xenon (Xe) play a critical role in determining the behavior and response of nuclear fuel. Given that Xe has little solubility in UO 2 , it accumulates and forms bubbles, which significantly impact fuel performance. Intra- and inter-granular bubble nucleation and growth can lead to fuel swelling, and once bubbles interconnect at grain boundaries, fission gas can be released into the plenum. At low temperatures, limited uranium vacancy mobility can restrict swelling, therefore causing the bubbles to become highly pressurized. Consequently, this can induce micro-cracking, promote fission gas release (increasing the likelihood of cladding failure), and even lead to fuel pulverization under accident conditions such as a loss of coolant accident. As bubble evolution is strongly influenced by local temperature and fission rate, markedly different behavior occurs across the radial profile of the fuel pellet. Capturing the mechanisms that underpin bubble evolution is therefore important to predict these behaviors in the fuel. Previous models describing important mechanisms informed by lower length scale simulations have been developed under the NEAMS program. These can describe the evolution of a single bubble type (i.e., single value for radius and pressure) at each position in the pellet, for instance using the Centipede cluster dynamic code. However, in reality, a full distribution in bubble sizes and pressures exists within the microstructure at a given position in the pellet. To address this the cluster dynamics code Xolotl, which can predict Xe and vacancy phase space (i.e., bubble distributions) for intra-granular bubbles, has been used before. Prior work benchmarked the Xolotl code against the Centipede cluster dynamics code to ensure compatibility and to verify that mobile defect properties are adequately transferred between the two codes, along with some physics improvements. In this work, we go further by introducing a physics-based set of improvements that will allow us to accurately predict bubble size distributions and internal bubble pressures under representative UO 2 irradiation conditions. The improvements include (i) coupling bubble-defect reaction energies to a virial equation of state (EOS), (ii) including a bubble surface tension contribution, (iii) incorporating radiation-induced re-solution of Xe and vacancies, (iv) enabling pressure-driven dislocation loop punching through an effective emission of interstitial clusters informed by interstitial loop energetics, (v) accounting for radiation induced athermal diffusion of Xe, and (vi) implementing a Booth-type grain boundary sink representation for all mobile defects and defect clusters. After these modifications, we observe good agreement of Xolotl fission gas bubble size and concentration predictions with legacy experimental measurements. Additionally, it allows the distribution of Xe bubble pressures and radius to also be predicted and compared to data produced through the Advanced Fuels Campaign (AFC) program. Here, we have done this by running simulations under conditions similar to the AFC post-irradiation examination (PIE) samples irradiated at North Anna 2 light water reactor (LWR). Our results shows excellent agreement with these experimental measurements.

11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS↗

Materials Data on CsXeF7 by Materials Project

XeCsF7 crystallizes in the cubic P2_13 space group. The structure is three-dimensional. Xe is bonded in a 7-coordinate geometry to seven F atoms. There are a spread of Xe–F bond distances ranging from 2.06–2.14 Å. Cs is bonded in a 9-coordinate geometry to fifteen F atoms. There are a spread of Cs–F bond distances ranging from 3.19–3.59 Å. There are three inequivalent F sites. In the first F site, F is bonded in a distorted single-bond geometry to one Xe and two equivalent Cs atoms. In the second F site, F is bonded in a distorted single-bond geometry to one Xe and two equivalent Cs atoms. In the third F site, F is bonded in a distorted single-bond geometry to one Xe and three equivalent Cs atoms.

36 MATERIALS SCIENCE↗

Materials Data on AsSXeNF10 by Materials Project

XeNSF4AsF6 crystallizes in the orthorhombic Pbca space group. The structure is zero-dimensional and consists of eight AsF6 clusters and eight XeNSF4 clusters. In each AsF6 cluster, As is bonded in an octahedral geometry to six F atoms. There is three shorter (1.77 Å) and three longer (1.78 Å) As–F bond length. There are six inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one As atom. In the second F site, F is bonded in a single-bond geometry to one As atom. In the third F site, F is bonded in a single-bond geometry to one As atom. In the fourth F site, F is bonded in a single-bond geometry to one As atom. In the fifth F site, F is bonded in a single-bond geometry to one As atom. In the sixth F site, F is bonded in a single-bond geometry to one As atom. In each XeNSF4 cluster, Xe is bonded in a linear geometry to one N and one F atom. The Xe–N bond length is 2.27 Å. The Xe–F bond length is 2.02 Å. N is bonded in a distorted bent 150 degrees geometry to one Xe and one S atom. The N–S bond length is 1.43 Å. S is bonded in a distorted tetrahedral geometry to one N and three F atoms. All S–F bond lengths are 1.54 Å. There are four inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one S atom. In the second F site, F is bonded in a single-bond geometry to one S atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom. In the fourth F site, F is bonded in a single-bond geometry to one S atom.

36 MATERIALS SCIENCE↗

Materials Data on Te2Xe(OF5)2 by Materials Project

Xe(OTeF5)2 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four Xe(OTeF5)2 clusters. Xe is bonded in a linear geometry to two equivalent O atoms. Both Xe–O bond lengths are 2.19 Å. Te is bonded in an octahedral geometry to one O and five F atoms. The Te–O bond length is 1.91 Å. There are a spread of Te–F bond distances ranging from 1.87–1.89 Å. O is bonded in a bent 120 degrees geometry to one Xe and one Te atom. There are five inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Te atom. In the second F site, F is bonded in a single-bond geometry to one Te atom. In the third F site, F is bonded in a single-bond geometry to one Te atom. In the fourth F site, F is bonded in a single-bond geometry to one Te atom. In the fifth F site, F is bonded in a single-bond geometry to one Te atom.

36 MATERIALS SCIENCE↗

Materials Data on S2XeNO4F3 by Materials Project

XeNS2O4F3 is alpha-like structured and crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four XeNS2O4F3 clusters. Xe is bonded in a linear geometry to one N and one F atom. The Xe–N bond length is 2.28 Å. The Xe–F bond length is 2.07 Å. N is bonded in a trigonal planar geometry to one Xe and two S atoms. Both N–S bond lengths are 1.65 Å. There are two inequivalent S sites. In the first S site, S is bonded to one N, two O, and one F atom to form corner-sharing SNO2F tetrahedra. Both S–O bond lengths are 1.42 Å. The S–F bond length is 1.60 Å. In the second S site, S is bonded to one N, two O, and one F atom to form corner-sharing SNO2F tetrahedra. Both S–O bond lengths are 1.43 Å. The S–F bond length is 1.59 Å. There are four inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one S atom. In the second O site, O is bonded in a single-bond geometry to one S atom. In the third O site, O is bonded in a single-bond geometry to one S atom. In the fourth O site, O is bonded in a single-bond geometry to one S atom. There are three inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one S atom. In the third F site, F is bonded in a single-bond geometry to one S atom.

36 MATERIALS SCIENCE↗

Materials Data on SXeO3F2 by Materials Project

XeSO3F2 is Cubic alpha N2 structured and crystallizes in the orthorhombic Pbca space group. The structure is zero-dimensional and consists of eight XeSO3F2 clusters. Xe is bonded in a linear geometry to one O and one F atom. The Xe–O bond length is 2.25 Å. The Xe–F bond length is 2.05 Å. S is bonded in a tetrahedral geometry to three O and one F atom. There is two shorter (1.43 Å) and one longer (1.53 Å) S–O bond length. The S–F bond length is 1.61 Å. There are three inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Xe and one S atom. In the second O site, O is bonded in a single-bond geometry to one S atom. In the third O site, O is bonded in a single-bond geometry to one S atom. There are two inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one S atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on XeO3 by Materials Project

XeO3 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is zero-dimensional and consists of four XeO3 clusters. Xe is bonded in a 3-coordinate geometry to three O atoms. There are a spread of Xe–O bond distances ranging from 1.88–1.92 Å. There are three inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Xe atom. In the second O site, O is bonded in a single-bond geometry to one Xe atom. In the third O site, O is bonded in a distorted single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on RuXeF11 by Materials Project

XeF5RuF6 crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four 13693-08-8 molecules and four XeF5 clusters. In each XeF5 cluster, Xe is bonded in a 5-coordinate geometry to five F atoms. There is two shorter (1.98 Å) and three longer (1.99 Å) Xe–F bond length. There are three inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on Sb3S2XeN(O2F9)2 by Materials Project

XeSb3NS2(O2F9)2 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four XeSb3NS2(O2F9)2 clusters. Xe is bonded in a linear geometry to one N and one F atom. The Xe–N bond length is 2.13 Å. The Xe–F bond length is 2.44 Å. There are three inequivalent Sb sites. In the first Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 29°. There are a spread of Sb–F bond distances ranging from 1.88–2.10 Å. In the second Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 29°. There are a spread of Sb–F bond distances ranging from 1.88–2.15 Å. In the third Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 29°. There are a spread of Sb–F bond distances ranging from 1.88–2.04 Å. N is bonded in a trigonal planar geometry to one Xe and two S atoms. There is one shorter (1.69 Å) and one longer (1.73 Å) N–S bond length. There are two inequivalent S sites. In the first S site, S is bonded to one N, two O, and one F atom to form distorted corner-sharing SNO2F tetrahedra. Both S–O bond lengths are 1.42 Å. The S–F bond length is 1.58 Å. In the second S site, S is bonded to one N, two O, and one F atom to form corner-sharing SNO2F tetrahedra. There is one shorter (1.42 Å) and one longer (1.43 Å) S–O bond length. The S–F bond length is 1.57 Å. There are four inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one S atom. In the second O site, O is bonded in a single-bond geometry to one S atom. In the third O site, O is bonded in a single-bond geometry to one S atom. In the fourth O site, O is bonded in a single-bond geometry to one S atom. There are eighteen inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Sb atom. In the second F site, F is bonded in a single-bond geometry to one Sb atom. In the third F site, F is bonded in a single-bond geometry to one Sb atom. In the fourth F site, F is bonded in a single-bond geometry to one Sb atom. In the fifth F site, F is bonded in a single-bond geometry to one Sb atom. In the sixth F site, F is bonded in a single-bond geometry to one Sb atom. In the seventh F site, F is bonded in a single-bond geometry to one Sb atom. In the eighth F site, F is bonded in a bent 150 degrees geometry to two Sb atoms. In the ninth F site, F is bonded in a bent 150 degrees geometry to two Sb atoms. In the tenth F site, F is bonded in a single-bond geometry to one Sb atom. In the eleventh F site, F is bonded in a single-bond geometry to one Sb atom. In the twelfth F site, F is bonded in a single-bond geometry to one S atom. In the thirteenth F site, F is bonded in a single-bond geometry to one S atom. In the fourteenth F site, F is bonded in a distorted linear geometry to one Xe and one Sb atom. In the fifteenth F site, F is bonded in a single-bond geometry to one Sb atom. In the sixteenth F site, F is bonded in a single-bond geometry to one Sb atom. In the seventeenth F site, F is bonded in a single-bond geometry to one Sb atom. In the eighteenth F site, F is bonded in a single-bond geometry to one Sb atom.

36 MATERIALS SCIENCE↗

Materials Data on PtXeF11 by Materials Project

XeF5PtF6 crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four PtF6 clusters and four XeF5 clusters. In each PtF6 cluster, Pt is bonded in an octahedral geometry to six F atoms. There are a spread of Pt–F bond distances ranging from 1.90–1.96 Å. There are five inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Pt atom. In the second F site, F is bonded in a single-bond geometry to one Pt atom. In the third F site, F is bonded in a single-bond geometry to one Pt atom. In the fourth F site, F is bonded in a single-bond geometry to one Pt atom. In the fifth F site, F is bonded in a single-bond geometry to one Pt atom. In each XeF5 cluster, Xe is bonded in a distorted square pyramidal geometry to five F atoms. There is two shorter (1.98 Å) and three longer (1.99 Å) Xe–F bond length. There are three inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on TeAsHXeNF11 by Materials Project

XeAsNHTeF11 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two XeAsNHTeF11 clusters. Xe is bonded in a linear geometry to one N and one F atom. The Xe–N bond length is 2.14 Å. The Xe–F bond length is 2.50 Å. As is bonded in an octahedral geometry to six F atoms. There are a spread of As–F bond distances ranging from 1.76–1.86 Å. N is bonded in a distorted single-bond geometry to one Xe, one H, and one Te atom. The N–H bond length is 1.04 Å. The N–Te bond length is 2.07 Å. H is bonded in a single-bond geometry to one N atom. Te is bonded in an octahedral geometry to one N and five F atoms. There are a spread of Te–F bond distances ranging from 1.86–1.89 Å. There are eleven inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Te atom. In the second F site, F is bonded in a single-bond geometry to one Te atom. In the third F site, F is bonded in a single-bond geometry to one Te atom. In the fourth F site, F is bonded in a single-bond geometry to one Te atom. In the fifth F site, F is bonded in a single-bond geometry to one Te atom. In the sixth F site, F is bonded in a single-bond geometry to one As atom. In the seventh F site, F is bonded in a single-bond geometry to one As atom. In the eighth F site, F is bonded in a single-bond geometry to one As atom. In the ninth F site, F is bonded in a single-bond geometry to one As atom. In the tenth F site, F is bonded in a single-bond geometry to one As atom. In the eleventh F site, F is bonded in a distorted bent 120 degrees geometry to one Xe and one As atom.

36 MATERIALS SCIENCE↗

Materials Data on AsSXeNF10 by Materials Project

XeAsNSF10 crystallizes in the monoclinic C2/c space group. The structure is zero-dimensional and consists of eight XeAsNSF10 clusters. Xe is bonded in a linear geometry to one N and one F atom. The Xe–N bond length is 2.18 Å. The Xe–F bond length is 2.69 Å. As is bonded in an octahedral geometry to six F atoms. There are a spread of As–F bond distances ranging from 1.76–1.83 Å. N is bonded in a distorted bent 120 degrees geometry to one Xe and one S atom. The N–S bond length is 1.57 Å. S is bonded in a trigonal bipyramidal geometry to one N and four F atoms. There are a spread of S–F bond distances ranging from 1.56–1.62 Å. There are ten inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one S atom. In the second F site, F is bonded in a single-bond geometry to one As atom. In the third F site, F is bonded in a single-bond geometry to one As atom. In the fourth F site, F is bonded in a single-bond geometry to one S atom. In the fifth F site, F is bonded in a single-bond geometry to one S atom. In the sixth F site, F is bonded in a single-bond geometry to one S atom. In the seventh F site, F is bonded in a single-bond geometry to one As atom. In the eighth F site, F is bonded in a single-bond geometry to one Xe and one As atom. In the ninth F site, F is bonded in a single-bond geometry to one As atom. In the tenth F site, F is bonded in a single-bond geometry to one As atom.

36 MATERIALS SCIENCE↗

Materials Data on MnSb3XeF23 by Materials Project

XeF5MnSb3F18 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional and consists of four XeF5 clusters and one MnSb3F18 framework. In each XeF5 cluster, Xe is bonded in a square pyramidal geometry to five F atoms. There is one shorter (1.95 Å) and four longer (1.96 Å) Xe–F bond length. There are three inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom. In the MnSb3F18 framework, Mn is bonded to six F atoms to form MnF6 octahedra that share corners with six SbF6 octahedra. The corner-sharing octahedra tilt angles range from 14–23°. There are four shorter (2.12 Å) and two longer (2.15 Å) Mn–F bond lengths. There are two inequivalent Sb sites. In the first Sb site, Sb is bonded to six F atoms to form SbF6 octahedra that share corners with two equivalent MnF6 octahedra. The corner-sharing octahedra tilt angles range from 20–23°. There are a spread of Sb–F bond distances ranging from 1.89–1.97 Å. In the second Sb site, Sb is bonded to six F atoms to form SbF6 octahedra that share corners with two equivalent MnF6 octahedra. The corner-sharing octahedral tilt angles are 14°. There are a spread of Sb–F bond distances ranging from 1.88–1.96 Å. There are eleven inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Sb atom. In the second F site, F is bonded in a single-bond geometry to one Sb atom. In the third F site, F is bonded in a single-bond geometry to one Sb atom. In the fourth F site, F is bonded in a single-bond geometry to one Sb atom. In the fifth F site, F is bonded in a bent 150 degrees geometry to one Mn and one Sb atom. In the sixth F site, F is bonded in a linear geometry to one Mn and one Sb atom. In the seventh F site, F is bonded in a single-bond geometry to one Sb atom. In the eighth F site, F is bonded in a bent 150 degrees geometry to one Mn and one Sb atom. In the ninth F site, F is bonded in a single-bond geometry to one Sb atom. In the tenth F site, F is bonded in a single-bond geometry to one Sb atom. In the eleventh F site, F is bonded in a single-bond geometry to one Sb atom.

36 MATERIALS SCIENCE↗

Materials Data on Sb2XeClF11 by Materials Project

XeSb2ClF11 crystallizes in the orthorhombic Pna2_1 space group. The structure is zero-dimensional and consists of eight XeSb2ClF11 clusters. Xe is bonded in a linear geometry to one Cl and one F atom. The Xe–Cl bond length is 2.36 Å. The Xe–F bond length is 2.67 Å. There are two inequivalent Sb sites. In the first Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 35°. There are a spread of Sb–F bond distances ranging from 1.89–2.08 Å. In the second Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 35°. There are a spread of Sb–F bond distances ranging from 1.89–2.08 Å. Cl is bonded in a single-bond geometry to one Xe atom. There are eleven inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Sb atom. In the second F site, F is bonded in a single-bond geometry to one Sb atom. In the third F site, F is bonded in a single-bond geometry to one Sb atom. In the fourth F site, F is bonded in a single-bond geometry to one Sb atom. In the fifth F site, F is bonded in a single-bond geometry to one Sb atom. In the sixth F site, F is bonded in a single-bond geometry to one Sb atom. In the seventh F site, F is bonded in a bent 150 degrees geometry to two Sb atoms. In the eighth F site, F is bonded in a single-bond geometry to one Sb atom. In the ninth F site, F is bonded in a single-bond geometry to one Xe and one Sb atom. In the tenth F site, F is bonded in a single-bond geometry to one Sb atom. In the eleventh F site, F is bonded in a single-bond geometry to one Sb atom.

36 MATERIALS SCIENCE↗

Materials Data on XeNO3F by Materials Project

XeNO3F crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four XeNO3F clusters. Xe is bonded in a linear geometry to one O and one F atom. The Xe–O bond length is 2.23 Å. The Xe–F bond length is 2.11 Å. N is bonded in a trigonal planar geometry to three O atoms. There are a spread of N–O bond distances ranging from 1.22–1.39 Å. There are three inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one N atom. In the second O site, O is bonded in a single-bond geometry to one N atom. In the third O site, O is bonded in a bent 120 degrees geometry to one Xe and one N atom. F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on TeAsXeO2F11 by Materials Project

XeAsTeO2F11 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two XeAsTeO2F11 clusters. Xe is bonded in a linear geometry to one O and one F atom. The Xe–O bond length is 2.08 Å. The Xe–F bond length is 2.32 Å. As is bonded in an octahedral geometry to six F atoms. There are a spread of As–F bond distances ranging from 1.74–1.94 Å. Te is bonded in an octahedral geometry to two O and four F atoms. There is one shorter (1.97 Å) and one longer (2.01 Å) Te–O bond length. There is two shorter (1.87 Å) and two longer (1.89 Å) Te–F bond length. There are two inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Xe and one Te atom. In the second O site, O is bonded in a water-like geometry to one Te and one F atom. The O–F bond length is 1.44 Å. There are eleven inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one O atom. In the second F site, F is bonded in a single-bond geometry to one Te atom. In the third F site, F is bonded in a single-bond geometry to one Te atom. In the fourth F site, F is bonded in a single-bond geometry to one Te atom. In the fifth F site, F is bonded in a single-bond geometry to one Te atom. In the sixth F site, F is bonded in a single-bond geometry to one As atom. In the seventh F site, F is bonded in a single-bond geometry to one As atom. In the eighth F site, F is bonded in a single-bond geometry to one As atom. In the ninth F site, F is bonded in a single-bond geometry to one As atom. In the tenth F site, F is bonded in a single-bond geometry to one As atom. In the eleventh F site, F is bonded in a distorted bent 120 degrees geometry to one Xe and one As atom.

36 MATERIALS SCIENCE↗

Materials Data on SbXeF11 by Materials Project

XeF5SbF6 crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four SbF6 clusters and four XeF5 clusters. In each SbF6 cluster, Sb is bonded in an octahedral geometry to six F atoms. There are a spread of Sb–F bond distances ranging from 1.90–1.95 Å. There are five inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Sb atom. In the second F site, F is bonded in a single-bond geometry to one Sb atom. In the third F site, F is bonded in a single-bond geometry to one Sb atom. In the fourth F site, F is bonded in a single-bond geometry to one Sb atom. In the fifth F site, F is bonded in a single-bond geometry to one Sb atom. In each XeF5 cluster, Xe is bonded in a distorted square pyramidal geometry to five F atoms. There is three shorter (1.97 Å) and two longer (1.98 Å) Xe–F bond length. There are three inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Self-Adjusting Metal–Organic Framework for Efficient Capture of Trace Xenon and Krypton

The capture of the xenon and krypton from nuclear reprocessing off-gas is essential to the treatment of radioactive waste. Although various porous materials have been employed to capture Xe and Kr, the development of high-performance adsorbents capable of trapping Xe/Kr at very low partial pressure as in the nuclear reprocessing off-gas conditions remains challenging. Herein, we report a self-adjusting metal-organic framework based on multiple weak binding interactions to capture trace Xe and Kr from the nuclear reprocessing off-gas. The self-adjusting behavior of ATC-Cu and its mechanism have been visualized by the in-situ single-crystal X-ray diffraction studies and theoretical calculations. The self-adjusting behavior endows ATC-Cu unprecedented uptake capacities of 2.65 and 0.52 mmol g -1 for Xe and Kr respectively at 0.1 bar and 298 K, as well as the record Xe capture capability from the nuclear reprocessing off-gas. Further, our work not only provides a benchmark Xe adsorbent but proposes a new route to construct smart materials for efficient separations.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗