Rotational spectra and structures of small clusters: the Ar4-H/DF pentamers

The 40Ar4–HF and –DF clusters have been identified and characterized by their microwave rotational spectra using a Flygare–Balle FT spectrometer with a pulsed supersonic nozzle to generate and detect the clusters. The observed J=2→3 to 6→7 transitions have fine structure limited to K=0, ±3 and ±6, i...

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Veröffentlicht in:The Journal of chemical physics 1988-03, Vol.88 (5), p.2919-2924
Hauptverfasser: GUTOWSKY, H. S, CHUANG, C, KLOTS, T. D, EMILSSON, T, RUOFF, R. S, KRAUSE, K. R
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container_end_page 2924
container_issue 5
container_start_page 2919
container_title The Journal of chemical physics
container_volume 88
creator GUTOWSKY, H. S
CHUANG, C
KLOTS, T. D
EMILSSON, T
RUOFF, R. S
KRAUSE, K. R
description The 40Ar4–HF and –DF clusters have been identified and characterized by their microwave rotational spectra using a Flygare–Balle FT spectrometer with a pulsed supersonic nozzle to generate and detect the clusters. The observed J=2→3 to 6→7 transitions have fine structure limited to K=0, ±3 and ±6, indicative of symmetric tops with a threefold axis of symmetry produced by I=0 nuclei. For Ar4–HF the rotational constants B0, DJ, and DJK are 623.4539(1) MHz, 1.062(1) kHz, and 0.611(31) kHz, respectively; and for Ar4–DF, 618.5846(1) MHz, 1.030(1) kHz, and 0.665(4) kHz. The results show that the clusters consist of the trigonal Ar3–H/DF tetramer reported earlier, with a fourth argon on the back side of the Ar3 group to form a tetrahedral or near tetrahedral Ar4. In both clusters the H/DF lies along the threefold axis of the Ar3 group, with the H/D end pointed at its face. If one assumes an Ar–Ar distance of 3.85 Å for both clusters, the Ar3 plane to HF c.m. distance for Ar4–HF with a tetrahedral Ar4 is 2.713 Å compared to 2.735 Å for Ar3–HF. The nuclear hyperfine structure of the rotational transitions shows that the H/DF experiences large amplitude bending vibrations with respect to the C3 symmetry axis. The average amplitude for HF (40.4°) is comparable with that reported for the smaller Arm–HF complexes (m=1, 2, 3). However, for DF the apparent 25.1 (1.6)° amplitude found is 10° less than that in the smaller complexes. The difference is attributed to an increased electric field gradient at the D in the pentamer. A possibly related feature is an Ar4 c.m. to F distance which is 0.013 Å longer for Ar4–DF than for Ar4–HF.
doi_str_mv 10.1063/1.453984
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In both clusters the H/DF lies along the threefold axis of the Ar3 group, with the H/D end pointed at its face. If one assumes an Ar–Ar distance of 3.85 Å for both clusters, the Ar3 plane to HF c.m. distance for Ar4–HF with a tetrahedral Ar4 is 2.713 Å compared to 2.735 Å for Ar3–HF. The nuclear hyperfine structure of the rotational transitions shows that the H/DF experiences large amplitude bending vibrations with respect to the C3 symmetry axis. The average amplitude for HF (40.4°) is comparable with that reported for the smaller Arm–HF complexes (m=1, 2, 3). However, for DF the apparent 25.1 (1.6)° amplitude found is 10° less than that in the smaller complexes. The difference is attributed to an increased electric field gradient at the D in the pentamer. 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The results show that the clusters consist of the trigonal Ar3–H/DF tetramer reported earlier, with a fourth argon on the back side of the Ar3 group to form a tetrahedral or near tetrahedral Ar4. In both clusters the H/DF lies along the threefold axis of the Ar3 group, with the H/D end pointed at its face. If one assumes an Ar–Ar distance of 3.85 Å for both clusters, the Ar3 plane to HF c.m. distance for Ar4–HF with a tetrahedral Ar4 is 2.713 Å compared to 2.735 Å for Ar3–HF. The nuclear hyperfine structure of the rotational transitions shows that the H/DF experiences large amplitude bending vibrations with respect to the C3 symmetry axis. The average amplitude for HF (40.4°) is comparable with that reported for the smaller Arm–HF complexes (m=1, 2, 3). However, for DF the apparent 25.1 (1.6)° amplitude found is 10° less than that in the smaller complexes. The difference is attributed to an increased electric field gradient at the D in the pentamer. 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R</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c252t-23c1484551ac8956f424bdd44b1de9c4b66c7eb8dfc53a7363cd3132c9b8795e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1988</creationdate><topic>Atomic and molecular clusters</topic><topic>Atomic and molecular physics</topic><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Studies of special atoms, molecules and their ions; clusters</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>GUTOWSKY, H. S</creatorcontrib><creatorcontrib>CHUANG, C</creatorcontrib><creatorcontrib>KLOTS, T. D</creatorcontrib><creatorcontrib>EMILSSON, T</creatorcontrib><creatorcontrib>RUOFF, R. S</creatorcontrib><creatorcontrib>KRAUSE, K. 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R</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Rotational spectra and structures of small clusters: the Ar4-H/DF pentamers</atitle><jtitle>The Journal of chemical physics</jtitle><date>1988-03-01</date><risdate>1988</risdate><volume>88</volume><issue>5</issue><spage>2919</spage><epage>2924</epage><pages>2919-2924</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><coden>JCPSA6</coden><abstract>The 40Ar4–HF and –DF clusters have been identified and characterized by their microwave rotational spectra using a Flygare–Balle FT spectrometer with a pulsed supersonic nozzle to generate and detect the clusters. The observed J=2→3 to 6→7 transitions have fine structure limited to K=0, ±3 and ±6, indicative of symmetric tops with a threefold axis of symmetry produced by I=0 nuclei. For Ar4–HF the rotational constants B0, DJ, and DJK are 623.4539(1) MHz, 1.062(1) kHz, and 0.611(31) kHz, respectively; and for Ar4–DF, 618.5846(1) MHz, 1.030(1) kHz, and 0.665(4) kHz. The results show that the clusters consist of the trigonal Ar3–H/DF tetramer reported earlier, with a fourth argon on the back side of the Ar3 group to form a tetrahedral or near tetrahedral Ar4. In both clusters the H/DF lies along the threefold axis of the Ar3 group, with the H/D end pointed at its face. If one assumes an Ar–Ar distance of 3.85 Å for both clusters, the Ar3 plane to HF c.m. distance for Ar4–HF with a tetrahedral Ar4 is 2.713 Å compared to 2.735 Å for Ar3–HF. The nuclear hyperfine structure of the rotational transitions shows that the H/DF experiences large amplitude bending vibrations with respect to the C3 symmetry axis. The average amplitude for HF (40.4°) is comparable with that reported for the smaller Arm–HF complexes (m=1, 2, 3). However, for DF the apparent 25.1 (1.6)° amplitude found is 10° less than that in the smaller complexes. The difference is attributed to an increased electric field gradient at the D in the pentamer. A possibly related feature is an Ar4 c.m. to F distance which is 0.013 Å longer for Ar4–DF than for Ar4–HF.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.453984</doi><tpages>6</tpages></addata></record>
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Atomic and molecular physics
Exact sciences and technology
Physics
Studies of special atoms, molecules and their ions
clusters
title Rotational spectra and structures of small clusters: the Ar4-H/DF pentamers
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