Structural and energetic properties of OC–BX3 complexes: unrealized potential for bond-stretch isomerism
We have explored the structural and energetic properties of OC–BX3 (X = F, Cl, or Br) complexes using computations and low-temperature infrared spectroscopy. Quantum-chemical calculations have provided equilibrium structures, binding energies, vibrational frequencies, and B–C potential energy curves...
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Veröffentlicht in: | Physical chemistry chemical physics : PCCP 2021-07, Vol.23 (27), p.14678-14686 |
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description | We have explored the structural and energetic properties of OC–BX3 (X = F, Cl, or Br) complexes using computations and low-temperature infrared spectroscopy. Quantum-chemical calculations have provided equilibrium structures, binding energies, vibrational frequencies, and B–C potential energy curves. The OC–BF3 system is a weak, long-bonded complex with a single minimum on the B–C potential (R(B–C) = 2.865 Å). For the remaining two complexes, OC–BCl3 and OC–BBr3, computations predict two stable minima on their B–C potential curves. The BCl3 system is a weak complex with a long bond (R(B–C) = 3.358 Å), but it exhibits a secondary, meta-stable minimum with a short bond length of 1.659 Å. For OC–BBr3, the system is a weak complex with a relatively short bond of 1.604 Å (according to wB97X-D/aug-cc-pVTZ), but also has a secondary minimum at R(B–C) = 3.483 Å. This long-bond structure is the global minimum according to CCSD/aug-cc-pVTZ. In addition, the long-bond forms of both OC–BCl3 and OC–BBr3 were observed in matrix-isolation IR experiments. The measured CO stretching frequencies were 2145 cm−1 and 2143 cm−1, respectively. No signals due to the short-bond forms of OC–BCl3 and OC–BBr3 were observed. |
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Quantum-chemical calculations have provided equilibrium structures, binding energies, vibrational frequencies, and B–C potential energy curves. The OC–BF3 system is a weak, long-bonded complex with a single minimum on the B–C potential (R(B–C) = 2.865 Å). For the remaining two complexes, OC–BCl3 and OC–BBr3, computations predict two stable minima on their B–C potential curves. The BCl3 system is a weak complex with a long bond (R(B–C) = 3.358 Å), but it exhibits a secondary, meta-stable minimum with a short bond length of 1.659 Å. For OC–BBr3, the system is a weak complex with a relatively short bond of 1.604 Å (according to wB97X-D/aug-cc-pVTZ), but also has a secondary minimum at R(B–C) = 3.483 Å. This long-bond structure is the global minimum according to CCSD/aug-cc-pVTZ. In addition, the long-bond forms of both OC–BCl3 and OC–BBr3 were observed in matrix-isolation IR experiments. The measured CO stretching frequencies were 2145 cm−1 and 2143 cm−1, respectively. No signals due to the short-bond forms of OC–BCl3 and OC–BBr3 were observed.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/d1cp02230j</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Bonding strength ; Boron chlorides ; Low temperature ; Potential energy ; Quantum chemistry</subject><ispartof>Physical chemistry chemical physics : PCCP, 2021-07, Vol.23 (27), p.14678-14686</ispartof><rights>Copyright Royal Society of Chemistry 2021</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27922,27923</link.rule.ids></links><search><creatorcontrib>Munos, Jordan A</creatorcontrib><creatorcontrib>Lowney, Diego T</creatorcontrib><creatorcontrib>Phillips, James A</creatorcontrib><title>Structural and energetic properties of OC–BX3 complexes: unrealized potential for bond-stretch isomerism</title><title>Physical chemistry chemical physics : PCCP</title><description>We have explored the structural and energetic properties of OC–BX3 (X = F, Cl, or Br) complexes using computations and low-temperature infrared spectroscopy. Quantum-chemical calculations have provided equilibrium structures, binding energies, vibrational frequencies, and B–C potential energy curves. The OC–BF3 system is a weak, long-bonded complex with a single minimum on the B–C potential (R(B–C) = 2.865 Å). For the remaining two complexes, OC–BCl3 and OC–BBr3, computations predict two stable minima on their B–C potential curves. The BCl3 system is a weak complex with a long bond (R(B–C) = 3.358 Å), but it exhibits a secondary, meta-stable minimum with a short bond length of 1.659 Å. For OC–BBr3, the system is a weak complex with a relatively short bond of 1.604 Å (according to wB97X-D/aug-cc-pVTZ), but also has a secondary minimum at R(B–C) = 3.483 Å. This long-bond structure is the global minimum according to CCSD/aug-cc-pVTZ. In addition, the long-bond forms of both OC–BCl3 and OC–BBr3 were observed in matrix-isolation IR experiments. The measured CO stretching frequencies were 2145 cm−1 and 2143 cm−1, respectively. No signals due to the short-bond forms of OC–BCl3 and OC–BBr3 were observed.</description><subject>Bonding strength</subject><subject>Boron chlorides</subject><subject>Low temperature</subject><subject>Potential energy</subject><subject>Quantum chemistry</subject><issn>1463-9076</issn><issn>1463-9084</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNpdj8tKxTAYhIMoeLxsfIKAGzfVP02btO704A0OnIUK7g5p8ldb2qQmKYgr38E39EkMKC7czMziY5gh5IjBKQNenxmmJ8hzDv0WWbBC8KyGqtj-y1Lskr0QegBgJeML0t9HP-s4ezVQZQ1Fi_4ZY6fp5N2EPnYYqGvpevn18Xn5xKl24zTgG4ZzOluPauje0dDJRbSxSyWt87Rx1mQheoz6hXbBjei7MB6QnVYNAQ9_fZ88Xl89LG-z1frmbnmxyqY0MmZGFRVroWlQGK1M0TbIJYe8NWWla6FZw3WpSlkmAeAIDRZSC6O4aCRnmu-Tk5_e9OB1xhA3Yxc0DoOy6OawycuiEnkt6iKhx__Q3s3epnWJKhkIBlLyb0tMakQ</recordid><startdate>20210721</startdate><enddate>20210721</enddate><creator>Munos, Jordan A</creator><creator>Lowney, Diego T</creator><creator>Phillips, James A</creator><general>Royal Society of Chemistry</general><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>20210721</creationdate><title>Structural and energetic properties of OC–BX3 complexes: unrealized potential for bond-stretch isomerism</title><author>Munos, Jordan A ; Lowney, Diego T ; Phillips, James A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p146t-da481f0bbe6dcad4fbe37302fd58c96c1b3c5a5755a5003e0be47c6da36b731c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Bonding strength</topic><topic>Boron chlorides</topic><topic>Low temperature</topic><topic>Potential energy</topic><topic>Quantum chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Munos, Jordan A</creatorcontrib><creatorcontrib>Lowney, Diego T</creatorcontrib><creatorcontrib>Phillips, James A</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Physical chemistry chemical physics : PCCP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Munos, Jordan A</au><au>Lowney, Diego T</au><au>Phillips, James A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural and energetic properties of OC–BX3 complexes: unrealized potential for bond-stretch isomerism</atitle><jtitle>Physical chemistry chemical physics : PCCP</jtitle><date>2021-07-21</date><risdate>2021</risdate><volume>23</volume><issue>27</issue><spage>14678</spage><epage>14686</epage><pages>14678-14686</pages><issn>1463-9076</issn><eissn>1463-9084</eissn><abstract>We have explored the structural and energetic properties of OC–BX3 (X = F, Cl, or Br) complexes using computations and low-temperature infrared spectroscopy. Quantum-chemical calculations have provided equilibrium structures, binding energies, vibrational frequencies, and B–C potential energy curves. The OC–BF3 system is a weak, long-bonded complex with a single minimum on the B–C potential (R(B–C) = 2.865 Å). For the remaining two complexes, OC–BCl3 and OC–BBr3, computations predict two stable minima on their B–C potential curves. The BCl3 system is a weak complex with a long bond (R(B–C) = 3.358 Å), but it exhibits a secondary, meta-stable minimum with a short bond length of 1.659 Å. For OC–BBr3, the system is a weak complex with a relatively short bond of 1.604 Å (according to wB97X-D/aug-cc-pVTZ), but also has a secondary minimum at R(B–C) = 3.483 Å. This long-bond structure is the global minimum according to CCSD/aug-cc-pVTZ. In addition, the long-bond forms of both OC–BCl3 and OC–BBr3 were observed in matrix-isolation IR experiments. The measured CO stretching frequencies were 2145 cm−1 and 2143 cm−1, respectively. No signals due to the short-bond forms of OC–BCl3 and OC–BBr3 were observed.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d1cp02230j</doi><tpages>9</tpages></addata></record> |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Bonding strength Boron chlorides Low temperature Potential energy Quantum chemistry |
title | Structural and energetic properties of OC–BX3 complexes: unrealized potential for bond-stretch isomerism |
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