{"title":"Ti3C2${rm Ti}_{3}{rm C}_{2}$二茂钛中氢原子和分子的混合轨道形成与多中心结合","authors":"Norbert H. Nickel","doi":"10.1002/andp.202400011","DOIUrl":null,"url":null,"abstract":"<p>The formation and stability of solids and molecules is not possible without chemical bonds, which are divided into covalent, ionic, metallic, and van der Waals bonds. A special type of intermolecular bond is hydrogen bonding, which plays a crucial role for chemical, biological, and physical processes. However, hydrogen shows a far more complex behavior when it is present in solids. In this paper, it is shown that the chemical bonding of hydrogen atoms and molecules extends far beyond the simple picture of conventional, ionic, covalent, and multicenter bonds. The interaction of H with its host material is particularly important for hydrogen storage in metallic materials such as <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>Ti</mi>\n <mn>3</mn>\n </msub>\n <msub>\n <mi>C</mi>\n <mn>2</mn>\n </msub>\n </mrow>\n <annotation>${\\rm Ti}_{3}{\\rm C}_{2}$</annotation>\n </semantics></math> MXenes. Hydrogen atoms and <span></span><math>\n <semantics>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n <annotation>${\\rm H}_2$</annotation>\n </semantics></math> molecules form multicenter bonds in <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>Ti</mi>\n <mn>3</mn>\n </msub>\n <msub>\n <mi>C</mi>\n <mn>2</mn>\n </msub>\n </mrow>\n <annotation>${\\rm Ti}_{3}{\\rm C}_{2}$</annotation>\n </semantics></math>. On the surface and between two <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>Ti</mi>\n <mn>3</mn>\n </msub>\n <msub>\n <mi>C</mi>\n <mn>2</mn>\n </msub>\n </mrow>\n <annotation>${\\rm Ti}_{3}{\\rm C}_{2}$</annotation>\n </semantics></math> sheets this is limited to the formation of H–Ti bonds. However, H and <span></span><math>\n <semantics>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n <annotation>${\\rm H}_2$</annotation>\n </semantics></math> on interstitial sites form multicenter bonds not only with nearest neighbor Ti atoms but also with carbon atoms. Interestingly, the H–C bonds are characterized by the formation of s–p hybrid orbitals. For <span></span><math>\n <semantics>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n <annotation>${\\rm H}_2$</annotation>\n </semantics></math> molecules, multicenter bond formation is accompanied by an increase of the bond length to 2.07 and 1.85 Å for <span></span><math>\n <semantics>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n <annotation>${\\rm H}_2$</annotation>\n </semantics></math> on the surface and at the interstitial site, respectively. On the other hand, placing <span></span><math>\n <semantics>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n <annotation>${\\rm H}_2$</annotation>\n </semantics></math> between two sheets of <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>Ti</mi>\n <mn>3</mn>\n </msub>\n <msub>\n <mi>C</mi>\n <mn>2</mn>\n </msub>\n </mrow>\n <annotation>${\\rm Ti}_{3}{\\rm C}_{2}$</annotation>\n </semantics></math> leads to dissociation. For all H and <span></span><math>\n <semantics>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n <annotation>${\\rm H}_2$</annotation>\n </semantics></math> complexes the vibrational eigenmodes are calculated. Their frequencies are in the range of 890 to 1610 <span></span><math>\n <semantics>\n <msup>\n <mi>cm</mi>\n <mrow>\n <mo>−</mo>\n <mn>1</mn>\n </mrow>\n </msup>\n <annotation>${\\rm cm}^{-1}$</annotation>\n </semantics></math>, which indicates that the bonds are remarkably strong.</p>","PeriodicalId":7896,"journal":{"name":"Annalen der Physik","volume":"536 6","pages":""},"PeriodicalIF":2.2000,"publicationDate":"2024-02-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/andp.202400011","citationCount":"0","resultStr":"{\"title\":\"Hybrid Orbital Formation and Multicenter Bonding of Hydrogen Atoms and Molecules in \\n \\n \\n \\n Ti\\n 3\\n \\n \\n C\\n 2\\n \\n \\n ${\\\\rm Ti}_{3}{\\\\rm C}_{2}$\\n MXenes\",\"authors\":\"Norbert H. Nickel\",\"doi\":\"10.1002/andp.202400011\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>The formation and stability of solids and molecules is not possible without chemical bonds, which are divided into covalent, ionic, metallic, and van der Waals bonds. A special type of intermolecular bond is hydrogen bonding, which plays a crucial role for chemical, biological, and physical processes. However, hydrogen shows a far more complex behavior when it is present in solids. In this paper, it is shown that the chemical bonding of hydrogen atoms and molecules extends far beyond the simple picture of conventional, ionic, covalent, and multicenter bonds. The interaction of H with its host material is particularly important for hydrogen storage in metallic materials such as <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>Ti</mi>\\n <mn>3</mn>\\n </msub>\\n <msub>\\n <mi>C</mi>\\n <mn>2</mn>\\n </msub>\\n </mrow>\\n <annotation>${\\\\rm Ti}_{3}{\\\\rm C}_{2}$</annotation>\\n </semantics></math> MXenes. Hydrogen atoms and <span></span><math>\\n <semantics>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n <annotation>${\\\\rm H}_2$</annotation>\\n </semantics></math> molecules form multicenter bonds in <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>Ti</mi>\\n <mn>3</mn>\\n </msub>\\n <msub>\\n <mi>C</mi>\\n <mn>2</mn>\\n </msub>\\n </mrow>\\n <annotation>${\\\\rm Ti}_{3}{\\\\rm C}_{2}$</annotation>\\n </semantics></math>. On the surface and between two <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>Ti</mi>\\n <mn>3</mn>\\n </msub>\\n <msub>\\n <mi>C</mi>\\n <mn>2</mn>\\n </msub>\\n </mrow>\\n <annotation>${\\\\rm Ti}_{3}{\\\\rm C}_{2}$</annotation>\\n </semantics></math> sheets this is limited to the formation of H–Ti bonds. However, H and <span></span><math>\\n <semantics>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n <annotation>${\\\\rm H}_2$</annotation>\\n </semantics></math> on interstitial sites form multicenter bonds not only with nearest neighbor Ti atoms but also with carbon atoms. Interestingly, the H–C bonds are characterized by the formation of s–p hybrid orbitals. For <span></span><math>\\n <semantics>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n <annotation>${\\\\rm H}_2$</annotation>\\n </semantics></math> molecules, multicenter bond formation is accompanied by an increase of the bond length to 2.07 and 1.85 Å for <span></span><math>\\n <semantics>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n <annotation>${\\\\rm H}_2$</annotation>\\n </semantics></math> on the surface and at the interstitial site, respectively. On the other hand, placing <span></span><math>\\n <semantics>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n <annotation>${\\\\rm H}_2$</annotation>\\n </semantics></math> between two sheets of <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>Ti</mi>\\n <mn>3</mn>\\n </msub>\\n <msub>\\n <mi>C</mi>\\n <mn>2</mn>\\n </msub>\\n </mrow>\\n <annotation>${\\\\rm Ti}_{3}{\\\\rm C}_{2}$</annotation>\\n </semantics></math> leads to dissociation. For all H and <span></span><math>\\n <semantics>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n <annotation>${\\\\rm H}_2$</annotation>\\n </semantics></math> complexes the vibrational eigenmodes are calculated. Their frequencies are in the range of 890 to 1610 <span></span><math>\\n <semantics>\\n <msup>\\n <mi>cm</mi>\\n <mrow>\\n <mo>−</mo>\\n <mn>1</mn>\\n </mrow>\\n </msup>\\n <annotation>${\\\\rm cm}^{-1}$</annotation>\\n </semantics></math>, which indicates that the bonds are remarkably strong.</p>\",\"PeriodicalId\":7896,\"journal\":{\"name\":\"Annalen der Physik\",\"volume\":\"536 6\",\"pages\":\"\"},\"PeriodicalIF\":2.2000,\"publicationDate\":\"2024-02-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1002/andp.202400011\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Annalen der Physik\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/andp.202400011\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Annalen der Physik","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/andp.202400011","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
固体和分子的形成与稳定离不开化学键,化学键分为共价键、离子键、金属键和范德华键。氢键是分子间键的一种特殊类型,在化学、生物和物理过程中起着至关重要的作用。然而,当氢存在于固体中时,其行为要复杂得多。本文表明,氢原子和分子的化学键远远超出了传统的离子键、共价键和多中心键的简单描述。氢与其宿主材料的相互作用对于金属材料(如二氧化二烯)中的氢储存尤为重要。氢原子和分子在......中形成多中心键。在表面和两个薄片之间,这仅限于形成 H-Ti 键。然而,氢原子和间隙位点上的氢原子不仅会与近邻的钛原子形成多中心键,还会与碳原子形成多中心键。有趣的是,H-C 键的特点是形成 s-p 混合轨道。对于分子来说,多中心键的形成伴随着键长的增加,表面和间隙部位的键长分别为 2.07 Å 和 1.85 Å。另一方面,放置在两个片层之间会导致解离。对所有 H 和复合物的振动特征模态都进行了计算。它们的频率在 890 到 1610 之间,这表明键的强度非常高。
Hybrid Orbital Formation and Multicenter Bonding of Hydrogen Atoms and Molecules in
Ti
3
C
2
${\rm Ti}_{3}{\rm C}_{2}$
MXenes
The formation and stability of solids and molecules is not possible without chemical bonds, which are divided into covalent, ionic, metallic, and van der Waals bonds. A special type of intermolecular bond is hydrogen bonding, which plays a crucial role for chemical, biological, and physical processes. However, hydrogen shows a far more complex behavior when it is present in solids. In this paper, it is shown that the chemical bonding of hydrogen atoms and molecules extends far beyond the simple picture of conventional, ionic, covalent, and multicenter bonds. The interaction of H with its host material is particularly important for hydrogen storage in metallic materials such as MXenes. Hydrogen atoms and molecules form multicenter bonds in . On the surface and between two sheets this is limited to the formation of H–Ti bonds. However, H and on interstitial sites form multicenter bonds not only with nearest neighbor Ti atoms but also with carbon atoms. Interestingly, the H–C bonds are characterized by the formation of s–p hybrid orbitals. For molecules, multicenter bond formation is accompanied by an increase of the bond length to 2.07 and 1.85 Å for on the surface and at the interstitial site, respectively. On the other hand, placing between two sheets of leads to dissociation. For all H and complexes the vibrational eigenmodes are calculated. Their frequencies are in the range of 890 to 1610 , which indicates that the bonds are remarkably strong.
期刊介绍:
Annalen der Physik (AdP) is one of the world''s most renowned physics journals with an over 225 years'' tradition of excellence. Based on the fame of seminal papers by Einstein, Planck and many others, the journal is now tuned towards today''s most exciting findings including the annual Nobel Lectures. AdP comprises all areas of physics, with particular emphasis on important, significant and highly relevant results. Topics range from fundamental research to forefront applications including dynamic and interdisciplinary fields. The journal covers theory, simulation and experiment, e.g., but not exclusively, in condensed matter, quantum physics, photonics, materials physics, high energy, gravitation and astrophysics. It welcomes Rapid Research Letters, Original Papers, Review and Feature Articles.