Abstract:The basic and the charge density wave (CDW) structures of the monoclinic NbS3-II polymorph were studied by synchrotron x-ray diffraction, ab-initio calculation, simulation of electron diffraction patterns and by atomicresolution transmission electron and low-temperature scanning tunneling microscopies. It is shown that the basic structure belongs to the space group P 21/m and is described with a unit cell, formed of four pairs of symmetry-related trigonal prismatic (TP) columns (a0 = 0.96509(8) nm, b0 = 0.3345… Show more
“…The calculated cell parameters, relative energy, and band gaps are reported in Table 1. One of them is the wellknown NbS 3 -I phase, 20 three correspond to the recently characterized NbS 3 -II, 19 NbS 3 -IV, 27 and NbS 3 -V 27 phases, and the remaining three are so-far unreported polymorphs with the structures of NbSe 3 , TiS 3 , and TaSe 3 . The agreement between experimental and theoretical structures for the four presently characterized compounds is excellent, thus lending reliability to these calculations.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…The unit cell of NbS 3 -II contains eight chains of Nb atoms trigonally coordinated with S atoms running along the b-direction (Figure 1d). There are four different types of NbS 3 chains which in order to simplify the discussion have been highlighted with different colors in Figure 1d (to help the comparison with experimental results, these colors are the same as those in the recent structural determination of the average structure 19 ). The purple and yellow chains are paired in the respective dimer units, whereas the red and orange chains form mixed red-orange pairs.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…1 Although different superstructures of the basic NbS 3 -I structure were proposed for this polymorph, a clear-cut structural determination remained elusive until recently (Figure 1d). 19 NbS 3 -II is metallic 23 and has been reported to exhibit three CDWs at around 450−475, 360, and 150 K, respectively. 24 This behavior is reminiscent of the NbSe 3 and m-TaS 3 systems, but now with an additional CDW transition.…”
Layered group V transition-metal trichalcogenides are paradigmatic low-dimensional materials providing an ever increasing series of unusual properties. They are all based on the same basic building units, one-dimensional MX 3 (M = Nb, Ta; X = S, Se) trigonal-prismatic chains that condense into layers, but their electronic structures exhibit significant differences leading to a broad spectrum of transport properties, ranging from metals with one, two, or three charge density wave instabilities to semimetals with potential topological properties or semiconductors. The different physical and chemical properties are shown to be related with subtle structural differences within the layers that result in half-, third-, or quarter-filled quasi-one-dimensional Nb d z 2 -type bands, providing a clear-cut illustration of the intimate link between structural and electronic features within a family of solids. An interesting yet not sufficiently explored feature of these solids is the polymorphism. Based on both experimental and new theoretical results, we examine this aspect for NbS 3 and show that at least seven different polymorphs with a stability compatible with the presently known phases of this compound are possible. We discuss a simple rationale for the physical properties of the presently known polymorphs as well as predictions for those that have still not been characterized or prepared. It is argued that some of the presently unknown polymorphs may have been prepared in an uncontrolled way as mixtures of different phases which could not be structurally characterized. The rich landscape of structures and properties found for this van der Waals material is suggested to represent an ideal platform for the preparation of flakes with finetuned properties for applications in new electronic and optoelectronic devices.
“…The calculated cell parameters, relative energy, and band gaps are reported in Table 1. One of them is the wellknown NbS 3 -I phase, 20 three correspond to the recently characterized NbS 3 -II, 19 NbS 3 -IV, 27 and NbS 3 -V 27 phases, and the remaining three are so-far unreported polymorphs with the structures of NbSe 3 , TiS 3 , and TaSe 3 . The agreement between experimental and theoretical structures for the four presently characterized compounds is excellent, thus lending reliability to these calculations.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…The unit cell of NbS 3 -II contains eight chains of Nb atoms trigonally coordinated with S atoms running along the b-direction (Figure 1d). There are four different types of NbS 3 chains which in order to simplify the discussion have been highlighted with different colors in Figure 1d (to help the comparison with experimental results, these colors are the same as those in the recent structural determination of the average structure 19 ). The purple and yellow chains are paired in the respective dimer units, whereas the red and orange chains form mixed red-orange pairs.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…1 Although different superstructures of the basic NbS 3 -I structure were proposed for this polymorph, a clear-cut structural determination remained elusive until recently (Figure 1d). 19 NbS 3 -II is metallic 23 and has been reported to exhibit three CDWs at around 450−475, 360, and 150 K, respectively. 24 This behavior is reminiscent of the NbSe 3 and m-TaS 3 systems, but now with an additional CDW transition.…”
Layered group V transition-metal trichalcogenides are paradigmatic low-dimensional materials providing an ever increasing series of unusual properties. They are all based on the same basic building units, one-dimensional MX 3 (M = Nb, Ta; X = S, Se) trigonal-prismatic chains that condense into layers, but their electronic structures exhibit significant differences leading to a broad spectrum of transport properties, ranging from metals with one, two, or three charge density wave instabilities to semimetals with potential topological properties or semiconductors. The different physical and chemical properties are shown to be related with subtle structural differences within the layers that result in half-, third-, or quarter-filled quasi-one-dimensional Nb d z 2 -type bands, providing a clear-cut illustration of the intimate link between structural and electronic features within a family of solids. An interesting yet not sufficiently explored feature of these solids is the polymorphism. Based on both experimental and new theoretical results, we examine this aspect for NbS 3 and show that at least seven different polymorphs with a stability compatible with the presently known phases of this compound are possible. We discuss a simple rationale for the physical properties of the presently known polymorphs as well as predictions for those that have still not been characterized or prepared. It is argued that some of the presently unknown polymorphs may have been prepared in an uncontrolled way as mixtures of different phases which could not be structurally characterized. The rich landscape of structures and properties found for this van der Waals material is suggested to represent an ideal platform for the preparation of flakes with finetuned properties for applications in new electronic and optoelectronic devices.
“…In a single batch of the crystal growth product, materials with different phases and compositions can coexist, which lead to challenges in studying and understanding both the growth mechanism and the physical properties of the material (4). Moreover, the charge density wave (CDW) transitions and therefore the associated periodic lattice distortions of NbS3 have been shown to depend on the material's crystal phase (5).…”
Section: Synthesis and Self-assembly Of One-dimensional Nanostructures Of A Transition Metal Trichalcogenidementioning
“…[58][59][60][61][62] The NbS 3-II polymorph was rst acknowledged in 1978 following electron diffraction experiments, with weak pair satellite diffraction streaks that resolve into rows of spots upon modications in temperature. 63,64 It is proposed that NbS 3-II is an elevated structure of NbS 3-I with different types of chain accretion, and the rows of spots arise at random positions with analogous separation to NbS 3-I (Table 2). NbS 3-II is testied to have three CDWs at 150 K, 330-370 K, and 620-650 K. 61 In 1982, Kikkawa and co-workers obtained monoclinic NbS 3-HP via the extraordinary high-pressure modi-cation of NbS 3 synthesized at 700 C with 2 GPa pressure.…”
Section: Crystal Structures and Properties Of V-x-type MXmentioning
The strong in-plane anisotropy and quasi-1D electronic structures of transition-metal trichalcogenides (MX3; M = group IV or V transition metal; X = S, Se, or Te) have pronounced influence on moulding the properties of MX3 materials.
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