87 research outputs found
Low-Frequency Raman Modes and Electronic Excitations In Atomically Thin MoS2 Crystals
Atomically thin MoS crystals have been recognized as a quasi-2D
semiconductor with remarkable physics properties. This letter reports our Raman
scattering measurements on multilayer and monolayer MoS, especially in
the low-frequency range (50 cm). We find two low-frequency Raman
modes with contrasting thickness dependence. With increasing the number of
MoS layers, one shows a significant increase in frequency while the other
decreases following a 1/N (N denotes layer-number) trend. With the aid of
first-principle calculations we assign the former as the shear mode
and the latter as the compression vibrational mode. The opposite
evolution of the two modes with thickness demonstrates novel vibrational modes
in atomically thin crystal as well as a new and more precise way to
characterize thickness of atomically thin MoS films. In addition, we
observe a broad feature around 38 cm (~5 meV) which is visible only
under near-resonance excitation and pinned at the fixed energy independent of
thickness. We interpret the feature as an electronic Raman scattering
associated with the spin-orbit coupling induced splitting in conduction band at
K points in their Brillouin zone.Comment: 5 pages, 4 figure
4-[(5-Chloro-3-methyl-1-phenyl-1H-pyrazol-4-yl)methylideneamino]-1,5-dimethyl-2-phenyl-1H-pyrazol-3(2H)-one
In the molecule of the title compound, C22H20ClN5O, the atoms of the two pyrazole rings and the –C=N– group which joins them are essentially coplanar, with an r.m.s. deviation of 0.054 (2) Å. The phenyl rings form dihedral angles of 41.24 (5) and 55.53 (5)° with this plane. The crystal structure is stabilized by weak intermolecular π–π interactions, with centroid-to-centroid distances of 3.6179 (13) Å between the imidazole rings
Bis[4-(1-iminoethyl)-3-methyl-1-phenyl-1H-pyrazol-5-olato-κ2 O,N 4]copper(II)
In the title complex, [Cu(C12H12N3O)2], the CuII ion is tetracoordinated by two N atoms and two O atoms from two bis-chelating 4-(1-iminoethyl)-3-methyl-1-phenyl-1H-pyrazol-5-olate ligands in a square-planar geometry. The two N atoms and two O atoms around the CuII atom are trans to each other, as the CuII atom lies on an inversion centre. The six-membered ring composed of the Cu, an O, an N and three C atoms of the ligand and the pyrazole ring is nearly planar, the largest deviation being 0.037 (4) Å for an N atom. In the crystal, weak intermolecular C—H⋯N hydrogen-bonding interactions link the molecules into chains along the c axis
Bis(4-acetyl-3-methyl-1-phenyl-1H-pyrazol-5-olato-κ2 O,O′)bis(N,N-dimethylformamide-κO)nickel(II)
The title complex, [Ni(C12H11N2O2)2(C3H7NO)2], lies on on an inversion center. The NiII ion is coordinated in a slightly distorted octahedral coordination enviroment by four O atoms from two bis-chelating 4-acety-3-methyl-1-phenyl-1H-pyrazol-5-olate ligands in the equatorial plane and two O atoms from two N,N-dimethylformamide ligands in the axial sites. In the crystal structure, weak intermolecular π–π stacking interactions with centroid–centroid distances of 3.7467 (13) Å link molecules into chains extending alongthe b axis
Methyl 2-{[(3-methyl-5-oxo-1-phenyl-4,5-dihydro-1H-pyrazol-4-ylidene)(thiophen-2-yl)methyl]amino}-3-phenylpropionate
In the title compound, C25H23N3O3S, an intramolecular N—H⋯O interaction generates an S(6) ring, which stabilizes the enamine–keto form of the compound. This S(6) ring and the pyrazole ring are essentially coplanar, making a dihedral angle of 1.49 (6)°. The bond lengths within the S(6) ring of the molecule lie between classical single- and double-bond lengths, indicating extensive conjugation. The structure exhibits a thienyl-ring flip disorder, with occupancy factors in the ratio 64.7 (3):35.3 (3)
Anomalously Robust Valley Polarization and Valley Coherence in Bilayer WS2
Coherence is a crucial requirement to realize quantum manipulation through
light-matter interactions. Here we report the observation of anomalously robust
valley polarization and valley coherence in bilayer WS2. The polarization of
the photoluminescence from bilayer WS2 inherits that of the excitation source
with both circularly and linearly polarized and retains even at room
temperature. The near unity circular polarization of the luminescence reveals
the coupling of spin, layer and valley degree of freedom in bilayer system,
while the linear polarized photoluminescence manifests quantum coherence
between the two inequivalent band extrema in momentum space, namely, the valley
quantum coherence in atomically thin bilayer WS2. This observation opens new
perspectives for quantum manipulation in atomically thin semiconductors
1,5-Dimethyl-4-{[(3-methyl-5-oxo-1-phenyl-4,5-dihydro-1H-pyrazol-4-ylidene)(thiophen-2-yl)methyl]amino}-2-phenyl-1H-pyrazol-3(2H)-one
In the title compound, C26H23N5O2S, an intramolecular N—H⋯O interaction generates an S(6) ring. The essentially planar S(6) and pyrazole rings [maximum deviations = −0.0270 (14) and 0.0195 (15) Å, respectively] are nearly coplanar, making a dihedral angle of 3.94 (6)°. The S(6) ring makes dihedral angles of 23.79 (6), 78.53 (6) and 67.91 (6)° with the pyrazolone ring, the pyrazole ring and the benzene ring of antipyrine, respectively. The structure exhibits a thienyl-ring flip disorder with occupancy factors in the ratio 0.82:0.18
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