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First‐order Raman scattering in three‐layered Mo‐based ternaries: MoAlB, Mo<sub>2</sub>Ga<sub>2</sub>C and Mo<sub>2</sub>GaC

https://doi.org/10.1002/jrs.5087
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Every reference with a DOI in the deposited reference list resolved to a known work in Crossref or DataCite at the dated check, and none carried a retraction, withdrawal, or removal notice.

The 41 checked references that resolve
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Ternary Borides Cr <sub>2</sub> AlB <sub>2</sub> , Cr <sub>3</sub> AlB <sub>4</sub> , and Cr <sub>4</sub> AlB <sub>6</sub> : The First Members of the Series (CrB <sub>2</sub> ) <sub> <i>n</i> </sub> CrAl with <i>n</i> = 1, 2, 3 and a Unifying Concept for Ternary Borides as MAB-Phases
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Infrared and Raman Selection Rules for Lattice Vibrations: The Correlation Method
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Origin of the <i>c</i>-axis ultraincompressibility of Mo2GaC above about 15 GPa from first principles
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New ternary nanolaminated carbide Mo2Ga2C: A first-principles comparison with the MAX phase counterpart Mo2GaC
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Synthesis and Characterization of 2D Molybdenum Carbide (MXene)
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Mo <sub>2</sub> Ga <sub>2</sub> C: a new ternary nanolaminated carbide
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On the Rapid Synthesis of the Ternary Mo <sub>2</sub> GaC
resolves10.1007/BF00902599
Die Kristallstruktur von MoAlB
resolves10.1088/1468-6996/15/1/014208
The effect of the interlayer element on the exfoliation of layered Mo <sub>2</sub> AC (A = Al, Si, P, Ga, Ge, As or In) MAX phases into two-dimensional Mo <sub>2</sub> C nanosheets
resolves10.1103/PhysRev.140.A1133
Self-Consistent Equations Including Exchange and Correlation Effects
resolves10.1038/srep26475
Synthesis and Characterization of an Alumina Forming Nanolaminated Boride: MoAlB
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resolves10.1016/j.actamat.2015.07.063
Structural and chemical determination of the new nanolaminated carbide Mo2Ga2C from first principles and materials analysis
resolves10.1002/jrs.3101
First‐order Raman scattering of the MAX phases Ta<sub>4</sub>AlC<sub>3</sub>, Nb<sub>4</sub>AlC<sub>3</sub>, Ti<sub>4</sub>AlN<sub>3</sub>, and Ta<sub>2</sub>AlC
resolves10.1557/JMR.2007.0376
On Raman scattering from selected <i>M</i><sub>2</sub><i>A</i>C compounds
resolves10.1016/j.actamat.2006.02.052
Atomic-scale microstructures of Zr2Al3C4 and Zr3Al3C5 ceramics
resolves10.1080/21663831.2016.1245682
Atomic structure and lattice defects in nanolaminated ternary transition metal borides
resolves10.1002/pssr.201409543
Theoretical stability, thin film synthesis and transport properties of the Mo<sub><i>n</i> +1</sub>GaC<i><sub>n</sub></i> MAX phase
resolves10.1016/j.scriptamat.2015.07.003
Synthesis of two-dimensional molybdenum carbide, Mo 2 C, from the gallium based atomic laminate Mo 2 Ga 2 C
resolves10.1016/j.jcrysgro.2013.12.061
Polarized Raman spectra in β-Ga2O3 single crystals
resolves10.1016/j.jcrysgro.2013.09.021
High temperature solution growth and characterization of Cr2AlC single crystals
resolves10.1103/PhysRevLett.77.3865
Generalized Gradient Approximation Made Simple
resolves10.1002/jrs.3036
First‐order Raman scattering of the MAX phases: Ti<sub>2</sub>AlN, Ti<sub>2</sub>AlC<sub>0.5</sub>N<sub>0.5</sub>, Ti<sub>2</sub>AlC, (Ti<sub>0.5</sub>V<sub>0.5</sub>)<sub>2</sub>AlC, V<sub>2</sub>AlC, Ti<sub>3</sub>AlC<sub>2</sub>, and Ti<sub>3</sub>GeC<sub>2</sub>
resolves10.1002/jrs.4325
Erratum: First‐order Raman scattering of the MAX phases: Ti<sub>2</sub>AlN, Ti<sub>2</sub>AlC<sub>0.5</sub> N<sub>0.5</sub>, Ti<sub>2</sub>AlC, (Ti<sub>0.5</sub> V<sub>0.5</sub>)<sub>2</sub>AlC, V<sub>2</sub>AlC, Ti<sub>3</sub>AlC<sub>2</sub>, and Ti<sub>3</sub>GeC<sub>2</sub>
resolves10.1002/jrs.1250100152
Normal mode determination in crystals
resolves10.1016/j.physc.2010.04.010
Structural, elastic, electronic properties and Fermi surface for superconducting Mo2GaC in comparison with V2GaC and Nb2GaC from first principles
resolves10.1002/pssb.201046163
Elastic properties of superconducting MAX phases from first‐principles calculations
resolves10.1016/j.actamat.2014.10.018
Synthesis of single crystals of V2AlC phase by high-temperature solution growth and slow cooling technique
resolves10.1103/PhysRevB.71.012103
Vibrational behavior of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mi>A</mml:mi><mml:msub><mml:mi>X</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow></mml:math>phases from first-order Raman scattering<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mo>(</mml:mo><mml:mi>M</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Ti</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">V</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">Cr</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Si</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>X</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">C</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">N</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math>
resolves10.1103/PhysRevB.81.174301
First-principles phonon calculations of thermal expansion in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>Ti</mml:mtext> </mml:mrow> <mml:mn>3</mml:mn> </mml:msub> <mml:msub> <mml:mrow> <mml:mtext>SiC</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>Ti</mml:mtext> </mml:mrow> <mml:mn>3</mml:mn> </mml:msub> <mml:msub> <mml:mrow> <mml:mtext>AlC</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math> , and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>Ti</mml:mtext> </mml:mrow> <mml:mn>3</mml:mn> </mml:msub> <mml:msub> <mml:mrow> <mml:mtext>GeC</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math>
resolves10.1103/PhysRevB.78.134106
First-principles calculations of the ferroelastic transition between rutile-type and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>CaCl</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math> -type <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mtext>SiO</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math> at high pressures
resolves10.1016/0022-5088(67)90055-0
High superconducting transition temperatures in the molybdenum carbide family of compounds
resolves10.1063/1.1873057
Raman active phonon modes and heat capacities of Ti2AlC and Cr2AlC ceramics: first-principles and experimental investigations
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