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Anharmonicity and the inverse isotope effect in the palladium-hydrogen system
45/45 checkable references clean · checked 2026-07-23
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.
7 without a DOI — not checked. A reference deposited without a DOI is never matched by title or guessed at; it stays outside the checked set, and this line discloses that.
The 45 checked references that resolve
resolves10.1016/0022-5088(87)90116-0
Electronic structure and total energy calculations for transition metal hydrides
resolves10.1088/0305-4608/12/1/013
Bond analysis of heats of formation: application to some group VIII and IB hydrides
resolves10.1002/pssa.2210110253
Superconductivity in the palladium-hydrogen and palladium-nickel-hydrogen systems
resolves10.1007/BF01391800
High frequency local modes, superconductivity and anomalous isotope effect in PdH(D) systems
resolves10.1103/PhysRevLett.39.574
Inverse Isotope Effect and the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>x</mml:mi></mml:math>Dependence of the Superconducting Transition Temperature in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevB.17.141
Band structure and superconductivity of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevB.18.2784
Coherent-potential-approximation calculations for<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevLett.33.1297
Lattice Dynamics of a Single Crystal of Pd<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mn>0.63</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevB.17.488
Inelastic-neutron-scattering line shapes in Pd<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mn>0.63</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevLett.34.144
Electronic Model for the Reverse Isotope Effect in Superconducting Pd-H(D)
resolves10.1103/PhysRevB.29.4140
Effect of zero-point motion on the superconducting transition temperature of PdH(D)
resolves10.1103/PhysRevLett.57.2955
Isotope Effects in the PdH System: Lattice Dynamics of Pd<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">T</mml:mi></mml:mrow><mml:mrow><mml:mn>0.7</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevB.41.282
Anomalous oxygen isotope effect in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi mathvariant="normal">−</mml:mi><mml:mi mathvariant="normal">x</mml:mi></mml:mrow></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:mi mathvariant="normal">Sr</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">x</mml:mi></mml:mrow></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:mi mathvariant="normal">CuO</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1126/science.250.4986.1390
Oxygen Isotope Effect and Structural Phase Transitions in La
<sub>2</sub>
CuO
<sub>4</sub>
-Based Superconductors
resolves10.1103/PhysRevLett.67.228
Lattice instabilities, isotope effect, and high-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="italic">T</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>superconductivity in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi mathvariant="normal">−</mml:mi><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></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:mi mathvariant="normal">Ba</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></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:mi mathvariant="normal">CuO</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRevB.24.864
Full-potential self-consistent linearized-augmented-plane-wave method for calculating the electronic structure of molecules and surfaces:<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>molecule
resolves10.1103/PhysRevLett.42.662
Semiconductor Charge Densities with Hard-Core and Soft-Core Pseudopotentials
resolves10.1103/PhysRevLett.55.1200
Local-Density-Functional Calculation of the Pressure-Induced Metallization of BaSe and BaTe
resolves10.1103/PhysRevB.32.7792
Linearized augmented-plane-wave calculation of the electronic structure and total energy of tungsten
resolves10.1002/pssb.2221440259
The Isotope Effect within the Anharmonic Model for High‐T<sub>c</sub> Superconductors
resolves10.1103/PhysRevLett.60.2191
Possible Origins of High-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>Superconductivity
resolves10.1103/PhysRevB.19.2540
Theory of the isotope effect in superconducting compounds: PdD and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Mo</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></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:mi mathvariant="normal">Se</mml:mi></mml:mrow><mml:mrow><mml:mn>8</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1016/0921-4526(91)90434-G
Ab initio pseudopotential calculations of total energies and forces for hydrogen in palladium
resolves10.1103/PhysRevLett.28.801
Electron-Phonon Interactions,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>d</mml:mi></mml:math>Resonances, and Superconductivity in Transition Metals
resolves10.1088/0305-4608/3/1/015
A simple theory of the electron-phonon mass enhancement in transition metals
resolves10.1088/0305-4608/6/6/026
On calculating the electron-phonon mass enhancement lambda for compounds
resolves10.1016/0375-9601(87)90744-4
On the critical temperature for any strength of the electron-phonon coupling
resolves10.1103/PhysRevB.12.117
Lattice constants of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>β</mml:mi><mml:mo>−</mml:mo><mml:mi mathvariant="normal">P</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>β</mml:mi><mml:mo>−</mml:mo><mml:mi mathvariant="normal">P</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>with<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>x</mml:mi></mml:math>near 1.0
resolves10.1103/PhysRevB.20.1339
Elastic constants of palladium and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>β</mml:mi></mml:math>-phase palladium hydride between 4 and 300 K
resolves10.1103/PhysRevB.26.1637
Contribution of optical phonons to the elastic moduli of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>
resolves10.1103/PhysRev.153.673
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>s</mml:mi><mml:mo>−</mml:mo><mml:mi>d</mml:mi></mml:math>Interaction in Transition Metals
resolves10.1002/pssb.2220630102
Effects of Pressure on the Electronic Structure of Transition d‐Metals
resolves10.1103/PhysRevB.10.3818
Concentration dependence of the superconducting transition temperature in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">H</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">D</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>
The 7 references without a DOI — listed, not checked
no DOI — not checkedMetals I
no DOI — not checkedPhysRevB.45.12405Cc10R1
no DOI — not checkedPhysRevB.45.12405Cc13R1
no DOI — not checkedPhysRevB.45.12405Cc18R1
no DOI — not checkedPhysRevB.45.12405Cc22R1
no DOI — not checkedProceedings of the Second Rochester Conference on Superconductivity in d- and f-Band Metals
no DOI — not checkedSuperconductivity in d- and f-Band Metals 1982
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