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Quantum criticality in heavy-fermion metals

115/115 checkable references clean · checked 2026-09-08

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.

12 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 115 checked references that resolve

resolves10.1063/1.2169444

Why Is Ice Slippery?

resolves10.1038/nature03279

Quantum criticality

resolves10.1103/RevModPhys.73.797

Non-Fermi-liquid behavior in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>d</mml:mi></mml:math>- and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>f</mml:mi></mml:math>-electron metals

resolves10.1103/RevModPhys.79.1015

Fermi-liquid instabilities at magnetic quantum phase transitions

resolves10.1103/PhysRevLett.72.3262

Non-Fermi-liquid behavior in a heavy-fermion alloy at a magnetic instability

resolves10.1038/35030039

Onset of antiferromagnetism in heavy-fermion metals

resolves10.1103/PhysRevLett.85.626

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>YbRh</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>: Pronounced Non-Fermi-Liquid Effects above a Low-Lying Magnetic Phase Transition

resolves10.1103/PhysRevB.14.1165

Quantum critical phenomena

resolves10.1103/PhysRevB.48.7183

Effect of a nonzero temperature on quantum critical points in itinerant fermion systems

resolves10.1143/JPSJ.64.960

Anomalous Properties around Magnetic Instability in Heavy Electron Systems

resolves10.1038/35101507

Locally critical quantum phase transitions in strongly correlated metals

resolves10.1088/0953-8984/13/35/202

How do Fermi liquids get heavy and die?

resolves10.1103/PhysRevB.69.035111

Weak magnetism and non-Fermi liquids near heavy-fermion critical points

resolves10.1103/PhysRevLett.35.1779

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>4</mml:mn><mml:mi>f</mml:mi></mml:math>-Virtual-Bound-State Formation in Ce<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Al</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>at Low Temperatures

resolves10.1103/PhysRevLett.43.1892

Superconductivity in the Presence of Strong Pauli Paramagnetism: Ce<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>2</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">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1103/PhysRevLett.52.469

Superconductivity in Ce<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>2</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">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Single Crystals

resolves10.1103/PhysRevLett.50.1595

U <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">Be</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>13</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> : An Unconventional Actinide Superconductor

resolves10.1103/PhysRevLett.52.679

Possibility of Coexistence of Bulk Superconductivity and Spin Fluctuations in U<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Pt</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1007/BF01323427

Superconductivity and magnetic order in a strongly interacting fermi-system: URu2Si2

resolves10.1143/PTP.32.37

Resistance Minimum in Dilute Magnetic Alloys

resolves10.1017/CBO9780511470752

The Kondo Problem to Heavy Fermions

resolves10.1063/1.1712502

Strongly Correlated Materials: Insights From Dynamical Mean-Field Theory

resolves10.1016/0378-4363(77)90190-5

The Kondo lattice and weak antiferromagnetism

resolves10.1103/RevModPhys.48.219

Mixed-valence compounds

resolves10.1103/PhysRevLett.67.2882

Evidence for non-Fermi liquid behavior in the Kondo alloy Y_{1-x}U_{x}Pd_{3}

resolves10.1103/PhysRevLett.67.2886

Observation of non-Fermi-liquid behavior in U_{0.2}Y_{0.8}Pd_{3}

resolves10.1103/PhysRevB.39.2344

Two-dimensional quantum Heisenberg antiferromagnet at low temperatures

resolves10.1103/PhysRevB.39.9734

Critical approach to the coherence transition in Kondo lattices

resolves10.1126/science.1091806

Deconfined Quantum Critical Points

resolves10.1103/PhysRevB.68.115103

Local fluctuations in quantum critical metals

resolves10.1103/PhysRevB.66.045111

Heavy-fermion and spin-liquid behavior in a Kondo lattice with magnetic frustration

resolves10.1103/PhysRevLett.91.156404

Continuous Quantum Phase Transition in a Kondo Lattice Model

resolves10.1103/PhysRevLett.99.227203

Magnetic Quantum Phase Transition in an Anisotropic Kondo Lattice

resolves10.1103/PhysRevLett.99.227204

Zero-Temperature Magnetic Transition in an Easy-Axis Kondo Lattice Model

resolves10.1103/PhysRevLett.91.066404

Universally Diverging Grüneisen Parameter and the Magnetocaloric Effect Close to Quantum Critical Points

resolves10.1103/PhysRevB.72.205129

Sign change of the Grüneisen parameter and magnetocaloric effect near quantum critical points

resolves10.1103/PhysRevLett.91.066405

Divergence of the Grüneisen Ratio at Quantum Critical Points in Heavy Fermion Metals

resolves10.1103/PhysRevLett.96.256403

Quantum Criticality in the Cubic Heavy-Fermion System <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:msub> <mml:mi>CeIn</mml:mi> <mml:mrow> <mml:mn>3</mml:mn> <mml:mo>−</mml:mo> <mml:mi>x</mml:mi> </mml:mrow> </mml:msub> <mml:msub> <mml:mi>Sn</mml:mi> <mml:mi>x</mml:mi> </mml:msub> </mml:math>

resolves10.1103/PhysRevLett.96.136402

Metamagnetic Quantum Criticality in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>Sr</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:msub><mml:mi>Ru</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>7</mml:mn></mml:msub></mml:math>Studied by Thermal Expansion

resolves10.1126/science.1136020

Multiple Energy Scales at a Quantum Critical Point

resolves10.1103/PhysRevLett.94.066402

Fractionalization and Fermi-Surface Volume in Heavy-Fermion Compounds: The Case of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">Y</mml:mi><mml:mi mathvariant="normal">b</mml:mi><mml:mi mathvariant="normal">R</mml:mi><mml:mi mathvariant="normal">h</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">S</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.93.096402

Grüneisen Ratio Divergence at the Quantum Critical Point in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">u</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">A</mml:mi><mml:mi mathvariant="normal">g</mml:mi></mml:mrow><mml:mi>x</mml:mi></mml:msub></mml:math>

resolves10.1103/PhysRevLett.63.1996

Phenomenology of the normal state of Cu-O high-temperature superconductors

resolves10.1103/PhysRevLett.75.725

Non-Fermi-Liquid Scaling of the Magnetic Response in UCu<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>5</mml:mn><mml:mo>−</mml:mo><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>Pd</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi/><mml:mo>(</mml:mo><mml:mi mathvariant="italic">x</mml:mi><mml:mspace/><mml:mo>=</mml:mo><mml:mspace/><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mn>1.5</mml:mn><mml:mn/><mml:mo>)</mml:mo></mml:math>

resolves10.1103/PhysRevLett.80.5627

Two-Dimensional Fluctuations at the Quantum-Critical Point of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>CeCu</mml:mi></mml:mrow><mml:mrow><mml:mn>6</mml:mn><mml:mo>−</mml:mo><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>Au</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1103/PhysRevLett.94.076402

Ferromagnetic Quantum Critical Fluctuations in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">Y</mml:mi> <mml:mi mathvariant="normal">b</mml:mi> <mml:mi mathvariant="normal">R</mml:mi> <mml:mi mathvariant="normal">h</mml:mi> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> <mml:mo stretchy="false">(</mml:mo> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">S</mml:mi> <mml:mi mathvariant="normal">i</mml:mi> </mml:mrow> <mml:mn>0.95</mml:mn> </mml:msub> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">G</mml:mi> <mml:mi mathvariant="normal">e</mml:mi> </mml:mrow> <mml:mn>0.05</mml:mn> </mml:msub> <mml:msub> <mml:mo stretchy="false">)</mml:mo> <mml:mn>2</mml:mn> </mml:msub> </mml:math>

resolves10.1143/JPSJ.77.093712

YbRh2Si2: Quantum Tricritical Behavior in Itinerant Electron Systems

resolves10.1103/PhysRevLett.91.156401

Low Temperature Electron Spin Resonance of the Kondo Ion in a Heavy Fermion Metal: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">Y</mml:mi> <mml:mi mathvariant="normal">b</mml:mi> <mml:mi mathvariant="normal">R</mml:mi> <mml:mi mathvariant="normal">h</mml:mi> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mrow> <mml:mi mathvariant="normal">S</mml:mi> <mml:mi mathvariant="normal">i</mml:mi> </mml:mrow> <mml:mn>2</mml:mn> </mml:msub> </mml:math>

resolves10.1103/PhysRevLett.96.016401

Quantum Critical Point of an Itinerant Antiferromagnet in a Heavy Fermion

resolves10.1038/nature01774

The break-up of heavy electrons at a quantum critical point

resolves10.1103/PhysRevLett.81.1501

Breakup of Heavy Fermions on the Brink of “Phase<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="italic">A</mml:mi></mml:math>” in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>CeCu</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mi>Si</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1103/PhysRevB.51.9253

Resistivity as a function of temperature for models with hot spots on the Fermi surface

resolves10.1103/PhysRevLett.82.4280

Interplay of Disorder and Spin Fluctuations in the Resistivity near a Quantum Critical Point

resolves10.1016/S0921-4526(97)81588-8

Scaling of the “Cp α T 1nT” dependence in Ce systems

resolves10.1038/nature03129

Hall-effect evolution across a heavy-fermion quantum critical point

resolves10.1103/PhysRevLett.90.116601

Hall Effect in Nested Antiferromagnets near the Quantum Critical Point

resolves10.1103/PhysRevLett.92.187201

High Resolution Study of Magnetic Ordering at Absolute Zero

resolves10.1143/JPSJ.74.1103

A Drastic Change of the Fermi Surface at a Critical Pressure in CeRhIn5: dHvA Study under Pressure

resolves10.1038/nature04571

Hidden magnetism and quantum criticality in the heavy fermion superconductor CeRhIn5

resolves10.1103/PhysRevLett.98.026402

Kondo Breakdown and Hybridization Fluctuations in the Kondo-Heisenberg Lattice

resolves10.1038/nature01044

Quantum phase transition in a common metal

resolves10.1103/PhysRevB.69.014415

Magnetic field induced non-Fermi-liquid behavior in YbAgGe single crystals

resolves10.1103/PhysRevB.72.172413

Field-dependent Hall effect in single-crystal heavy-fermion YbAgGe below<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mn>1</mml:mn><mml:mspace width="0.3em"/><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math>

resolves10.1103/PhysRevB.73.094435

Low-temperature thermodynamic properties of the heavy-fermion compound YbAgGe close to the field-induced quantum critical point

resolves10.1143/JPSJ.69.3955

Enhanced Valence Fluctuations Caused by f-c Coulomb Interaction in Ce-Based Heavy Electrons: Possible Origin of Pressure-Induced Enhancement of Superconducting Transition Temperature in CeCu2Ge2and Related Compounds

resolves10.1016/0375-9601(92)90860-O

Pressure induced heavy fermion superconductivity of CeCu2Ge2

resolves10.1126/science.1091648

Observation of Two Distinct Superconducting Phases in CeCu 2 Si 2

resolves10.1038/35066519

Strong coupling between local moments and superconducting ‘heavy’ electrons in UPd2Al3

resolves10.1038/35020500

Superconductivity on the border of itinerant-electron ferromagnetism in UGe2

resolves10.1126/science.1115498

Magnetic Field-Induced Superconductivity in the Ferromagnet URhGe

resolves10.1103/PhysRevLett.99.067006

Superconductivity on the Border of Weak Itinerant Ferromagnetism in UCoGe

resolves10.1103/PhysRevLett.92.136401

Nature of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>A</mml:mi></mml:math>Phase in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi>CeCu</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi>Si</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:math>

resolves10.1038/27838

Magnetically mediated superconductivity in heavy fermion compounds

resolves10.1103/PhysRevB.34.8190

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>d</mml:mi></mml:math>-wave pairing near a spin-density-wave instability

resolves10.1088/0953-8984/13/17/103

Heavy-fermion superconductivity in CeCoIn 5 at 2.3 K

resolves10.1016/j.physc.2004.02.070

Non-Fermi liquid normal state of the heavy-fermion superconductor UBe13

resolves10.1126/science.1140970

Is There Glue in Cuprate Superconductors?

resolves10.1103/PhysRevLett.99.016401

Fermi Surface and Antiferromagnetism in the Kondo Lattice: An Asymptotically Exact Solution in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>d</mml:mi><mml:mo>></mml:mo><mml:mn>1</mml:mn></mml:math>Dimensions

resolves10.1016/j.physb.2006.01.156

Global magnetic phase diagram and local quantum criticality in heavy fermion metals

resolves10.1143/JPSJ.76.051003

Recent Advances in Ce-Based Heavy-Fermion Superconductivity and Fermi Surface Properties

resolves10.1103/PhysRevLett.89.056402

Magnetic-Field Induced Quantum Critical Point in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi/><mml:mi mathvariant="normal">Y</mml:mi><mml:mi mathvariant="normal">b</mml:mi><mml:mi mathvariant="normal">R</mml:mi><mml:msub><mml:mi mathvariant="normal">h</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">S</mml:mi><mml:msub><mml:mi mathvariant="normal">i</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevB.66.024426

Critical local-moment fluctuations in the Bose-Fermi Kondo model

resolves10.1103/PhysRevB.66.024427

Quantum phase transitions in the Bose-Fermi Kondo model

resolves10.1103/PhysRevLett.90.157203

Pseudogap Fermi-Bose Kondo Model

resolves10.1103/PhysRevLett.95.067202

Numerical Renormalization-Group Study of the Bose-Fermi Kondo Model

resolves10.1103/PhysRevLett.100.026403

Scaling and Enhanced Symmetry at the Quantum Critical Point of the Sub-Ohmic Bose-Fermi Kondo Model

resolves10.1103/PhysRevLett.95.207207

Undressing the Kondo Effect near the Antiferromagnetic Quantum Critical Point

resolves10.1103/PhysRevLett.96.016601

Schwinger Boson Approach to the Fully Screened Kondo Model

resolves10.1103/PhysRevB.74.020501

Coexistence of antiferromagnetism and superconductivity in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="normal">Ce</mml:mi><mml:mi mathvariant="normal">Rh</mml:mi><mml:msub><mml:mi mathvariant="normal">In</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:mrow></mml:math>under high pressure and magnetic field

resolves10.1103/PhysRevLett.91.246405

Field-Induced Quantum Critical Point in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">o</mml:mi><mml:mi mathvariant="normal">I</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:mrow><mml:mn>5</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.91.257001

Avoided Antiferromagnetic Order and Quantum Critical Point in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">o</mml:mi><mml:mi mathvariant="normal">I</mml:mi><mml:msub><mml:mi mathvariant="normal">n</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.98.057001

Probing the Quantum Critical Behavior of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>CeCoIn</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math>via Hall Effect Measurements

resolves10.1103/PhysRevLett.100.136401

Dimensional Crossover of Quantum Critical Behavior in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>CeCoIn</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.97.056404

Reversible Tuning of the Heavy-Fermion Ground State in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>CeCoIn</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.82.1293

Non-Fermi-Liquid Effects at Ambient Pressure in a Stoichiometric Heavy-Fermion Compound with Very Low Disorder:<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>CeNi</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>Ge</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1002/andp.19925040203

Local‐moment and itinerant antiferromagnetism in the heavy‐fermion system Ce(Cu1−xNix)2Ge2

resolves10.1103/PhysRevB.70.174401

Anomalous scaling behavior of the dynamical spin susceptibility of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ce</mml:mi></mml:mrow><mml:mrow><mml:mn>0.925</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>0.075</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ru</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">Si</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow></mml:math>

resolves10.1103/PhysRevLett.91.087202

Extended versus Local Fluctuations in Quantum Critical<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msub><mml:mrow><mml:mi mathvariant="normal">R</mml:mi><mml:mi mathvariant="normal">u</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">F</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:mrow><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">G</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:math>(<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>x</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn>0.76</mml:mn></mml:math>)

resolves10.1103/PhysRevB.58.R15959

Disappearance of hyperscaling at low temperatures in non-Fermi-liquid<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">CeCu</mml:mi></mml:mrow><mml:mrow><mml:mn>5.2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ag</mml:mi></mml:mrow><mml:mrow><mml:mn>0.8</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1103/PhysRevLett.99.237203

Magnetic Fluctuations at a Field-Induced Quantum Phase Transition

resolves10.1103/RevModPhys.77.579

How generic scale invariance influences quantum and classical phase transitions

resolves10.1103/PhysRevLett.84.5608

Spin-Fermion Model near the Quantum Critical Point: One-Loop Renormalization Group Results

resolves10.1103/PhysRevLett.82.2963

Doniach Phase Diagram, Revisited: From Ferromagnet to Fermi Liquid in Pressurized<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>CeRu</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mi>Ge</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi/></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

resolves10.1103/PhysRevB.67.224419

Magnetic phase diagram of the ferromagnetic Kondo-lattice compound<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">CeAgSb</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>up to 80 kbar

resolves10.1038/nature01968

Fermi-liquid breakdown in the paramagnetic phase of a pure metal

resolves10.1103/PhysRevLett.93.256404

Quantum Phase Transitions in the Itinerant Ferromagnet<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">Z</mml:mi><mml:mi mathvariant="normal">r</mml:mi><mml:mi mathvariant="normal">Z</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.98.047204

Metallic State in Cubic FeGe Beyond Its Quantum Phase Transition

resolves10.1103/PhysRevLett.88.217204

Metamagnetic Quantum Criticality in Metals

resolves10.1126/science.1063539

Magnetic Field-Tuned Quantum Criticality in the Metallic Ruthenate Sr 3 Ru 2 O 7

resolves10.1126/science.1104306

Disorder-Sensitive Phase Formation Linked to Metamagnetic Quantum Criticality

resolves10.1016/S0921-4526(02)01126-2

Itinerant metamagnetism of CeRu2Si2: bringing out the dead. Comparison with the new Sr3Ru2O7 case

resolves10.1016/j.physb.2004.12.059

Search for a quantum critical end-point in CeRu(SiGe)

resolves10.1103/PhysRevLett.96.026401

Continuous Evolution of the Fermi Surface of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>CeRu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Si</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>across the Metamagnetic Transition

resolves10.1103/PhysRevLett.91.256401

Magnetic-Field-Induced Quantum Critical Point and Competing Order Parameters in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">U</mml:mi><mml:mi mathvariant="normal">R</mml:mi><mml:mi mathvariant="normal">u</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi mathvariant="normal">S</mml:mi><mml:mi mathvariant="normal">i</mml:mi></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:math>

resolves10.1103/PhysRevLett.94.226402

Field-Induced Suppression of the Heavy-Fermion State in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>YbRh</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Si</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>

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