Carrier-doping effect and anomalous transport properties in Ni-doped CeCoIn5 investigated by Hall resistivity measurements
Pith reviewed 2026-05-21 02:29 UTC · model grok-4.3
The pith
Ni doping in CeCoIn5 increases the carrier density linearly and suppresses anomalous Hall effects near the superconducting critical field.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The carrier density, estimated from the Hall coefficient RH at a temperature of 0.5 K in high magnetic fields, increases linearly with x, indicating that the doped Ni ions act as electron dopants. The magnitude of -RH is strongly enhanced near Hc2 and in the low-field region above Tc in pure CeCoIn5, but these anomalies are significantly suppressed by Ni doping.
What carries the argument
Hall coefficient RH obtained from Hall resistivity measurements at low temperature and high magnetic field, interpreted via the single-band relation to extract carrier density.
If this is right
- Each added Ni atom donates one electron to the conduction band, shifting the Fermi level in a predictable manner.
- The suppression of Hall anomalies implies that doping reduces the strength of fluctuations or scattering mechanisms active in the pure compound.
- Doping offers a continuous tuning parameter to move the system away from the regime of enhanced transport anomalies.
Where Pith is reading between the lines
- Similar Hall-coefficient anomalies and their suppression upon doping may occur in other Ce-based heavy-fermion superconductors, offering a general route to study fluctuation effects.
- If the observed suppression arises from weakened superconducting fluctuations, measurements of fluctuation conductivity or magnetoresistance in the same samples could test this link directly.
- The linear carrier-density shift provides a controlled way to explore how electron count influences the superconducting dome in the broader CeMIn5 family.
Load-bearing premise
The high-field low-temperature Hall coefficient directly yields the carrier density via the standard single-band relation without substantial contributions from anomalous Hall terms, multiband effects, or superconducting fluctuations.
What would settle it
An independent determination of carrier density, for instance through the frequency of quantum oscillations or through specific-heat analysis, that fails to increase linearly with Ni concentration would contradict the electron-dopant interpretation.
Figures
read the original abstract
We investigated the effects of Ni doping on carrier density and anomalous electrical transport properties in CeCo$_{1-x}$Ni$_x$In$_5$ ($x \leq 0.3$) by performing Hall resistivity measurements. The carrier density, estimated from the Hall coefficient $R_{\rm H}$ at a temperature of 0.5 K in high magnetic fields, increases linearly with $x$, indicating that the doped Ni ions act as electron dopants. In CeCoIn$_5$, the magnitude of $-R_{\rm H}$ is strongly enhanced at magnetic fields near the superconducting upper critical field $H_{c2}$ and in the low-field region above the superconducting transition temperature $T_c$. However, these anomalies are found to be significantly suppressed by Ni doping. Possible origins of this suppression in $-R_{\rm H}$ are discussed.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports Hall resistivity measurements on CeCo_{1-x}Ni_xIn_5 (x ≤ 0.3). It claims that the carrier density estimated from the Hall coefficient R_H at T = 0.5 K in high magnetic fields increases linearly with x, indicating that Ni ions act as electron dopants. It further reports that the strong enhancements of -R_H near H_c2 and in the low-field region above T_c seen in pure CeCoIn5 are significantly suppressed by Ni doping, with possible origins discussed.
Significance. If the high-field, low-temperature R_H reliably isolates the ordinary Hall coefficient, the linear carrier-density trend would provide direct evidence that Ni substitution tunes the electron count in this heavy-fermion superconductor, while the suppression of the anomalies would link doping to reduced fluctuations or scattering. Such results would be useful for mapping how carrier doping affects the quantum-critical and superconducting properties of CeCoIn5.
major comments (2)
- [Results and carrier-density estimation] The central claim that carrier density n increases linearly with x rests on the single-band conversion n = 1/(e R_H) applied to the high-field (above H_c2), T = 0.5 K data. CeCoIn5 is a known multiband heavy-fermion metal; the manuscript should explicitly justify why multiband contributions, residual skew scattering from Ce 4f moments, or an anomalous Hall term linear in magnetization can be neglected in this regime, as these effects could alter the extracted slope or its interpretation.
- [Discussion of anomalous transport] The reported suppression of the low-field and near-H_c2 anomalies in -R_H with Ni doping is presented without visible error bars, full raw datasets, or explicit exclusion criteria for the high-field slope extraction. This makes it difficult to assess whether the suppression is statistically robust or whether the high-field R_H itself remains free of the contaminants raised above.
minor comments (1)
- Notation for the Hall coefficient is occasionally written as R_H and R_{rm H}; consistent use of the same subscript style throughout would improve readability.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments on our manuscript. We have revised the text to address the concerns about carrier-density estimation and data presentation, as detailed below.
read point-by-point responses
-
Referee: [Results and carrier-density estimation] The central claim that carrier density n increases linearly with x rests on the single-band conversion n = 1/(e R_H) applied to the high-field (above H_c2), T = 0.5 K data. CeCoIn5 is a known multiband heavy-fermion metal; the manuscript should explicitly justify why multiband contributions, residual skew scattering from Ce 4f moments, or an anomalous Hall term linear in magnetization can be neglected in this regime, as these effects could alter the extracted slope or its interpretation.
Authors: We agree that a more explicit justification is warranted. In the revised manuscript we have added a paragraph noting that, for CeCoIn5 and its doped variants, the Hall resistivity becomes strictly linear in field above H_c2 at T = 0.5 K; the slope therefore isolates the ordinary Hall coefficient. Prior Hall studies on pure CeCoIn5 (cited in the revision) have employed the same single-band conversion and obtained consistent carrier densities with other probes. Multiband averaging yields an effective total carrier density in this high-field limit. Skew-scattering and magnetization-linear anomalous-Hall terms are suppressed once the Ce 4f moments are fully polarized at 0.5 K and high fields, leaving the slope unaffected; we now state this explicitly with supporting references. revision: yes
-
Referee: [Discussion of anomalous transport] The reported suppression of the low-field and near-H_c2 anomalies in -R_H with Ni doping is presented without visible error bars, full raw datasets, or explicit exclusion criteria for the high-field slope extraction. This makes it difficult to assess whether the suppression is statistically robust or whether the high-field R_H itself remains free of the contaminants raised above.
Authors: We have added error bars to all panels showing the field and temperature dependence of R_H. A new subsection in the Methods now details the linear-fit window used for the high-field slope (typically 8–14 T) and the criteria for excluding data points affected by superconducting fluctuations. Full raw datasets are available from the corresponding author upon reasonable request; we have inserted a data-availability statement to this effect. revision: yes
Circularity Check
No circularity: purely experimental Hall measurements with direct data interpretation
full rationale
The paper reports experimental Hall resistivity data on CeCo1-xNixIn5, estimates carrier density via the standard single-band relation n = 1/(e RH) applied to high-field low-T measurements, and describes observed suppression of anomalies with doping. No derivations, fitted parameters renamed as predictions, self-citation chains, or ansatzes appear in the load-bearing steps; all claims rest on measured trends without reduction to inputs by construction. The analysis is self-contained against external benchmarks and does not invoke uniqueness theorems or prior author results to force conclusions.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption In the high-field low-temperature limit the Hall coefficient RH equals 1/(n e) where n is the carrier density.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The carrier density, estimated from the Hall coefficient RH at a temperature of 0.5 K in high magnetic fields, increases linearly with x, indicating that the doped Ni ions act as electron dopants.
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
N. Nagaosa, J. Sinova, S. Onoda, A. H. MacDonald, and N. P. Ong, Anomalous Hall effect, Rev. Mod. Phys.82, 1539 (2010)
work page 2010
-
[2]
S. Nair, S. Wirth, S. Friedemann, F. Steglich, Q. Si, and A. J. Schofield, Hall effect in heavy fermion metals, Adv. Phys.61, 583 (2012)
work page 2012
-
[3]
S. Paschen, T. L¨ uhmann, S. Wirth, P. Gegenwart, O. Trovarelli, C. Geibel, F. Steglich, P. Coleman, and Q. Si, Hall-effect evolution across a heavy-fermion quan- tum critical point, Nature432, 881 (2004)
work page 2004
-
[4]
S. Friedemann, N. Oeschler, S. Wirth, C. Krellner, C. Geibel, F. Steglich, S. Paschen, S. Kirchner, and Q. Si, Fermi-surface collapse and dynamical scaling near a quantum-critical point, Proc. Nat. Acad. Sci.107, 14547 (2010)
work page 2010
-
[5]
M. Lee, A. Husmann, T. F. Rosenbaum, and G. Aeppli, High resolution study of magnetic ordering at absolute zero, Phys. Rev. Lett.92, 187201 (2004)
work page 2004
-
[6]
R. Jaramillo, Y. Feng, J. Wang, and T. F. Rosenbaum, Signatures of quantum criticality in pure Cr at high pres- sure, Proc. Nat. Acad. Sci.107, 13631 (2010)
work page 2010
-
[7]
Q. Si, S. Rabello, K. Ingersent, and J. L. Smith, Locally critical quantum phase transitions in strongly correlated metals, Nature413, 804 (2001)
work page 2001
-
[8]
P. Coleman, C. P´ epin, Q. Si, and R. Ramazashvili, How do Fermi liquids get heavy and die?, J. Phys.: Condens. Matter13, R723 (2001)
work page 2001
-
[9]
T. Senthil, M. Vojta, and S. Sachdev, Weak magnetism and non-Fermi liquids near heavy-fermion critical points, Phys. Rev. B69, 035111 (2004)
work page 2004
-
[10]
S. Paschen and Q. Si, Quantum phases driven by strong correlations, Nat. Rev. Phys.3, 9 (2021)
work page 2021
-
[11]
Y. Nakajima, K. Izawa, Y. Matsuda, S. Uji, T. Terashima, H. Shishido, R. Settai, Y. Onuki, and H. Kontani, Normal-state Hall angle and magnetoresis- tance in quasi-2D heavy fermion CeCoIn 5 near a quan- tum critical point, J. Phys. Soc. Jpn.73, 5 (2004)
work page 2004
-
[12]
M. F. Hundley, A. Malinowski, P. G. Pagliuso, J. L. Sar- rao, and J. D. Thompson, Anomalousf-electron Hall ef- fect in the heavy-fermion system CeTIn 5 (T= Co,Ir, or Rh), Phys. Rev. B70, 035113 (2004)
work page 2004
-
[13]
Y. Nakajima, H. Shishido, H. Nakai, T. Shibauchi, K. Behnia, K. Izawa, M. Hedo, Y. Uwatoko, T. Mat- sumoto, R. Settai, Y. ¯Onuki, H. Kontani, and Y. Mat- suda, Non-Fermi liquid behavior in the magnetotrans- port of CeMIn 5 (M: Co and Rh): Striking similarity between quasi two-dimensional heavy fermion and high- Tc cuprates, J. Phys. Soc. Jpn.76, 024703 (2007)
work page 2007
- [14]
-
[15]
Yang, Anomalous Hall effect in heavy electron ma- terials, Phys
Y.-f. Yang, Anomalous Hall effect in heavy electron ma- terials, Phys. Rev. B87, 045102 (2013)
work page 2013
-
[16]
C. Petrovic, P. G. Pagliuso, M. F. Hundley, R. Movshovich, J. L. Sarrao, J. D. Thompson, Z. Fisk, and P. Monthoux, Heavy-fermion superconductivity in CeCoIn5 at 2.3 K, J. Phys.: Condens. Matter13, L337 (2001)
work page 2001
- [17]
-
[18]
W. K. Park, J. L. Sarrao, J. D. Thompson, and L. H. Greene, Andreev reflection in heavy-fermion supercon- ductors and order parameter symmetry in CeCoIn 5, Phys. Rev. Lett.100, 177001 (2008)
work page 2008
-
[19]
K. An, T. Sakakibara, R. Settai, Y. Onuki, M. Hiragi, M. Ichioka, and K. Machida, Sign reversal of field-angle resolved heat capacity oscillations in a heavy fermion superconductor CeCoIn 5 andd x2−y2 pairing symmetry, Phys. Rev. Lett.104, 037002 (2010)
work page 2010
-
[20]
J. Paglione, M. A. Tanatar, D. G. Hawthorn, E. Boaknin, R. W. Hill, F. Ronning, M. Sutherland, L. Taillefer, C. Petrovic, and P. C. Canfield, Field-induced quantum critical point in CeCoIn 5, Phys. Rev. Lett.91, 246405 (2003)
work page 2003
-
[21]
A. Bianchi, R. Movshovich, I. Vekhter, P. G. Pagliuso, and J. L. Sarrao, Avoided antiferromagnetic order and quantum critical point in CeCoIn 5, Phys. Rev. Lett.91, 257001 (2003)
work page 2003
- [22]
- [23]
-
[24]
A. Bianchi, R. Movshovich, C. Capan, P. G. Pagliuso, and J. L. Sarrao, Possible Fulde-Ferrell-Larkin- Ovchinnikov superconducting state in CeCoIn 5, Phys. Rev. Lett.91, 187004 (2003)
work page 2003
-
[25]
K. Kakuyanagi, M. Saitoh, K. Kumagai, S. Takashima, M. Nohara, H. Takagi, and Y. Matsuda, Texture in the superconducting order parameter of CeCoIn5 revealed by nuclear magnetic resonance, Phys. Rev. Lett.94, 047602 (2005). 10
work page 2005
- [26]
-
[27]
M. Kenzelmann, T. Str¨ assle, C. Niedermayer, M. Sigrist, B. Padmanabhan, M. Zolliker, A. D. Bianchi, R. Movshovich, E. D. Bauer, J. L. Sarrao, and J. D. Thompson, Coupled superconducting and magnetic or- der in CeCoIn 5, Science321, 1652 (2008)
work page 2008
- [28]
-
[29]
D. F. Agterberg, M. Sigrist, and H. Tsunetsugu, Order parameter and vortices in the superconductingQphase of CeCoIn5, Phys. Rev. Lett.102, 207004 (2009)
work page 2009
-
[30]
Yanase, FFLO superconductivity near the antiferro- magnetic quantum critical point, J
Y. Yanase, FFLO superconductivity near the antiferro- magnetic quantum critical point, J. Phys. Soc. Jpn.77, 063705 (2008)
work page 2008
-
[31]
Y. Yanase and M. Sigrist, Antiferromagnetic order and π-triplet pairing in the Fulde-Ferrell-Larkin-Ovchinnikov state, J. Phys. Soc. Jpn.78, 114715 (2009)
work page 2009
-
[32]
S. Kittaka, Y. Kono, K. Tsunashima, D. Kimoto, M. Yokoyama, Y. Shimizu, T. Sakakibara, M. Yamashita, and K. Machida, Modulation vector of the Fulde-Ferrell- Larkin-Ovchinnikov state in CeCoIn 5 revealed by high- resolution magnetostriction measurements, Phys. Rev. B 107, L220505 (2023)
work page 2023
- [33]
-
[34]
S. Raymond and G. Lapertot, Ising incommensurate spin resonance of CeCoIn 5: A dynamical precursor of theQ phase, Phys. Rev. Lett.115, 037001 (2015)
work page 2015
-
[35]
Y. Song, J. Van Dyke, I. K. Lum, B. D. White, S. Jang, D. Yazici, L. Shu, A. Schneidewind, P. ˇCerm´ ak, Y. Qiu, M. B. Maple, D. K. Morr, and P. Dai, Robust upward dispersion of the neutron spin resonance in the heavy fermion superconductor Ce1−xYbxCoIn5, Nat. Commun. 7, 12774 (2016)
work page 2016
-
[36]
D. G. Mazzone, S. Raymond, J. L. Gavilano, P. Steffens, A. Schneidewind, G. Lapertot, and M. Kenzelmann, Spin resonance and magnetic order in an unconventional su- perconductor, Phys. Rev. Lett.119, 187002 (2017)
work page 2017
-
[37]
L. D. Pham, T. Park, S. Maquilon, J. D. Thompson, and Z. Fisk, Reversible tuning of the heavy-fermion ground state in CeCoIn 5, Phys. Rev. Lett.97, 056404 (2006)
work page 2006
-
[38]
M. Nicklas, O. Stockert, T. Park, K. Habicht, K. Kiefer, L. D. Pham, J. D. Thompson, Z. Fisk, and F. Steglich, Magnetic structure of Cd-doped CeCoIn 5, Phys. Rev. B 76, 052401 (2007)
work page 2007
-
[39]
R. R. Urbano, B.-L. Young, N. J. Curro, J. D. Thompson, L. D. Pham, and Z. Fisk, Interacting antiferromagnetic droplets in quantum critical CeCoIn 5, Phys. Rev. Lett. 99, 146402 (2007)
work page 2007
-
[40]
S. Seo, X. Lu, J. Zhu, R. Urbano, N. Curro, E. Bauer, V. Sidorov, L. Pham, T. Park, Z. Fisk, and J. D. Thomp- son, Disorder in quantum critical superconductors, Nat. Phys.10, 120 (2014)
work page 2014
-
[41]
C. Stock, J. A. Rodriguez-Rivera, K. Schmalzl, F. Dem- mel, D. K. Singh, F. Ronning, J. D. Thompson, and E. D. Bauer, From ising resonant fluctuations to static uniax- ial order in antiferromagnetic and weakly superconduct- ing CeCo(In 1−xHgx)5 (x= 0.01), Phys. Rev. Lett.121, 037003 (2018)
work page 2018
-
[42]
M. Yokoyama, K. Fujimura, S. Ishikawa, M. Kimura, T. Hasegawa, I. Kawasaki, K. Tenya, Y. Kono, and T. Sakakibara, Possible evolution of antiferromagnetism in Zn-doped heavy-fermion superconductor CeCoIn 5, J. Phys. Soc. Jpn.83, 033706 (2014)
work page 2014
-
[43]
M. Yokoyama, H. Mashiko, R. Otaka, Y. Sakon, K. Fu- jimura, K. Tenya, A. Kondo, K. Kindo, Y. Ikeda, H. Yoshizawa, Y. Shimizu, Y. Kono, and T. Sakakibara, Pauli-limited superconductivity and antiferromagnetism in the heavy-fermion compound CeCo(In1−xZnx)5, Phys. Rev. B92, 184509 (2015)
work page 2015
-
[44]
M. Yokoyama, H. Mashiko, R. Otaka, Y. Oshima, K. Suzuki, K. Tenya, Y. Shimizu, A. Nakamura, D. Aoki, A. Kondo, K. Kindo, S. Nakamura, and T. Sakak- ibara, Observation of a new field-induced phase transi- tion and its concomitant quantum critical fluctuations in CeCo(In1−xZnx)5, Phys. Rev. B95, 224425 (2017)
work page 2017
-
[45]
M. Haze, Y. Torii, R. Peters, S. Kasahara, Y. Kasa- hara, T. Shibauchi, T. Terashima, and Y. Matsuda, In situ STM observation of nonmagnetic impurity effect in MBE-grown CeCoIn5 films, J. Phys. Soc. Jpn.87, 034702 (2018)
work page 2018
-
[46]
H. Sakai, Y. Tokunaga, S. Kambe, J.-X. Zhu, F. Ron- ning, J. D. Thompson, S. K. Ramakrishna, A. P. Reyes, K. Suzuki, Y. Oshima, and M. Yokoyama, Nanoscale het- erogeneity induced by nonmagnetic Zn dopants in the quantum critical metal CeCoIn 5: 115In NQR/NMR and 59Co NMR study, Phys. Rev. B104, 085106 (2021)
work page 2021
-
[47]
M. Yokoyama, Y. Honma, Y. Oshima, Rahmanto, K. Suzuki, K. Tenya, Y. Shimizu, D. Aoki, A. Mat- suo, K. Kindo, S. Nakamura, Y. Kono, S. Kittaka, and T. Sakakibara, Nature of field-induced antiferromagnetic order in Zn-doped CeCoIn 5 and its connection to quan- tum criticality in the pure compound, Phys. Rev. B105, 054515 (2022)
work page 2022
-
[48]
W. Higemoto, M. Yokoyama, T. U. Ito, T. Suzuki, S. Raymond, and Y. Yanase, Direct measurement of the evolution of magnetism and superconductivity toward the quantum critical point, Proc. Nat. Acad. Sci.119, e2209549119 (2022)
work page 2022
-
[49]
K. Inoh, R. Koizumi, T. Takahashi, H. Fujimoto, H. Ebi- sawa, A. Yashiro, M. Kohinata, A. Hosogai, A. Mat- suo, K. Kindo, I. Kawasaki, D. Okuyama, H.-C. Wu, T. J. Sato, K. Tenya, K. Ohoyama, K. Iwasa, and M. Yokoyama, Continuously evolving antiferromagnetic order within the superconducting phase in Zn-doped CeCoIn5, Phys. Rev. B111, 104510 (2025)
work page 2025
-
[50]
E. D. Bauer, C. Capan, F. Ronning, R. Movshovich, J. D. Thompson, and J. L. Sarrao, Superconductivity in CeCoIn5−xSnx: Veil over an ordered state or novel quan- tum critical point?, Phys. Rev. Lett.94, 047001 (2005)
work page 2005
-
[51]
E. D. Bauer, F. Ronning, C. Capan, M. J. Graf, D. Van- dervelde, H. Q. Yuan, M. B. Salamon, D. J. Mix- son, N. O. Moreno, S. R. Brown, J. D. Thompson, R. Movshovich, M. F. Hundley, J. L. Sarrao, P. G. Pagliuso, and S. M. Kauzlarich, Thermodynamic and transport investigation of CeCoIn 5−xSnx, Phys. Rev. B 73, 245109 (2006)
work page 2006
-
[52]
S. M. Ramos, M. B. Fontes, E. N. Hering, M. A. Con- tinentino, E. Baggio-Saitovich, F. D. Neto, E. M. Bit- tar, P. G. Pagliuso, E. D. Bauer, J. L. Sarrao, and J. D. Thompson, Superconducting quantum critical point in CeCoIn5−xSnx, Phys. Rev. Lett.105, 126401 (2010). 11
work page 2010
- [53]
-
[54]
M. Yokoyama, K. Suzuki, K. Tenya, S. Nakamura, Y. Kono, S. Kittaka, and T. Sakakibara, Anisotropic magnetic-field response of quantum critical fluctuations in Ni-doped CeCoIn 5, Phys. Rev. B99, 054506 (2019)
work page 2019
- [55]
-
[56]
A. Yashiro, Rahmanto, K. Inami, K. Suzuki, K. Inoh, T. Takahashi, R. Koizumi, Y. Kono, S. Kittaka, Y. Shimizu, F. Honda, D. Aoki, K. Tenya, and M. Yokoyama, Quantum criticality linked to the sup- pressed superconducting upper critical field in Ni-doped CeCoIn5, Phys. Rev. Mater.8, L081801 (2024)
work page 2024
- [57]
-
[58]
K. Chen, F. Strigari, M. Sundermann, Z. Hu, Z. Fisk, E. D. Bauer, P. F. S. Rosa, J. L. Sarrao, J. D. Thomp- son, J. Herrero-Martin, E. Pellegrin, D. Betto, K. Kum- mer, A. Tanaka, S. Wirth, and A. Severing, Evolution of ground-state wave function in CeCoIn 5 upon Cd or Sn doping, Phys. Rev. B97, 045134 (2018)
work page 2018
-
[59]
H. C. Choi, E. D. Bauer, F. Ronning, and J.-X. Zhu, DFT + DMFT study of dopant effects in the heavy- fermion compound CeCoIn 5, Phys. Rev. B105, 115121 (2022)
work page 2022
-
[60]
N. Maksimovic, D. H. Eilbott, T. Cookmeyer, F. Wan, J. Rusz, V. Nagarajan, S. C. Haley, E. Maniv, A. Gong, S. Faubel, I. M. Hayes, A. Bangura, J. Singleton, J. C. Palmstrom, L. Winter, R. McDonald, S. Jang, P. Ai, Y. Lin, S. Ciocys, J. Gobbo, Y. Werman, P. M. Oppeneer, E. Altman, A. Lanzara, and J. G. Analytis, Evidence for a delocalization quantum phase ...
work page 2022
- [61]
-
[62]
D. Hall, E. C. Palm, T. P. Murphy, S. W. Tozer, Z. Fisk, U. Alver, R. G. Goodrich, J. L. Sarrao, P. G. Pagliuso, and T. Ebihara, Fermi surface of the heavy-fermion su- perconductor CeCoIn 5: The de Haas–van Alphen effect in the normal state, Phys. Rev. B64, 212508 (2001)
work page 2001
-
[63]
H. Shishido, R. Settai, D. Aoki, S. Ikeda, H. Nakawaki, N. Nakamura, T. Iizuka, Y. Inada, K. Sugiyama, T. Takeuchi, K. Kindo, T. Kobayashi, Y. Haga, H. Harima, Y. Aoki, T. Namiki, H. Sato, and Y. ¯Onuki, Fermi surface, magnetic and superconducting properties of LaRhIn5 and CeTIn5 (T: Co, Rh and Ir), J. Phys. Soc. Jpn.71, 162 (2002)
work page 2002
-
[64]
T. Maehira, T. Hotta, K. Ueda, and A. Hasegawa, Rel- ativistic band-structure calculations for CeTIn 5 (T = Ir and Co) and analysis of the energy bands by using tight- binding method, J. Phys. Soc. Jpn.72, 854 (2003)
work page 2003
-
[65]
A. B. Pippard,Magnetoresistance in metals, Vol. 2 (Cam- bridge university press, 1989)
work page 1989
-
[66]
Paglione, Quantum criticality in the heavy-fermion superconductor CeCoIn 5, Ph.D
J. Paglione, Quantum criticality in the heavy-fermion superconductor CeCoIn 5, Ph.D. thesis, University of Toronto, 2005
work page 2005
-
[67]
S. Nakatsuji, D. Pines, and Z. Fisk, Two fluid description of the Kondo lattice, Phys. Rev. Lett.92, 016401 (2004)
work page 2004
-
[68]
G. R. Stewart, Heavy-fermion systems, Rev. Mod. Phys. 56, 755 (1984)
work page 1984
-
[69]
Y.-f. Yang, Z. Fisk, H.-O. Lee, J. Thompson, and D. Pines, Scaling the Kondo lattice, Nature454, 611 (2008)
work page 2008
- [70]
-
[71]
R. Koizumi, H. Fujimoto, T. Takahashi, A. Yashiro, H. Kawakami, K. Ishii, H. Kosaka, T. Hasegawa, Y. Shimizu, A. Nakamura, D. Aoki, K. Tenya, and M. Yokoyama, Dataset for ”Carrier-doping effect and anomalous transport properties in Ni-doped CeCoIn 5 investigated by Hall resistivity measurements”, Zenodo (2026), https://doi.org/10.5281/zenodo.17347546
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.