Luis Palma-Chilla
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Luis Palma-Chilla has a total of 16 co-authors. Here are the top co-authors by number of shared publications:
- Juan A. Lazzús
Departamento de Física, Universidad de La Serena, Casilla 554, La Serena 1700000, Chile
8 shared publications J.C. Flores
Instituto de Alta Investigación IAI, Universidad de Tarapacá, Casilla 7-D, Arica, Chile
6 shared publications- Juan Cesar Flores
Departamento de Física, FACI, Universidad de Tarapacá, Casilla 7-D, Arica 1000000, Chile
4 shared publications - Pedro Vega-Jorquera
Universidad de La Serena
3 shared publications - Alfredo Pizarro
Departamento de Física, Universidad de La Serena, La Serena, Chile
2 shared publications - Erick de la Barra
School of Business, Universidad Católica del Norte, Coquimbo 1781421, CO, Chile
2 shared publications
Latest Publications
- Open Access
Golden-Ratio Exceptional Contours in a Non-Hermitian RH/LH Quadrilayer Metamaterial
A non-Hermitian LC quadrilayer metamaterial formed by alternating right-handed (RH) and left-handed (LH) circuit layers is investigated. The layers are connected through identical nearest-neighbor imaginary couplings, providing a minimal multilayer extension of the RH/LH bilayer. The quadrilayer connectivity generates two non-Hermitian spectral scales related by the golden ratio, giving rise to two exceptional families and up to four exceptional contours in the two-dimensional reciprocal space. The RH/LH circuit duality organizes the exceptional solutions into reciprocal pairs, while the golden-ratio structure determines the relative scale of the critical couplings. Increasing the coupling consequently changes the number of physically accessible exceptional contours from four to three and finally two. In the four-contour regime, the nested exceptional structure separates reciprocal-space regions containing zero, two, and four complex eigenfrequencies. These results show that the connectivity of an LC multilayer can generate multiple exceptional boundaries and golden-ratio spectral scaling using a single microscopic non-Hermitian coupling.
Open AccessGolden-Ratio Exceptional Contours in a Non-Hermitian RH/LH Quadrilayer Metamaterial
A non-Hermitian LC quadrilayer metamaterial formed by alternating right-handed (RH) and left-handed (LH) circuit layers is investigated. The layers are connected through identical nearest-neighbor imaginary couplings, providing a minimal multilayer extension of the RH/LH bilayer. The quadrilayer connectivity generates two non-Hermitian spectral scales related by the golden ratio, giving rise to two exceptional families and up to four exceptional contours in the two-dimensional reciprocal space. The RH/LH circuit duality organizes the exceptional solutions into reciprocal pairs, while the golden-ratio structure determines the relative scale of the critical couplings. Increasing the coupling consequently changes the number of physically accessible exceptional contours from four to three and finally two. In the four-contour regime, the nested exceptional structure separates reciprocal-space regions containing zero, two, and four complex eigenfrequencies. These results show that the connectivity of an LC multilayer can generate multiple exceptional boundaries and golden-ratio spectral scaling using a single microscopic non-Hermitian coupling.
- Open Access
Electromagnetic Duality and Exceptional-Point Transitions in Non-Hermitian RH/LH LC Bilayers
An analytical non-Hermitian bilayer composed of coupled right-handed and left-handed lattices is investigated. The uncoupled lattices exhibit exact dual dispersions characterized by complementary direct and inverse excitation spectra. When the layers are coupled through a purely imaginary interlayer coupling, the resulting non-Hermitian Hamiltonian undergoes exceptional-point transitions that separate regions with purely real eigenenergies from regions with complex eigenenergies. It is shown that the spectral splitting is progressively transferred from the real-energy sector to the imaginary-energy sector, giving rise to hybridized modes with finite lifetimes. The corresponding relaxation time, which is directly related to the mobility of the excitations, is governed by the imaginary-energy splitting and diverges at the exceptional-point boundary. These findings establish a direct connection between electromagnetic duality, non-Hermitian spectral properties, and transport phenomena in mesoscopic networks. Possible extensions of the present approach may be relevant for artificial circuit platforms, including Josephson-junction arrays.Open AccessElectromagnetic Duality and Exceptional-Point Transitions in Non-Hermitian RH/LH LC Bilayers
An analytical non-Hermitian bilayer composed of coupled right-handed and left-handed lattices is investigated. The uncoupled lattices exhibit exact dual dispersions characterized by complementary direct and inverse excitation spectra. When the layers are coupled through a purely imaginary interlayer coupling, the resulting non-Hermitian Hamiltonian undergoes exceptional-point transitions that separate regions with purely real eigenenergies from regions with complex eigenenergies. It is shown that the spectral splitting is progressively transferred from the real-energy sector to the imaginary-energy sector, giving rise to hybridized modes with finite lifetimes. The corresponding relaxation time, which is directly related to the mobility of the excitations, is governed by the imaginary-energy splitting and diverges at the exceptional-point boundary. These findings establish a direct connection between electromagnetic duality, non-Hermitian spectral properties, and transport phenomena in mesoscopic networks. Possible extensions of the present approach may be relevant for artificial circuit platforms, including Josephson-junction arrays. - Open Access
Analytical Description of Strain-Controlled Transport Anisotropy in Graphene
We develop an analytical framework to describe the impact of in-plane strain on the electronic and transport properties of graphene. Starting from a strain-modified nearest-neighbor tight-binding model, we derive the energy spectrum and group velocities, explicitly incorporating bond-dependent hopping renormalization. A dimensionless anisotropy parameter, derived from velocity fluctuations, is introduced to quantify directional transport imbalance. We show that this parameter admits a closed-form expression entirely determined by the strain tensor, linking lattice deformation directly to measurable transport quantities. In the small-strain regime, a compact expression is obtained, , revealing an angular dependence controlled solely by the orientation of the applied deformation. This establishes that strain acts as a purely geometric control parameter, separating magnitude and orientation effects. Within the semiclassical Boltzmann framework, the same parameter fully determines the conductivity tensor, leading to simple expressions for the longitudinal components and a clear identification of the preferred transport direction. Importantly, the total conductivity remains constant, while strain redistributes transport between orthogonal directions. These results provide a transparent and predictive description of strain-induced transport anisotropy, demonstrating that the directional electronic response can be tuned without modifying the material composition, offering a practical route to control electronic response in graphene through purely mechanical means.Open AccessAnalytical Description of Strain-Controlled Transport Anisotropy in Graphene
We develop an analytical framework to describe the impact of in-plane strain on the electronic and transport properties of graphene. Starting from a strain-modified nearest-neighbor tight-binding model, we derive the energy spectrum and group velocities, explicitly incorporating bond-dependent hopping renormalization. A dimensionless anisotropy parameter, derived from velocity fluctuations, is introduced to quantify directional transport imbalance. We show that this parameter admits a closed-form expression entirely determined by the strain tensor, linking lattice deformation directly to measurable transport quantities. In the small-strain regime, a compact expression is obtained, , revealing an angular dependence controlled solely by the orientation of the applied deformation. This establishes that strain acts as a purely geometric control parameter, separating magnitude and orientation effects. Within the semiclassical Boltzmann framework, the same parameter fully determines the conductivity tensor, leading to simple expressions for the longitudinal components and a clear identification of the preferred transport direction. Importantly, the total conductivity remains constant, while strain redistributes transport between orthogonal directions. These results provide a transparent and predictive description of strain-induced transport anisotropy, demonstrating that the directional electronic response can be tuned without modifying the material composition, offering a practical route to control electronic response in graphene through purely mechanical means. - Open Access
Thermal Layer Polarization in Asymmetric Doped Bilayer Graphene
We present a minimal model that isolates the effect of hopping asymmetry on the thermal redistribution of particles in a bilayer graphene system composed of one pristine and one doped layer. The behavior of the system is governed by a single control parameter , which uniformly reduces the intralayer hopping in the doped sheet and defines the only source of spectral asymmetry. Particle conservation fixes the total density at all temperatures, so thermal effects appear exclusively as a redistribution relative to the zero-temperature reference state. This redistribution is quantified by the temperature-induced change of the layer populations, which measures how thermal occupation modifies the particle density in each layer without creating or destroying carriers. With this, the difference between the thermal population corrections of the doped and pristine layers defines the polarization. Thus, thermal excitations probe the asymmetric spectrum, exposing the intrinsic layer imbalance. Results show that for , band deformation produces unequal occupations between doped and pristine layers, and temperature amplifies this imbalance. The resulting polarization increases monotonically with temperature and systematically with hopping reduction, establishing a direct quantitative link between microscopic spectral asymmetry and macroscopic thermally induced layer imbalance.Open AccessThermal Layer Polarization in Asymmetric Doped Bilayer Graphene
We present a minimal model that isolates the effect of hopping asymmetry on the thermal redistribution of particles in a bilayer graphene system composed of one pristine and one doped layer. The behavior of the system is governed by a single control parameter , which uniformly reduces the intralayer hopping in the doped sheet and defines the only source of spectral asymmetry. Particle conservation fixes the total density at all temperatures, so thermal effects appear exclusively as a redistribution relative to the zero-temperature reference state. This redistribution is quantified by the temperature-induced change of the layer populations, which measures how thermal occupation modifies the particle density in each layer without creating or destroying carriers. With this, the difference between the thermal population corrections of the doped and pristine layers defines the polarization. Thus, thermal excitations probe the asymmetric spectrum, exposing the intrinsic layer imbalance. Results show that for , band deformation produces unequal occupations between doped and pristine layers, and temperature amplifies this imbalance. The resulting polarization increases monotonically with temperature and systematically with hopping reduction, establishing a direct quantitative link between microscopic spectral asymmetry and macroscopic thermally induced layer imbalance. - Open Access
Electronic Particle-Density Asymmetry in Doped Bilayer Graphene with Effective Fractional Dimensionality
This work investigates how effective fractional dimensionality and substitutional doping jointly affect particle-density symmetry in AA-stacked bilayer graphene (BLG). The system consists of one pristine graphene layer and one doped layer, where 50% of the atomic sites are substituted. Doping is described within a tight-binding framework through a dimensionless parameter (with ), which uniformly reduces the intralayer hopping energy in the doped layer, while an effective fractional dimension phenomenologically accounts for structural inhomogeneities such as ripples or corrugations. Analytical expressions for the energy spectrum and number of states are obtained, and the electronic asymmetry between layers is characterized by a symmetry parameter . We find that substitutional doping breaks the particle-density symmetry of pristine BLG and strongly enhances the number of states near the Fermi level as decreases, due to the accumulation of low-energy states in the doped layer. Departures from the ideal dimensionality further amplify this enhancement. The combined effects of reduced and increased lead to a pronounced layer asymmetry, reflected in a nonzero , while stronger interlayer coupling partially counteracts this imbalance. Results show that doping, effective fractional dimensionality, and interlayer coupling offer tunable control over the low-energy electronic properties of BLG.Open AccessElectronic Particle-Density Asymmetry in Doped Bilayer Graphene with Effective Fractional Dimensionality
This work investigates how effective fractional dimensionality and substitutional doping jointly affect particle-density symmetry in AA-stacked bilayer graphene (BLG). The system consists of one pristine graphene layer and one doped layer, where 50% of the atomic sites are substituted. Doping is described within a tight-binding framework through a dimensionless parameter (with ), which uniformly reduces the intralayer hopping energy in the doped layer, while an effective fractional dimension phenomenologically accounts for structural inhomogeneities such as ripples or corrugations. Analytical expressions for the energy spectrum and number of states are obtained, and the electronic asymmetry between layers is characterized by a symmetry parameter . We find that substitutional doping breaks the particle-density symmetry of pristine BLG and strongly enhances the number of states near the Fermi level as decreases, due to the accumulation of low-energy states in the doped layer. Departures from the ideal dimensionality further amplify this enhancement. The combined effects of reduced and increased lead to a pronounced layer asymmetry, reflected in a nonzero , while stronger interlayer coupling partially counteracts this imbalance. Results show that doping, effective fractional dimensionality, and interlayer coupling offer tunable control over the low-energy electronic properties of BLG. - Open Access
Thermodynamic Behavior of Doped Graphene: Impact of Heavy Dopant Atoms
This study investigates the effect of incorporating heavy dopant atoms on the topological transitions in the energy spectrum of graphene, as well as on its thermodynamic properties. A tight-binding model is employed that incorporates a lattice composition parameter associated with the dopant’s effect to obtain the electronic spectrum of graphene. Thus, the substitutional atoms in the lattice impact the electronic structure of graphene by altering the connectivity of the Dirac cones and the symmetry of the energy surface in their spectrum. The Gibbs entropy is numerically calculated from the energy surface of the electronic spectrum, and other thermodynamic properties, such as temperature, specific heat, and Helmholtz free energy, are derived from theoretical principles. The results show that topological changes induced by the heavy dopant atoms in the graphene lattice significantly affect its electronic structure and thermodynamic properties, leading to observable changes in the distances between Dirac cones, the range of the energy spectrum, entropy, positive and negative temperatures, divergences in specific heat, and instabilities within the system.
Open AccessThermodynamic Behavior of Doped Graphene: Impact of Heavy Dopant Atoms
This study investigates the effect of incorporating heavy dopant atoms on the topological transitions in the energy spectrum of graphene, as well as on its thermodynamic properties. A tight-binding model is employed that incorporates a lattice composition parameter associated with the dopant’s effect to obtain the electronic spectrum of graphene. Thus, the substitutional atoms in the lattice impact the electronic structure of graphene by altering the connectivity of the Dirac cones and the symmetry of the energy surface in their spectrum. The Gibbs entropy is numerically calculated from the energy surface of the electronic spectrum, and other thermodynamic properties, such as temperature, specific heat, and Helmholtz free energy, are derived from theoretical principles. The results show that topological changes induced by the heavy dopant atoms in the graphene lattice significantly affect its electronic structure and thermodynamic properties, leading to observable changes in the distances between Dirac cones, the range of the energy spectrum, entropy, positive and negative temperatures, divergences in specific heat, and instabilities within the system.
- Open Access
Entropy and Negative Specific Heat of Doped Graphene: Topological Phase Transitions and Nernst’s Theorem Revisited
This study explores the thermodynamic properties of doped graphene using an adapted electronic spectrum. We employed the one-electron tight-binding model to describe the hexagonal lattice structure. The dispersion relation for graphene is expressed in terms of the hopping energies using a compositional parameter that characterizes the different dopant atoms in the lattice. The focus of the investigation is on the impact of the compositions, specifically the presence of dopant atoms, on the energy spectrum, entropy, temperature, and specific heat of graphene. The numerical and analytical results reveal distinct thermodynamic behaviors influenced by the dopant composition, including topological transitions, inflection points in entropy, and specific heat divergences. In addition, the use of Boltzmann entropy and the revision of Nernst’s theorem for doped graphene are introduced as novel aspects.
Open AccessEntropy and Negative Specific Heat of Doped Graphene: Topological Phase Transitions and Nernst’s Theorem Revisited
This study explores the thermodynamic properties of doped graphene using an adapted electronic spectrum. We employed the one-electron tight-binding model to describe the hexagonal lattice structure. The dispersion relation for graphene is expressed in terms of the hopping energies using a compositional parameter that characterizes the different dopant atoms in the lattice. The focus of the investigation is on the impact of the compositions, specifically the presence of dopant atoms, on the energy spectrum, entropy, temperature, and specific heat of graphene. The numerical and analytical results reveal distinct thermodynamic behaviors influenced by the dopant composition, including topological transitions, inflection points in entropy, and specific heat divergences. In addition, the use of Boltzmann entropy and the revision of Nernst’s theorem for doped graphene are introduced as novel aspects.
- 25 April 2024
- Published by Springer Nature in Pure and Applied Geophysics
- Vol. 181 (5) , 1427-1454
Characterization of Seismicity and Seismic Hazard in the Coquimbo Region, Chile: A Probabilistic Study
- 25 April 2024
- Published by Springer Nature in Pure and Applied Geophysics
- Vol. 181 (5) , 1427-1454
Characterization of Seismicity and Seismic Hazard in the Coquimbo Region, Chile: A Probabilistic Study
- Open Access
- 18 May 2023
- Published by Springer Nature in Research Square
Characterization and seismic hazard in the Coquimbo Region, Chile: A probabilistic study
In order to characterize seismically the Coquimbo Region, Chile, data from 1943 to 2020 were considered. The region was divided into 30 zones of 0.5 • latitude and 0.5 • longitude and the non-extensive statistical physics was used. Both, the Sotolongo-Costa-Posadas and Mathai models were proposed to analyze the magnitude-frequency distribution. The subdivision into cells of the catalog allowed to demonstrate that systems with value of q ∼ 1 present exponential behavior, while with the superposition of subsystems it was expected to obtain q > 1, supporting the su-perstatistical model. Thus, by subdividing the Coquimbo region into the South and North regions, we find that in both the entropic index is greater than one, q > 1, however , according to the value obtained, in the southern sector the long-range effects are greater than in the northern sector. This means that both sectors ae well described by the nonextensive statistical model, either by SCP model or Mathai model; the entropic index is q > 1 and in both cases R 2 > 0.99. As the Coquimbo region is considered as a all, the nonextensive statistical distribution is the more adequated. With respect to the probabilistic seismic hazard assessment, we showed that the Mathai’s model has the better fit. Thus, in the frequency-interevent time distribution was used for different limite magnitudes values. Our analysis shows that the probability occurrence of an seismic event in the northern sector of the region is lower than in the southern sector for the same period; in the former the behavior is of Poissonian type. Thus, the region’s northern and southern zones show different behaviors in terms of earthquake occurrence probability.
- 18 May 2023
- Published by Springer Nature in Research Square
Open AccessCharacterization and seismic hazard in the Coquimbo Region, Chile: A probabilistic study
In order to characterize seismically the Coquimbo Region, Chile, data from 1943 to 2020 were considered. The region was divided into 30 zones of 0.5 • latitude and 0.5 • longitude and the non-extensive statistical physics was used. Both, the Sotolongo-Costa-Posadas and Mathai models were proposed to analyze the magnitude-frequency distribution. The subdivision into cells of the catalog allowed to demonstrate that systems with value of q ∼ 1 present exponential behavior, while with the superposition of subsystems it was expected to obtain q > 1, supporting the su-perstatistical model. Thus, by subdividing the Coquimbo region into the South and North regions, we find that in both the entropic index is greater than one, q > 1, however , according to the value obtained, in the southern sector the long-range effects are greater than in the northern sector. This means that both sectors ae well described by the nonextensive statistical model, either by SCP model or Mathai model; the entropic index is q > 1 and in both cases R 2 > 0.99. As the Coquimbo region is considered as a all, the nonextensive statistical distribution is the more adequated. With respect to the probabilistic seismic hazard assessment, we showed that the Mathai’s model has the better fit. Thus, in the frequency-interevent time distribution was used for different limite magnitudes values. Our analysis shows that the probability occurrence of an seismic event in the northern sector of the region is lower than in the southern sector for the same period; in the former the behavior is of Poissonian type. Thus, the region’s northern and southern zones show different behaviors in terms of earthquake occurrence probability.
- 1 March 2021
- Published by Pleiades Publishing Ltd in Geomagnetism and Aeronomy
- Vol. 61 (2) , 287-292
Geomagnetic Field Variations during the Total Solar Eclipse of 2 July 2019 in La Serena, Chile
The total solar eclipse on July 2, 2019, has been studied by using data of the La Serena ground magnetic station in Chile located in the path of the totality (at geographic coordinates: 29.827° S, 71.261° W). The event reached 100% darkness and occurred from 1522:34 hr to 1746:36 hr LT. We monitored the X, Y, Z‑components of the geomagnetic field with a fluxgate magnetometer to investigate their variation caused by the passing of the Moon in front of the Sun. Our results show positive growth up to ∼12 nT for all components in the same time window during the eclipse and in total synchrony with its phases. Having to discard any effect on the observations such as magnetic and solar activities, seasonal and geographical conditions, and instrumental effects, we report a total increase of the geomagnetic field during this phenomenon.
- 1 March 2021
- Published by Pleiades Publishing Ltd in Geomagnetism and Aeronomy
- Vol. 61 (2) , 287-292
Geomagnetic Field Variations during the Total Solar Eclipse of 2 July 2019 in La Serena, Chile
The total solar eclipse on July 2, 2019, has been studied by using data of the La Serena ground magnetic station in Chile located in the path of the totality (at geographic coordinates: 29.827° S, 71.261° W). The event reached 100% darkness and occurred from 1522:34 hr to 1746:36 hr LT. We monitored the X, Y, Z‑components of the geomagnetic field with a fluxgate magnetometer to investigate their variation caused by the passing of the Moon in front of the Sun. Our results show positive growth up to ∼12 nT for all components in the same time window during the eclipse and in total synchrony with its phases. Having to discard any effect on the observations such as magnetic and solar activities, seasonal and geographical conditions, and instrumental effects, we report a total increase of the geomagnetic field during this phenomenon.