{"results":[{"id":"crossref_10.15388/baltistica.43.3.1282","title":"Dėl 3 cond. galūnės -tuo","authors":[{"name":"Zigmas Zinkevičius"}],"abstract":"–","source":"CrossRef","year":2026,"language":"en","subjects":null,"doi":"10.15388/baltistica.43.3.1282","url":"https://doi.org/10.15388/baltistica.43.3.1282","pdf_url":"https://www.zurnalai.vu.lt/baltistica/article/download/39595/37175","is_open_access":true,"published_at":"","score":70},{"id":"crossref_10.15381/escrypensam.v24i52.30164","title":"El grado de realidad en las oraciones condicionales con la estructura cond + imperfecto desubjuntivo + condicional de indicativo en el español de Lima Metropolitana","authors":[{"name":"Paulo Augusto Arteaga Uribe"}],"abstract":"Las condicionales del español con la estructura cond + imperfecto de subjuntivo + condicional simple de indicativo evidencian la aparición de la flexión condicional en la prótasis, contrario a lo establecido en el español estándar. Además, de acuerdo con Lavandera (1984) y De Granda (1998), la diferencia entre grado de realidad podría motivar la aparición de dicha flexión de condicional en prótasis. Así, se busca vincular el grado de realidad con la aparición de la flexión de condicional simple de indicativo en la prótasis. A partir de lo propuesto por Thompson, Longacre y Hwang (2007) sobre grados de realidad, la Gramática de Construcciones (Hoffman y Trousdale, 2013), así como las investigaciones de Lavandera (1984) y De Granda (1998), se pone a prueba esa variable con cuestionarios escritos1.","source":"CrossRef","year":2025,"language":"en","subjects":null,"doi":"10.15381/escrypensam.v24i52.30164","url":"https://doi.org/10.15381/escrypensam.v24i52.30164","pdf_url":"https://revistasinvestigacion.unmsm.edu.pe/index.php/letras/article/download/30164/22326","is_open_access":true,"published_at":"","score":69},{"id":"crossref_10.22529/stromata.2025.81.2.(3)","title":"El doble papel de la vergüenza en el Sofista de Platón","authors":[{"name":"Tomás Scarpatti"}],"abstract":"En el presente artículo expongo el papel prospectivo y retrospectivo de la vergüenza (αἰδώς, αἰσχύνη) en el Sofista de Platón. El primer caso se presenta en el íncipit (216a-219a4), donde el Extranjero de Elea expresa su vergüenza al admitir que la investigación propuesta conllevaría un “discurso extenso”. La disposición anímica del Eleata puede explicarse, en particular, por la necesidad de demostrar su condición de filósofo. Esta misma actitud de respeto hacia la filosofía se remarca en la sexta definición (226a6- 231b9) por la decisión de desligar al típico sofista del refutador y purificador del alma.","source":"CrossRef","year":2025,"language":"en","subjects":null,"doi":"10.22529/stromata.2025.81.2.(3)","url":"https://doi.org/10.22529/stromata.2025.81.2.(3)","pdf_url":"https://revistas.bibdigital.uccor.edu.ar/index.php/STRO/article/download/scarpatti/scarpatti","is_open_access":true,"published_at":"","score":69},{"id":"crossref_10.22529/stromata.2024.80.2.(1)","title":"Pensar el Santo, pensar en el Santo","authors":[{"name":"Tommaso Bertolasi"}],"abstract":"En 1966, el filósofo y teólogo Klaus Hemmerle escribía un ensayo fundamental para el desarrollo de su pensamiento: Das Heilige und das Denken. El corazón de este trabajo es la problemática de la pensabilidad del Misterio Santo (Heilige). La pregunta que mueve su investigaciónes: ¿cómo puede ser pensado el Santo para que sea Santo al pensar? Siguiendo esta cuestión y la propuesta que al respecto hace Hemmerle, en este trabajo queremos, primero, destacar los que podríamos definir los “prolegómenos” para pensar el S/ser. El desarrollo del planteo será típicamente filosófico.En un segundo momento, tomando en cuenta algunas páginas del último ensayo hemmerliano, Leben aus der Einheit, queremos mostrar, como proyección del desarrollo del autor, el movimiento del pensar en su arraigo en la existencia de quienes reciben en sí y entre sí el manifestarse del Misterio Santo, revelado en Jesús en la fuerza del Espíritu. En esta segunda parte se quiere, entonces, esbozar el camino para el paso de un pensar filosófico-fenomenológico a un pensar teológico-filosófico fenomenológicamente cualificado.","source":"CrossRef","year":2024,"language":"en","subjects":null,"doi":"10.22529/stromata.2024.80.2.(1)","url":"https://doi.org/10.22529/stromata.2024.80.2.(1)","pdf_url":"https://revistas.bibdigital.uccor.edu.ar/index.php/STRO/article/download/5681/7776","is_open_access":true,"published_at":"","score":68},{"id":"arxiv_2306.10894","title":"Half-filled stripe to N$\\acute e$el antiferromagnetism transition in the $t'$-Hubbard model on honeycomb lattice","authors":[{"name":"Yang Shen"},{"name":"Mingpu Qin"}],"abstract":"We study the ground state of the doped Hubbard model on honeycomb lattice with both nearest ($t$) and next-nearest neighboring hoppings ($t'$) in the small doping and strongly interacting region. Previous study on the model without $t'$ showed the ground state is a half-filled stripe. We employ density matrix renormalization group and extrapolate the results with truncation errors in the converged region. In the $t' \u003c 0$ side, we find the half-filled stripe phase at $t' = 0$ is stable against the frustration of $t'$ until a critical point $-0.4 \u003c t'_c \u003c -0.3$, beyond which the ground state switches to anti-ferromagnetic N$\\acute e$el phase with charge modulation. With further increase of $t'$ to $-0.7$, the ground state becomes paramagnetic. In the $t' \u003e 0$ side, the half-filled stripe stretches to $t' \\approx 0.7$. We don't find obvious enhancement of pairing for the range of $t'$ studied. We study width-4 cylinders in this work but the results for spin, charge, and pairing correlation agree qualitatively for periodic and anti-periodic boundary conditions in the half-filled stripe and anti-ferromagnetic N$\\acute e$el phases, suggesting the results are likely to be representative for true two-dimensional systems. The half-filled stripe to anti-ferromagnetic N$\\acute e$el phase transition can be realized on real materials or ultra-cold atom platform.","source":"arXiv","year":2023,"language":"en","subjects":["cond-mat.str-el","cond-mat.supr-con"],"doi":"10.1103/PhysRevB.109.024505","url":"https://arxiv.org/abs/2306.10894","pdf_url":"https://arxiv.org/pdf/2306.10894","is_open_access":true,"published_at":"2023-06-19T12:47:00Z","score":67},{"id":"crossref_10.1007/bf01475921","title":"Stability of lamellar eutectics","authors":[{"name":"S. Str�ssler"},{"name":"W. R. Schneider"}],"abstract":"","source":"CrossRef","year":1974,"language":"en","subjects":null,"doi":"10.1007/bf01475921","url":"https://doi.org/10.1007/bf01475921","pdf_url":"http://link.springer.com/content/pdf/10.1007/BF01475921.pdf","is_open_access":true,"citations":40,"published_at":"","score":51.2},{"id":"arxiv_cond-mat/0701417","title":"REPLY to Comments on \"Giant Dielectric Response in the One-Dimensional Charge-Ordered Semiconductor (NbSe4)3I\" and \"Colossal Magnetocapacitance and Colossal Magnetoresistance in HgCr2S4\" (cond-mat/0607500)","authors":[{"name":"P. Lunkenheimer"},{"name":"J. Hemberger"},{"name":"V. Tsurkan"},{"name":"D. Staresinic"},{"name":"K. Biljakovic"},{"name":"A. Loidl"}],"abstract":"In the present work we reply to the Comment by Catalan and Scott (cond-mat/0607500) on two of our papers. This Comment has been rejected from publication in Physical Review Letters and, hence, our Reply is based on the cond-mat version.","source":"arXiv","year":2007,"language":"en","subjects":["cond-mat.mtrl-sci","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0701417","pdf_url":"https://arxiv.org/pdf/cond-mat/0701417","is_open_access":true,"published_at":"2007-01-17T17:00:44Z","score":51},{"id":"arxiv_cond-mat/0404537","title":"Exponential Convergence of Cellular Dynamical Mean Field Theory: Reply to the comment by K. Aryanpour, Th. Maier and M. Jarrell (cond-mat/0301460)","authors":[{"name":"G. Biroli"},{"name":"G. Kotliar"}],"abstract":"We reply to the comment by K. Aryanpour, Th. Maier and M. Jarrell (cond-mat/0301460) on our paper (Phys. Rev. B {\\bf 65} 155112 (2002)). We demonstrate using general arguments and explicit examples that whenever the correlation length is finite, local observables converge exponentially fast in the cluster size, $L_{c}$, within Cellular Dynamical Mean Field Theory (CDMFT). This is a faster rate of convergence than the $1/L_{c}^{2}$ behavior of the Dynamical Cluster approximation (DCA) thus refuting the central assertion of their comment.","source":"arXiv","year":2004,"language":"en","subjects":["cond-mat.str-el"],"doi":"10.1103/PhysRevB.71.037102","url":"https://arxiv.org/abs/cond-mat/0404537","pdf_url":"https://arxiv.org/pdf/cond-mat/0404537","is_open_access":true,"published_at":"2004-04-22T18:50:06Z","score":50},{"id":"arxiv_cond-mat/0610723","title":"Supplementary Information for cond-mat/0610721: Potok et al. \"Observation of the two-channel Kondo effect\"","authors":[{"name":"R. M. Potok"},{"name":"I. G. Rau"},{"name":"Hadas Shtrikman"},{"name":"Yuval Oreg"},{"name":"D. Goldhaber-Gordon"}],"abstract":"This document provides detailed descriptions of data acquisition and data analysis in support of the accompanying Article, cond-mat/0610721: Observation of the two-channel Kondo effect.   Some of the most intriguing problems in solid state physics arise when the motion of one electron dramatically affects the motion of surrounding electrons. Traditionally, such highly-correlated electron systems have been studied mainly in materials with complex transition metal chemistry. Over the past decade, researchers have learned to confine one or a few electrons within a nanoscale semiconductor \"artificial atom\", and to understand and control this simple system in exquisite detail. In the accompanying Article, we combine such individually well-understood components to create a novel highly-correlated electron system within a nano-engineered semiconductor structure. We tune the system in situ through a quantum phase transition between two distinct states, one familiar and one subtly new. The boundary between these states is a quantum critical point: the exotic and previously elusive two-channel Kondo state, in which electrons in two reservoirs are entangled through their interaction with a single localized spin.","source":"arXiv","year":2006,"language":"en","subjects":["cond-mat.mes-hall","cond-mat.stat-mech","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0610723","pdf_url":"https://arxiv.org/pdf/cond-mat/0610723","is_open_access":true,"published_at":"2006-10-26T03:20:42Z","score":50},{"id":"arxiv_cond-mat/0112478","title":"Comment on cond-mat/0007299 by Schofield and Sandeman : inconsistency with experiments","authors":[{"name":"George Kastrinakis"}],"abstract":"The inconsistency of cond-mat/0007299 and Phys. Rev. B 63 094510 (2001) with ARPES and resistivity data is pointed-out.","source":"arXiv","year":2001,"language":"en","subjects":["cond-mat.str-el","cond-mat.supr-con"],"url":"https://arxiv.org/abs/cond-mat/0112478","pdf_url":"https://arxiv.org/pdf/cond-mat/0112478","is_open_access":true,"published_at":"2001-12-28T13:13:32Z","score":50},{"id":"arxiv_cond-mat/0310139","title":"On the applicability of an equation of motion method at low-temperatures: comments on cond-mat/0309458 and cond-mat/0308413","authors":[{"name":"Akira Oguri"}],"abstract":"The equation of motion method (EOM) is one of the approximations to calculate transport coefficients of interacting electron systems. The method is known to be useful to examine high-temperature properties. However, sometimes a naive application of the EOM fails to capture an important physics at low-energy scale, and it happens in recent preprints cond-mat/0309458 and cond-mat/0308413 which study a series of quantum dots. These preprints concluded that a unitarity-limit transport due to the Kondo resonance, which has been deduced from a Fermi-liquid behavior of the self-energy at T=0, $ω=0$ [A.O., PRB {\\bf 63}, 115305 (2001)], does not occur. We show that the EOM self-energy obtained with a finite cluster has accidentally a singular $1/ω$ dependence around the Fermi energy, and it misleads one to the result incompatible with a Fermi-liquid ground state.","source":"arXiv","year":2003,"language":"en","subjects":["cond-mat.mes-hall","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0310139","pdf_url":"https://arxiv.org/pdf/cond-mat/0310139","is_open_access":true,"published_at":"2003-10-07T10:00:09Z","score":50},{"id":"arxiv_cond-mat/0105026","title":"Comment on \"Non-equilibrium Electron Distribution in Presence of Kondo Impurities\" (cond-mat/0102150v2)","authors":[{"name":"J. Kroha"},{"name":"A. Zawadowski"}],"abstract":"An inadequate approximation and its consequences as well as an incorrect statement made in cond-mat/0102150v2 are pointed out.","source":"arXiv","year":2001,"language":"en","subjects":["cond-mat.mes-hall","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0105026","pdf_url":"https://arxiv.org/pdf/cond-mat/0105026","is_open_access":true,"published_at":"2001-05-02T22:41:12Z","score":50},{"id":"arxiv_cond-mat/0102064","title":"Comment on ``Specific heat of a Fermi system near ferromagnetic quantum phase transition'' by Grosu, Bodea, and Crisan (cond-mat/0101392)","authors":[{"name":"D. Belitz"},{"name":"T. R. Kirkpatrick"}],"abstract":"We comment on various incorrect claims made in a recent paper by Grosu et al. (cond-mat/0101392).","source":"arXiv","year":2001,"language":"en","subjects":["cond-mat.stat-mech","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0102064","pdf_url":"https://arxiv.org/pdf/cond-mat/0102064","is_open_access":true,"published_at":"2001-02-05T20:22:55Z","score":50},{"id":"arxiv_cond-mat/0107372","title":"Comment on \"Discovery of microscopic electronic inhomogeneity in the high-$T_c$ superconductor $Bi_2Sr_2CaCu_2O_{8+x}$\", cond-mat/0107347","authors":[{"name":"J. E. Hirsch"}],"abstract":"The paper by Pan et al, cond-mat/0107347, reports the discovery of 'electronic inhomogeneity' and 'spatial variations in the local density of states' in high $T_c$ cuprates. In my paper ``Effect of local potential variations in the model of hole superconductivity'', Physica C {\\bf 194}, 119 (1992), many of the findings of Pan et al were foreshadowed.","source":"arXiv","year":2001,"language":"en","subjects":["cond-mat.supr-con","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0107372","pdf_url":"https://arxiv.org/pdf/cond-mat/0107372","is_open_access":true,"published_at":"2001-07-17T22:56:33Z","score":50},{"id":"arxiv_cond-mat/0002121","title":"Comment on: \"Auger decay, Spin-exchange, and their connection to Bose-Einstein condensation of excitons in Cu_2O \" by G.M. Kavoulakis, A. Mysyrowicz (cond-mat/0001438)","authors":[{"name":"A. B. Kuklov"}],"abstract":"It is shown that the interconversion mechanism for the triplet excitons in Cu_2O suggested recently by G.M. Kavoulakis and A. Mysyrowicz in cond-mat/0001438 can be tested by the two-photon direct creation of the triplet excitons.","source":"arXiv","year":2000,"language":"en","subjects":["cond-mat.stat-mech","cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0002121","pdf_url":"https://arxiv.org/pdf/cond-mat/0002121","is_open_access":true,"published_at":"2000-02-08T21:53:43Z","score":50},{"id":"arxiv_cond-mat/0601003","title":"Reply to the comment to Phy. Rev. Lett. 86, 3392 (2001) (cond-mat/0511607)","authors":[{"name":"B. A. Bernevig"},{"name":"D. Giuliano"},{"name":"R. B. Laughlin"}],"abstract":"We provide our reply to the comment by Greiter and Schuricht (cond-mat/0511607).","source":"arXiv","year":2005,"language":"en","subjects":["cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0601003","pdf_url":"https://arxiv.org/pdf/cond-mat/0601003","is_open_access":true,"published_at":"2005-12-31T12:55:33Z","score":50},{"id":"arxiv_cond-mat/0302058","title":"Spin-charge separation and recombination in quantum disordered d-wave superconductors","authors":[{"name":"Igor F. Herbut"}],"abstract":"Some of the results of this paper have been superseded in the meantime. See, cond-mat/0410557.","source":"arXiv","year":2003,"language":"en","subjects":["cond-mat.str-el","cond-mat.supr-con","hep-th"],"url":"https://arxiv.org/abs/cond-mat/0302058","pdf_url":"https://arxiv.org/pdf/cond-mat/0302058","is_open_access":true,"published_at":"2003-02-04T01:22:08Z","score":50},{"id":"arxiv_cond-mat/0508452","title":"Reply to the comment by C. Capan and K. Behnia on \"Nernst effect in poor conductors and in the cuprate superconductors\" (cond-mat/0501288)","authors":[{"name":"A. S. Alexandrov"}],"abstract":"The comment criticisms (cond-mat/0501288) are completely out of line with the context of the commented theory (Phys. Rev. Lett. v.93, 217002 (2004)). The comment neglected essential parts of the theory, which actually addressed all relevant experimental observations. I argue that the coexistence of the large Nernst signal and the insulating-like in-plane resistivity in underdoped cuprates rules out the vortex scenario, but agrees remarkably well with our theory.","source":"arXiv","year":2005,"language":"en","subjects":["cond-mat.supr-con","cond-mat.str-el"],"doi":"10.1103/PhysRevLett.95.259704","url":"https://arxiv.org/abs/cond-mat/0508452","pdf_url":"https://arxiv.org/pdf/cond-mat/0508452","is_open_access":true,"published_at":"2005-08-19T11:15:05Z","score":50},{"id":"arxiv_cond-mat/0410605","title":"Shashkin et al. reply to cond-mat/0410409","authors":[{"name":"A. A. Shashkin"},{"name":"S. Anissimova"},{"name":"M. R. Sakr"},{"name":"S. V. Kravchenko"},{"name":"V. T. Dolgopolov"},{"name":"T. M. Klapwijk"}],"abstract":"We show that the Comment by Reznikov and Sivan (cond-mat/0410409) is erroneous because the authors do not distinguish between Pauli and Curie spin susceptibility.","source":"arXiv","year":2004,"language":"en","subjects":["cond-mat.str-el"],"url":"https://arxiv.org/abs/cond-mat/0410605","pdf_url":"https://arxiv.org/pdf/cond-mat/0410605","is_open_access":true,"published_at":"2004-10-25T14:17:10Z","score":50},{"id":"arxiv_cond-mat/0008342","title":"Spectroscopic evidence for unconventional superconductivity in UBe$_{13}$","authors":[{"name":"Ch. Wälti"},{"name":"H. R. Ott"},{"name":"Z. Fisk"},{"name":"J. L. Smith"}],"abstract":"Reply to cond-mat/0007006 by Gloos","source":"arXiv","year":2000,"language":"en","subjects":["cond-mat.str-el","cond-mat.supr-con"],"doi":"10.1103/PhysRevLett.84.5616","url":"https://arxiv.org/abs/cond-mat/0008342","pdf_url":"https://arxiv.org/pdf/cond-mat/0008342","is_open_access":true,"published_at":"2000-08-23T16:59:59Z","score":50}],"total":1762685,"page":1,"page_size":20,"sources":["CrossRef","arXiv"],"query":"cond-mat.str-el"}