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1.
Nat Mater ; 12(6): 535-41, 2013 Jun.
Artículo en Inglés | MEDLINE | ID: mdl-23524373

RESUMEN

Josephson plasma waves are linear electromagnetic modes that propagate along the planes of cuprate superconductors, sustained by interlayer tunnelling supercurrents. For strong electromagnetic fields, as the supercurrents approach the critical value, the electrodynamics become highly nonlinear. Josephson plasma solitons (JPSs) are breather excitations predicted in this regime, bound vortex-antivortex pairs that propagate coherently without dispersion. We experimentally demonstrate the excitation of a JPS in La1.84Sr0.16CuO4, using intense narrowband radiation from an infrared free-electron laser tuned to the 2-THz Josephson plasma resonance. The JPS becomes observable as it causes a transparency window in the opaque spectral region immediately below the plasma resonance. Optical control of magnetic-flux-carrying solitons may lead to new applications in terahertz-frequency plasmonics, in information storage and transport and in the manipulation of high-Tc superconductivity.

3.
Science ; 331(6014): 189-91, 2011 Jan 14.
Artículo en Inglés | MEDLINE | ID: mdl-21233381

RESUMEN

One of the most intriguing features of some high-temperature cuprate superconductors is the interplay between one-dimensional "striped" spin order and charge order, and superconductivity. We used mid-infrared femtosecond pulses to transform one such stripe-ordered compound, nonsuperconducting La(1.675)Eu(0.2)Sr(0.125)CuO(4), into a transient three-dimensional superconductor. The emergence of coherent interlayer transport was evidenced by the prompt appearance of a Josephson plasma resonance in the c-axis optical properties. An upper limit for the time scale needed to form the superconducting phase is estimated to be 1 to 2 picoseconds, which is significantly faster than expected. This places stringent new constraints on our understanding of stripe order and its relation to superconductivity.

4.
Leuk Res ; 33(2): 348-50, 2009 Feb.
Artículo en Inglés | MEDLINE | ID: mdl-18573526

RESUMEN

The fms-related tyrosine kinase 3 internal tandem duplication (FLT3-ITD) can be found in about one quarter of patients with acute myeloid leukemia (AML) [Small D. FLT3 mutations: biology and treatment. Hematology Am Soc Hematology. Educ. Program 2006;178-84 [Review]]. Patients who carry this mutation have a high risk of relapse even after allogeneic stem cell transplantation [Sheikhha MH, Awan A, Tobal K, Liu Yin JA. Prognostic significance of FLT3 ITD and D835 mutations in AML patients. Hematol J 2003;4:41-6; Meshinchi S, Arceci RJ, Sanders JE, Smith FO, Woods WB, Radich JP, et al. Role of allogeneic stem cell transplantation in FLT3/ITD-positive AML. Blood 2006;108(1):400-1]. Recent reports show that Sorafenib, a multikinase inhibitor has significant activity against FLT3-ITD(+) blasts in vitro [Auclair D, Miller D, Yatsula V, Pickett W, Carter C, Chang Y, et al. Antitumor activity of sorafenib in FLT3-driven leukemic cells. Leukemia 2007;21(3):439-45]. We here report the first clinical case of molecular remission induced by Sorafenib in a patient with FLT3-ITD(+) AML and extramedullary disease after allogenic stem cell transplantation.


Asunto(s)
Bencenosulfonatos/uso terapéutico , Leucemia Mieloide Aguda/tratamiento farmacológico , Piridinas/uso terapéutico , Tirosina Quinasa 3 Similar a fms/genética , Humanos , Leucemia Mieloide Aguda/genética , Niacinamida/análogos & derivados , Compuestos de Fenilurea , Inducción de Remisión/métodos , Sorafenib , Secuencias Repetidas en Tándem
5.
Chaos ; 17(3): 033104, 2007 Sep.
Artículo en Inglés | MEDLINE | ID: mdl-17902986

RESUMEN

We determine the probability distribution of the first passage time for a class of non-Markovian processes. This class contains, amongst others, the well-known continuous time random walk (CTRW), which is able to account for many properties of anomalous diffusion processes. In particular, we obtain the mean first passage time for CTRW processes with truncated power-law transition time distribution. Our treatment is based on the fact that the solutions of the non-Markovian master equation can be obtained via an integral transform from a Markovian Langevin process.

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