Influence of composition on the structure and properties of Fe-Pd-P and Ni-Pd-P amorphous alloys

Ternary alloys of nickel-palladium-phosphorus and iron-palladium- phosphorus containing 20 atomic % phosphorus were rapidly quenched from the liquid state. The structure of the quenched alloys was investigated by X-ray diffraction. Broad maxima in the diffraction patterns, indicative of a glass-like structure, were obtained for 13 to 73 atomic % nickel and 13 to 44 atomic % iron, with palladium adding up to 80%.

Radial distribution functions were computed from the diffraction data and yielded average interatomic distances and coordination numbers. The structure of the amorphous alloys could be explained in terms of structural units analogous to those existing in the crystalline Pd₃P, Ni₃P and Fe₃P phases, with iron or nickel substituting for palladium. A linear relationship between interatomic distances and composition, similar to Vegard's law, was shown for these metallic glasses.

Electrical resistivity measurements showed that the quenched alloys were metallic. Measurements were performed from liquid helium temperatures (4.2°K) up to the vicinity of the melting points (900°K- 1000°K). The temperature coefficient in the glassy state was very low, of the order of 10^-4/°K. A resistivity minimum was found at low temperature, varying between 9°K and 14°K for Ni_x-Pd_80-x -P₂₀ and between 17°K and 96°K for Fe_x-Pd_80-x -P₂₀, indicating the presence of a Kondo effect. Resistivity measurements, with a constant heating rate of about 1.5°C/min,showed progressive crystallization above approximately 600°K.

The magnetic moments of the amorphous Fe-Pd-P alloys were measured as a function of magnetic field and temperature. True ferromagnetism was found for the alloys Fe₃₂-Pd₄₈-P₂₀ and Fe₄₄-Pd₃₆-P₂₀ with Curie points at 165° K and 380° K respectively. Extrapolated values of the saturation magnetic moments to 0° K were 1.70 µ_B and 2.10 µ_B respectively. The amorphous alloy Fe₂₃-Pd₅₇-P₂₀ was assumed to be superparamagnetic. The experimental data indicate that phosphorus contributes to the decrease of moments by electron transfer, whereas palladium atoms probably have a small magnetic moment. A preliminary investigation of the Ni-Pd-P amorphous alloys showed that these alloys are weakly paramagnetic.

Properties of superconducting CU-rich composites containing V_3SI or V_3GA

Superconducting Cu-rich composites containing the A-15 compounds V₃Si or V₃Ga have been made by the "Tsuei" process, which consists of melting the constituent elements into ingots followed by subsequent cold working and heat treatment. The superconducting transition temperatures of the resulting composites have been measured. X-ray diffraction analyses have been performed to identify the phases in the alloys. The microstructures have been studied using both the optical metallograph and the scanning electron-microscope. For some composites containing V₃Ga, the critical current densities as functions of transverse magnetic field up to 60 kG, and as functions of temperature from 4.2°K to 12°K have been measured. It was found that the Tsuei process does not work for the composites containing V₃Si, but works satisfactorily for the composites containing V₃Ga. The reasons are discussed based on the results of microstructure studies, electrical resistivity measurements, and also the relevant binary phase diagrams. The relations between the measured properties and the various metallurgical factors such as the alloy compositions, the cross-section reduction ratios of the materials, and the heat treatment are discussed. The basic mechanism for the observed superconductivity in the materials is also discussed. In addition, it was found that the Tsuei composites are expected to have high inherent magneto-thermal stability based on the stability theory of superconducting composites.

Investigation of bulk indium antimonide as heterodyne detector for the submillimeter wavelength region

Bulk n-lnSb is investigated at a heterodyne detector for the submillimeter wavelength region. Two modes or operation are investigated: (1) the Rollin or hot electron bolometer mode (zero magnetic field), and (2) the Putley mode (quantizing magnetic field). The highlight of the thesis work is the pioneering demonstration or the Putley mode mixer at several frequencies. For example, a double-sideband system noise temperature of about 510K was obtained using a 812 GHz methanol laser for the local oscillator. This performance is at least a factor or 10 more sensitive than any other performance reported to date at the same frequency. In addition, the Putley mode mixer achieved system noise temperatures of 250K at 492 GHz and 350K at 625 GHz. The 492 GHz performance is about 50% better and the 625 GHz is about 100% better than previous best performances established by the Rollin-mode mixer. To achieve these results, it was necessary to design a totally new ultra-low noise, room-temperature preamp to handle the higher source impedance imposed by the Putley mode operation. This preamp has considerably less input capacitance than comparably noisy, ambient designs.

In addition to advancing receiver technology, this thesis also presents several novel results regarding the physics of n-lnSb at low temperatures. A Fourier transform spectrometer was constructed and used to measure the submillimeter wave absorption coefficient of relatively pure material at liquid helium temperatures and in zero magnetic field. Below 4.2K, the absorption coefficient was found to decrease with frequency much faster than predicted by Drudian theory. Much better agreement with experiment was obtained using a quantum theory based on inverse-Bremmstrahlung in a solid. Also the noise of the Rollin-mode detector at 4.2K was accurately measured and compared with theory. The power spectrum is found to be well fit by a recent theory of non- equilibrium noise due to Mather. Surprisingly, when biased for optimum detector performance, high purity lnSb cooled to liquid helium temperatures generates less noise than that predicted by simple non-equilibrium Johnson noise theory alone. This explains in part the excellent performance of the Rollin-mode detector in the millimeter wavelength region.

Again using the Fourier transform spectrometer, spectra are obtained of the responsivity and direct detection NEP as a function of magnetic field in the range 20-110 cm^-1. The results show a discernable peak in the detector response at the conduction electron cyclotron resonance frequency tor magnetic fields as low as 3 KG at bath temperatures of 2.0K. The spectra also display the well-known peak due to the cyclotron resonance of electrons bound to impurity states. The magnitude of responsivity at both peaks is roughly constant with magnet1c field and is comparable to the low frequency Rollin-mode response. The NEP at the peaks is found to be much better than previous values at the same frequency and comparable to the best long wavelength results previously reported. For example, a value NEP=4.5x10^-13/Hz^1/2 is measured at 4.2K, 6 KG and 40 cm^-1. Study of the responsivity under conditions of impact ionization showed a dramatic disappearance of the impurity electron resonance while the conduction electron resonance remained constant. This observation offers the first concrete evidence that the mobility of an electron in the N=0 and N=1 Landau levels is different. Finally, these direct detection experiments indicate that the excellent heterodyne performance achieved at 812 GHz should be attainable up to frequencies of at least 1200 GHz.

Luminescence properties of electron-hole-droplets in pure and doped germanium

This work contains 4 topics dealing with the properties of the luminescence from Ge.

The temperature, pump-power and time dependences of the photoluminescence spectra of Li-, As-, Ga-, and Sb-doped Ge crystals were studied. For impurity concentrations less than about 10¹⁵cm^-3, emissions due to electron-hole droplets can clearly be identified. For impurity concentrations on the order of 10¹⁶cm^-3, the broad lines in the spectra, which have previously been attributed to the emission from the electron-hole-droplet, were found to possess pump-power and time dependent line shape. These properties show that these broad lines cannot be due to emission of electron-hole-droplets alone. We interpret these lines to be due to a combination of emissions from (1) electron-hole- droplets, (2) broadened multiexciton complexes, (3) broadened bound-exciton, and (4) plasma of electrons and holes. The properties of the electron-hole-droplet in As-doped Ge were shown to agree with theoretical predictions.

The time dependences of the luminescence intensities of the electron-hole-droplet in pure and doped Ge were investigated at 2 and 4.2°K. The decay of the electron-hole-droplet in pure Ge at 4.2°K was found to be pump-power dependent and too slow to be explained by the widely accepted model due to Pokrovskii and Hensel et al. Detailed study of the decay of the electron-hole-droplets in doped Ge were carried out for the first time, and we find no evidence of evaporation of excitons by electron-hole-droplets at 4.2°K. This doped Ge result is unexplained by the model of Pokrovskii and Hensel et al. It is shown that a model based on a cloud of electron-hole-droplets generated in the crystal and incorporating (1) exciton flow among electron-hole-droplets in the cloud and (2) exciton diffusion away from the cloud is capable of explaining the observed results.

It is shown that impurities, introduced during device fabrication, can lead to the previously reported differences of the spectra of laser-excited high-purity Ge and electrically excited Ge double injection devices. By properly choosing the device geometry so as to minimize this Li contamination, it is shown that the Li concentration in double injection devices may be reduced to less than about 10¹⁵cm^-3 and electrically excited luminescence spectra similar to the photoluminescence spectra of pure Ge may be produced. This proves conclusively that electron-hole-droplets may be created in double injection devices by electrical excitation.

The ratio of the LA- to TO-phonon-assisted luminescence intensities of the electron-hole-droplet is demonstrated to be equal to the high temperature limit of the same ratio of the exciton for Ge. This result gives one confidence to determine similar ratios for the electron-hole-droplet from the corresponding exciton ratio in semiconductors in which the ratio for the electron-hole-droplet cannot be determined (e.g., Si and GaP). Knowing the value of this ratio for the electron-hole-droplet, one can obtain accurate values of many parameters of the electron-hole-droplet in these semiconductors spectroscopically.

Hall coefficient and resistivity of an amorphous palladium-silicon alloy

The Hall coefficient and resistance in several specimens of an amorphous metallic alloy containing 80 at.% palladium and 20 at.% silicon have been investigated at temperatures between 4.2°K and room temperature. An ideal limiting behavior of these transport coefficients was analyzed on the basis of the nearly free electron model to yield a carrier density of 9 x 10²² cm.^-3, or about 1.7 electrons per palladium atom, and a mean free path of about 9Å which is almost constant with temperature. The deviations of the individual specimens from this ideal behavior, which were small but noticeable in the relative resistivity and much greater in the Hall coefficient, can be explained by invoking disk-shaped crystalline regions with low resistivity and a positive Hall coefficient. A detailed calculation shows how a volume fraction of such crystalline material too small to be noticed in X-ray diffraction could have a significant effect on the resistivity and a much greater effect on the Hall coefficient.

Radio frequency studies of surface resistance and critical magnetic field of type I and type II superconductors

The surface resistance and the critical magnetic field of lead electroplated on copper were studied at 205 MHz in a half-wave coaxial resonator. The observed surface resistance at a low field level below 4.2°K could be well described by the BCS surface resistance with the addition of a temperature independent residual resistance. The available experimental data suggest that the major fraction of the residual resistance in the present experiment was due to the presence of an oxide layer on the surface. At higher magnetic field levels the surface resistance was found to be enhanced due to surface imperfections.

The attainable rf critical magnetic field between 2.2°K and T_c of lead was found to be limited not by the thermodynamic critical field but rather by the superheating field predicted by the one-dimensional Ginzburg-Landau theory. The observed rf critical field was very close to the expected superheating field, particularly in the higher reduced temperature range, but showed somewhat stronger temperature dependence than the expected superheating field in the lower reduced temperature range.

The rf critical magnetic field was also studied at 90 MHz for pure tin and indium, and for a series of SnIn and InBi alloys spanning both type I and type II superconductivity. The samples were spherical with typical diameters of 1-2 mm and a helical resonator was used to generate the rf magnetic field in the measurement. The results of pure samples of tin and indium showed that a vortex-like nucleation of the normal phase was responsible for the superconducting-to-normal phase transition in the rf field at temperatures up to about 0.98-0.99 T_c' where the ideal superheating limit was being reached. The results of the alloy samples showed that the attainable rf critical fields near T_c were well described by the superheating field predicted by the one-dimensional GL theory in both the type I and type II regimes. The measurement was also made at 300 MHz resulting in no significant change in the rf critical field. Thus it was inferred that the nucleation time of the normal phase, once the critical field was reached, was small compared with the rf period in this frequency range.

Some generalizations of commutativity for linear transformations on a finite dimensional vector space

Let L be the algebra of all linear transformations on an n-dimensional vector space V over a field F and let A, B, ƐL. Let A_i+1 = A_iB - BA_i, i = 0, 1, 2,…, with A = A_o. Let f_k (A, B; σ) = A_2K+1 - ^σ1^A2K-1 ^{+ σ}2^A2K-3 -… +(-1)^Kσ_KA₁ where σ = (σ₁, σ₂,…, σ_K), σ_i belong to F and K = k(k-1)/2. Taussky and Wielandt [Proc. Amer. Math. Soc., 13(1962), 732-735] showed that f_n(A, B; σ) = 0 if σ_i is the i^th elementary symmetric function of (β₄- β_s)², 1 ≤ r ˂ s ≤ n, i = 1, 2, …, N, with N = n(n-1)/2, where β₄ are the characteristic roots of B. In this thesis we discuss relations involving f_k(X, Y; σ) where X, Y Ɛ L and 1 ≤ k ˂ n. We show: 1. If F is infinite and if for each X Ɛ L there exists σ so that f_k(A, X; σ) = 0 where 1 ≤ k ˂ n, then A is a scalar transformation. 2. If F is algebraically closed, a necessary and sufficient condition that there exists a basis of V with respect to which the matrices of A and B are both in block upper triangular form, where the blocks on the diagonals are either one- or two-dimensional, is that certain products X₁, X₂…X_r belong to the radical of the algebra generated by A and B over F, where X_i has the form f₂(A, P(A,B); σ), for all polynomials P(x, y). We partially generalize this to the case where the blocks have dimensions ≤ k. 3. If A and B generate L, if the characteristic of F does not divide n and if there exists σ so that f_k(A, B; σ) = 0, for some k with 1 ≤ k ˂ n, then the characteristic roots of B belong to the splitting field of g_k(w; σ) = w^2K+1 - σ₁w^2K-1 + σ₂w^2K-3 - …. +(-1)^K σ_Kw over F. We use this result to prove a theorem involving a generalized form of property L [cf. Motzkin and Taussky, Trans. Amer. Math. Soc., 73(1952), 108-114]. 4. Also we give mild generalizations of results of McCoy [Amer. Math. Soc. Bull., 42(1936), 592-600] and Drazin [Proc. London Math. Soc., 1(1951), 222-231].

The global optimization of phase-incoherent signals

The problem of global optimization of M phase-incoherent signals in N complex dimensions is formulated. Then, by using the geometric approach of Landau and Slepian, conditions for optimality are established for N = 2 and the optimal signal sets are determined for M = 2, 3, 4, 6, and 12.

The method is the following: The signals are assumed to be equally probable and to have equal energy, and thus are represented by points ṡ_i, i = 1, 2, …, M, on the unit sphere S₁ in C^N. If W_ik is the halfspace determined by ṡ_i and ṡ_k and containing ṡ_i, i.e. W_ik = {ṙϵC^N:| ≥ | ˂ṙ, ṡ_k˃|}, then the Ʀ_i = ∩/k≠i W_ik, i = 1, 2, …, M, the maximum likelihood decision regions, partition S₁. For additive complex Gaussian noise ṅ and a received signal ṙ = ṡ_ie^jϴ + ṅ, where ϴ is uniformly distributed over [0, 2π], the probability of correct decoding is P_C = 1/π^N ∞/ʃ/0 r^2N-1e^-(r2+1)U(r)dr, where U(r) = 1/M M/Ʃ/i=1 Ʀ_i ʃ/∩ S₁ I₀(2r | ˂ṡ, ṡ_i˃|)dσ(ṡ), and r = ǁṙǁ.

For N = 2, it is proved that U(r) ≤ ʃ/C_α I₀(2r|˂ṡ, ṡ_i˃|)dσ(ṡ) – 2K/M. h(1/2K [Mσ(C_α)-σ(S₁)]), where C_α = {ṡϵS₁:|˂ṡ, ṡ_i˃| ≥ α}, K is the total number of boundaries of the net on S₁ determined by the decision regions, and h is the strictly increasing strictly convex function of σ(C_α∩W), (where W is a halfspace not containing ṡ_i), given by h = ʃ/C_α∩W I₀ (2r|˂ṡ, ṡ_i˃|)dσ(ṡ). Conditions for equality are established and these give rise to the globally optimal signal sets for M = 2, 3, 4, 6, and 12.

Spontaneous and stimulated light emission due to radiative recombination in forward biased lead telluride P-N junctions

Since the discovery in 1962 of laser action in semiconductor diodes made from GaAs, the study of spontaneous and stimulated light emission from semiconductors has become an exciting new field of semiconductor physics and quantum electronics combined. Included in the limited number of direct-gap semiconductor materials suitable for laser action are the members of the lead salt family, i.e . PbS, PbSe and PbTe. The material used for the experiments described herein is PbTe . The semiconductor PbTe is a narrow band- gap material (E_g = 0.19 electron volt at a temperature of 4.2°K). Therefore, the radiative recombination of electron-hole pairs between the conduction and valence bands produces photons whose wavelength is in the infrared (λ ≈ 6.5 microns in air).

The p-n junction diode is a convenient device in which the spontaneous and stimulated emission of light can be achieved via current flow in the forward-bias direction. Consequently, the experimental devices consist of a group of PbTe p-n junction diodes made from p –type single crystal bulk material. The p - n junctions were formed by an n-type vapor- phase diffusion perpendicular to the (100) plane, with a junction depth of approximately 75 microns. Opposite ends of the diode structure were cleaved to give parallel reflectors, thereby forming the Fabry-Perot cavity needed for a laser oscillator. Since the emission of light originates from the recombination of injected current carriers, the nature of the radiation depends on the injection mechanism.

The total intensity of the light emitted from the PbTe diodes was observed over a current range of three to four orders of magnitude. At the low current levels, the light intensity data were correlated with data obtained on the electrical characteristics of the diodes. In the low current region (region A), the light intensity, current-voltage and capacitance-voltage data are consistent with the model for photon-assisted tunneling. As the current is increased, the light intensity data indicate the occurrence of a change in the current injection mechanism from photon-assisted tunneling (region A) to thermionic emission (region B). With the further increase of the injection level, the photon-field due to light emission in the diode builds up to the point where stimulated emission (oscillation) occurs. The threshold current at which oscillation begins marks the beginning of a region (region C) where the total light intensity increases very rapidly with the increase in current. This rapid increase in intensity is accompanied by an increase in the number of narrow-band oscillating modes. As the photon density in the cavity continues to increase with the injection level, the intensity gradually enters a region of linear dependence on current (region D), i.e. a region of constant (differential) quantum efficiency.

Data obtained from measurements of the stimulated-mode light-intensity profile and the far-field diffraction pattern (both in the direction perpendicular to the junction-plane) indicate that the active region of high gain (i.e. the region where a population inversion exists) extends to approximately a diffusion length on both sides of the junction. The data also indicate that the confinement of the oscillating modes within the diode cavity is due to a variation in the real part of the dielectric constant, caused by the gain in the medium. A value of τ ≈ 10^-9 second for the minority- carrier recombination lifetime (at a diode temperature of 20.4°K) is obtained from the above measurements. This value for τ is consistent with other data obtained independently for PbTe crystals.

Data on the threshold current for stimulated emission (for a diode temperature of 20. 4°K) as a function of the reciprocal cavity length were obtained. These data yield a value of J’_th = (400 ± 80) amp/cm² for the threshold current in the limit of an infinitely long diode-cavity. A value of α = (30 ± 15) cm^-1 is obtained for the total (bulk) cavity loss constant, in general agreement with independent measurements of free- carrier absorption in PbTe. In addition, the data provide a value of n_s ≈ 10% for the internal spontaneous quantum efficiency. The above value for n_s yields values of t_b ≈ τ ≈ 10^-9 second and t_s ≈ 10^-8 second for the nonradiative and the spontaneous (radiative) lifetimes, respectively.

The external quantum efficiency (n_d) for stimulated emission from diode J-2 (at 20.4° K) was calculated by using the total light intensity vs. diode current data, plus accepted values for the material parameters of the mercury- doped germanium detector used for the measurements. The resulting value is n_d ≈ 10%-20% for emission from both ends of the cavity. The corresponding radiative power output (at λ = 6.5 micron) is 120-240 milliwatts for a diode current of 6 amps.

宽频带激光自由空间传输的调制特性研究

基于惠更斯-菲涅耳衍射积分公式，研究了宽带光束在菲涅耳衍射区的自由空间传输特性，得到宽带光束传输的调制深度与光束带宽出及菲涅耳数F的变化关系。结果表明：一定的带宽对光束的均匀性有适当的改善；当光束的带宽△λ〈2λ。／F时，带宽越大，光束越均匀；当带宽满足条件△λ=2λ。／F时，菲涅耳衍射完全消失；在一定的菲涅耳数范围内，宽带光束的调制深度随菲涅耳数振荡变化，振荡曲线的主极大值和次极大值分别出现在菲涅耳数为奇数和偶数处，而极小值则出现在菲涅耳数F-2k± 1／3（k=1，2，3，…）处，在极小值处光束的均匀

Estudo da bioenergética mitocondrial de cardiomiócitos de camundongos obesos

A obesidade é uma doença crônica, resultante do excesso de gordura no organismo. O aumento da obesidade no mundo, tem se revelado como um dos fenômenos clínicos e epidemiológicos da atualidade. Estudos populacionais e em modelos animais demonstram que a origem da epidemia da obesidade está relacionada a fatores genéticos, modificações de hábitos nutricionais, redução da atividade física, e alterações nutricionais durante a lactação, desempenhando um papel relevante no desenvolvimento da obesidade, DM2 e cardiomiopatias. As mitocôndrias são os coordenadores centrais do metabolismo energético, assim, alterações funcionais e estruturais dessa organela têm sido associadas à desordens metabólicas. Elas exercem um papel na sobrevivência e função dos cardiomiócitos devido à alta demanda energética do miocárdio. Desta forma, disfunções mitocondriais estão relacionadas com disfunções no miocárdio e conseqüente progressão de cardiomiopatias. Neste estudo, avaliamos a bioenergética e a ultraestrutura de cardiomiócitos de camundongos obesos e controle hiperalimentados durante a lactação. O consumo de oxigênio das fibras cardíacas foi avaliado por respirometria de alta-resolução, utilizando um oxígrafo-2K-Oroboros. A ultraestrutura dos cardiomiócitos foi analisada por microscopia eletrônica de transmissão e o conteúdo das proteínas Carnitina palmitoil transferase 1 (CPT1), Proteína desacopladora 2 (UCP2) , Transportador de glicose 1 e 4 (GLUT1) e (GLUT4), Proteína Kinase ativada por AMP (AMPK) e Proteína kinase ativada por AMP fosforilada p(AMPK) por Western blotting (WB). Além disso, o peso dos animais, a gordura retroperitoneal, epididimal e a glicemia em jejum foram determinadas. Nossos resultados confirmaram que os animais do grupo hiperalimentados (GH), aos 90 dias de vida, apresentaram aumento da massa corporal, de gordura epididimária e retroperitoneal comparado ao grupo controle (GC). As taxas respiratórias foram semelhantes nos dois grupos quando foram utilizados os substratos dos complexos I e II. Entretanto, quando o ácido graxo palmitoil-L-carnitina foi utilizado, a taxa respiratória máxima do GH foi significativamente menor. A análise ultraestrutural dos cardiomiócitos do GH demonstrou intenso dano na matriz mitocondrial e maior presença de gotículas de lipídios, caracterizando deposição ectópica. Os resultados do WB mostraram aumento significativo do conteúdo de CPT1 e UCP2 no GH comparado ao GC. Não foram encontradas diferenças significativas no conteúdo de GLUT1 entre os grupos, entretanto, observamos maior conteúdo do GLUT4 no GH. Além disso, encontramos maior conteúdo de AMPK no GH, ao passo que o conteúdo de pAMPK foi semelhante entre os grupos. Entretanto, a razão pAMPK/AMPK é significativamente menor no GH. Esses resultados sugerem que a hiperalimentação durante a lactação leva a obesidade na vida adulta com alterações na bioenergética e ultraestrutura dos cardiomiócitos.

千瓦级双包层光纤激光器冷却方案设计理论和实验研究

尽管双包层光纤激光器的散热性能好于传统的固体激光器的散热性能,光纤激光器中的热沉积仍然是限制提高其输出功率的重要因素.以双端抽运的400W双包层光纤激光器为实例,定量分析了光纤内的热沉积分布.根据所建立的散热模型,为了确保千瓦级双包层光纤激光器安全稳定的运行,抽运端附近的对流换热系数应大于2.8×10-2W·cm-2K-1.据此设计出高功率双包层光纤激光器抽运端冷却装置并成功应用在激光系统中,获得了千瓦级的激光输出.

Sinalização da grelina no coração de camundongos obesos após hipernutrição durante a lactação

A grelina é um ligante endógeno do receptor secretagogo do hormônio do crescimento (GHSR), potente estimulador da liberação do hormônio de crescimento (GH), ingestão alimentar, e adiposidade. Além disso, sua ação hormonal inclui regulação do metabolismo energético cardíaco. Entretanto, a hipernutrição no início da vida leva ao desenvolvimento da obesidade, induz hipertrofia cardíaca, compromete a função cardíaca, e gera insuficiência cardíaca na vida adulta. Avaliar proteínas chaves no processo de sinalização da grelina no remodelamento cardíaco no coração de camundongos obesos após a hipernutrição na lactação. A obesidade foi induzida por redução de ninhada e camundongos adultos (180 dias) foram divididos em: grupo hiperalimentado, GH com obesidade decorrente de hipernutrição na lactação e controle, GC. Cardiomiócitos (cmi) do ventrículo esquerdo foram analisados por microscopia de luz e estereologia, o conteúdo e fosforilação de proteínas cardíacas: receptor de grelina (hormônio do crescimento secretagogo receptor 1a, GHSR-1a), proteína quinase-B (AKT e pAKT), phosphatidil inositol 3-quinase (PI3K), proteína quinase ativada por AMP (AMPK e pAMPK), m-TOR, pmTOR, Bax, Bcl2 e actina foram analizados por western blotting. A expressão gênica do GHSR-1a foi analisada por PCR em tempo real. A respirometria de alta resolução dos cardiomiócitos foi analisada por oxígrafo OROBOROS. Significância estatística (P< 0,05) determinada por teste t-Student não-pareado. Nossos dados demonstram que a hipernutrição na lactação induz aumento no peso corporal, iniciado aos 10 dias de idade, persistindo até os 180 dias de idade. A glicemia, peso do fígado, e da gordura visceral foram maiores no grupo GH. Além disso, o grupo GH também apresentou aumento no peso do coração e razão peso do coração/CT (comprimento da tíbia), indicando hipertrofia e remodelamento cardíaco, aumento na expressão e conteúdo de GHSR-1a no coração, associado ao maior conteúdo de PI3K e maior conteúdo e fosforilação de AKT, diminuição no conteúdo de Bcl2. Em contraste, o conteúdo e fosforilação da AMPK e mTOR no coração não foram diferentes entre os grupos. Os níveis de grelina plasmático no GH foram menores. A respiração do GH com grelina foi menor que no GC com grelina. A incubação das fibras cardíacas com grelina resultou em aumento do fluxo respiratório após adição de citocromo c nos grupos com grelina, indicando dano à membrana mitocondrial e extravazamento de citocromo c. Os grupos GC com grelina e GH sem grelina apresentaram RCR menor comparado ao GC sem grelina, indicando desacoplamento mitocondrial. Nossos resultados mostram que a hipernutrição na lactação induz diminuição do nível de grelina plasmática e aumento da expressão do GHS-R1a no cardiomiócito do animal quando adulto. Tal processo determina aumento da sensibilidade a grelina no coração, processo que ocorre independentemente de variações do AMPK e mTOR. Sugerimos uma redução no efeito protetor da ação da grelina na AMPK. Também, demonstramos que o remodelamento do miocárdio nestes animais adultos associa-se a GHSR-1a, PI3K, e fosforilação da AKT, mas não com AMPK e mTOR na vida adulta.

Efeito do extrato de Euterpe oleracea Mart.(Açaí) sobre a disfunção endotelial, estresse oxidativo e alterações vasculares e renais associados à hipertensão renovascular dois rins, 1 clip (2R,1C)

Estudos recentes mostram que o açaí é rico em polifenóis e uma dieta rica em polifenóis pode estar envolvida na proteção contra o risco cardiovascular. O objetivo deste estudo foi avaliar o efeito do tratamento crônico de animais hipertensos 2R,1C com extrato hidroalcoólico do caroço do açaí (ASE) sobre o desenvolvimento da hipertensão e disfunção endotelial; estresse oxidativo e sobre as alterações vasculares e renais. Ratos Wistar machos foram utilizados para obtenção da hipertensão renovascular 2R,1C e ratos controles 2R (sham) foram somente submetidos à laparotomia e receberam tratamento diário com veículo ou ASE (200 mg/Kg/dia) durante 40 dias. A pressão arterial sistólica (PAS) foi aferida por pletismografia de cauda e os efeitos vasodilatadores da acetilcolina (ACh) e nitroglicerina (NG) foram estudados em leito arterial mesentérico (LAM) perfundido e pré-contraído com norepinefrina. A atividade das enzimas SOD, CAT, GPx, os níveis de MDA, a carbonilação de proteínas e os níveis de nitrito foram avaliados por espectrofotometria. As expressões de enzimas pró e antioxidantes foram avaliadas por western blot. A atividade de MMP-2 foi avaliada por zimografia. Os níveis séricos de creatinina foram avaliados através de kit, por espectrofotometria. As alterações vasculares e renais foram avaliadas por microscopia de luz. A PAS foi maior nos animais 2R,1C, e o tratamento com ASE preveniu o desenvolvimento da hipertensão. O efeito vasodilatador reduzido da ACh em animais 2R,1C foi recuperado pelo ASE. O efeito vasodilatador da NG não foi diferente entre os grupos. O dano oxidativo avaliado pela peroxidação lipídica e carbonilação de proteínas foi maior nos animais 2R,1C, e reduzido pelo tratamento com ASE. As atividades da SOD, CAT e GPx foram menores em amostras de mesentério, plasma, rim e coração de animais 2R,1C e o tratamento com ASE aumentou estas atividades. A produção de NO foi menor no plasma, mesentério e rim dos animais 2R,1C, e o tratamento com ASE aumentou a produção de NO somente no rim e mesentério destes animais. A expressão de SOD-1, 2, eNOS e TIMP-1 foram menores nos animais 2R,1C e o tratamento com ASE aumentou a expressão destas enzimas. A expressão de NOX-4 e MMP-2 e a atividade de MMP-2 foram maiores nos animais 2R,1C e o tratamento com ASE reduziu a expressão destas enzimas e a atividade de MMP-2. Os animais 2R,1C apresentaram um aumento na espessura da camada média da aorta e artéria mesentérica e um aumento na relação média/lúmen da aorta, e estas alterações foram prevenidas pelo ASE. Os níveis séricos aumentados de creatinina nos animais 2R,1C foram reduzidos por ASE. As alterações morfológicas renais nos animais 2R,1C foram prevenidas pelo ASE. Portanto, o tratamento com ASE previne o desenvolvimento da hipertensão, melhora a disfunção endotelial e previne as alterações vasculares e renais em ratos 2R,1C. A redução da atividade antioxidante e o aumento na peroxidação lipídica e carbonilação de proteínas sugerem o envolvimento de um mecanismo deficiente da defesa antioxidante e de um dano oxidativo aumentado, os quais foram revertidos pelo ASE.

Unusual carrier thermalization in a dilute GaAs1-xNx alloy

Photoluminescence (PL) properties of the E-0, E-0+Delta(0), and E+ bands in an x=0.62% GaAs1-xNx alloy were investigated in detail, including their peak position, linewidth, and line shape dependences on the excitation energy, excitation power, and temperature, using micro-PL. The hot electrons within the E+ band are found to exhibit highly unusual thermalization, which results in a large blueshift in its PL peak energy by >2k(B)T, suggesting peculiar density of states and carrier dynamics of the E+ band.