Search PubMed⌕ Search

SEARCH · Search PubMed

Results for “fiber”

Search indexed PubMed citations on genomics, clinical trials, systematic reviews and public health. Explore titles, authors and supplied subject terms, then open the PubMed record.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

At least 361 records · Page 20Linked to original sources

Climbing fiber action on the responsiveness of Purkinje cells to parallel fiber inputs.

Recent work in our laboratory has demonstrated that spontaneous or evoked climbing fiber inputs are associated with an increased responsiveness of Purkinje cells to mossy fiber inputs activated by natural peripheral stimuli. These experiments were designed to test the hypothesis that this increased responsiveness occurs in the cerebellar cortex. In decerebrate, unanesthetized cats Purkinje cells in the surface folium were isolated and their simple and complex spikes discriminated. A bipolar concentric stimulating electrode was placed on the surface of the folium to activate the parallel fiber volley and modulate the Purkinje cell's simple spike discharge. The cell's simple spike discharge was evaluated when the surface stimulus was presented randomly and when this stimulus was timed to occur at a fixed interval after the spontaneous complex spike activity. When the surface stimulus was timed to occur at short intervals after the spontaneous complex spike, the response to the surface stimulus was accentuated. This increase in simple spike modulation occurred independent of whether the simple spike discharge increased or decreased in response to the surface stimulus. These results support the hypothesis that the climbing fiber input changes the gain of Purkinje cells' simple spike responses to mossy fiber inputs due to interactions occurring in the cerebellar cortex.

Afferent Pathways↗

Effects of pressure on equatorial x-ray fiber diffraction from skeletal muscle fibers.

When skeletal muscle fibers are subjected to a hydrostatic pressure of 10 MPa (100 atmospheres), reversible changes in tension occur. Passive tension from relaxed muscle is unaffected, rigor tension rises, and active tension falls. The effects of pressure on muscle structure are unknown: therefore a pressure-resistant cell for x-ray diffraction has been built, and this paper reports the first study of the low-angle equatorial patterns of pressurized relaxed, rigor, and active muscle fibers, with direct comparisons from the same chemically skinned rabbit psoas muscle fibers at 0.1 and 10 MPa. Relaxed and rigor fibers show little change in the intensity of the equatorial reflections when pressurized to 10 MPa, but there is a small, reversible expansion of the lattice of 0.7 and 0.4%, respectively. This shows that the order and stability of the myofilament lattice is undisturbed by this pressure. The rise in rigor tension under pressure is thus probably due to axial shortening of one or more components of the sarcomere. Initial results from active fibers at 0.1 MPa show that when phosphate is added the lattice spacing and equatorial intensities change toward their relaxed values. This indicates cross-bridge detachment, as expected from the reduction in tension that phosphate induces. 10 MPa in the presence of phosphate at 11 degrees C causes tension to fall by a further 12%, but not change is detected in the relative intensity of the reflections, only a small increase in lattice spacing. Thus pressure appears to increase the proportion of attached cross-bridges in a low-force state.

Animals↗

The effect of fiber orientation on the thermal expansion coefficients of fiber-reinforced composites.

OBJECTIVES: The aim of this study was to characterize the thermal expansion and dimensional changes of fiber-reinforced composite (FRC) according to the fiber orientation, brand of FRC product and polymerization conditions. METHODS: Cubic specimens (n=5) were prepared from different brands of FRC and particulate filler composites and dimethacrylate monomer resin. The specimens were polymerized with a light-curing device for 40 s or additionally with prolonged polymerization in the light-curing oven for 15 min. Linear coefficients of thermal expansion (LCTE) values for different materials and for FRC with different fiber orientations were determined using a thermomechanical analyzer. RESULTS: All specimens exhibited linear increase in the value of LCTE between 37 and 67 degrees C. The analysis of ANOVA revealed that orientation of fiber and brand of material had significant effect (P<0.001) on LCTE values for 37-67 degrees C interval. Some interaction between factors also existed. Also, temperature interval 110-150 degrees C had significant effect on the LCTE values according to the curing unit, brand and orientation of fibers. SIGNIFICANCE: The results of this study suggest that the anisotropic nature of FRC exists also with regard to thermal expansion. The variation of LCTE of FRC compared to that of particulate filler composites might influence the interfacial adhesion of FRC appliances.

Analysis of Variance↗

Novel method for the preparation of N-acylchitosan fiber and N-acylchitosan-cellulose fiber.

A novel method for the preparation of N-acylchitosan fiber and N-acylchitosan-cellulose fiber is described. Each aqueous solution of sodium N-acetyl and N-propionylchitosan salts in aqueous 14% NaOH was spun through a viscose-type spinneret at 10-15 degrees C into a coagulating bath containing aqueous 10%, H2SO4. 25% Na2SO4 and 1.3% ZnSO4 to afford the corresponding white fiber. By the same method, a clear solution of sodium N-acetyl and N-propionyl chitosan salts were respectively mixed with sodium cellulose xanthate in aqueous 14% NaOH and spun to afford the corresponding white N-acylchitosan-cellulose fiber. Their filament tenacity and elongation values were 0.4-0.7 times as large as cellulose. These fibers were digestible in reactions by chitinase and lysozyme, and the digestibility was controlled by the structure of the N-acyl group.

Bandages↗

Excitation of skinned muscle fibers by imposed ion gradients. III. Distribution of permeant ions in unstimulated and stimulated fibers.

Ion gradients imposed across an internal membrane system stimulate skinned muscle fibers; to evaluate the sarcoplasmic reticulum (SR) as the primary target site, SR polarization under resting and stimulatory conditions was assessed from fiber uptake of permeant probe ions. Solvent spaces were estimated from simultaneous [14C]urea (U) or [3H]deoxyglucose (DOG) uptake in segments of fibers from bullfrog semitendinosus muscle, skinned by microdissection. The distribution spaces, i.e., virtual solvent volumes at bath concentrations (Vu and VDOG), of these uncharged probes correlated well with the protein content of the same segments, which validated the tracer methodology for volume normalization. The membrane-bounded volume fraction (Vm), derived from the difference between total solvent volume (Vs) and the non-membrane-bounded solvent volume (Vc), was sufficient to detect appreciable SR ion accumulation. The Vm estimated from the difference between VU and VDOG assayed simultaneously with 2 or 5-6 min exposures was 10-11%, which is consistent with the morphometric volume fraction (mostly SR) in frog fibers; however, the change in this difference after membrane permeabilization corresponded to Vm only 5%. The change in permeant ion distribution space caused by member permeabilization was used to assess SR membrane polarization, assuming the free ions distribute across the intact membrane according to the Nernst ratio. Resting polarization (SR lumen positive) was assessed from [14C]SCN- or [14C]propionate- distribution spaces in unstimulated fibers, expressed relative to VDOG (assayed simultaneously). The ratios for (a) [14C]SCN- space (carrier 2 mM) and (b) [14C]propionate- space (carrier 120 mM) were not decreased by membrane permeabilization. This indicated that anion distribution was independent of membrane integrity and did not reflect an SR transmembrane potential, although a was more and b was less than 1. Polarization under stimulatory conditions (lumen negative) was assessed from 86Rb+ distribution, before and after an imposed ion gradient (choline Cl replacement of K methanesulfonate (KMes) at constant [K+] [Cl-]) that theoretically could generate a 48-fold transmembrane cation ratio; Ca release was minimized by EGTA. The ratio of 86Rb+ space to VU, greater than 1 in KMes (120 mM K, the effective carrier), was higher in choline Cl (2.5 mM K) but not decreased by membrane permeabilization; this indicated that 86Rb+ distribution did not reflect an SR transmembrane potential. Similar results in the presence of valinomycin ruled out the possibility of inadequate 86Rb+ equilibration.(ABSTRACT TRUNCATED AT 400 WORDS)

Animals↗

Age-related conversion of dystrophin-negative to -positive fiber segments of skeletal but not cardiac muscle fibers in heterozygote mdx mice.

Immunoreactive dystrophin was examined in muscle fibers of quadriceps, extraocular muscles and cardiac ventricular muscles of female heterozygote mdx mice at 10, 35 and 60 days of age, with microscopic immunoperoxidase method and by immunoblots. In quadriceps muscle fibers there was a marked gradual diminution of the dystrophin-negative fiber segments between age 10 and 60 days. We suggest that this was partly due to a spontaneous fusion of dystrophin-competent satellite cells into the dystrophin-negative fiber segments and partly to an expansion of the cytoplasmic domain of dystrophin expression related to the original myonuclei. In cardiac muscle that lacks satellite cells, there was persistence of a large number of dystrophin-negative fiber segments even at age 60 days and probably beyond. The findings of this study have implications for the detection of heterozygote female carriers of Duchenne muscular dystrophy (DMD) and for the possible therapy of DMD muscles by myoblast transfer.

Aging↗

Operating curves to characterize the contraction of fibroblast-seeded collagen gel/collagen fiber composite biomaterials: effect of fiber mass.

BACKGROUND: Collagen is a well-established and important biomaterial that could be used to help meet significant medical needs for various soft-tissue replacements. Many efforts to create engineered soft-tissue constructs by seeding cells within collagen gels have been hampered because constituent cells contract collagen gels over time, resulting in a construct that is only a fraction of the original size and that contains a cell population that has suffered a large degree of cell death. However, the presence of embedded short collagen fibers has been shown to significantly limit contraction and dramatically enhance permeability in fibroblast-seeded collagen gels. METHODS: Five volume fractions of short collagen fibers were embedded in fibroblast-seeded collagen gels. Collagen gel contraction (n > or = 4 for all groups) and cell viability (n > or = 3 for all groups) were examined after up to 2 weeks in culture. RESULTS: The present study demonstrated that increasing the volume fraction of short collagen fibers in fibroblast-seeded collagen gels correspondingly reduced the amount of gel contraction without negatively impacting cell viability after 2 weeks of culture. Furthermore, operating curves that describe the quantitative relationships between the contraction of fibroblast-seeded collagen gel/collagen fiber composite biomaterials, time in culture, and volume fraction of embedded fibers were obtained. CONCLUSION: The resulting operating curves enable investigators to tailor initial fabrication procedures to ultimately yield cell-seeded collagen composites of specifically desired sizes-a critical step toward developing clinically useful engineered soft-tissue constructs.

Animals↗

All-fiber format compression of frequency chirped pulses in air-guiding photonic crystal fibers.

Air-cored, photonic band-gap crystal fibers exhibiting low nonlinearity and anomalous chromatic dispersion in spectral ranges inaccessible to conventional fibers can be used in the realization of all-fiber-format pulse compressors with unprecedented peak powers and wavelength diversity. Linear compression of inherently chirped and prestretched pulses by factors ranging from 20 to 80 around 1.0 and 1.5 microm have allowed generation of pulses as short as 163 fs. The results show that totally integrated femtosecond fiber laser sources can be realized throughout the visible and near-infrared and point to the possibility of megawatt peak and tens of watt average in-fiber power levels.

Journal Article↗

Left ventricular chamber filling and midwall fiber lengthening in patients with left ventricular hypertrophy: overestimation of fiber velocities by conventional midwall measurements.

Observations that the inner (subendocardial) half of the left ventricular wall contributes more to total left ventricular wall thickening than the outer (subepicardial) half may have important implications in the analysis of myocardial fiber length transients. Accordingly, we measured endocardial and midwall shortening and lengthening rates in normal and hypertrophic heart and compared the results obtained with conventional methods of measurement with those obtained with a modified model that does not depend on use of conventional assumptions about the midwall. This modified (two-shell) cylindrical model) method considers the substantial contribution of inner wall thickening and thus does not require the assumption of a theoretical midwall fiber that remains at the midwall throughout the cardiac cycle. Echocardiographic data from six normal subjects and six patients with concentric left ventricular hypertrophy (LVH) were examined; left ventricular wall thickness ranged from 8 to 10 mm in normal subjects and from 11 to 16 mm in the patients with LVH. By design, the standard measurements of left ventricular size (diastolic and systolic dimensions) and systolic function (fractional shortening and endocardial fiber shortening velocities) were equal in the two groups. Endocardial, conventional midwall, and modified midwall methods all indicate reduced fiber lengthening rates in patients with LVH; peak fiber lengthening rates for normal and LVH groups were 4.5 +/- 0.7 vs 3.1 +/- 0.8 sec-1 (p less than .02) at the endocardium, 2.3 +/- 0.4 vs 1.6 +/- 0.4 sec-1 (p less than .02) at the midwall (conventional method), and 2.1 +/- 0.3 vs 1.4 +/- 0.3 sec-1 (p less than .01) at the midwall (modified method).(ABSTRACT TRUNCATED AT 250 WORDS)

Cardiomegaly↗

Extrahypothalamic neurophysin-containing perikarya, fiber pathways and fiber clusters in the rat brain.

Immunoreactive neurophysin (Np) is demonstrated by the immunoperoxidase technique not only within neurones of the classical hypothalamo-neurohypophyseal system, but also in extrahypothalamic perikarya and fibers. Np-positive perikarya are found in the triangular nucleus of the septum. Np fibers join the stria terminalis (ST) at the level of the anterior hypothalamus, and course medially in the ST to the central nucleus of the amygdala. Np fibers are found in the brain stem and spinal cord. Fine caliber Np fibers from the suprachiasmatic nucleus ascend to the medial dorsal thalamus and lateral septum. The presence of Np within neurones implies the presence of either vasopressin or oxytocin. Np-positive fibers in extrahypothalamic sites may interact with non-neurosecretory neurones involved in neuroendocrine regulation, or may serve as yet unknown functions.

Animals↗

Eigenvalue and field equations of three-layered uniaxial fibers and their applications to the characteristics of long-period fiber gratings with applied axial strain.

By using the Debye potentials, the exact eigenvalue equations and the corresponding field distributions of the core and cladding modes for three-layered, radially stratified, and dielectric uniaxial optical fibers are derived completely; the modes include TE, TM, and hybrid HE/EH modes. The strain characteristics of long-period fiber gratings' (LPFGs') with applied axial strain are investigated theoretically by studying three-layered uniaxial optical fibers. When uniform axial strain is applied to fiber, the core, and inner and outer cladding become uniaxial crystal optically; that is, the optical axes are parallel to the fiber's axis. Analytic expressions of the strain sensitivities of LPFGs are derived. The analysis reveals that the strain sensitivities of LPFGs based on various cladding modes, including the shift value and direction of the resonance wavelength, differ greatly.

Journal Article↗

Single-mode Raman fiber laser based on a multimode fiber.

Single-mode operation of a Raman fiber laser based on a multimode fiber has been demonstrated for what is to our knowledge the first time. Single-mode operation was achieved through the beam cleanup effect of stimulated Raman scattering in multimode fibers. The Raman laser, consisting of a 50-microm-core multimode fiber and a multimode Nd:YAG laser pump, produced an output beam corresponding to the fundamental mode of the fiber.

Journal Article↗

High-temperature sustainability of strong fiber Bragg gratings written into Sb-Ge-codoped photosensitive fiber: decay mechanisms involved during annealing.

An antimony--germanium- (Sb--Ge-) codoped fiber specially designed for the fabrication of fiber Bragg gratings (FBGs) with high temperature sustainability has been developed. The photosensitivity and the high-temperature sustainability of FBGs that have been written into this fiber were tested. The results obtained showed that the FBG written into this fiber has a very high temperature sustainability of 900 degrees C. A decay mechanism that involves cation hopping is presented to explain the observed high temperature sustainability of the grating written into this fiber.

Journal Article↗

All-fiber single-mode fiber frequency-modulated continuous-wave Sagnac gyroscope.

An all-fiber single-mode fiber unbalanced Sagnac gyroscope is described. The gyroscope is based on optical frequency-modulated continuous-wave interference and consists primarily of four Y-type single-mode fiber directional couplers and a single-mode fiber coil. The rotational velocity of the fiber coil is determined simultaneously by detection of the phase shift of the beat signal. The advantages and limitations of the gyroscope are discussed.

Journal Article↗

Long-distance simultaneous measurement of strain and temperature based on a fiber Raman laser with a single fiber Bragg grating embedded on a quartz plate.

We propose and experimentally demonstrate long-distance remote simultaneous measurement of strain and temperature based on a Raman fiber laser with a single fiber Bragg grating embedded on a quartz plate. A Raman fiber laser output with a high extinction ratio of more than approximately 50 dB is achieved by the fiber grating cavity. In the sensing probe, half of the fiber Bragg grating is fixed steadily on the quartz plate to respond to temperature only, while the other half of the grating is free to respond to both temperature and strain. Based on the proposed scheme, lasing wavelength shift and separation occur with temperature and strain change, respectively. Efficient simultaneous measurement of strain and temperature for long-distance sensing applications of more than 50 km is readily obtained.

Journal Article↗

Sensitivity enhancement of fiber Bragg gratings to transverse stress by using microstructural fibers.

We present simulation and experimental results of fiber Bragg grating responses to transverse stress in microstructure fibers. The grating wavelength shifts and peak splits are studied as a function of external load and fiber orientation. Both simulation and measurement results indicate that the sensitivity of grating sensors to the transverse stress can be enhanced by a factor of eight in a two-hole fiber over that in a standard fiber.

Journal Article↗

Tuning of fiber lasers by use of a single-mode biconic fiber taper.

We report a novel scheme to build a compact, tunable fiber laser. The tuning mechanism is based on the transmission property of a single-mode biconic fiber taper. While pulling the taper, we observe oscillations in the transmitted optical power that are due primarily to interference between a pair of excited modes within the tapered region, which are eventually coupled into the unstretched single-mode fiber at the end of the taper. A similar mechanism causes the modulation of the transmitted optical spectrum after the taper has been pulled and stabilized. It is this spectral modulation by the taper that is exploited here to control the wavelength of a fiber laser. The modulation can be adjusted by stretching the taper, thus enabling the tuning of the laser wavelength. We have built a 32 mW Er-doped tunable ring fiber laser with a continuous tuning range of over 20 nm and a signal-to-noise ratio of better than 45 dB over the entire tuning range; our output power is limited only by the available pump power.

Journal Article↗

Long-distance fiber Bragg grating sensor system with a high optical signal-to-noise ratio based on a tunable fiber ring laser configuration.

A novel tunable fiber ring laser configuration with a combination of bidirectional Raman amplification and dual erbium-doped fiber (EDF) amplification is proposed for realizing high optical signal-to-noise ratio (SNR), long-distance, quasi-distributed fiber Bragg grating (FBG) sensing systems with large capacities and low cost. The hybrid Raman-EDF amplification configuration arranged in the ring laser can enhance the optical SNR of FBG sensor signals significantly owing to the good combination of the high gain of the erbium-doped fiber amplifier (EDFA) and the low noise of the Raman amplification. Such a sensing system can support a large number of FBG sensors because of the use of a tunable fiber Fabry-Perot filter located within the ring laser and spatial division multiplexing for expansion of sensor channels. Experimental results show that an excellent optical SNR of approximately 60 dB has been achieved for a 50 km transmission distance with a low Raman pump power of approximately 170 mW at a wavelength of 1455 nm and a low EDFA pump power of approximately 40 mW at a wavelength of 980 nm, which is the highest optical SNR achieved so far for a 50 km long FBG sensor system, to our knowledge.

Journal Article↗