Modulation of the effectiveness of 17-alpha-hydroxy-20-beta-dihydroprogesterone or of a gonadotrophic extract on the in vitro intrafollicular maturation of oocytes of the rainbow trout Salmo gairdnerii by various non-maturing steroids [Translation from: Compte Rendu Hebdomadaire des Seances de l'Academie des Sciences, Paris, Series D 281, 811-814, 1975]

The effectiveness of 17 α-hydroxy-20 β-dihydroprogesterone (17 α-20 β Pg) or of a trout hypophyseal gonadotrophic extract on the in vitro intrafollicular maturation of trout oocytes can be modulated by steroids which do not have a direct maturing effect; the effectiveness of the gonadotrophic extract is lowered by oestradiol and oestrone and increased by testosterone. As these steroids have no significant effect on maturation induced by 17 α-20 β Pg, the site of their activity is probably in the follicular envelopes. Corticosteroids, and Cortisol and cortisone in particular increase the effectiveness of the gonadotrophic extract, but increase the effectiveness of 17 α-20 β Pg even more strongly, suggesting that this 'progestagen' has a direct effect on oocyte sensitivity.

Lq estimates for rearrangements of Fourier series

This work is concerned with estimating the upper envelopes S* of the absolute values of the partial sums of rearranged trigonometric sums. A.M. Garsia [Annals of Math. 79 (1964), 634-9] gave an estimate for the L₂ norms of the S*, averaged over all rearrangements of the original (finite) sum. This estimate enabled him to prove that the Fourier series of any function in L₂ can be rearranged so that it converges a.e. The main result of this thesis is a similar estimate of the L_q norms of the S*, for all even integers q. This holds for finite linear combinations of functions which satisfy a condition which is a generalization of orthonormality in the L₂ case. This estimate for finite sums is extended to Fourier series of L_q functions; it is shown that there are functions to which the Men’shov-Paley Theorem does not apply, but whose Fourier series can nevertheless be rearranged so that the S* of the rearranged series is in L_q.

Series representation of the Gaussian beam far-field diffracted by annular aperture

Accurate, analytical series expressions for the far-field diffraction of it Gaussian beam normally incident on a circular and central obscured aperture are derived with the help of the integration of parts method. With this expression, the far-field intensity distribution pattern can be obtained and the divergence angle is deduced too. Using the first five items of the series, the accuracy can satisfy most laser application fields. Compared with the conventional numerical integral method, the series representation is very convenient for understanding the physical meanings. (C) 2007 Elsevier GmbH. All rights reserved.

Spin wave resonance in ferromagnetic films

The objective of this investigation has been a theoretical and experimental understanding of ferromagnetic resonance phenomena in ferromagnetic thin films, and a consequent understanding of several important physical properties of these films. Significant results have been obtained by ferromagnetic resonance, hysteresis, torque magnetometer, He ion backscattering, and X-ray fluorescence measurements for nickel-iron alloy films.

Taking into account all relevant magnetic fields, including the applied, demagnetizing, effective anisotropy and exchange fields, the spin wave resonance condition applicable to the thin film geometry is presented. On the basis of the simple exchange interaction model it is concluded that the normal resonance modes of an ideal film are expected to be unpinned. The possibility of nonideality near the surface of a real film was considered by means of surface anisotropy field, inhomogeneity in demagnetizing field and inhomogeneity of magnetization models. Numerical results obtained for reasonable parameters in all cases show that they negligibly perturb the resonance fields and the higher order mode shapes from those of the unpinned modes of ideal films for thicknesses greater than 1000 Å. On the other hand for films thinner than 1000 Å the resonance field deviations can be significant even though the modes are very nearly unpinned. A previously unnoticed but important feature of all three models is that the interpretation of the first resonance mode as the uniform mode of an ideal film allows an accurate measurement of the average effective demagnetizing field over the film volume. Furthermore, it is demonstrated that it is possible to choose parameters which give indistinguishable predictions for all three models, making it difficult to uniquely ascertain the source of spin pinning in real films from resonance measurements alone.

Spin wave resonance measurements of 81% Ni-19% Fe coevaporated films 30 to 9000 Å thick, at frequencies from 1 to 8 GHz, at room temperature, and with the static magnetic field parallel and perpendicular to the film plane have been performed. A self-consistent analysis of the results for films thicker than 1000 Å, in which multiple excitations can be observed, shows for the first time that a unique value of exchange constant A can only be obtained by the use of unpinned mode assignments. This evidence and the resonance behavior of films thinner than 1000 Å strongly imply that the magnetization at the surfaces of permalloy films is very weakly pinned. However, resonance measurements alone cannot determine whether this pinning is due to a surface anisotropy, an inhomogeneous demagnetizing field or an inhomogeneous magnetization. The above analysis yields a value of 4πM=10,100 Oe and A = (1.03 ± .05) x 10^-6 erg/cm for this alloy. The ability to obtain a unique value of A suggests that spin wave resonance can be used to accurately characterize the exchange interaction in a ferromagnet.

In an effort to resolve the ambiguity of the source of pinning of the magnetization, a correlation of the ratio of magnetic moment and X-ray film thickness with the value of effective demagnetizing field 4πNM as determined from resonance, for films 45 to 300 Å has been performed. The remarkable agreement of both quantities and a comparison with the predictions of five distinct models, strongly imply that the thickness dependence of both quantities is related to a thickness dependent average saturation magnetization, which is far below 10,100 Oe for very thin films. However, a series of complementary experiments shows that this large decrease of average saturation magnetization cannot be simply explained by either oxidation or interdiffusion processes. It can only be satisfactorily explained by an intrinsic decrease of the average saturation magnetization for very thin films, an effect which cannot be justified by any simple physical considerations.

Recognizing that this decrease of average saturation magnetization could be due to an oxidation process, a correlation of resonance measurements, He ion backscattering, X-ray fluorescence and torque magnetometer measurements, for films 40 to 3500 Å thick has been performed. On basis of these measurements it is unambiguously established that the oxide layer on the surface of purposefully oxidized 81% Ni-19% Fe evaporated films is predominantly Fe-oxide, and that in the oxidation process Fe atoms are removed from the bulk of the film to depths of thousands of angstroms. Extrapolation of results for pure Fe films indicates that the oxide is most likely α-Fe₂O₃. These conclusions are in agreement with results from old metallurgical studies of high temperature oxidation of bulk Fe and Ni-Fe alloys. However, X-ray fluorescence results for films oxidized at room temperature, show that although the preferential oxidation of Fe also takes place in these films, the extent of this process is by far too small to explain the large variation of their average saturation magnetization with film thickness.

Interpretación litoestratigráfica y paleogeográfica del Jurásico marino del este Cantabria-oeste de Vizcaya en base a diagrafías de sondeo y su correlación con series tipo

Este trabajo se centra en el estudio del Jurásico marino (Lías y Dogger) de un área de la parte central de La Cuenca Vasco-Cantábrica situada en el este de Cantabria y oeste de Vizcaya donde sus afloramientos son muy escasos pero se dispone de datos de sondeos de exploración petrolífera (Fig 1A y B), poniendo especial interés en la localización y distribución lateral de los niveles de rocas madre de hidrocarburos (black shales) y de potenciales almacenes (unidades carbonatadas fracturadas o dolomitizadas). La sucesión del Jurásico de la Cuenca Vasco-Cantábrica (CVC) está formada por dos unidades diferenciadas por edad y ambiente sedimentario. Por una parte tenemos los materiales del “Jurásico marino” (Robles et al., 1989) que representan la mayor parte de la sucesión (Lías y Dogger) y por otro lado, tenemos los materiales del “Jurásico continental” pertenecientes exclusivamente al Tithoniense Superior y que se engloban en las facies Purbeck que abarcan hasta el Berriasiense (Rat 1962).

La vegetación de la Comunidad Autónoma del País Vasco. Leyenda del mapa de series de vegetación a escala 1:50.000

Índice: 1. Marco geográfico. El medio físico: - Situación, extensión y límites. - Estructura, morfología y relieve. - Rasgos generales de los Pirineos. - Los Montes Vasco-Cantábricos. - La depresión del Ebro. 2. Los cambios de la vegetación en el tiempo: paleogeobotánica o geobotánica histórica: - Introducción. Las glaciaciones del Cuaternario. - La vegetación de Europa en el Terciario. - El tránsito Plioceno-Pleistoceno y el Pleistoceno antiguo. - El Pleistoceno medio y reciente. - El Tardiglaciar y el Holoceno. - La expansión de Fagus sylvatica en el Holoceno. - La Península Ibérica. 3. El clima actual del la Comunidad Autónoma del País Vasco y regiones limítrofes: - El régimen climático general del territorio noribérico. - La ubicación geográfica. - Centros de acción. - El contexto geográfico. - La clasificación bioclimática. - El paisaje vegetal a través de las unidades bioclimáticas: macroclimas, bioclimas y pisos bioclimáticos. - El macroclima Templado. - El macroclima Mediterráneo. 4. Biogeografía: - Biogeografía: definición y concepto. - Corionomía. - Biogeografía del norte-centro de la Península Ibérica. - Descripción y caracterización de las principales unidades biogeográficas. 5. Flora de la CAPV y territorios limítrofes: - La flora eurosiberiana. - La flora mediterránea. - La flora endémica. 6. Series, Geoseries y Geopermaseries de Vegetación de la Comunidad Autónoma del País Vasco: - Los cambios de la vegetación en escala temporal reducida: dinamismo y sucesión. Concepto de Serie, Geoserie y Geopermaserie de Vegetación - Series climatófilas y temporihigrófilas. - Geoseries fluviales. - Halogeopermaseries (Geopermaseries costeras): los sistemas costeros. - Saxigeopermaseries (Geopermaseries rupícolas): crestas, acantilados y gleras. - Higrogeopermaseries (Geopermaseries higrófilas): turberas, charcas y lagunas.