Abstract: A method for assessing risk to a marine hydrocarbon recovery operation involves collecting a set of training images and labeling sea surface anomalies on the set of training images. The set of training images and associated labels are used to train a model via backpropagation. A set of non-training images is collected and the trained model is applied to identify a potentially disruptive sea surface anomaly on the set of non-training images. Any risk to the marine hydrocarbon recovery operation by the potentially disruptive sea surface anomaly is then assessed.

Abstract: A backpropagation-enabled method for identifying a sea surface anomaly involves collecting an initial set of images and labeling the anomaly on the initial set of images. The initial set of images are selected from satellite-acquired images and/or simulated satellite images. The labels are used to train a model via backpropagation. A subsequent set of images, including satellite-acquired, airborne-acquired images, and combinations thereof, is collected and the trained model is applied to identify a sea surface anomaly on the subsequent set of images.

Abstract: A magnetic system for uniformly scanning an ion beam across a semiconductor wafer comprises a magnetic scanner having ac and dc coil windings each of which extend linearly along internal pole faces of a magnetic core. The ac and dc coil windings are mutually orthogonal; a time dependent magnetic component causes ion beam scanning while a substantially static (dc) field component allows the ion beam to be bent in an orthogonal plane. The current density in the ac and dc coil windings is uniformly dispersed along the pole faces leading to an improved beam spot uniformity at the wafer. The magnetic system also includes a collimator having first and second mutually opposed symmetrical dipoles defining an aperture between them. The poles of each dipole have a pole face varying monotonically and polynomially in a direction perpendicular to a central axis of the collimator: an increasing pole gap is formed towards that central axis.

Abstract: A magnetic system for uniformly scanning an ion beam across a semiconductor wafer comprises a magnetic scanner having ac and dc coil windings each of which extend linearly along internal pole faces of a magnetic core. The ac and dc coil windings are mutually orthogonal; a time dependent magnetic component causes ion beam scanning whilst a substantially static (dc) field component allows the ion beam to be bent in an orthogonal plane. The current density in the ac and dc coil windings is uniformly dispersed along the pole faces leading to an improved beam spot uniformity at the wafer. The magnetic system also includes a collimator having first and second mutually opposed symmetrical dipoles defining an aperture between them. The poles of each dipole have a pole face varying monotonically and polynomially in a direction perpendicular to a central axis of the collimator: an increasing pole gap is formed towards that central axis.

Abstract: An ion beam bending magnet provides a curved path through the magnet for bending a ribbon-shaped ion beam having its major cross-sectional dimension normal to the bending plane of the magnet. The magnet comprises a ferromagnetic yoke surrounding the beam path and having an internal profile in cross-section formed of four angled sides. These sides are angled to the major dimension of the ribbon beam passing through the magnet, so that the internal profile of the yoke is relatively wide in the center of the ribbon beam and relatively narrow near the top and bottom edges of the ribbon beam. Electrical conductors against the internal surfaces of the yoke provide a uniform distribution of electrical current per unit length along the angled sides of the profile, providing a substantially uniform magnetic bending field within the magnet yoke.

Abstract: An ion beam bending magnet provides a curved path through the magnet for bending a ribbon-shaped ion beam having its major cross-sectional dimension normal to the bending plane of the magnet. The magnet comprises a ferromagnetic yoke surrounding the beam path and having an internal profile in cross-section formed of four angled sides. These sides are angled to the major dimension of the ribbon beam passing through the magnet, so that the internal profile of the yoke is relatively wide in the center of the ribbon beam and relatively narrow near the top and bottom edges of the ribbon beam. Electrical conductors against the internal surfaces of the yoke provide a uniform distribution of electrical current per unit length along the angled sides of the profile, providing a substantially uniform magnetic bending field within the magnet yoke.