LOFAR, the LOw-Frequency ARray, is a new-generation radio interferometer constructed in the north of the Netherlands and across europe. Utilizing a novel phased-array design, LOFAR covers the largely unexplored low-frequency range from 10-240 MHz and provides a number of unique observing capabilities. Spreading out from a core located near the village of Exloo in the northeast of the Netherlands, a total of 40 LOFAR stations are nearing completion. A further five stations have been deployed throughout Germany, and one station has been built in each of France, Sweden, and the UK. Digital beam-forming techniques make the LOFAR system agile and allow for rapid repointing of the telescope as well as the potential for multiple simultaneous observations. With its dense core array and long interferometric baselines, LOFAR achieves unparalleled sensitivity and angular resolution in the low-frequency radio regime. The LOFAR facilities are jointly operated by the International LOFAR Telescope (ILT) foundation, as an observatory open to the global astronomical community. LOFAR is one of the first radio observatories to feature automated processing pipelines to deliver fully calibrated science products to its user community. LOFAR's new capabilities, techniques and modus operandi make it an important pathfinder for the Square Kilometre Array (SKA). We give an overview of the LOFAR instrument, its major hardware and software components, and the core science objectives that have driven its design. In addition, we present a selection of new results from the commissioning phase of this new radio observatory.

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The low frequency array (LOFAR), is the first radio telescope designed with the capability to measure radio emission from cosmic-ray induced air showers in parallel with interferometric observations. In the first ∼2 years of observing, 405 cosmic-ray events in the energy range of 10 16 −10 18 eV have been detected in the band from 30−80 MHz. Each of these air showers is registered with up to ∼1000 independent antennas resulting in measurements of the radio emission with unprecedented detail. This article describes the dataset, as well as the analysis pipeline, and serves as a reference for future papers based on these data. All steps necessary to achieve a full reconstruction of the electric field at every antenna position are explained, including removal of radio frequency interference, correcting for the antenna response and identification of the pulsed signal.

Low frequency radio waves, while challenging to observe, are a rich source of information about pulsars. The LOw Frequency ARray (LOFAR) is a new radio interferometer operating in the lowest 4 octaves of the ionospheric "radio window": 10-240 MHz, that will greatly facilitate observing pulsars at low radio frequencies. Through the huge collecting area, long baselines, and flexible digital hardware, it is expected that LOFAR will revolutionize radio astronomy at the lowest frequencies visible from Earth. LOFAR is a next-generation radio telescope and a pathfinder to the Square Kilometre Array (SKA), in that it incorporates advanced multi-beaming techniques between thousands of individual elements. We discuss the motivation for low-frequency pulsar observations in general and the potential of LOFAR in addressing these science goals. We present LOFAR as it is designed to perform high-time-resolution observations of pulsars and other fast transients, and outline the various relevant observing modes and data reduction pipelines that are already or will soon be implemented to facilitate these observations. A number of results obtained from commissioning observations are presented to demonstrate the exciting potential of the telescope. This paper outlines the case for low frequency pulsar observations and is also intended to serve as a reference for upcoming pulsar/fast transient science papers with LOFAR.

A versatile crystal-growth simulation program, based on the Monte Carlo algorithm, is introduced. It enables the handling of any crystallographic orientation. The crystal is modeled by a set of molecular interactions, which are obtained from molecular mechanics calculations. The motherphase is parametrized by its bulk thermodynamic properties. As an example, the program was used to simulate the growth of various fat crystals. The results show the importance of the details of the crystal structure, its energetics, and the actual growth conditions upon the crystal morphology. The model intends to fill the gap which exists by the fact that supersaturation, temperature, concentration, and dissolution free energy are not taken into account by the established morphology prediction models.

Single crystals of pure CT0 are grown from the vapour phase and the structure and morphology of these crystals is studied. By means of X-ray diffractron and TEM measurements five drfferent phases are observed. The observed phases are (from high to low tem~ratures) fee, rhom~hed~i, ideal hcp (c/a = I .63), deformed hcp (c/a= 1.82) and a monoclinic phase. The occurrence of these different phases and the phase transmons IS accounted for in a simple model. For the monoclinic structure a model for the stackmg of the orientationaily ordered molecules in the lattice IS proposed. For both the hcp and fee phases a Lennard-Jones type mteraction potential is used to calculate bond strengths, lattxe energies and the theoretical morphology.

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The morphology of naphthalene and anthracene crystals has been studied both theoretically and experimentally. A connected net analysis shows that the faces {011} and {21 h1 h} contain a pair of symmetry-related connected nets giving rise to a new phenomenon called symmetry roughening. Experimentally the {011} and {21 h1 h} faces have only been observed on naphthalene crystals grown from the vapor at very low driving forces. Upon increasing the driving force, the {011} faces grow out very rapidly as flat faces at very low supersaturation. For anthracene these faces have never been observed. In this paper the relation between the connected net structure of crystal faces and the experimentally observed growth behavior is discussed.