107 research outputs found

    Here and Now : An Evaluation of Barnardo's Trauma, Bereavement and Loss Service in Schools

    Get PDF
    In the United Kingdom it is estimated that 92% of young people will experience a bereavement of a 'close' relationship that includes family, friends and pets, before the age of 16 (Harrison & Harrington, 2001). In Scotland, a more recent survey found that 79% of secondary school pupils, aged 12 to 17 years, have experienced the death of someone important to them (Del Carpio, Rasmussen, & Paul, 2018).Bereavement during childhood is therefore a majority experience, yet whilst it may be a universal part of growing up, experiencing a death can also be a major life event that places a young person at increased risk of a range of negative outcomes. For example, it is suggested that bereaved young people are at greater risk of developing depressive symptoms (Harrison & Harrington, 2001), being abused (Cross, 2002) and teenage pregnancy (Sweeting, West, & Richards, 1998). Vulnerable populations of young people, such as those involved in offending, are also more likely than the general population to have experienced multiple, parental or traumatic bereavements (Finlay & Jones, 2000; Vaswani, 2008; Vaswani, 2014)

    Here and Now : An Evaluation of Barnardo's Trauma, Bereavement and Loss Service in Schools

    Get PDF
    In the United Kingdom it is estimated that 92% of young people will experience a bereavement of a 'close' relationship that includes family, friends and pets, before the age of 16 (Harrison & Harrington, 2001). In Scotland, a more recent survey found that 79% of secondary school pupils, aged 12 to 17 years, have experienced the death of someone important to them (Del Carpio, Rasmussen, & Paul, 2018).Bereavement during childhood is therefore a majority experience, yet whilst it may be a universal part of growing up, experiencing a death can also be a major life event that places a young person at increased risk of a range of negative outcomes. For example, it is suggested that bereaved young people are at greater risk of developing depressive symptoms (Harrison & Harrington, 2001), being abused (Cross, 2002) and teenage pregnancy (Sweeting, West, & Richards, 1998). Vulnerable populations of young people, such as those involved in offending, are also more likely than the general population to have experienced multiple, parental or traumatic bereavements (Finlay & Jones, 2000; Vaswani, 2008; Vaswani, 2014)

    Benchmarking the power of amateur observatories for TTV exoplanets detection

    Get PDF
    This document is the Accepted Manuscript version of the following article: Roman v. Baluev, et al, ‘Benchmarking the power of amateur observatories for TTV exoplanets detection’, Monthly Notices of the Royal Astronomical Society, Vol. 450(3): 3101-3113, first published online 9 May 2015. The version of record is available at doi: https://doi.org/10.1093/mnras/stv788 © 2015 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society.We perform an analysis of ~80000 photometric measurements for the following 10 stars hosting transiting planets: WASP-2, -4, -5, -52, Kelt-1, CoRoT-2, XO-2, TrES-1, HD 189733, GJ 436. Our analysis includes mainly transit lightcurves from the Exoplanet Transit Database, public photometry from the literature, and some proprietary photometry privately supplied by other authors. Half of these lightcurves were obtained by amateurs. From this photometry we derive 306 transit timing measurements, as well as improved planetary transit parameters. Additionally, for 6 of these 10 stars we present a set of radial velocity measurements obtained from the spectra stored in the HARPS, HARPS-N, and SOPHIE archives using the HARPS-TERRA pipeline. Our analysis of these TTV and RV data did not reveal significant hints of additional orbiting bodies in almost all of the cases. In the WASP-4 case, we found hints of marginally significant TTV signals having amplitude 10-20 sec, although their parameters are model-dependent and uncertain, while radial velocities did not reveal statistically significant Doppler signals.Peer reviewe

    Trauma, Bereavement and Loss : Key Learning and Messages from Research and Practice

    Get PDF
    Professionals, and wider society, are becoming increasingly aware of the prevalence of traumatic and adverse childhood experiences, and of the potentially enduring and detrimental impact of such experiences on emotional, psychological and physical health and wellbeing. As a result, there is increased policy and practice attention paid to identifying, understanding and addressing trauma and adversity among individuals. Importantly, this attention is not solely focused on trauma-specialist provision for individuals who are known to have experienced trauma, but also on ensuring that the entire workforce is trauma-informed, as outlined in the Transforming Psychological Trauma framework (NHS Education for Scotland, 2017)

    Refined stellar, orbital and planetary parameters of the eccentric HAT-P-2 planetary system

    Get PDF
    We present refined parameters for the extrasolar planetary system HAT-P-2 (also known as HD 147506), based on new radial velocity and photometric data. HAT-P-2b is a transiting extrasolar planet that exhibits an eccentric orbit. We present a detailed analysis of the planetary and stellar parameters, yielding consistent results for the mass and radius of the star, better constraints on the orbital eccentricity, and refined planetary parameters. The improved parameters for the host star are M_star = 1.36 +/- 0.04 M_sun and R_star = 1.64 +/- 0.08 R_sun, while the planet has a mass of M_p = 9.09 +/- 0.24 M_Jup and radius of R_p = 1.16 +/- 0.08 R_Jup. The refined transit epoch and period for the planet are E = 2,454,387.49375 +/- 0.00074 (BJD) and P = 5.6334729 +/- 0.0000061 (days), and the orbital eccentricity and argument of periastron are e = 0.5171 +/- 0.0033 and omega = 185.22 +/- 0.95 degrees. These orbital elements allow us to predict the timings of secondary eclipses with a reasonable accuracy of ~15 minutes. We also discuss the effects of this significant eccentricity including the characterization of the asymmetry in the transit light curve. Simple formulae are presented for the above, and these, in turn, can be used to constrain the orbital eccentricity using purely photometric data. These will be particularly useful for very high precision, space-borne observations of transiting planets.Comment: Revised version, accepted for publication in MNRAS, 11 pages, 6 figure

    A chemical survey of exoplanets with ARIEL

    Get PDF
    Thousands of exoplanets have now been discovered with a huge range of masses, sizes and orbits: from rocky Earth-like planets to large gas giants grazing the surface of their host star. However, the essential nature of these exoplanets remains largely mysterious: there is no known, discernible pattern linking the presence, size, or orbital parameters of a planet to the nature of its parent star. We have little idea whether the chemistry of a planet is linked to its formation environment, or whether the type of host star drives the physics and chemistry of the planet’s birth, and evolution. ARIEL was conceived to observe a large number (~1000) of transiting planets for statistical understanding, including gas giants, Neptunes, super-Earths and Earth-size planets around a range of host star types using transit spectroscopy in the 1.25–7.8 μm spectral range and multiple narrow-band photometry in the optical. ARIEL will focus on warm and hot planets to take advantage of their well-mixed atmospheres which should show minimal condensation and sequestration of high-Z materials compared to their colder Solar System siblings. Said warm and hot atmospheres are expected to be more representative of the planetary bulk composition. Observations of these warm/hot exoplanets, and in particular of their elemental composition (especially C, O, N, S, Si), will allow the understanding of the early stages of planetary and atmospheric formation during the nebular phase and the following few million years. ARIEL will thus provide a representative picture of the chemical nature of the exoplanets and relate this directly to the type and chemical environment of the host star. ARIEL is designed as a dedicated survey mission for combined-light spectroscopy, capable of observing a large and well-defined planet sample within its 4-year mission lifetime. Transit, eclipse and phase-curve spectroscopy methods, whereby the signal from the star and planet are differentiated using knowledge of the planetary ephemerides, allow us to measure atmospheric signals from the planet at levels of 10–100 part per million (ppm) relative to the star and, given the bright nature of targets, also allows more sophisticated techniques, such as eclipse mapping, to give a deeper insight into the nature of the atmosphere. These types of observations require a stable payload and satellite platform with broad, instantaneous wavelength coverage to detect many molecular species, probe the thermal structure, identify clouds and monitor the stellar activity. The wavelength range proposed covers all the expected major atmospheric gases from e.g. H2O, CO2, CH4 NH3, HCN, H2S through to the more exotic metallic compounds, such as TiO, VO, and condensed species. Simulations of ARIEL performance in conducting exoplanet surveys have been performed – using conservative estimates of mission performance and a full model of all significant noise sources in the measurement – using a list of potential ARIEL targets that incorporates the latest available exoplanet statistics. The conclusion at the end of the Phase A study, is that ARIEL – in line with the stated mission objectives – will be able to observe about 1000 exoplanets depending on the details of the adopted survey strategy, thus confirming the feasibility of the main science objectives.Peer reviewedFinal Published versio

    KPS-1b: The First Transiting Exoplanet Discovered Using an Amateur Astronomer's Wide-field CCD Data

    Get PDF
    We report the discovery of the transiting hot Jupiter KPS-1b. This exoplanet orbits a V = 13.0 K1-type main sequence star every 1.7 days, has a mass of 1.090 (+0.086 -0.087) MJup and a radius of 1.03 (+0.13 -0.12) RJup. The discovery was made by the prototype Kourovka Planet Search (KPS) project, which used wide-field CCD data gathered by an amateur astronomer using readily available and relatively affordable equipment. Here we describe the equipment and observing technique used for the discovery of KPS-1b, its characterization with spectroscopic observations by the SOPHIE spectrograph and with high-precision photometry obtained with 1m class telescopes. We also outline the KPS project evolution into the Galactic Plane eXoplanet survey. The discovery of KPS-1b represents a new major step of the contribution of amateur astronomers to the burgeoning field of exoplanetology

    Two transiting hot Jupiters from the WASP survey : WASP-150b and WASP-176b

    Get PDF
    Funding: The research leading to these results has received funding from the European Research Council under the FP/2007-2013 ERC grant Agreement No. 336480 and from the ARC grant for Concerted Research Actions financed by the Wallonia-Brussels Federation. A.C.C. acknowledges support from the UK Science and Technology Facilities Council (STFC)consolidated grant No. ST/R000824/1.We report the discovery of two transiting exoplanets from the WASP survey, WASP-150b and WASP-176b. WASP-150b is an eccentric (e = 0.38) hot Jupiter on a 5.6 day orbit around a V = 12.03, F8 main-sequence host. The host star has a mass and radius of 1.4 M⊙ and 1.7 R⊙ respectively. WASP-150b has a mass and radius of 8.5 MJ and 1.1 RJ, leading to a large planetary bulk density of 6.4 ρJ. WASP-150b is found to be ~3 Gyr old, well below its circularization timescale, supporting the eccentric nature of the planet. WASP-176b is a hot Jupiter planet on a 3.9 day orbit around a V = 12.01, F9 sub-giant host. The host star has a mass and radius of 1.3 M⊙ and 1.9 R⊙. WASP-176b has a mass and radius of 0.86 MJ and 1.5 RJ, respectively, leading to a planetary bulk density of 0.23 ρJ.Publisher PDFPeer reviewe
    corecore