Solar and heliosheric WG

Slides:



Advertisements
Similar presentations
The Science of Solar B Transient phenomena – this aim covers the wide ranges of explosive phenomena observed on the Sun – from small scale flaring in the.
Advertisements

On the link between the solar energetic particles and eruptive coronal phenomena On the link between the solar energetic particles and eruptive coronal.
The Physics of Solar Flares Examining Solar Flares and Radio Bursts By Caylin Mendelowitz and Claire Rosen.
Flare Luminosity and the Relation to the Solar Wind and the Current Solar Minimum Conditions Roderick Gray Research Advisor: Dr. Kelly Korreck.
The Focusing Optics X-ray Solar Imager (FOXSI) Steven Christe 1, S. Krucker 2, L. Glesener 2, S. Ishikawa 3, B. Ramsey 4, T. Takahashi 3, R.P. Lin 2 1.
Planets and Solar System Science at Low Frequencies Philippe Zarka LESIA, CNRS-Observatoire de Paris France Towards a European.
Plasmas in Space: From the Surface of the Sun to the Orbit of the Earth Steven R. Spangler, University of Iowa Division of Plasma Physics, American Physical.
M. J. Reiner, 1 st STEREO Workshop, March, 2002, Paris.
STEREO AND SPACE WEATHER Variable conditions in space that can have adverse effects on human life and society Space Weather: Variable conditions in space.
Solar Energetic Particle Production (SEPP) Mission Primary Contacts: Robert P. Lin (UC Berkeley), John L. Kohl (Harvard-Smithsonian CfA) Primary Science.
NASA Sun-Solar System Connection Roadmap 1 Targeted Outcome: Phase , Safeguarding our Outbound Journey Determine Extremes of the Variable Radiation.
From Geo- to Heliophysical Year: Results of CORONAS-F Space Mission International Conference «50 Years of International Geophysical Year and Electronic.
NASA Sun-Solar System Connection Roadmap 1 Targeted Outcome: Phase , Safeguarding our Outbound Journey Determine Extremes of the Variable Radiation.
Solar system science using X-Rays Magnetosheath dynamics Shock – shock interactions Auroral X-ray emissions Solar X-rays Comets Other planets Not discussed.
DOPPLER DOPPLER A Space Weather Doppler Imager Mission Concept Exploration Science Objectives What are the most relevant observational signatures of flare,
F1B: Determine the Dominant Processes of Particle Acceleration Phase , Open the Frontier UV Spectroscopic determin- ation of pre/post-shock density,
NASA Sun-Solar System Connection Roadmap 1 Targeted Outcome: Phase , Safeguarding our Outbound Journey Determine Extremes of the Variable Radiation.
4th LOFAR solar KSP meeting Potsdam4th LOFAR KSP meeting Potsdam 2010 November 8-9 4th LOFAR KSP meeting Potsdam 2010 November 8-9 NRH and LOFAR Scientific.
Solar Polar Orbit Radio Telescope (SPORT): A Mission Concept for Interplanetary CMEs Imaging WU Ji, LIU Hao, SUN Weiying, ZHENG Jianhua, FENG Xueshang,
Stuart D. BaleFIELDS iCDR – Science Requirements Solar Probe Plus FIELDS Instrument CDR Science and Instrument Overview Science Requirements Stuart D.
1 Future solar missions (Based on the summary by R.A. Harrison) S. Kamio
The Sun and the Heliosphere: some basic concepts…
Radio Remote Sensing of the Corona and the Solar Wind Steven R. Spangler University of Iowa.
Solar observation modes: Commissioning and operational C. Vocks and G. Mann 1. Spectrometer and imaging modes 2. Commissioning proposals 3. Operational.
Solar System Missions Division Solar Orbiter Next major Solar and Heliospheric mission ESA ILWS flagship Now with the Inner Heliospheric Sentinels.
Probing Energy Release of Solar Flares M. Prijatelj Carnegie Mellon University Advisors: B. Chen, P. Jibben (SAO)
Array Configuration Divya Oberoi MIT Haystack Observatory.
IHY Workshop A PERSONAL VIEW OF SOLAR DRIVERS for Solar Wind Coronal Mass Ejections Solar Energetic Particles Solar Flares.
Stuart D. BaleFIELDS iPDR – Science Requirements Solar Probe Plus FIELDS Instrument PDR Science and Instrument Overview Science Requirements Stuart D.
Coronal hard X-ray sources and associated decimetric/metric radio emissions N. Vilmer D. Koutroumpa (Observatoire de Paris- LESIA) S.R Kane G. Hurford.
195 Å image – behind 195 Å image – Sun- Earth line – SOHO/ EIT image 195 Å image – Sun- Earth line – SOHO/ EIT image 195 Å image – ahead SECCHI Extreme.
Solar Wind and Coronal Mass Ejections
STEREO Planned Launch November, Stereo imaging of Sun; coronal mass ejections from birth to Earth impact. What determines geo-effectiveness of solar.
STEREO: Beyond 3D. Why the Sun? The sun provides energy for the development of life on our planet. Our orbit looks calm and peaceful, but there is nothing.
Why Solar Electron Beams Stop Producing Type III Radio Emission Hamish Reid, Eduard Kontar SUPA School of Physics and Astronomy University of Glasgow,
Murchison Widefield Array (MWA) : Design and Status Divya Oberoi, Lenoid Benkevitch MIT Haystack Observatory doberoi, On behalf.
Heliophysics Research Focus Areas for a new Heliophysics Roadmap A summary of suggested updates to the current RFA, and some possible outcomes.
3 rd RSIH&SWA Workshop – Morelia, Mexico – 21 October 2015 Radio Heliophysics with the Square Kilometre Array (SKA) M.M. Bisi (1),
Topics in Space Weather Earth Atmosphere & Ionosphere
Space Research Institute Russian magnetospheric & heliospheric missions.
SOLAR RADIO PHYSICS RESEARCH IN INDONESIA
Probing Electron Acceleration with X-ray Lightcurves Siming Liu University of Glasgow 9 th RHESSI Workshop, Genova, Italy, Sep
Dec 1, FIELDS Top Level Requirements Review S. Harris (UCB)
Solar Astronomy Space Science Lab 2008 Pisgah Astronomical Research Institute.
Stuart D. BaleFIELDS SOC CDR – Science Requirements Solar Probe Plus FIELDS SOC CDR Science and Instrument Overview Science Requirements Stuart D. Bale.
Solar observations with single LOFAR stations C. Vocks 1. Introduction: Solar Radio radiation 2. Observations with single LOFAR stations 3. Spectrometer.
한 미 려 – Introduction (1) 2.Instrument & Observe 3.Science 2.
Our Sun. About the Sun The sun is by far the largest object in the solar system, containing more than 99.8% of the total mass of the solar system (Jupiter.
Joe Khan Lyndsay Fletcher, Eduard Kontar, Alec MacKinnon, Graham Woan Solar Physics and Space Weather Science with LOFAR: The UK Perspective.
An Introduction to Observing Coronal Mass Ejections
Chengming Tan National Astronomical Observatories
Physics of Solar Flares
Solar Probe Plus Scheduled to be launched in 2018 Solar Probe Plus will come closer to the Sun than any spacecraft has ever flown - and what it finds could.
Scientists Propose Mechanism to Describe Solar Eruptions of All Sizes
SWAVES-like radio instrument?
ARTEMIS – solar wind/ shocks
L4+L5 Mission as an Ideal Project for International Collaboration
Introduction to Space Weather Interplanetary Transients
Upcoming Facilities of IIA
NASA NASA's Parker Solar Probe mission set off to explore the Sun's atmosphere on Sunday morning August 12, It will swoop to within 4 million miles.
Corona Mass Ejection (CME) Solar Energetic Particle Events
Solar and Heliospheric Physics
Investigation of Heliospheric Faraday Rotation Due to a Coronal Mass Ejection (CME) Using the LOw Frequency ARray (LOFAR) and Space-Based Imaging Techniques.
Series of high-frequency slowly drifting structure mapping the magnetic field reconnection M. Karlicky, A&A, 2004, 417,325.
Introduction to Space Weather
Introduction to Space Weather
Grades 9-12: Introduction
Transition Region and Coronal Explorer (TRACE)
Slit and Slot Interchange
Richard B. Horne British Antarctic Survey Cambridge UK
Presentation transcript:

SOLAR & HELIOSPHERIC PHYSICS COST CONTROL Eduard Kontar, Divya Oberoi On behalf of the solar & heliospheric physics SWG

Solar and heliosheric WG “Solar & Heliospheric physics” Working Group http://astronomers.skatelescope.org/science-working-groups/solar-heliospheric-physics/ Over 60 members solar radio astronomers from 4 continents and 20 countries (e.g. UK, Belgium, France, USA, India, China, France, Australia, Greece, Portugal, Kenya, Ireland, Brazil,…) Broad science interests include: the Sun (both active and quiet Sun), magnetic reconnection, solar corona/solar wind, solar flares, coronal mass ejections, Sun-Earth system, and ionosphere

Solar and heliosheric WG This report is based on: Responses from the Solar-Heliosphere WG members Face-to-face discussions with a few colleagues

Motivations Solar radio emission as a diagnostic to study fundamental processes in solar atmosphere (e.g. conversion of magnetic energy into particle energy, turbulence, particle acceleration, physics of shocks) Sun-Earth connection and ‘space weather’

Basic solar requirements Sun is highly variable, non-uniform source (1/2 degree); radio sources could be both small (~10 arcsec ) and large (~1 degree) => large dynamic range => snap-shot imaging required Flux variations ms time scales are known => high cadence observations => snapshot imaging or multi-beaming Solar radio spectrum is complex with narrowband features of 1-0.01 % often observed /frequency synthesis often not suitable/ => modest frequency resolution required

Solar radio emission is complex A typical dynamic spectrum of an active Sun Benz, 2004

Large instantaneous band Time DecametricType III bursts Frequency, MHz Interplanetary type III bursts Acceleration site Hard X-rays upward beams Earth's orbit 10MHz 20-30kHz 240MHz Sun 0.15R 1.5R Sun Sun 1AU Plasma frequency radio range <= plasma frequency

Important considerations from a solar science perspective for SKA1-Low and SKA1-Mid: Large instantaneous bandwidth is the key enabler of new science. (Some of the key science targets are to study the plasma emission related to energetic events ranging from largest flares to smallest magnetic reconnection events. These comparatively narrow-band coherent emissions arise at the local plasma frequency and its harmonic, and hence the frequency of observation carries direct information about the local plasma density in the region of emission.) SKA1-low band of 50-350 MHz is only an incremental improvement over the80-300 MHz already available from the MWA and 30 -240 MHz LOFAR

Heliophysics science with SKA1-Low: Observation of Galactic synchrotron background and the discreet sources to diagnose plasma in the heliopshere. A key science objective of this science is to measure the 3D magnetic field of coronal mass ejections (CMEs) while they are still in interplanetary space. This requires the use of RM synthesis technique, which in turn, benefits from having simultaneous access large bandwidth or at least the ability to spread the observing bandwidth over a large spectral span.

Solar Probe Plus, Solar Orbiter and SKA NASA Solar Probe Plus is in the definition stage and is scheduled to launch in 2018: Science objectives: 1) Coronal heating and solar wind acceleration 2) Production, evolution and transport of solar energetic particles First close approach in December, 2024 9 R_sun SKA observations will be complemented with new in-situ and remote observation of the Sun in the inner heliosphere ESA Solar Orbiter to be launched in 2018 (approach the Sun ~0.3AU )

General comments: Possible cost savings with minimum science impact: - Reducing the number elements in the array for Mid and Low, especially in the core where all the infra-structure is already deployed. -Savings not only from the reduced cost of construction and installation, but also the attendant reduction in the data transport, correlation process. -have all the feeds on all the SKA-Mid antennas, but populate a sufficiently dense sub-array at each of the frequencies to start getting reasonable experience with the hardware and instrument performance, and do some interesting science. Perhaps some thought should be paid explore the savings it brings about.

Summary Reduction of science for reduced instantaneous bandwidth. SKA-Low 350-50 MHz covers essential range of solar heights complementarity with the major space missions observation (Solar Orbiter and Solar Probe Plus ) Prefer changes which do not lead a lasting impact and are easy to 'undo' once more resources can be made available.