Heliophysics Events Knowledgebase Coverage Registry (HCR)
Observation Details
SOT: HOP 126 and 166 on AR 11108
2010-09-22T07:56:32 to 2010-09-22T09:02:56
Science Goal: Active Region Tracking
Program: HOP 126, 2010, H-alpha 3 blue wings, Na IVDG
Target: Active Region
xcen=-29 ycen=-592
Instrument: SOT
HOP/JOP: 0
Description: Request to SOT HOP Number 0126 Context programs: SP: fast map large enough to cover the AR, perhaps 123x123 or 164x164 arcsec, avoiding SAA NFI: Program 0x3b4 AR mode case2 (Large), G-band 120min, Na IV 5min, Ca H 5min, during the SP map High-cadence programs: NFI: Program 03bd H-alpha sequence: H-alpha at -2.1A, at -1.28A and -0.87A, 112"x112", 2x2 summed, at 13 s cadence, and Na D IVDG every 5 minutes, same FOV SP : Program 0xed fast raster (dynamics), 4.8"x60" at 1 min cadence The NFI high cadence program should run for the prime observing time in La Palma, 2-3 hours depending on telemetry. The SP high cadence should run for 30 minutes in the middle of this period (avoiding SAA). The context programs should run once before the high cadence observing begins and again once after it ends. The CT should cycle off/on before the start of each of the SP programs. Other Instruments: SST: Ca-H, Ca 8542, H alpha TRACE: TRACE 1600 every half hour, TRACE 195 every minute (if operating, for context and coalignment) Scientific Objectives: The goal is to investigate the physics of the disk counterparts of type II spicules through coordinated observations with Hinode and SST (and TRACE, if available). Using Ca 8542 and H-alpha spectra from CRISP, we have recently identified high velocity jets that are similar to type II spicules observed in Ca H with Hinode at the limb. We want to determine the formation mechanism and thermodynamic (heating) and dynamic (Doppler and projected velocity) properties of these chromospheric jets. We also want to get statistics on transversal motions. We will try to achieve these goals through simultaneous, very high resolution, high cadence observations from the Swedish Solar Telescope (SST) with a broadband Ca-H filter (core), as well as CRISP FPI observations in the Ca 8542 and H-alpha lines. In addition, we would like to ask for H-alpha blue wing images at high cadence and Na D magnetograms and Dopplergrams from Hinode SOT (to study the effect of magnetic fields on the formation mechanism), and a fast raster in various lines with EIS (to study the thermal evolution). For targeting, we will focus on AR plage, quiet Sun and equatorial coronal holes. Best chances of good seeing are UT 8:30-11:30. Request to SOT HOP Number 0166 ?E Spectro-Polarimeter: High resolution vector magnetic field measurements in Fe i 630 nm, single-side fast maps 100 x 123?h, Q=75, two maps each day. Data requirement = 276 Mbits/day. ?E NFI: Na IVDG Longitudinal magnetogram/Dopplergram sequences, FOV=164x164?h, 2kx2k, sum=2x2, cadence = 10 minutes, Q1=65, Q2=75. Data requirement = 165 Mbits/day ?E NFI: H line center intensity and Doppler imaging sequences, FOV=164x164?h, 2kx2k, sum=2x2, cadence = 10 minutes, Q1=65, Q2=75. Data requirement = 165 Mbits/day ?E BFI: Ca ii H-line and G-band images, FOV=111x111?h, 2kx2k, sum 2x2, cadence=10 min, Q=65. Data requirement = 144 Mbits/day The low cadence of these observations will not use a large fraction of the typical Hinode/SOT allocation
there should be ample telemetry remaining for other programs during the proposed coordinated observing period. Other Instruments: Teide Observatory VTT: ?E Spectro-polarimetry in the chromospheric He i and upper photospheric Si i lines near 1083 nm with the Tenerife Infrared Polarimeter (TIP) ?E Spectro-polarimetry in Fe i 630 nm and Ca ii H-line spectroscopy with POLIS If appropriate, we will also employ vector magnetic field measurements from the HMI instrument on the Solar Dynamics Observatory. We will employ several techniques to carry out the analysis of the He i spectro-polarimetry. The computer codes HAZEL (IAC) and the HAO code developed by Casini to fit the observed profiles affected by both Hanle and Zeeman effects. Scientific Objectives: The twist of magnetic field lines, or magnetic helicity, is a physical property of the field that plays a crucial role in many aspects of solar activity, including the stability of magnetic flux against disruption as it rises buoyantly through the solar convection zone, the basis for supporting and thermally isolating the dense, cool material of filaments/prominences within the hot and tenuous corona, and the initiation of coronal mass ejections (CMEs). Prominences/filaments are intimately linked to the CME process, so understanding their magnetic field structure and how helical magnetic flux arises is a key issue for solar physics. Few reliable measurements exist for magnetic fields in filaments, yet such measurements are essential to understand the structure and evolution of the filaments and the related magnetic structures such as filament channels and the overlying coronal cavity. In recent times significant progress has been made toward understanding the structure of the field in the photosphere below active region filaments (Lites 2005, Okamoto et al. 2008, 2009, Lites et al. 2010), largely because of access to the consistently high angular resolution spectro-polarimetric measurements afforded by Hinode. However, the status of observations of the field within the filament structure itself is not nearly as well-defined. Most of the observations to date have employed the Hanle effect for prominences above the limb. Due to line-of-sight integration and lack of spatial resolution, these measurements have afforded only limited information regarding the field vector within the filament/prominences. This proposal aims to establish an observational picture of the magnetic field vector within and under active region filaments. Active region filaments are particularly interesting because the fields are strong enough, and the filament structures are generally low enough in the solar atmosphere, that traditional Zeeman effect measurements of the field in the photosphere consistently show signatures characteristic of the magnetic structure of the filament at that level. It is now appropriate to attempt similar measurements of the photosphere below filaments coupled with simultaneous measurements of the filament structure at chromospheric temperatures and densities. The latter measurements of filaments on the disk are made possible by significant advances within the past few years toward interpretation of polarization measurements in chromospheric lines sensitive to both the Hanle and Zeeman effects If such measurements can be obtained with good spatial resolution, and then coupled to the proven measurements of the vector field in the photosphere below the filament, we hope to develop a glimpse of the actual 3-dimensional structure of the entire filament magnetic field system. The proposed Hinode observations would be carried out during the 3-hour period 09 - 12UT. Hinode observations will follow closely the ?gstandard?h Case 1 mode of HOP 0139 similar to that run on 05 November 2009 (FG program 0x360, SP program 0xb2). The observations needed to carry out this study include:

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Chief Observer
Myers(RCO)
Related Links
Cites: HOP 126 and 166 on AR 11108     
Timeline: gif use
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wavelength: TF Na I 5896 cadence: 5.4 min fov: 81,81 images: 13 JavaScript Landing Page
wavelength: TF H I 6563 base cadence: 0.07 min fov: 81,81 images: 954 JavaScript Landing Page