SPD – June 2006 Solar Polar Flux – 1996-2006 - MDI The Sun’s Polar Magnetic Flux 1996-2006 Observed with SOHO/MDI J. Todd Hoeksema E.E. Benevolenskaya,

Slides:



Advertisements
Similar presentations
1 GONG Magnetogram pipeline. 2 The GONG Data Processing Pipeline
Advertisements

The Solar Polar Field Reversal Observed By SOHO/MDI Yang Liu, J. Todd Hoeksema, X-P Zhao – Stanford University
Back Reaction on the Photospheric Magnetic field in Solar Eruptions Dandan Ye.
3/2/2005MUG Meeting, Tucson1 Status of GONG+ Magnetograms How GONG makes magnetograms Performance Problems Solutions Schedule Data availability Pilot Projects.
Farside Helioseismic Holography: Recent Advances I. González Hernández (1), D. Braun (2), S. M. Hanasoge(3), F. Hill (1), C. Lindsey (2), P. Scherrer (3)
East-West Asymmetry of the Yohkoh Soft X-ray Corona L.W. Acton 1, D.E. McKenzie 1, A. Takeda 1, B.T. Welsch 2,and H.S. Hudson 2,3 1 Montana State University,
AGU – Fall 2006 The Solar Polar Field – Cycles 21 – 23 The Solar Polar Field During Solar Cycles J. Todd Hoeksema, Yang Liu, XuePu Zhao & Elena Benevolenskaya.
High-latitude activity and its relationship to the mid-latitude solar activity. Elena E. Benevolenskaya & J. Todd Hoeksema Stanford University Abstract.
A particularly obvious example of daily changing background noise level Constructing the BEST High-Resolution Synoptic Maps from MDI J.T. Hoeksema, Y.
HMI – Synoptic Data Sets HMI Team Meeting Jan. 26, 2005 Stanford, CA.
Solar Polar Field Observed by SOHO/MDI and Hinode Yang Liu Stanford University 10/01/ Hinode Workshop.
September 2006 CISM All Hand Meeting Progress in the Past Year and Plan for Next Year Yang Liu and the Solar Group in Stanford University
Identifying and Modeling Coronal Holes Observed by SDO/AIA, STEREO /A and B Using HMI Synchronic Frames X. P. Zhao, J. T. Hoeksema, Y. Liu, P. H. Scherrer.
1 Synoptic Maps of Magnetic Field from MDI Magnetograms: polar field interpolation. Y. Liu, J. T. Hoeksema, X. P. Zhao, R. M. Larson – Stanford University.
Relationship between the High and mid latitude Solar Magnetic Field Elena E. Benevolenskaya J. Todd Hoeksema Stanford University.
The May 1,1998 and May 12, 1997 MURI events George H. Fisher UC Berkeley.
Active Region Flux Dispersal (SH13A-1518) B.T. Welsch & Y.Li Space Sciences Lab, UC-Berkeley The ultimate fate of the magnetic flux introduced into the.
Accurate Polar and small scale observations during the solar cycle Elena E. Benevolenskaya Yang Liu J. Todd Hoeksema Stanford University HMI/AIA meeting,
1 July 31, 2007 SHINE 2007 – Heliospheric Plasma Sheet The Unusual Heliospheric Current Sheet at the End of Cycle 23 A Comparison of Cycles 21,22,& 23.
1 A Statistical Study about Transequatorial loops Jie Chen National Astronomical Observatories Chinese Academy of Sciences.
HMI MDI Comparison Y. Liu. CR 2104 CR 2109 MDI = 1.2 * HMI 720s / 45s.
Study of magnetic helicity in solar active regions: For a better understanding of solar flares Sung-Hong Park Center for Solar-Terrestrial Research New.
Absence of a Long Lasting Southward Displacement of the HCS Near the Minimum Preceding Solar Cycle 24 X. P. Zhao, J. T. Hoeksema and P. H. Scherrer Stanford.
Helioseismic Holography & some experiments on “field effects” in CR1988 NorthWest Research Associates Colorado Research Associates Division D. Braun.
A particularly obvious example of daily changing background noise level Constructing the BEST High-Resolution Synoptic Maps from MDI J.T. Hoeksema, Y.
Polar Network Index as a magnetic proxy for the solar cycle studies Priyal, Muthu, Karak, Bidya Binay, Munoz-Jaramillo, Andres, Ravindra, B., Choudhuri,
MDI Level 1.8 Magnetograms Yang Liu Stanford University 6/23/ SHINE 2008.
1 Synoptic Maps of Magnetic Field from MDI/WSO Magnetograms Y. Liu, J. T. Hoeksema, X. P. Zhao, R. M. Larson – Stanford University
This work utilizes data obtained by the Global Oscillation Network Group (GONG) Program and the SOI/MDI instrument on SoHO. GONG is managed by the National.
1 Test rescale methods Y. Liu, J. T. Hoeksema, X. P. Zhao, R. M. Larson – Stanford University
The May 1997 and May 1998 MURI events George H. Fisher UC Berkeley.
The Asymmetric Polar Field Reversal – Long-Term Observations from WSO J. Todd Hoeksema, Solar Observatories H.E.P.L., Stanford University SH13C-2278.
Synoptic Solar Cycle observed by Solar Dynamics Observatory Elena Benevolenskaya Pulkovo Astronomical Observatory Saint Petersburg State University ‘Differential.
Seething Horizontal Magnetic Fields in the Quiet Solar Photosphere J. Harvey, D. Branston, C. Henney, C. Keller, SOLIS and GONG Teams.
Comparison on Calculated Helicity Parameters at Different Observing Sites Haiqing Xu (NAOC) Collaborators: Hongqi, Zhang, NAOC Kirill Kuzanyan, IZMIRAN,
1 C. “Nick” Arge Space Vehicles Directorate/Air Force Research Laboratory SHINE Workshop Aug. 2, 2007 Comparing the Observed and Modeled Global Heliospheric.
Proxies of the Entire Surface Distribution of the Photospheric Magnetic Field Xuepu Zhao NAOC, Oct. 18, 2011.
Sky Coordinate Image Specs Fully processed: –Merged –10-min cadence –“sky to sky” interpolation –Gaussian temporal filter –Renormalized such that time.
A Presentation to the SHINE ’02 Workshop by J.G. Luhmann (August 19, 2002) CME initiation: A zoo not an animal (Images from the on-line CDAW CME catalogue.
GONG Magnetograms - Raw to Synoptic Map J. Harvey.
Imaging Solar Tachocline Using Numerical Simulations and SOHO/MDI Data Junwei Zhao 1, Thomas Hartlep 2, Alexander G. Kosovichev 1, Nagi N. Mansour 2 1.W.W.Hansen.
Solar Maximum ! A Double Peaked Sunspot Cycle ?
Zasshikai S.UeNo MDI Measurement Errors: The Magnetic Perspective Y. Liu & A.A. Norton SOI-Technical Note Zasshikai S.UeNo.
PCI analysis of Sunspot and Background Magnetic Field variations in the cycles V.V. Zharkova 1, S.I. Zharkov 2, Shepherd S.J. 3 and Popova 4 Zharkov.
1 Synoptic Maps of Magnetic Field from MDI Magnetograms: polar field interpolation. Y. Liu, J. T. Hoeksema, X. P. Zhao, R. M. Larson – Stanford University.
1 GONG Magnetogram Data Products. 2 Sky-coordinate images Single-site or merged? –Single-site requires users to select. –Merge has lower noise, may require.
1 Mei Zhang ( National Astronomical Observatory, Chinese Academy of Sciences ) Solar cycle variation of kinetic helicity Collaborators: Junwei Zhao (Stanford,
Session 10 SHINE Workshop, June 23-27, 2008 Vector Magnetic Data Input into Global Models (Session 10) Chairs: Marc DeRosa and Ilia Roussev Working Group.
Polar Magnetic Field Elena E. Benevolenskaya Stanford University SDO Team Meeting 2009.
Three-Dimensional Power Spectra of GONG++ High- Cadence Magnetograms F. Hill, J. Bolding, R. Clark, K. Donaldson-Hanna, J. Harvey, G. Petrie, C. Toner.
Sunspot activity and reversal of polar fields in the current cycle 24 A.V. Mordvinov 1, A.A. Pevtsov 2 1 Institute of Solar-Terrestrial Physics of SB RAS,
Synoptic Chart of Magnetic Field from MDI Magnetograms J. T. Hoeksema, Y. Liu, X.P. Zhao, A. Amezcua – Stanford University
The Helioseismic and Magnetic Imager (HMI) on NASA’s Solar Dynamics Observatory (SDO) has continuously measured the vector magnetic field, intensity, and.
CSI /PHYS Solar Atmosphere Fall 2004 Lecture 04 Sep. 22, 2004 Solar Magnetic Field, Solar Cycle, and Solar Dynamo.
1 NSSC National Space Science Center, Chinese academy of Sciences FACs connecting the Ionosphere and Magnetosphere: Cluster and Double Star Observations.
Long-term measurements of the Sun’s poles show that reversal of the dominant magnetic polarity generally occurs within a year of solar maximum. Current.
The HMI Instrument. HMI Science Goals Line-of-Sight Observables.
SOLIS-VSM Magnetic Synoptic Maps
HMI-WSO Solar Polar Fields and Nobeyama 17 GHz Emission
Predictions for solar cycle 25
A Comparison of Solar Polar Coronal Hole Areas
Large-Scale Solar Magnetic Fields – How is Solar Cycle 24 Different?
MDI Level 1.8 Magnetograms
Carrington Rotation 2106 – Close-up of AR Mr 2106 Bt 2106
Current HMI Polar Fields
Exploring Large-scale Coronal Magnetic Field Over Extended Longitudes With EUVI EUVI B EIT EUVI A 23-Mar UT Nariaki Nitta, Marc DeRosa, Jean-Pierre.
Soothing Massage of HMI Magnetic Field Data
A Presentation to the SHINE ’02 Workshop by J.G. Luhmann
Closing the Books on Cycle 24 J
106.13: A Makeover for HMI Magnetic Field Data
Presentation transcript:

SPD – June 2006 Solar Polar Flux – MDI The Sun’s Polar Magnetic Flux Observed with SOHO/MDI J. Todd Hoeksema E.E. Benevolenskaya, Y. Liu P.H. Scherrer & X.P. Zhao Stanford University

SPD – June 2006 Solar Polar Flux – MDI Figure 1 a)Apparent values of the magnetic flux of the radial field component in the latitude zones from 78 o to 88 o in Northern (blue line) and Southern (red line) hemispheres b)The fraction of positive polarity magnetic flux in Northern (blue line) and Southern (red line) hemispheres c) Total signed magnetic flux. The polar magnetic field reversal was in CR1975± 2 (April 2001) in the North and in CR1981± 2 (September 2001) in South. Figure 1

SPD – June 2006 Solar Polar Flux – MDI The apparent values of the total unsigned magnetic flux Fr = |F+| + |F-| for the polar caps 78 o – 88 o are presented in Figure 1a for reduced- resolution synoptic maps (1 o in both latitude and longitude). There is a N-S asymmetry in the distributions of the total polar magnetic flux for low-resolution maps: F r = x Mx and F r = x Mx for the North and South polar caps before CR2007 (September 2003). After that, the total magnetic flux increases slightly in North and decreases in the South. The positive |F+| /Fr fraction of the magnetic flux is plotted in Figure 1b. Total signed flux is present in Figure 1c. The time of reversals can be easily determined at |F+| /Fr = 0.5. This was in CR1974 (March 2001) in the North and in CR1980 (August 2001) in South. This is close to the periods obtained by Durrant and Wilson ( Solar Physics, 2003): CR1975 in North and CR1981 in South using the Kitt Peak synoptic maps. Figure 1

SPD – June 2006 Solar Polar Flux – MDI Figure 2 a) b) c) d) Magnetic Field Observational Variation SOHO Rotated SOHO Nominal

SPD – June 2006 Solar Polar Flux – MDI Figure 2 - MDI Spatial Noise Pattern Left column: Magnetic maps averaged over 60 min periods a) Upper: B when SOHO/MDI was rotated, P_angle = o. b) Lower: B when SOHO/MDI was not rotated, P_angle = 0.0 o. Right Column: The Noise level as σ - distribution of 1 min images in 60 min series: c) Upper: σ-distribution when SOHO/MDI was rotated, P_angle = o d) Lower: σ-distribution when SOHO/MDI was not rotated, P_angle = 0.0 o Figure 3 – MDI Noise for 5-min and 1-min Magnetograms One-hour noise level along the central meridian as σ-distribution for the two kinds of MDI magnetograms Left: images averaged over 5 minutes on-board (a, c) and Right: 1 min magnetograms (b, d) for two time sets in 1 hour series. Upper: SOHO/MDI was rotated. Lower: SOHO/MDI was not rotated. Figure 2, 3

SPD – June 2006 Solar Polar Flux – MDI N-S sigma distributions along CM Figure 3 MDI Rotated MDI Nominal 5min Mags1min Mags

SPD – June 2006 Solar Polar Flux – MDI Figure 4. Variations of the value of apparent total unsigned flux as function of the number of images averaged for the polar caps: a) for North and b) for South Figure 5. Synoptic magnetic maps of CR2027 (25 February – 25 March, 2005) a) is constructed from a single image at each point, i.e. without any averaging. b) is constructed by averaging 60 images at each point. Latitude in sin (latitude). Resolution is 1 o in both latitude and longitude. Figure 6. Noise level (σ – distribution) versus latitude for CR 1993 and CR 2020 for 5 min and 1 hour averaged magnetograms. a) σ=9.3G for 87 o N-88 o N and σ=10.7G for 80 o S-81 o S; (P_angle = 0.0 o ) b) σ=2.7G for 87 o N-88 o N and σ=4.8G for 80 o S-81 o S; (P_angle = 0.0 o ) c) σ=9.7G for 87 o N-88 o N and σ=12.3G for 80 o S-81 o S; (P_angle = o ) d) σ=3.9G for 87 o N-88 o N and σ=4.8G for 80 o S-81 o S; (P_angle = o )

SPD – June 2006 Solar Polar Flux – MDI Figure 4 The apparent total unsigned magnetic flux of polar caps, o computed using various numbers of averaged images during favorable polar viewing conditions. NORTH: CR1993-Aug 2002; CR2020-Aug 2004; CR2033-Aug 2005 SOUTH: CR1960-Mar 2000; CR2013-Feb 2004; CR 2027-Mar 2005 P-angle = 180 for CR 2013, CR2020, CR2027 & CR 2033 P-angle = 0 for CR 1960 and CR 1993

SPD – June 2006 Solar Polar Flux – MDI Figure 5 Single Mag 60 Mags Sine

SPD – June 2006 Solar Polar Flux – MDI Figure 6 SOHO Rotated SOHO Nominal

SPD – June 2006 Solar Polar Flux – MDI The value of the apparent total polar magnetic flux depends on the number of averaged images (Figures 4, 5). The pixel noise level of the MDI magnetograms was estimated by Ortiz et.al (2002). The 1-σ noise level for 1-min longitudinal magnetograms is 20 G. The magnetic noise level for 5-min magnetograms is about 9G. The random noise level decreases as 1/√N, where N is number of observations. The noise level is 2.8G for 50 min and 2.6 G for 60 min. They concluded that 20-min averages have a reasonably low noise level. They also noted the increase of the noise in the bottom right of the image, which we can see in Figure 2 (c,d). This is caused by systematic errors in the tuning of MDI. There is some discrepancy in the apparent values of the total magnetic flux estimated from synoptic maps obtained from 15 averaged images per day and the consecutive 1 min images averaged for 60 min (see Figures 1a and 4a ). For example, for CR 2033 (8 Aug – 4 Sep 2005) the total magnetic flux was Mx for 15 images taken during day but it is higher for any number of averaged images up to N=60. We expect this is connected with the reduction of the supergranulation noise, which is more completely suppressed in the first case.

SPD – June 2006 Solar Polar Flux – MDI The effect of MDI shutter noise on the apparent polar magnetic flux. The shutter noise of the SOHO/MDI instrument induces a small random offset into the magnetic measurements that is uniform over the disk. (Liu, Zhao & Hoeksema, 2004). The offset is removed from each magnetogram. We have estimated the magnetic flux of north polar cap (78 o N-88 o N) during the CR2033 with offset correction and without offset correction. There is a small difference in the relative positive magnetic flux and magnetic strength. With correction we obtain (|F + |/ F r )= and the averaged radial component of the magnetic field is B r =- 8.13G. Without the correction (|F + |/ F r )= and the averaged radial component of the magnetic field is B r = -7.62G. There is only a small difference in the apparent total magnetic flux. For example, the total unsigned magnetic flux in CR2021 is x Mx without correction and it is x Mx with correction.

SPD – June 2006 Solar Polar Flux – MDI Summary The value of the apparent total magnetic flux depends on the number of averaged magnetograms in the synoptic map. The apparent values decreases with the number of the averaged magnetograms due to random noise reduction. Shutter noise contributes a small portion to the estimation of the total unsigned magnetic flux of polar caps. Systematic errors are not reduced. Individual magnetograms reveal the non-uniform σ-distribution over solar disk. The noise increases to the SW on normal magnetograms, and in the NE when SOHO/MDI is rotated by 180 o. Other effects make it difficult to estimate the “true” polar flux. References Benevolenskaya, E.E., 2004, A&A, 428, L5. Durrant, C.J., & P.R. Wilson, 2003, Solar Phys., 214, 23. Liu, Y., X.P. Zhao, & J.T. Hoeksema, 2004, Solar Phys., 219, 39. Ortiz, S.K. Solanki, V. Domingo, M. Fligge, & B. Sanahuja, 2002, A&A, 388, 1036.