Principal component analysis of the solar magnetic field I: The axisymmetric field at the photosphere

被引:15
作者
Lawrence, JK [1 ]
Cadavid, AC
Ruzmaikin, A
机构
[1] Calif State Univ Northridge, Northridge, CA 91330 USA
[2] CALTECH, Jet Prop Lab, Pasadena, CA 91109 USA
基金
美国国家航空航天局;
关键词
D O I
10.1007/s11207-004-3257-2
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
A principal component analysis, or proper orthogonal decomposition, of the axisymmetric magnetic field at the photosphere is carried out to find an optimal representation of the observed solar cycle. The 22-year periodic field requires just two modes. NSO Kitt Peak synoptic maps for Carrington rotations 1664-2007 were reduced by taking both the mean and the median field over longitude to produce two sequences of functions of sine latitude spanning 25.7 years. The lowest modes of each are determined by the polar fields. The mean field is most efficient at representing the periodic field, but the median field is more efficient at representing the evolution of the diffuse field patterns.
引用
收藏
页码:1 / 19
页数:19
相关论文
共 16 条
[1]  
ALTSCHULER MD, 1971, IAU S, V43, P588
[2]   Impulses of activity and the solar cycle [J].
Benevolenskaya, EE .
SOLAR PHYSICS, 2003, 216 (1-2) :325-341
[3]   DOUBLE MAGNETIC CYCLE OF SOLAR-ACTIVITY [J].
BENEVOLENSKAYA, EE .
SOLAR PHYSICS, 1995, 161 (01) :1-8
[4]  
Choudhuri AR, 2003, DYNAMIC SUN, P103
[5]  
ELSNER JB, 1996, SINGULAR SPECTRUM AN
[6]   PIPS AND POPS - THE REDUCTION OF COMPLEX DYNAMICAL-SYSTEMS USING PRINCIPAL INTERACTION AND OSCILLATION PATTERNS [J].
HASSELMANN, K .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 1988, 93 (D9) :11015-11021
[7]  
HOEKSEMA JT, 1984, ESA220 EUR SPAC AG S, P269
[8]  
Holmes P., 1996, Turbulence, coherent structures, dynamical systems, and symmetry
[9]  
Jackson JE, 1991, A user's guide to principal components
[10]  
Karhunen K., 1946, Annales Academiae Scientiarum Fennicae. Series A, V34, DOI DOI 10.1007/s11071-005-2803-2