Polarization in Spectral Lines

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Springer Science & Business Media, 2004/08/24 - 890 ページ
The scientific research based on spectropolarimetric techniques is undergoing a phase of rapid growth. Instruments of unprecedented sensitivity are nowadays available, particularly for solar observations. To fully exploit the rich diagnostic content of such observations, it is necessary to understand the physical mechanisms involved in the generation and transfer of polarized radiation in astrophysical (or laboratory) plasmas. After an introductory part based on classical physics, this book tackles the subject by a rigorous quantum-mechanical approach. The transfer equations for polarized radiation and the statistical equilibrium equations for the atomic density matrix are derived directly from the principles of Quantum Electrodynamics. The two sets of equations are then used to present a number of applications, mainly concerning the diagnostics of solar magnetic fields. This book is primarily addressed to scientists working in the field of spectropolarimetry. It may also serve as a textbook for a course at the graduate or advanced undergraduate level.
 

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目次

CHAPTER 1
1
EPt
11
EPt
12
P
27
CHAPTER 2
29
The norm Nn of the vector Om j1121112 can
35
J3
41
2+12+1
48
nb
481
MW
490
c We assume that each given ray path crosses
497
MM
501
MM
502
additional contribution to Eq 9268 of the
503
CHAPTER 10
509
x 6xx 20+108vo
552

1
71
CHAPTER 3
73
B
80
SP1
83
IC
85
the sum over M₁ and M2 by the same method
94
F3
113
Jz
129
CHAPTER 4
131
CHAPTER 5
147
B
158
from which we deduce
168
This formula proves that the profiles da in Eqs
169
Z
185
1
191
Comparison of Eqs 5110 and 5109
195
Fig516 Qualitative description of a 90 scattering event
213
MATTERRADIATION INTERACTION CLASSICAL
214
0
215
CHAPTER 6
237
where X is the coordinate of the center of mass
245
The terms in square brackets of Eqs 639
249
and transform the summation over the various modes of the
256
CHAPTER 7
277
0
340
CHAPTER 8
349
CHAPTER 9
375
M
392
Bo j
412
W
416
MMAN
420
jo
435
Let us consider the second possibility According to Magain
457
equivalent width for the line considered Defining the new
462
32
566
PQ
596
δ
608
CHAPTER 11
625
MEN
638
MEN
639
HAV
656
CHAPTER 12
663
θ
674
0+
675
h
679
h
680
α
682
CHAPTER 13
689
δ
699
δ
723
20
726
CHAPTER 14
737
Z
744
and assuming that the stellar atmosphere is not illuminated by
751
VA
756
which is the same as Eq 5166
759
where
765
MA
774
1
791
k Special case J₁ 0 J₁₁
833
or by means of the inverse transformations to those
839
Ja
846
Finally from Eq A2010 one can
850
θ
851
is the Planck function at the kinetic temperature of the
854
LIST OF TABLES
867
REFERENCES
869
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