Polarization in Spectral LinesSpringer 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 |
869 | |
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多く使われている語句
6-j symbols absorption aeJe angle angular momentum anisotropy approximation atomic polarization auJu circular polarization coefficients collisional collisions components consider corresponding defined in Eq density matrix depolarizing Doppler eigenvectors evolution operator expression frequency given by Eq h₁ Hamiltonian Hanle effect help of Eqs hyperfine structure integral J₁ K₁ Landé factor Landi Degl'Innocenti linear polarization lower level M₁ magnetic field magnetic field vector matrix elements multiplet multipole multipole moments non-LTE optical depth oscillator phase matrix physical profiles propagation matrix properties quantities quantum numbers radiation field tensor radiative transfer equations reference system rotation scattering Sect solar spectral lines statistical equilibrium equations statistical tensors Stokes parameters Stokes vector sublevels Substitution T₁ term transition two-level atom unit vectors unpolarized upper level V₁ values velocity wavelength Zeeman zero Δλ νο