-
1
-
-
4243122606
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-
note
-
Except in the surface layers of the sun, the characteristic cooling time is much longer than the periods of the seismic waves, so the wave motion is essentially adiabatic. Near the surface, the sun is highly turbulent and is not well understood.
-
-
-
-
2
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4243086549
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-
note
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2.
-
-
-
-
3
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0038852456
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D. O. Gough, Sol. Phys. 100, 65 (1985); A. G. Kosovichev, Bull. Crimean Astrophys. Obs. 75, 36 (1986); D. O. Gough and A. G. Kosovichev, in Inside the Sun, Proceedings of International Astronomical Union Colloquium 121, G. Berthomieu and M. Cribier, Eds. (Kluwer, Dordrecht, Netherlands, 1990), pp. 327-340; D. O. Gough and M. J. Thompson, in Solar Interior and Atmosphere, A. N. Cox, W. C. Livingston, M. Matthews, Eds. (Univ. of Arizona Press, Tucson, AZ), pp. 519-561 (1991); W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991).
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Gough, D.O.1
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4
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0038852456
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D. O. Gough, Sol. Phys. 100, 65 (1985); A. G. Kosovichev, Bull. Crimean Astrophys. Obs. 75, 36 (1986); D. O. Gough and A. G. Kosovichev, in Inside the Sun, Proceedings of International Astronomical Union Colloquium 121, G. Berthomieu and M. Cribier, Eds. (Kluwer, Dordrecht, Netherlands, 1990), pp. 327-340; D. O. Gough and M. J. Thompson, in Solar Interior and Atmosphere, A. N. Cox, W. C. Livingston, M. Matthews, Eds. (Univ. of Arizona Press, Tucson, AZ), pp. 519-561 (1991); W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991).
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Kosovichev, A.G.1
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Proceedings of International Astronomical Union Colloquium 121, G. Berthomieu and M. Cribier, Eds. Kluwer, Dordrecht, Netherlands
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D. O. Gough, Sol. Phys. 100, 65 (1985); A. G. Kosovichev, Bull. Crimean Astrophys. Obs. 75, 36 (1986); D. O. Gough and A. G. Kosovichev, in Inside the Sun, Proceedings of International Astronomical Union Colloquium 121, G. Berthomieu and M. Cribier, Eds. (Kluwer, Dordrecht, Netherlands, 1990), pp. 327-340; D. O. Gough and M. J. Thompson, in Solar Interior and Atmosphere, A. N. Cox, W. C. Livingston, M. Matthews, Eds. (Univ. of Arizona Press, Tucson, AZ), pp. 519-561 (1991); W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991).
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Gough, D.O.1
Kosovichev, A.G.2
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6
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A. N. Cox, W. C. Livingston, M. Matthews, Eds. (Univ. of Arizona Press, Tucson, AZ)
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D. O. Gough, Sol. Phys. 100, 65 (1985); A. G. Kosovichev, Bull. Crimean Astrophys. Obs. 75, 36 (1986); D. O. Gough and A. G. Kosovichev, in Inside the Sun, Proceedings of International Astronomical Union Colloquium 121, G. Berthomieu and M. Cribier, Eds. (Kluwer, Dordrecht, Netherlands, 1990), pp. 327-340; D. O. Gough and M. J. Thompson, in Solar Interior and Atmosphere, A. N. Cox, W. C. Livingston, M. Matthews, Eds. (Univ. of Arizona Press, Tucson, AZ), pp. 519-561 (1991); W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991).
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Gough, D.O.1
Thompson, M.J.2
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7
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85076896343
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D. O. Gough, Sol. Phys. 100, 65 (1985); A. G. Kosovichev, Bull. Crimean Astrophys. Obs. 75, 36 (1986); D. O. Gough and A. G. Kosovichev, in Inside the Sun, Proceedings of International Astronomical Union Colloquium 121, G. Berthomieu and M. Cribier, Eds. (Kluwer, Dordrecht, Netherlands, 1990), pp. 327-340; D. O. Gough and M. J. Thompson, in Solar Interior and Atmosphere, A. N. Cox, W. C. Livingston, M. Matthews, Eds. (Univ. of Arizona Press, Tucson, AZ), pp. 519-561 (1991); W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991).
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Pamjatnykh, A.A.2
Sienkiewicz, R.3
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9
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0347921179
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J. Patron, F. Hill, E. J. Rhodes Jr., S. G. Korzennik, A. Cacciani, Astrophys. J. 455, 746 (1995); T. L. Duvall Jr., S. D'Silva, S. M. Jefferies, J. W. Harvey, J. Schou, Nature 379, 235 (1996); A. G. Kosovichev, Asfrophys J. Lett. 461, L55 (1996).
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10
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J. Patron, F. Hill, E. J. Rhodes Jr., S. G. Korzennik, A. Cacciani, Astrophys. J. 455, 746 (1995); T. L. Duvall Jr., S. D'Silva, S. M. Jefferies, J. W. Harvey, J. Schou, Nature 379, 235 (1996); A. G. Kosovichev, Asfrophys J. Lett. 461, L55 (1996).
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11
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0040513503
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J. Patron, F. Hill, E. J. Rhodes Jr., S. G. Korzennik, A. Cacciani, Astrophys. J. 455, 746 (1995); T. L. Duvall Jr., S. D'Silva, S. M. Jefferies, J. W. Harvey, J. Schou, Nature 379, 235 (1996); A. G. Kosovichev, Asfrophys J. Lett. 461, L55 (1996).
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J. B. Keller and S. I. Rubinow, Ann. Phys. 9, 24 (1960); D. O. Gough, in Astrophysical Fluid Dynamics, J. P. Zahn and J. Zinn-Justin, Eds. (North-Holland, Amsterdam, 1993), pp. 399-560. In a sphere, such as the sun, the phases of waves on adjacent planes containing the center of the sphere must also be in appropriate relative phase for resonance to occur.
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Ann. Phys.
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Keller, J.B.1
Rubinow, S.I.2
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0001433409
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J. P. Zahn and J. Zinn-Justin, Eds. North-Holland, Amsterdam
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J. B. Keller and S. I. Rubinow, Ann. Phys. 9, 24 (1960); D. O. Gough, in Astrophysical Fluid Dynamics, J. P. Zahn and J. Zinn-Justin, Eds. (North-Holland, Amsterdam, 1993), pp. 399-560. In a sphere, such as the sun, the phases of waves on adjacent planes containing the center of the sphere must also be in appropriate relative phase for resonance to occur.
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Astrophysical Fluid Dynamics
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Gough, D.O.1
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14
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4243074924
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-
note
-
Frequencies also depend on the variation of density but to a lesser extent than they depend on sound speed [see (9)].
-
-
-
-
15
-
-
4243164044
-
-
note
-
That time is inversely proportional to the magnitude of the group velocity and is directly proportional to the relative density of ray-path segments.
-
-
-
-
16
-
-
4243150296
-
-
note
-
2 or u = p/ρ rather than c because, being proportional to T/μ, it is more readily comprehended.
-
-
-
-
18
-
-
0001722830
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-
This technique has been carried out with only asymptotic representations of the resonance conditions [for example, see J. Christensen-Dalsgaard et al., Nature 315, 378 (1985)].
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(1985)
Nature
, vol.315
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-
Christensen-Dalsgaard, J.1
-
19
-
-
4243145815
-
-
note
-
i divided by the modal inertia, which is the functional form of any surface uncertainty [see (3)].
-
-
-
-
20
-
-
2542548666
-
-
That sets the radius of the base of the adiabatically stratified part of the convection zone at about 0.709R. This value is somewhat less than the value 0.713R obtained previously by J. Christensen-Dalsgaard, D. O. Gough, and M, J. Thompson [Astrophys. J. 378, 413 (1991)], and by A. G. Kosovichev and A. V. Fedorova [Sov. Astron. 35, 507 (1991)]. A study of the transition at the base of the convection zone [see (30)] is consistent with the new result, although a repeat of the analysis with the use of the reference models of Richard et al. (15) yields 0.714R.
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Astrophys. J.
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Christensen-Dalsgaard, J.1
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Thompson, M.J.3
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21
-
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2542548666
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-
That sets the radius of the base of the adiabatically stratified part of the convection zone at about 0.709R. This value is somewhat less than the value 0.713R obtained previously by J. Christensen-Dalsgaard, D. O. Gough, and M, J. Thompson [Astrophys. J. 378, 413 (1991)], and by A. G. Kosovichev and A. V. Fedorova [Sov. Astron. 35, 507 (1991)]. A study of the transition at the base of the convection zone [see (30)] is consistent with the new result, although a repeat of the analysis with the use of the reference models of Richard et al. (15) yields 0.714R.
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Sov. Astron.
, vol.35
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Fedorova, A.V.2
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26
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4243161624
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note
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2 tends to be associated with corresponding relative decreases in ρ and μ.
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27
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85076896343
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W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991); W. Däppen et al., in Challenges to Theories of the Structure of Moderate-Mass Stars, D. O. Gough and J. Toomre, Eds. (Lecture Notes-in Physics 388, Springer, Heidelberg, Germany, 1991), pp. 111-120. A. Kosovichev et al., Mon. Not. R. Atron. Soc. 259, 536 (1992); H. M. Antia and S. Basu, Astrophys. J. 426, 801 (1994); A. G. Kosovichev, Adv. Space Res. 15, 95 (1995).
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W. A. Dziembowski, A. A. Pamjatnykh, R. Sienkiewicz, Mon. Not. R. Astron. Soc. 249, 602 (1991); W. Däppen et al., in Challenges to Theories of the Structure of Moderate-Mass Stars, D. O. Gough and J. Toomre, Eds. (Lecture Notes-in Physics 388, Springer, Heidelberg, Germany, 1991), pp. 111-120. A. Kosovichev et al., Mon. Not. R. Atron. Soc. 259, 536 (1992); H. M. Antia and S. Basu, Astrophys. J. 426, 801 (1994); A. G. Kosovichev, Adv. Space Res. 15, 95 (1995).
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4243157033
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note
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The wave is also advected by azimuthal flow, but the axisymmetric component of that flow is rotation, which is addressed in (20).
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34
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4243100210
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J. T. Hoeksema et al., Eds. European Space Agency (ESA) Special Publication (SP)-379, Noordwijk, Netherlands
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E. G. Zweibel and D. O Gough, in Procedings of the Fourth SOHO Workshop: Helioseismology, J. T. Hoeksema et al., Eds. [European Space Agency (ESA) Special Publication (SP)-379, Noordwijk, Netherlands, 1995], Although one cannot distiguish between possible sources of asphericity by analyzing frequencies alone, the different anisotropies of the wave-speed perturbations from different sources renders it possible in principle to distinguish them by their eigenfunctions. That might be possible in the future with the use of techniques such as time-distance seismology.
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4243115972
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note
-
The averaging kernels in this case are quadratic in the horizontal structure of the eigenfunctions. They are therefore even functions of latitude and are sensitive only to the north-south symmetric component of the asphericity. It requires some knowledge of the form of the eigenfunctions to determine the asymmetric component.
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36
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D, O Gough and M. J. Thompson, in Advances in Helio- and Asteroseismology, J. Christensen-Dalsgaard and S. Frandsen, Eds. (Reidel, Dordrecht, Netherlands, 1988), pp. 175-180; J. R. Kuhn, Astmphys. J. Lett. 331, L131 (1988); P. R. Goode and J. R. Kuhn. Astrophys. J. 356, 310 (1990); K. G. Libbrecht and M. F. Woodard, ibid. 402, L77 (1993).
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We have investigated the structure of the transition between the convection zone and the radiative interior by first considering how mode frequency varies with the phase difference between the surface of the sun and the base of the convection zone, after having filtered out surface effects, and then comparing it with theoretical models (32). The signature of the transition oscillates with phase, in step with the eigenfunctions, with an amplitude that is smaller than that of the reference model, confirming that, if spherical, the transition is smoother than that of the model. The apparent smoothness might have come about because what has been observed is actually the spherical average of an aspherical structure. Adiabatic convective overshooting is likely to increase the amplitude; therefore, if such overshooting occurs in the sun, the physical discrepancy is actually greater than It appears at first sight. There is some indication that the amplitude of the oscillatory signal varies with the ratio m/( of azimuthal order to degree. This suggests that the structure of the lower boundary layer of the convection zone might vary with latitude. Although at present this is no more than a hint, it points to an exciting direction of research with further longterm seismic data.
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M. J. P. F. G. Monteiro and M. J. Thompson, Astron. Astrophys. 283, 247 (1994), J. Christensen-Dalsgaard, M. J. P. F. G. Monteiro, M. J. Thompson, Mon. Not. R Astron. Soc. 276, 283 (1995); I. W. Roxburgh and S. V. Vorontsov, ibid. 268, 880 (1994); S. Basu, H. M. Antia, D. Narasimha, ibid. 267, 207 (1994).
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M. J. P. F. G. Monteiro and M. J. Thompson, Astron. Astrophys. 283, 247 (1994), J. Christensen-Dalsgaard, M. J. P. F. G. Monteiro, M. J. Thompson, Mon. Not. R Astron. Soc. 276, 283 (1995); I. W. Roxburgh and S. V. Vorontsov, ibid. 268, 880 (1994); S. Basu, H. M. Antia, D. Narasimha, ibid. 267, 207 (1994).
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M. J. P. F. G. Monteiro and M. J. Thompson, Astron. Astrophys. 283, 247 (1994), J. Christensen-Dalsgaard, M. J. P. F. G. Monteiro, M. J. Thompson, Mon. Not. R Astron. Soc. 276, 283 (1995); I. W. Roxburgh and S. V. Vorontsov, ibid. 268, 880 (1994); S. Basu, H. M. Antia, D. Narasimha, ibid. 267, 207 (1994).
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GONG is managed by the National Solar Observatory, a division of the National Optical Astronomy Observatories, operated by AURA under a cooperative agreement with NSF. We acknowledge financial support from the U.K. Particle Physics and Astronomy Research Council, NSF, NASA, and Danmarks Gruncfforskningsfond.
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