Far‐Ultraviolet Echoes from the Frontier between the Solar Wind and the Local Interstellar Cloud

2000 ◽  
Vol 533 (2) ◽  
pp. 924-930 ◽  
Author(s):  
L. Ben‐Jaffel ◽  
O. Puyoo ◽  
R. Ratkiewicz
2000 ◽  
Vol 198 ◽  
pp. 224-233 ◽  
Author(s):  
George Gloeckler ◽  
Johannes Geiss

New measurements of the isotopic composition of helium in the solar wind obtained from the Solar Wind Ion Composition Spectrometer (SWICS) on Ulysses are presented and compared with earlier SWICS results and previous mass spectrometric determinations of this ratio with the Apollo Solar Wind Composition (SWC) experiment and the Ion Composition Instrument (ICI) on the International Sun Earth Explorer 3 (ISEE 3). The new SWICS data from both the fast and slow solar wind are extrapolated to the photosphere to obtain a representative value of the present-day ratio of 3He/4He = (3.75 ± 0.27) × 10−4 in the Outer Convective Zone (OCZ) of the Sun. After corrections of this ratio for secular changes caused by diffusion, mixing and 3He production by incomplete H-burning (Vauclair 1998), we obtain (D + 3He)/H = (3.6 ± 0.38) × 10−5 for the Protosolar Cloud (PSC). Adopting the Jovian 3He/4He ratio = (1.66 ±0.05) × 10−4 measured by the Galileo Probe mass spectrometer (Mahaffy et al. 1998) as representative for the PSC, we obtain (D/H)protosolar = (1.94 ±0.39) × 10−5. Using results of galactic evolution studies (Tosi 1998, 2000) and the D and 3He abundances in the Protosolar Cloud and the Local Interstellar Cloud (Linsky 1998; Gloeckler &Geiss 1998), we estimate (D/H)primordial = (2.4 − 4.2) × 10−5. This range corresponds to a universal baryon/photon ratio of (5.9−4.2) × 10−10.


1996 ◽  
Author(s):  
L. L. Williams ◽  
H. L. Pauls ◽  
G. P. Zank ◽  
D. T. Hall

2013 ◽  
Author(s):  
Robert Kane ◽  
Nicholas Nell ◽  
Ted Schultz ◽  
Kevin France ◽  
Matthew Beasley ◽  
...  

1997 ◽  
Vol 166 ◽  
pp. 17-28
Author(s):  
R. Lallement

AbstractConstraints on the ambient (circumsolar) interstellar medium can be derived from observations of interstellar neutrals or their derivatives in the heliosphere. New results have been recently obtained which, when combined with optical and UV observations of the nearby stars (HST-GHRS, EUVE), remove long-standing contradictions and allow us to infer for our local cloud, pressure, ionization and limits on the magnetic field. The electron density in the circumsolar gas is found to be between 0.04 and 0.15 cm−3. Its total thermal pressure is within the interval 1700 – 2600 cm−3 K. If the local magnetic field is nearly perpendicular to the interstellar wind flow, which is likely, then its intensity is smaller than 3.6 μG. Our Sun is located very close to the edge of the local cloud (the volume of gas which has the same physical properties as the circumsolar gas), while there are at least 5 other cloudlets within 10 pc. Abundances vary from cloudlet to cloudlet. How they are located and whether they are separated by tenuous gas or shock discontinuities is not clear yet. Semi-hot (105 K) gas has been detected in absorption towards nearby stars (Wood et al, 1996), which probably originates in the “H walls” surrounding our heliosphere and other asterospheres. This shows that semi-hot gas is not necessarily linked with cloud interfaces with the hot gas of the Local Bubble.


2004 ◽  
Vol 219 ◽  
pp. 623-634 ◽  
Author(s):  
A. K. Dupree

Recent spectroscopic results from the far ultraviolet and X-ray region coupled with infrared observations demonstrate that winds from luminous stars can be warm (300000K) and fast (speeds of several hundred km s—1) linking the hot solar wind to the cool, massive winds of luminous M-type supergiant stars. Hot coronal material (T ∼107 K) appears to be confined near the star, and not expanding in the wind. These new spectra enable a comprehensive picture to be constructed of the presence and character of winds in cool stars.


2004 ◽  
Vol 606 (1) ◽  
pp. L81-L84 ◽  
Author(s):  
D. Bodewits ◽  
Z. Juhsz ◽  
R. Hoekstra ◽  
A. G. G. M. Tielens

Author(s):  
R. HOEKSTRA ◽  
D. BODEWITS ◽  
R. MORGENSTERN ◽  
C. M. LISSE ◽  
A. G. G. M. TIELENS

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