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Comparative statistics and origin of triple and quadruple stars
The statistics of catalogued quadruple stars consisting of two binaries(hierarchy 2 + 2), is studied in comparison with triple stars, withrespective sample sizes of 81 and 724. Seven representative quadruplesystems are discussed in greater detail. The main conclusions are asfollows. (i) Quadruple systems of ? Lyr type with similar massesand inner periods are common, in 42 per cent of the sample the outermass ratio is above 0.5 and the inner periods differ by less than 10times. (ii) The distributions of the inner periods in triple andquadruple stars are similar and bimodal. The inner mass ratios do notcorrelate with the inner periods. (iii) The statistics of outer periodsand mass ratios in triples and quadruples are different. The medianouter mass ratio in triples is 0.39 independently of the outer period,which has a smooth distribution. In contrast, the outer periods of 25per cent quadruples concentrate in the narrow range from 10 to 100yr,the outer mass ratios of these tight quadruples are above 0.6 and theirtwo inner periods are similar to each other. (iv) The outer and innermass ratios in triple and quadruple stars are not mutually correlated.In 13 per cent of quadruples both inner mass ratios are above 0.85(double twins). (v) The inner and outer orbital angular momenta andperiods in triple and quadruple systems with inner periods above 30dshow some correlation, the ratio of outer-to-inner periods is mostlycomprised between 5 and 104. In the systems with small periodratios the directions of the orbital spins are correlated, while in thesystems with large ratios they are not. The properties of multiple starsdo not correspond to the products of dynamical decay of small clusters,hence the N-body dynamics is not the dominant process of theirformation. On the other hand, rotationally driven (cascade)fragmentation possibly followed by migration of inner and/or outerorbits to shorter periods is a promising scenario to explain the originof triple and quadruple stars.
| Hyades Morphology and Star Formation
Perryman and collaborators found that for the Hyades cluster thefraction of multiple stars increases from G stars to early-A stars. Wediscuss here whether this may be a general property of star formation orwhether collisions in the cluster environment change the fractions ofbinary stars. A star ring of mainly F and G stars is seen around theHyades cluster core, supposedly created by a shock wave due to asupernova explosion. These ring stars show the same fraction of binarystars as observed for the F and G stars in the core of the cluster. Thissuggests that collisions in the high stellar density cluster center didnot measurably change the multiple-star fractions. There is so far onlyevidence of this one supernova explosion in the Hyades. If this isindeed the only one, then only one massive star was born in the cluster.There are also fewer than 10 white dwarf descendants of B stars found inthe cluster. Unless many white dwarfs and neutron stars evaporated fromthe cluster, the initial mass function for stellar masses >2Msolar must have been very steep, corresponding to a Salpeterfunction with an exponent of less than -3.3.
| Two-colour photometry for 9473 components of close Hipparcos double and multiple stars
Using observations obtained with the Tycho instrument of the ESAHipparcos satellite, a two-colour photometry is produced for componentsof more than 7 000 Hipparcos double and multiple stars with angularseparations 0.1 to 2.5 arcsec. We publish 9473 components of 5173systems with separations above 0.3 arcsec. The majority of them did nothave Tycho photometry in the Hipparcos catalogue. The magnitudes arederived in the Tycho B_T and V_T passbands, similar to the Johnsonpassbands. Photometrically resolved components of the binaries withstatistically significant trigonometric parallaxes can be put on an HRdiagram, the majority of them for the first time. Based on observationsmade with the ESA Hipparcos satellite.
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Pozíciós és asztrometriai adatok
| Csillagkép: | Háló |
| Rektaszcenzió: | 04h24m12.97s |
| Deklináció: | -64°11'21.8" |
| Vizuális fényesség: | 9.093 |
| Távolság: | 201.613 parszek |
| RA sajátmozgás: | -13.3 |
| Dec sajátmozgás: | -8.2 |
| B-T magnitude: | 9.737 |
| V-T magnitude: | 9.147 |
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