Alpha Centauri

1981 ◽  
Vol 4 (2) ◽  
pp. 212-214 ◽  
Author(s):  
M. S. Bessell

The nearest star α Centauri is a triple system. The star α Cen, one of the pointers to the Southern Cross, is itself a −0.3 mag visual binary consisting of a α Cen A, a G2V star popularly considered to resemble the Sun, and α Cen B, a KOV star. The orbital period is 80.089 years, the semimajor axis is 23.5 AU, the distance 1.34 pc, the masses are 1.11 and 0.92 (±0.03) M⊙ (Kamper & Wesselink 1977). The third star, Proxima Cen (V645 Cen) is a faint common proper-motion companion separated from α Cen AB by about 2°. It is known to most people only by virtue of being slightly closer to the Sun than is α Cen A, and therefore actually the closest star.. This 11th mag flare star is undoubtedly coeval with a α Cen AB, but being the least massive by a considerable margin, may have been ejected from the system shortly after formation.

2019 ◽  
Vol 622 ◽  
pp. A45
Author(s):  
T. Iijima ◽  
H. Naito ◽  
S. Narusawa

Context. CH Cyg is one of the most studied symbiotic stars. Its properties, however, are still not well known. Two main periods, about 15 years and 750 days, are known in the photometric and spectroscopic variations, and two models are proposed for these origins. One is a binary system with an orbital period of 15 years consisting of a hot component and pulsating red giant with a 750-day period. The other is a triple system consisting of an inner symbiotic binary with an orbital period of about 750 days and third component with an orbital period of 15 years. Several active stages have been observed since the 1970s during which the object brightened up by ΔU = 3−5 mag and prominent emission lines appeared. Large mass outflows were observed at some active stages. Aims. The spectral variation of CH Cyg has been monitored at Asiago Observatories to understand the problems mentioned above. We have analysed spectra obtained in the time period from 1995 to 2004 which covers an active stage during the years 1998−2000. Methods. High- and low-resolution optical spectra obtained at the Asiago Observatories are used. Results. Narrow absorption lines of Fe I, Cr I, Ti I, and so on appeared in 1998 at an early phase of the active stage. These lines are clearly distinguished from those of the M-type giant and are typically found on the spectrum of early A-type dwarfs. They were redshifted by about 30 km s−1 with respect to the absorption lines of the M-type giant. Assuming that their radial velocities represent the orbital motion of the hot component, its semi-amplitude is estimated to be 37.0 ± 0.5 km s−1. The masses of the hot component and the M-type giant are estimated to be 0.32 ± 0.02 M⊙ and 4.6 ± 0.2 M⊙, respectively, where a circular orbit with a period of 756 days is adopted. If the inner binary system has an elliptical orbit, e = 0.33, and a period of 750.1 days, the masses of the two components are 0.21 ± 0.01 M⊙ and 2.2 ± 0.1 M⊙, respectively. Our results lend support to the triple system model, because if the period of the symbiotic binary were 15 years, the mass of the hot component would be expected to exceed the Chandrasekhar limit. Highly blueshifted absorption components of H I and He I lines appeared at a later phase of the active stage. Mass ejections with velocities on the order of 1000 km s−1 seem to have occurred along the orbital plane from December 1998 to March 1999. The highest outflow velocity, − 2383 km s−1, was observed on 1999 February 26. Narrow absorption components of Na I D1, D2, and Fe II lines redshifted by 10−15 km s−1 coexisted with the highly blueshifted broad absorption components of H I and He I lines. This phenomenon might have been related to an inner disc inflow expected in wind-compressed discs. In contrast to the bipolar mass outflows at the past active stages, high-velocity equatorial mass ejections likely occurred at the active stage during the years 1998−2000. There should have been an eclipse of the hot component by the M-type giant in the inner binary system in the time period of December 1998 to January 1999. A clear light curve of the eclipse, however, was not detected. Possibly, the luminosity of the hot component was due mainly to free-free emission from the ejected circumstellar matter which was likely more extended than the M-type giant. On the other hand, another eclipse by the third component with the period of 15 years began at the end of May 1999 during which the hot component as well as the emitting regions of Hβ and Fe II lines were well eclipsed. The obscuring matter around the third component should have been much more extended than the M-type giant, and it was likely semi-transparent, because the spectrum of the M-type giant was well seen during the eclipse. The third component appears to be similar to the invisible secondary component in the long-period eclipsing binary ϵ Aur.


2017 ◽  
Vol 598 ◽  
pp. L7 ◽  
Author(s):  
P. Kervella ◽  
F. Thévenin ◽  
C. Lovis

Proxima and α Centauri AB have almost identical distances and proper motions with respect to the Sun. Although the probability of such similar parameters is, in principle, very low, the question as to whether they actually form a single gravitationally bound triple system has been open since the discovery of Proxima one century ago. Owing to HARPS high-precision absolute radial velocity measurements and the recent revision of the parameters of the α Cen pair, we show that Proxima and α Cen are gravitationally bound with a high degree of confidence. The orbital period of Proxima is ≈ 550 000 yr. With an eccentricity of 0.50+0.08-0.09, Proxima comes within 4.3+1.1-0.9 kau of α Cen at periastron, and is currently close to apastron (13.0+0.3-0.1 kau). This orbital motion may have influenced the formation or evolution of the recently discovered planet orbiting Proxima, as well as circumbinary planet formation around α Cen.


1983 ◽  
Vol 71 ◽  
pp. 481-483
Author(s):  
K.E. Egge ◽  
B.R. Pettersen

Almost twenty years ago a large flare event was observed on the prototype contact binary W UMa by Kuhi (1964). Similar events have been reported on 44 i Boo (Eggen 1948) and U Peg (Huruhata 1952) . In this paper we present photoelectric observations at three wavelengths of a flare on VW Cep. This is the first event of this kind to be reported for this star. VW Cep is a triple system. The main contributor to the visual flux is the eclipsing binary, consisting of a Kl primary and a G6 secondary (Kopal 1978), classified to be in contact. The orbital period is 6h 41m. Seven per cent of the total flux in the visual filter is due to the third component, a late K type dwarf at a distance of 12 AU from the eclipsing system (Hershey 1975).


2020 ◽  
Vol 498 (1) ◽  
pp. 1319-1334
Author(s):  
S Marino ◽  
A Zurlo ◽  
V Faramaz ◽  
J Milli ◽  
Th Henning ◽  
...  

ABSTRACT Radial substructure in the form of rings and gaps has been shown to be ubiquitous among protoplanetary discs. This could be the case in exo-Kuiper belts as well, and evidence for this is emerging. In this paper, we present ALMA observations of the debris/planetesimal disc surrounding HD 206893, a system that also hosts two massive companions at 2 and 11 au. Our observations reveal a disc extending from 30 to 180 au, split by a 27 au wide gap centred at 74 au, and no dust surrounding the reddened brown dwarf (BD) at 11 au. The gap width suggests the presence of a 0.9MJup planet at 74 au, which would be the third companion in this system. Using previous astrometry of the BD, combined with our derived disc orientation as a prior, we were able to better constrain its orbit finding it is likely eccentric ($0.14^{+0.05}_{-0.04}$). For the innermost companion, we used radial velocity, proper motion anomaly, and stability considerations to show its mass and semimajor axis are likely in the ranges 4–100MJup and 1.4–4.5 au. These three companions will interact on secular time-scales and perturb the orbits of planetesimals, stirring the disc and potentially truncating it to its current extent via secular resonances. Finally, the presence of a gap in this system adds to the growing evidence that gaps could be common in wide exo-Kuiper belts. Out of six wide debris discs observed with ALMA with enough resolution, four to five show radial substructure in the form of gaps.


1996 ◽  
Vol 158 ◽  
pp. 343-344
Author(s):  
D. Chochol ◽  
S. Tamura ◽  
O. Kanamitsu ◽  
T. Pribulla ◽  
A. Tajitsu

AbstractThe very slow nova PU Vul was discovered by Honda and Kuwano in 1979 after the rise from B ~ 15…16 mag to a maximum B ~ 9 mag. The object has been studied by many authors (for references see Belyakina et al. 1989; Vogel & Nussbaumer 1992) but a clear picture of the system was not given. Two minima of different duration were observed in the system in the active stage, in 1980-81 and 1993-94 (Kolotilov et al. 1995). Nussbaumer & Vogel (1996) ascribed the minima to eclipses of the hot component by the cool M giant in a binary with orbital period of 4900±100 d. Our period analysis of the preoutburst B data (Liller & Liller 1979) by Stellingwerf’s (1978) method revealed a period of 4858 d. We found the third minimum in 1926-28 (lasting for 500…630 d) in these data.


2007 ◽  
Vol 22 (29) ◽  
pp. 5379-5389 ◽  
Author(s):  
LORENZO IORIO ◽  
MATTEO LUCA RUGGIERO

In this paper we use ΔP = -1.772341 ± 13.153788 s between the phenomenologically determined orbital period P b of the PSR J0737-3039A/B double pulsar system and the purely Keplerian period [Formula: see text] calculated with the system's parameters, determined independently of the third Kepler law itself, in order to put constraints on some models of modified gravity (f(R), Yukawa-like fifth force, MOND). The major source of error affecting ΔP is not the one in the phenomenologically measured period (δP b = 4×10-6 s ), but the systematic uncertainty δP(0) in the computed Keplerian one due to the relative semimajor axis a mainly caused, in turn, by the errors in the ratio [Formula: see text] of the pulsars' masses and in sin i. We get |κ| ≤ 0.8 × 10-26 m -2 for the parameter that in the f(R) framework is a measure of the nonlinearity of the theory, |α| ≤ 5.5 × 10-4 for the fifth-force strength parameter (for λ ≈ a = 0.006 AU ). The effects predicted by the strong-acceleration regime of MOND are far too small to be constrained with some effectiveness today and in the future as well. In view of the continuous timing of such an important system, it might happen that in the near future it will be possible to obtain somewhat tighter constraints.


2019 ◽  
Vol 29 (6) ◽  
pp. 23-46

Michael Heinrich, one of the leading Marx scholars, provides a general introduction into Das Kapital with emphasis on the latest interpretations of it. The circumstances surrounding its writing and publication are shown to have interfered with an adequate appreciation of it. The formal structure and organization of the first volume are obstacles to readers and demand much from their education and intellect. The article summarizes the basic trajectories of Marx’s criticisms of political economy, including the critique of naturalizing social forms arising under capitalism and Marx’s original monetary theory of value. The author disentangles Marx’s Das Kapital from views mistakenly ascribed to it, such as the idea that value is determined solely by labor and the prediction of pauperization of the masses. First, Marx’s theory of value goes well beyond explaining prices under capitalism. Second, his main prophecy concerned the inevitable growth of inequality between the masters of capital and the employed classes and did not forecast impoverishment. The paper also points out that the sequence of publication of different volumes of Das Kapital caused lacunae in interpreting Marx’s oeuvre. For instance Engels’ efforts made the third volume more accessible to readers but also obscured the overall pattern of Marx’s thinking. the article shows that Das Kapital was a dynamic and fluctuating project to such an extent that Marx himself several times revisited his views of the causes of economic crises and falling profits and also intended to deal extensively with ecological issues. Reaching an adequate understanding of the theory contained in Das Kapital cannot depend on the manuscripts of those volumes alone. Marx’s notebooks, which have only recently published, are an indispensable aid to understanding it.


2020 ◽  
Vol 12 (2) ◽  
pp. 203-227
Author(s):  
Kyriakos Tsantsanoglou

AbstractAfter preparing a detailed new edition of Sappho’s frr. 95 and 96 V., continuously transmitted in the parchment codex P. Berol. 9722, the author proposes that they constitute a ‘cycle’ of three homometric poems with a common theme articulated in successive episodes (i. 95, ii. 96.1–20, iii. 96.21–36). In the first, Sappho conveys her despair for her separation from her beloved pupils, Arignota being one of them. In the second, Arignota is presented in Sardis, where she excels among the Lydian women. She expresses a strong feeling of nostalgia for her stay in Lesbos with Sappho and for her beloved friend there, Atthis. In the third, Sappho addresses Atthis and, employing the mythological exemplum of Aphrodite’s love to Adonis and their distant meetings, declares that they will sail to the port of Geraistion in Asia Minor’s Aegean coast, whence they will travel to Sardis for meeting their old friend. The author also meditates on the possibility that the name Ἀριγνώτα (= ‘One-easy-to-be-known, Easy-to-identify’), is a renaming by Sappho of Ἀρύηνιc, the daughter of the Lydian king Alyattes, who is yearning to see her old teacher and her childhood girlfriend before her marriage to Astyages, son of Kyaxares, king of the Medes. The marriage was negotiated for ending a many years war between the two nations, a peace that coincided with the eclipse of the sun, usually dated on May 28, 585 BC.


2020 ◽  
Vol 499 (3) ◽  
pp. 3738-3748
Author(s):  
R H Østensen ◽  
C S Jeffery ◽  
H Saio ◽  
J J Hermes ◽  
J H Telting ◽  
...  

ABSTRACT The Kepler spacecraft observed the hot subdwarf star PHL 417 during its extended K2 mission, and the high-precision photometric light curve reveals the presence of 17 pulsation modes with periods between 38 and 105 min. From follow-up ground-based spectroscopy, we find that the object has a relatively high temperature of 35 600 K, a surface gravity of $\log g / {\rm cm\, s^{-2}}\, =\, 5.75$ and a supersolar helium abundance. Remarkably, it also shows strong zirconium lines corresponding to an apparent +3.9 dex overabundance compared with the Sun. These properties clearly identify this object as the third member of the rare group of pulsating heavy-metal stars, the V366-Aquarii pulsators. These stars are intriguing in that the pulsations are inconsistent with the standard models for pulsations in hot subdwarfs, which predicts that they should display short-period pulsations rather than the observed longer periods. We perform a stability analysis of the pulsation modes based on data from two campaigns with K2. The highest amplitude mode is found to be stable with a period drift, $\dot{P}$, of less than 1.1 × 10−9 s s−1. This result rules out pulsations driven during the rapid stages of helium flash ignition.


2015 ◽  
Vol 105 (4) ◽  
pp. 374-376
Author(s):  
Morteza Khaladj ◽  
Rose-Mary Mbibong ◽  
Nisha Shah ◽  
Ayesha Mohiuddin ◽  
Aqsa Siddiqui

Squamous cell carcinomas are often seen on the sun-exposed areas of the skin and are rarely observed on the digits of the foot. However, there have been incidences of squamous cell carcinoma developing in the presence of chronic wounds with osteomyelitis, thus complicating the treatment. We present a patient with osteomyelitis who developed invasive squamous cell carcinoma of the third digit. We conclude that wounds with osteomyelitis may have underlying pathologic abnormalities that are not obvious on initial presentation.


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