by Andrew B Collins

from AndrewCollins Website
 

Photograph of Cygnus X-3 taken by the Chandra X-ray Observatory in November 2000.
The horizontal line is thought to be an artefact of the image(Pic: (Credit: NASA/SRON/MPE).
 

Abstract

Cygnus X-3 is a high mass X-ray binary and microquasar, with a compact star, either a neutron star or a black hole, and a companion star, most probably a Wolf-Rayet (WN7 or 8) with huge mass loss and powerful stellar wind.

First observed in 1966 (Giacconi, et al, 1967), Cygnus X-3 has been monitored across multiple frequencies, from radio, infrared, optical, X-ray to gamma-rays.

It is one of the brightest galactic X-ray sources, and is the outright brightest during the production of bright radio flares, which can reach 20 Jy. Criticisms regarding Cygnus X-3 being a source of cosmic rays up to PeV (Meinels, personal communication, 11 July 2006) will necessitate a review of findings and theories since 1985.

I will review recent evidence of Cygnus X-3's production of relativistic jets, as well as speculation that its core might be a source of strange quark matter, producing exotic primary particles, with the H being a possible candidate.

 

1 - Introduction

Cygnus X-3 (RA 307.6 dec 40.8) has been identified as a source of ultra high energy (UHE) gamma-rays of an extremely energetic nature. Indeed, their initial discovery in the 1970s was responsible for a complete reassessment of particle acceleration in compact stars.

As early as 1973 the SAS-2 satellite reported gamma-radiation with a narrow phase interval of 4.8 h, noted separately in connection with x-ray and infrared observations of Cygnus X-3, estimated to be at 10 kiloparsecs (kpc, about 30,000 light years).

This periodicity is most likely caused by the eclipsing of the compact star by its companion (Hillas, 1984), since jet precession is now calculated to be in the range of 5 days (Miller-Jones, et al 2004).

Cygnus X-3 is also thought to be a sporadic 12.6 ms pulsar (Chadwick, 1985) with gamma-rays produced at or near the maximum (phase 0.6) in the 4.8 h X-ray cycle (Bowden et al, 1992).
 

2 - Cygnus X-3 as a gamma-ray source

The gamma-ray emissions in association with Cygnus X-3 are known to range between 35 and 200 MeV, although the COS-B satellite between 1975 and 1982 reported no radiation between 70 and 5000 MeV with the point-source signature of 4.8 h (Cordova, 1986).

Yet up to 1986 more than a dozen groups had reported the detection of gamma-rays from Cygnus X-3 with energies of at least 1011 eV. Gamma-rays in the higher range E> 1014 ev were subsequently reported and verified by ground-based collaborations in Germany, England, the United States, India and Italy (Cordova, 1986, and sources quoted).

The extremely energetic gamma-rays from Cygnus X-3 were early considered to be 'the products of interactions between even more energetic particles within the source, mainly protons', leading to speculation that Cygnus X-3 was 'the first astronomical object to be identified with reasonable certainty as a source of cosmic rays', i.e. any cosmic radiation above 108 eV (Cordova, 1986), or, indeed, a 'cosmic accelerator' (Dar, 1986).

Moreover, gamma-rays from Cygnus X-3 indicated that 'only a very small number of sources of like nature would be required to produce most of the observed high-energy cosmic rays.' (Cordova, 1986).

Among the suspected method of production of gamma-rays were two popular models.

Either they were protons accelerated by the electric field induced in the accretion disk held in the magnetic field of the compact star, or they were accelerated by shocks in the matter accreted on to a neutron star or black hole.
 

3 - Characteristics of Cygnet Primaries

Between 1983 and 30 October 1985 various ground-based air shower arrays, including Kiel (Samorski and Stamm, 1983a, 1983b) and Fly's Eye (the latter from 1981 through till 1988) reported extensive air showers with the direction and periodicity of Cygnus X-3 (See Marshak et al, 1985; Cassiday et al, 1989).

In Kiel's case, particles were detected in the 1016 eV range (initially assumed to be gamma-rays).

This was later confirmed (Lloyd-Evans et al, 1983) with the pulse being narrow (duty cycle 2%) and occurring at a phase 0.25 after the X-ray maximum. Thus it was concluded that Cygnus X-3 accelerated particles to at least 1016 eV, and that if these were electrons, then protons might reach a higher level still (Hillas, 1984). Indeed, at Kiel the EAS reached energies of > 1018 eV (Cassiday et al, 1989; Sommer and Elbert, 1990).

At the same time two underground nucleon-decay detectors set up originally to observe proton decay, Soudon (Marshak et al, 1985) and NUSEX (Battistoni, 1985, Baym, 1985), reported excessive muon fluxes either with a time modulation of the 4.8-h period of Cygnus X-3, or coincident to its daily transit.

The flux from single-muon events was greater than several orders than that expected from high energy photon flux, suggesting most probably either a primary of unique characteristics, dubbed the 'cygnet', or a new mechanism for very efficient muon production in high energy photon-initiated air cascades (Dar, 1986).

 

3.1 - Production of Muon Flux Deep Underground

Excess muon quanta reported deep underground (at a depth equivalent of 2 to 5 kilometers of water) produced an angular spread highly suggestive of the primaries interacting in the rock overhang down to a depth of a few hundred meters (Kolb, 1985, Ruddick, 1986).

This was confirmed by the differences in flux between the Soudon and NUSEX detectors, with the latter's flux being ten times less than the former, leading to the conclusion that this effect 'can only be explained by attenuation of the cygnet beam in the rock' (Ruddick, 1986). It also explained the zenith angles of the muons, which were similar to the background flux produced by EAS.

Furthermore, the underground muon energy measurements predicted a characteristic variation of the quanta according to depth, with detectors on the surface only being able to detect them at near the horizontal, due to the large interaction length of the primaries.

This meant,

'such detectors would have to be very large to detect a signal' (Ruddick, 1986).

4 - Cygnet Identification

Identification of the relativistic primaries (Ruddick, 1986) responsible for these signal events has proved extremely difficult, highly controversial and even questionable (Thomsen, 1986).

The enhanced muon flux recorded, particularly by the Soudon I group, was far too high for them to be gamma-rays, which produced a mere 1/300 of the muons (µ-mesons) characteristic of the reported muon excess (Baym, 1986).

Their 4.8-hour periodicity meant that they had to have travelled in a more or less straight line at relativistic speeds, otherwise a spread of lower velocities would have washed out the signal. Clearly, the path of the cygnets was not curved by the galactic magnetic field, otherwise this would have randomized or deflected their arrival directions (Dar, Lord and Wilkes, 1986).

The fact that the cygnets produced excessive muon (µ-mesons) quanta, implied that they acted to produce hadron-induced cascades. In other words, they were strongly-interacting particles, rather than electromagnetic particles, like gamma-rays or weak particles such as neutrinos (Dar, Lord and Wilkes, 1986).

Further evidence against them being neutrinos was the fact that the cygnet-produced muon flux increased when Cygnus X-3 was overhead, and faded when it was not in view, the so-called 'horizon effect'. This is not a characteristic of neutrinos, which do not interact in this manner.

Thus the conclusion was that cygnet primaries, either measured in ground-based air shower arrays or in underground detectors, were long-lived neutral particles with energies anything up to at least PeV (Kolb, 1985; Maiani, 1985; Berezinsky, Ellis and Ioffe, 1986; Cordova, 1986; Ruddick, 1986; Cassiday et al, 1989; Czapek et al, 1990). However, the only obvious candidate was the neutron, which is unstable to beta decay and has a half-life of approximately 10-15 minutes. Thus the only way that they could have reached the earth was by travelling at relativistic speeds.

Quashing this possibility was the fact that it would require neutrons with 100 times the energy of the monitored cygnet events. Neutral atoms could be eliminated since their electrons would have been stripped away by the 5g per cm² interstellar hydrogen, causing their decay long before they ever reached the Earth.

This is unless they had an incredibly high energy in the range of 10¹⁸ eV (Baym, 1986). As already noted, the Kiel collaboration did indeed register EAS with energies >10¹⁸ eV.

Initial findings strongly indicated that the cygnet primary bore the following characteristics:

1) no electric charge

2) no magnetic charge

3) a rest mass estimated to be between zero and 1/20 of a proton mass, and less than its energy by a factor of around 10⁴ (Baym, 1986; Ruddick, 1986)

4) it was strongly interacting, in that it was hadron-inducing

5) it possessed a half-life relative to its assumed passage at relativistic speed. Protons, neutrons, nuclei, atoms, and micrograins of ordinary matter could all be ruled out

The cygnets were not charged cosmic particles since they are affected by the galactic magnetic field which randomizes their directional flow and ruins any chances of ascertaining their astronomical source, which can only be determined if they correlate with activity in other frequencies that might contain a known periodicity or direction.

Since neutral primaries arrive directly from source without being affected by the galactic magnetic field, they are crucial to determining the original trajectory of any cosmic ray. Gamma-rays are neutral, and so can also arrive directly from source, why we can trace the astronomical source of GRBs.

Thus in order to determine point sources of cosmic rays it is better to examine neutral particles, which retain their primary trajectory across the galaxy and when travelling at relativistic speeds will also retain their unique signature, which has been the case with Cygnus X-3 and Hercules X-1.

Indeed, as long ago as 1983 it was suggested that 'since the galactic magnetic field seems sufficient to randomize all charged particles during their long flights through space, pristine cosmic rays may not be charged particles at all.' (See Hecht and Torrey, 1983).

A study of the five strongest recorded UHE cosmic ray events (E>10²⁰ eV) by Farrar and Torrey (1998) led to the conclusion that their trajectory pointed back to extra-galactic QSOs (quasar stellar objects) with a margin of error of 0.005.

In order that the primaries do not violate the Greisen-Zatsepin-Kuzmin (GZK) cutoff for distance travel of a photon or nuclei, they saw them as long-living, neutral hadrons of a possible exotic nature (Farrar, et al, 1998).

 

5 - Cygnets and Strange Quark Matter

As far back as the mid 1980s it was proposed that cygnets were exotic hadrons resulting from strange quarks produced in strange quark matter in the core of Cygnus X-3.

Maiani (1985), for instance, noted the observation of 'very energetic particles' arriving from Cygnus X-3, with estimated energies up to 10⁴ TeV, as well as the observation underground of high energy muons correlated with a 4.8h modulation.

He also accepted that poorer statistics might have been behind why other collaborations failed to register these increased muon fluxes underground, such as FREJUS and HPW. The primaries, he suggested, could be photons, which produce high energy showers in the atmosphere, and might well explain underground muon fluxes like those observed by Soudon and NUSEX. Yet results from these collaborations showed an increased muon flux too high for photons to be the simple answer (Dar, 1986).

In contrast to Kolb and Ruddick, Maiani saw an anticorrelation in the reported muon flux versus the depth of the traversed rock, and the fact that NUSEX results were less than Soudon I.

This was evidence, he felt, merely of the 'absorption effect' (Maiani, 1985).
 

6 - Strange Matter

Kolb (1985) asserted that quark nuggets might lead to an enhancement in muon production over normal nuclear matter, yet even then only by a factor of two.

He additionally considered the R-odd particle from super-symmetry and also the H-particle, after Jaffe. This last cited he saw as having a lifetime long enough to reach the earth, because of its double beta decay. Moreover, it bears four of the main characteristics of the proposed cygnet, although whether it can produce the enhanced muon flux depended upon its method of production.

Despite this, the mass of the H, might not be low enough, something that only experimentation could determine. Even if the mass was close to that of the cygnet, the muon flux would be smaller than that reported.

Moreover, the H cannot account for the angular spread of the underground muon flux. For instance, the NUSEX signal was seen coming from a 10 degree by 10 degree window in celestial coordinates, larger than the 0.5 degrees expected for an angular resolution.

Baym (1986) likewise proposed that the cygnet primary was the theorized H particle. Should its mass be less than that of the lambda (?) (1.1¹⁶ GeV) plus that of the neutron (0.938 GeV), then it was possible that the lifetime of the H could be sufficiently long for it to be the cygnet primary, since it would not undergo the rapid decay into a single lambda or neutron.

Wilk and Wlodarczyk (1996) acknowledged 'anomalous cosmic ray bursts from Cygnus X-3' as the result of strange quark matter existing in its presumed neutron star (Wilk and Wlodarczyk, 1996). This supposition was explored further by Rybczynski, Wlodarczyk and Wilk (2004).

In similar to Kolb and Baym, Weber (2005) saw further support for the existence of strange matter in Cygnus X-3, which he speculates produces cosmic rays that to arrive as point-source signal events means that they have to be 'electrically neutral', like the cygnet primaries.

Acknowledging their main characteristics, he confirms also that to survive the trip from Cygnus X-3 such particles are 'long-lived'. In his opinion, the 'only known particle which can quantitatively satisfy this constraint is the photon'.

This is despite the fact that, as he states, they would only produce air showers with a 'small muon component'.

Weber goes on to predict that the 'natural candidate' for the cygnet is the H particle. Their potentially long lifetime means that they 'may be present as components of existing neutral particle beams' (Weber, 2005). Yet in order to give it long life, it would need to have 'mass below single weak decay stability'. Furthermore, in order to generate enough H particles, the source would have to be a strange star.

Weber admits that the problem with Cygnus X-3 is that,

'it is accreting mass and thus has a crust, such that there is no exposed strange matter surface where small strangelets could be produced and subsequently accelerated electrodynamically to high energies into the atmosphere of the companion star where H particles were created via spallation reactions.'

(Weber, 2005)

Yet other evidence of strangelets in balloon-borne counter experiments, air-shower arrays and large emulsion chambers has convinced Weber that,

'some primary cosmic rays may contain non-nucleus components which generate extended air showers that contain both a large number of muons as well as very high energetic photons', with Cygnus X-3 being a unique candidate.

7 - Cygnets, Neutrons and Relativistic Flow

The idea that cygnet primaries are the result of exotic nuclei within Cygnus X-3's compact star being accelerated towards the earth is based on the view that they interact as hadrons to induce cascades uncommon to the normal production of muons in the atmosphere.

However, should it be shown that the particles travel at relativistic speeds and thus contain considerably higher energies than previously reported, then they might be explainable in more conventional terms.

Soudon reported that the muon excess from Cygnus X-3 was coincident to major radio flares (from 0.1 mJy up to 20Jy), which have themselves occurred coincident with X-ray and infrared observations (Baym, 1986). Moreover, gamma-rays with the 4.8 h periodicity of Cygnus X-3 monitored by ground-based air arrays have also coincided with considerable excess muon flux underground as mentioned earlier.

Sommers and Elbert (1989) examined the evidence for EeV neutrons and/or photons from Cygnus X-3, based on the Fly's Eye data, and stated that 'because of synchroton radiation losses, EeV particle acceleration cannot occur gradually while a particle orbits in a strong magnetic field.' As a consequence, Sommers and Elbert suspected that 'if particles are accelerated in a neutron star's magnetosphere, some type of linear accelerator must be responsible (my italics)'.

Accepting that the cosmic rays from Cygnus X-3 are neutral, since charged particles would be dispersed by the galactic magnetic field at EeV energies, the question remains of how neutral particles might be produced by accelerated charged particles.

According to Sommers and Elbert, the range of possible models for the production of EeV neutral particles 'is greater than the range considered for the production of 10¹⁵ eV neutral particles from Cyg X-3. This is partly because the EeV neutral particles can be neutrons as well as gamma-rays' (Sommers and Elbert, 1989).

Crucially, Sommers and Elbert go on to state that 'although free neutrons decay with a mean proper lifetime of 898 seconds', time dilation allows some neutrons at these energies to travel the distance from Cyg X-3. On this basis, the energy threshold (0.5 EeV) for the data used in the Fly's Eye analysis suggests that the reported increased muon flux could be neutrons, even though the collaboration was at the time unable to distinguish between a neutron-initiated shower and a gamma-ray shower (Sommers and Elbert, 1989).

In final conclusion, they stated that 'Cyg X-3 is a strong source of EeV cosmic rays'.

The significance of Sommers and Elbert's proposal is that with a relativistic linear acceleration through jet production, the view that cygnets are exotic strange quark particles becomes unnecessary.

The neutral particles might indeed be neutrons, reliant on a new model based upon synchrotron radiation loss through relativistic flow.

Cygnus X-3 during its major radio flare

in September 2001 (after Miller Jones, et al, 2004).

A one-side relativistic jet was observed in association with radio flare activity in Cygnus X-3 by Mioduszewski, et al (2001) using the VLBA in February 1997.

It was estimated to have an opening angle of 12 degrees, and a small inclination angle of > 12 degrees towards the Earth, leading to the conclusion that it constituted the galaxy's first blazar.

A precessional phase of 30 days with an anticlockwise movement was also noted in association with jet production. These parameters were comparable with those obtained during the observation in September 2001 of a separate major radio flare by Miller-Jones, et al. (2004) using the VLBA over a period of six days following a peak outburst.

The southern jet was estimated to be moving within 10.5 degrees to the line of sight, with a precessional phase in a clockwise motion of 5.3 days. The northern jet was weakly observed.

Clearly, the implication was that both the precession cycle and the direction of the jets had shifted between 1997 and 2001. Through extrapolation of the jet motion back to source Miller-Jones estimated that the jets were ejected about 2.5 days after the radio brightness of Cygnus X-3 began to increase.

Overall the parameters of the southern jet have been found to be consistent with what Mioduszewski et al. had previously observed.

Bipolar jets were also observed in October-November 2000 using the VLA and examined by the NRAO (Marti, et al, 2002), although whether or not these were a separate mechanism to the observed north-south orientated jets observed in 2001 has still to be decided.

The speed of Cygnus X-3's suspected one-sided jet was originally estimated at 0.35c (Cordova, 1986). More recent assessments of the relativistic jets following the 1997 VLBA observations by Mioduszewski, et al (2001), provided a revised speed up to 0.81c, while Miller Jones, et al, following the 2001 observations concluded that the rate was 0.63c. Yet they accepted that faster speeds could precede the observable appearance of the series of bead-like knots marking the whereabouts of the jets; see also Hannikainen, et al (2003, poster) for further discussion on this subject.

Such speeds might be enough to enable short-lived neutrons to reach the Earth, indicating a realistic process for the arrival of low-mass neutral particles, and the possible production of increased air showers and underground muon quanta from Cygnus X-3.

It has been pointed out that an observed velocity of Cygnus X-3s jet at a maximum of 0.81c would be too slow to compress time so that neutrons might have time to decay into protons (Meinel, private communication, 11 July 2006).

The 0.81c for the speed of Cygnus X-3s southern jet for the February 1997 observations (Mioduszewski et al, 2001) is based on estimates of jet motion in radio flaring, and does not necessarily relate to the initial velocity of ejecta on all frequencies.

Moreover, it is clear that the speed of the jets change, as is seen in the 2001 observations, where a velocity of just 0.63c was deduced (Miller-Jones, 2004).

Earlier estimates of jet speed were even lower. Moreover, the bipolar jets monitored by the NRAO using the VLA in 2000 (Marti, et al, 2001) determined that they had an infrared speed of just 0.48c, which is much slower than the higher speed radio flares. Thus there is no reason why UHE and HE cosmic rays and gamma-rays from Cygnus X-3, or indeed any point source, might not exceed the velocity speed of radio flares.

Signal events from Cygnus X-3 which feature the arrival of GeV gamma-ray emissions and hadron-like neutral particles have coincided with intense bursts of energies across multiple frequencies during the production of jets. For instance, this occurred in October 1985 when an increased muon flux at PeV levels coincided with intense bursts of radio emissions (Berenzinsky, 1988).

In addition to this, there was a correlation between the excess muon flux recorded by the Soudon II deep underground experiment between 1991 and 2000 and Cygnus X-3's production of large or intermediate radio flares (Thomson, 1991; Marshak, 2000; Allison, 1999).

Thus there is every reason to conclude that the production of gamma-rays and long-lived neutral particles in Cygnus X-3 might well be the result of narrow, magnetically driven relativistic jets within a small angle of the Earth.

NRAO image showing the production

of bipolar jets by Cygnus X-3 in October-November 2000

(pic: NRAO/AUI) .
 

8 - Some Criticisms of Cygnus X-3 as a Cosmic Accelerator

It has been suggested that the cone angle of Cygnus X-3 poses a problem regarding any working model for it being a cosmic accelerator in its role as a blazar.

In order to send cosmic rays in the Earth's direction with the solar region being significantly inside the limit to the probability distribution has been estimated to be about 0.5 radian (Meinel, private communication, 11 July 2006).

Work has yet to be undertaken on this level, and the recorded data from both particle physics and astrophysics needs careful evaluation in this respect. Much of the findings cited from the 1980s of long lasting neutral particles from Cygnus X-3 has largely been ignored. This is a shame, for it clearly suggests that Cygnus X-3 possesses an extraordinary acceleration mechanism for the production of cosmic rays.

As we have seen , their appearance correlates well with radio flaring and hard X-ray outbursts. Nothing has so far been published on any possible correlations between cygnets and major radio flaring during the years 1997, 2000, 2001 and 2006.

The question with regards Cygnus X-3 is not whether it can accelerate out cosmic rays and UHE gamma-rays, but how exactly they might be produced. In my opinion, it is the production of relativistic jets, or shock waves in association with their production, that remain the best mechanism for their production, something predicted by Sommers and Elbert as far back as 1989.

What is important about this and other similar conclusions during the 1980s is that there was no hard data available then suggesting that Cygnus X-3 might be a blazar. This came only through the February 1997 observations (see Mioduszewski, et al, 2001), and confirmed during the 2001 observations (Miller-Jones, et al, 2004).

In other words, working models for the acceleration process of cosmic rays from Cygnus X-3 were shown to be correct, making the evidence of long-lasting neutral particles originating from here an extremely likely possibility.

What is more, they have continued to be reported. Soudon II, announced in 1999 that in its first ten years of operation the collaboration had regularly tracked excess muon events in the Tev range or above from the direction of Cygnus X-3, and again in 2000 (Marshak, 2000). There is every likelihood that cygnets are accelerated from source during jet production, and that at such energies only stable, neutral particles can travel the 10 kpc distance from Cygnus X-3 to the earth 'along trajectories which point back to the source' (Allison, 1999).

Moreover, the Soudon II collaboration conclude that since known stable neutral particles - photons and neutrinos - have only small probabilities of producing detectable muons,

'Tev muons associated with Cygnus X-3 requires either exotic interactions of known primaries, exotic primaries or very large fluxes of neutrinos or photons'.

(Allison, 1999)

9 - Conclusions

Despite the Soudon and NUSEX observations of an increased muon flux underground during the 1980s remaining controversial, there exists good evidence for the existence of long-lived, low-mass, strongly-interacting neutral primaries from Cygnus X-3.

Exotic primaries have been proposed to explain the reported EAS and increased muon flux underground, with strange quark matter from a strange matter compact star, most likely a neutron star, being currently the most popular model.

However, with the introduction of a relativistic flow for the acceleration of the neutral primaries, it is possible that cygnet primaries are simply neutrons.

Regardless of this, the idea of them being produced within neutron stars by strange matter remains an attractive theory, and exploration into this area of astrophysics is to be encouraged.

It is ironic that the absence of a well-defined mechanism of production of these neutral primaries, along with their erratic data, has diminished the impact of these extremely important findings, which arguably hold the key to determining the first confirmed point source of galactic cosmic rays.

 

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