Artist's impression of the occulting object that passed in front of KIC 8462852 on Kepler Day 792 (Copyright: Russell M. Hossain, July 2017).
* UPDATED JULY 08, 2017 *
8462852- The Incredible Story of Tabby's Star and the Growing Mystery of its Cyclic
Andrew Collins and Rodney Hale
KIC 8462852, popularly known as Tabby's Star or, more correctly, Boyajian's Star after its discoverer astronomer Tabatha S. Boyajian, is an F-type main sequence star, one and a half times larger than the Sun. It lies around 1,280 light years (390 pc) away in the constellation of Cygnus, the swan, at coordinates RA.: 20h 06m 15.457s Dec.: +44° 27" 24.61' (see fig. 1.1). It has been called the "weirdest star in our galaxy" (Andersen, 2015) due to the strange fluctuations in light it has experienced since it first came to the attention of the astronomical community following the completion of the Kepler space mission's initial phase in 2013.
Various theories have been proposed to explain KIC 8462852's curious light fluctuations. Tabatha Boyajian and her colleagues, following a detailed study of the Kepler data, concluded that a swarm of exo-comets in a highly eccentric orbit following a single previous breakup event might be the cause (Boyajian et al, 2016). A team led by Fernando J. Ballesteros of the University of Valencia considers them the product of a giant ringed planet, five times the size of Jupiter, along with a large cluster of Trojan asteroids in the same or a similar orbit (Ballesteros et al, 2017). Brian Metzger of Columbia University and his colleagues propose that the star is recovering from a collision with an orbiting planet (Metzger et al, 2017), while Valeri V. Makarov of the United States Naval Observatory identifies the culprit as liberated planetary debris in the interstellar medium between here and the star (Makarov, 2016). In a similar vein, I. I. Katz proposes that the light dips are simply a combination of the Kepler space telescope generating false cyclic data based on its repeated observation of circumstellar rings in our own solar system (Katz, 2017). Jason Wright of Penn State University, on the other hand, has proposed that the star's dimming episodes could be the result of alien megastructures in orbit around the star (Andersen, 2015; Wright and Sigurdsson, 2016), while Eduard Heindl of Hochschule Furtwangen University argues that the occulting objects orbiting KIC 8462852 are artificial and involved in a long-term mining or "star lifting" operation to remove the star's mass (Heindl, 2016).
Figure. 1.1. The Cygnus constellation showing the location of KIC 8462852 (Credit: Stellarium/Rodney Hale).
of the Kepler Data for KIC 8462852
In an attempt to throw further light on the matter, one of the authors, Rodney Hale, examined the Kepler data for KIC 8462852 with the intention of physically modelling the transiting object or objects seen as responsible for the four biggest light dipping episodes. The first of these occurred on Kepler day 792 (henceforth D792), corresponding to March 5, 2011 (see fig. 1.2 for a listing of all the major dipping events recorded by Kepler between 2009-2013 and fig. 1.3 for their photometry). On this occasion the light dipped by a maximum of 16 percent. The second event took place on Kepler day 1519 (D1519), corresponding to February 28, 2013, when the light dipped by as much as 22 percent. The third occurred on Kepler day 1540 (D1540), corresponding to March 21, 2013, when a dip of 3.3 percent was reported. The last major light dipping episode occurred on Kepler day 1568 (D1568), corresponding to April 17, 2013. On this occasion the resulting light curve showed that the star's flux had dipped by a maximum of 8 percent.
The D792 event would appear to have involved just one main occulting object. This passed in front of the star, causing a slow gradual dip before the flux dropped sharply by a maximum of 16 percent (see fig. 1.4 for the photometry of all four major dipping events). Thereafter it took the star a few days to recover its normal brightness. The other three events would all appear to be linked in some manner. They occurred across a period of approximately 40 days during which time the star's light fluctuated not only with the three major dips cited above but also with a succession of minor dips, suggesting a more complex series of events involving several occulting objects.
Figure. 1.2. List of the major dimming events recorded in the Kepler data for KIC 8462852 between 2009 and 2013.
Figure 1.3. The photometry from the Kepler data for KIC 8462852 from May 1, 2009, through till May 11, 2013. The D792, D1519, D1540 and D1568 dates are all marked.
Figure. 1.4. Photometry of all four major dimming episodes for KIC 8462852 as recorded in the Kepler data.
Before any physical modelling of the objects could begin it was essential to establish whether or not the cause of the light dimming events existed independently of the star. For this Hale focused his attentions on the 0.88-day fluctuations first reported in connection with KIC 8462852 by Tabatha Boyajian and her colleagues (Boyajian et al, 2016). A Fourier analysis of the data reveals much the same as their own results with two separate sets of harmonics present (see fig. 2.1). The data was expanded at the low frequency end so that the main peaks with the days per cycle could be highlighted. This shows that the 0.88-day periodicity is in actuality a clump of frequencies close together (see fig. 2.2). In addition to this, we see that the 0.88-day fluctuations adhere to a larger cyclic pattern of approximately 11 days, a 10.7- and 13-day cycle having previously been recognised.(1)
confirmation of the 0.88-day periodicity is easily obtained, Valeri Makarov argues
that it could be interference from a nearby star (Makarov et al, 2016), a theory
unsubstantiated at this time. More likely is that it defines KIC 8462852's rotational
pattern, the conclusion of Boyajian and her colleagues (2016).
Figure 2.1. Fourier analysis of KIC 8462852's 0.88-day cycle.
Figure 2.2. The Fourier analysis expanded to show the clusters of close frequencies at approximately 11-day intervals.
Using the Kepler data(2) Hale was able to demonstrate how regularly occurring changes of light levels across the entire four-year period of observation of the star can be shown as a spectrogram, with its base line covering the entire period of observation of KIC 8462852 and its vertical scale indicating the cyclic frequency of light level changes (see fig. 2.3).
2.3. Spectrogram showing the cyclic fluctuations and dimming episodes recorded
in the Kepler data for KIC 8462852. The random light grey peppering of the area
of the plot comes from a general background of noisy signals. Persistent signals
with a regular repeating pattern show up as darker horizontal bands, while short-term,
larger changes show as narrow vertical bands. Although difficult to reproduce
in printed form, the 0.88-day fluctuation represented by the thick horizontal
line at the base continues unabated during all the major dimming events represented
by the vertical lines.
The spectrogram's lowest horizontal band indicates KIC 8462852's 0.88-day fluctuation, equivalent to a rate of approximately 1.14 cycles per earth day. The two bands above it are second and third harmonics of this fluctuation. The significant fact gleaned from this exercise is that the lowest band representing the 0.88-day fluctuation continues without interruption throughout the entire duration of Kepler's observation of the star, even during the major dimming events. This implies two possible scenarios. Either the 0.88-day periodicity is unconnected with KIC 8462852 and is, as Valeri Makarov suggests, simply interference from a nearby star, or the 0.88-day fluctuation is reflective of an orbital periodicity connected with the star itself. If it does represent a rotational cycle, this raises the question of what exactly is causing this 0.88-day fluctuation. It cannot be sunspots as these occur randomly, and not in the same position time after time. The only logical explanation is that the fluctuations signify either a periodic light dimming on the star's surface, or they relate to something in low orbit around the star.
Whatever the cause of the 0.88-day fluctuation seen in connection with KIC 8462852, the fact that it continues unabated during the light dipping episodes means that the occulting objects responsible for the star's major light fluctuations are most likely independent of the star itself for if they were a product of the star there is a strong likelihood that the cycle would be interrupted in some way. Thus either the occulting objects causing the light dimming episodes belong to liberated planetary material existing in our line of sight between here and KIC 8462852, the conclusion of Valeri Makarov (2016), or they are in orbit around the star.
A Further Periodicity
these two alternatives, the second can be shown to be more plausible. Tabatha
Boyajian and her colleagues noted a second possible periodicity in the Kepler
data for KIC 8462852 based on the timing between several major and minor dimming
events. They seemed separated by periods of 48.8 days, later refined to 48.4 days,
with the presence also of a half cycle of 24.2 days (Boyajian et al, 2016, gdsacco
(3), and see section 4.2 of this study). An inter-relationship seems to exist
between these various periodicities since 48.4 days is exactly 55 cycles of 0.88
days, while a half cycle of 24.2 days amounts to 27.5 periods of 0.88 days.
under the assumption that the objects creating KIC 8462852's major light fluctuations
are indeed in orbit around the star, what exactly might they look like? Having
established that the occulting objects responsible for KIC 8462852's light fluctuations
were almost certainly transiting the star, Hale looked at how solid objects of
different shapes affect the appearance of resulting light curves. To achieve this
he created a computer simulation showing a dark shape transiting a white disk
representing the star. The output from a photocell monitoring the light level
from the computer screen was recorded and plotted by a second computer, thus comparisons
between light curves arising from different shapes were readily made. The transits
may be equatorial (as viewed from earth) or at higher latitudes (see Hale, 2016).
Hale found was that transiting objects with regular shapes of appropriate sizes,
including spheres, squares, triangles, etc., produce a characteristic light curve
with a flat base (see fig. 3.1). This was completely unlike the sharp dips produced
in connection with KIC 8462852. To create a light curve with a pointed tip the
object has to have a diameter matching the star's width at the particular latitude
of the crossing, as well as a thickness to produce the relevant light drop.
the similarity between the four major dips reported in connection with KIC 8462852,
Hale superimposed all four together, keeping their scale yet synchronizing them
in a manner corresponding to their lowest point. The resemblance in sharpness
and form of all four is remarkable and is unlikely to be without meaning (see
fig. 3.2). In addition to this, when five minor dipping events found in the Kepler
data for KIC 8462852 were synchronised these also displayed a similar width and
sharpness (see fig. 3.3). Not one of these dips, whether major or minor, display
a characteristic flattened base.
Figure 3.1. Transiting objects with regular shapes, such as spheres, squares, triangles, etc., produce a characteristic light curve with a flat base when they pass in front of a star (appropriate to the amount of dimming observed), while those with elliptical profiles create light curves with characteristic narrow tips.
Figure 3.2. The sharp tips of all four major light dips recorded in the Kepler data for KIC 8462852. Note the similarity in their narrow tips.
Figure 3.3. The sharp dips of five minor events as extracted from the Kepler data for KIC 8462852. The day 261 event has some missing data.
Figure 3.4. The profiles of the D1519 event as determined from the physical modelling of the Kepler data for KIC 8462852. It shows that at least three occulting objects were responsible for this light curve, all of them ideally either elongated ellipses, disks in profile, or rotating irregular shards.
Hale determined that one basic shape profile corresponded closely with the resulting light curves seen in the Kepler data for KIC 8462852. This was either an ellipse with a flat base and top or a slim disk seen edge on. A similar profile could also be created by an irregular shard, which if rotating along the line of sight as it transited across the face of the star would average out its profile to create the impression of an ellipse or disk. Hale was able to apply this information to Kepler event D1519 to demonstrate that it could have been caused by three elongated ellipses, disks or rotating shards of irregular shape (see fig. 3.4). Similar objects could be seen to be behind the D1540 and D1568 events (see below for more on the physical modelling of the D1540 event).
3.2. Modelling the D792 Event
Reconstructing the obscuring object that created the D792 light curve was more difficult since this had to include the long, slow gradual dips that occurred before and after the sharp dip of 16 percent. These can only be explained by something extremely long and thin crossing in front of the star's face both before and after the appearance of the main object. Arguably they are dust trails. Whether or not they extend behind and in front of the main occulting object, showing they are in fact rings, is unclear from the data.
Some indication of a ring around an ellipse or disk-like profile is shown in two events, D1540 and another minor dip on Kepler day 1206 (D1206). Rodney Hale overlaid these two events to show their close relationship(see fig. 3.5).
Figure 3.5. Photometric comparison between two light dipping events in the Kepler data for KIC 8462852, one a major event, D1540, and the other a minor event, D1206. Note that both have shallow depressions on either side of the main dip, suggesting the presence of a ring surrounding an ellipse or disk-like object.
can be seen to have a shallow depression either side of the main object, suggesting
the presence of a ring. This tells us that the extremely long trail seen during
the D792 object's ingress and egress is either an incredibly large ring seen almost
along the line of sight, or it is some kind of twin trail, one perhaps a dust
tail and the other an ion tail. The only argument against the identification of
these anomalies as either rings, trails, or tails is that they would most likely
re-radiate heat and so should be visible within the IR frequency range, something
so far not noted in connection with KIC 8462852 (Boyajian et al, 2016).
The profile of the occulting object behind the D792 episode indicates that, like those of the D1519 event, it too bears a profile consistent with an ellipse showing a flat top and bottom. Equally, it could be a disk viewed edge on, or, once again, an irregular shard rotating along the line of sight. Hale has provided a black and white image showing the profile of the D792 object complete with its "wings" (see fig. 3.6). Accompanying this study also is an artist's impression of what the D792 object might have looked like as it transited the star during its ingress and egress (see fig. 3.7), while at the top of the page is artist Russell M. Hossain's impression of this object based on the findings of this story. This painting is, however, for promotional purposes and is not meant to reflect an exact representation of KIC 8462852's occulting objects.
Figure 3.6. The profile of the D792 event as determined from the physical modelling of the Kepler data for KIC 8462852. The extending "wings" have been severely shortened to better show the object's profile.
clearly the elliptical or discoid profile of the occulting objects almost rules
out the possibility that the D792 event was caused by the transit of a giant-sized
planet. As we have seen, a round object like a planet would create a light curve
with a characteristic flat bottom, and that is certainly not what we see in the
case of D792. It remains possible that the object is a large planet surrounded
by enormous rings, which we see at a slightly up-tilted or down-titled angle of
anything up to 45º. Their presence would give the impression that the object
has a strong elliptical profile. However, the idea that three such planets, all
with enormous rings tilted at an angle, transited the star one after the other
during the D1519 event stretches the imagination indeed. That the occulting objects
are either swarms of exo-comets or large clusters of Trojan asteroids does remain
possible. Yet accurately modelling such hypothetical swarms or clusters of objects
from light curves alone is practically impossible.
3.7. Suggested ingress and egress of the D792 event's occulting object against
the background of a star. Not to scale.
said this, the elliptical or perhaps discoid appearance of the occulting objects
certainly does not rule out a more exotic explanation to the dimming episodes.
Ellipses or slim disks (although not irregular shards) might well conform to the
appearance of artificial structures contained within clouds and/or rings of dust.
What is more, since we see only part of a disk it could be re-radiating its waste
heat in a non-isotropic manner. In other words, it could be directed, whether
purposely or otherwise, away from our line of sight, a possibility acknowledged
by Jason Wright.(4) This could explain why no significant IR excess has been detected
in connection with Boyajian's Star's light dimming episodes.
The Probability of Recurring Cycles
A better understanding of the nature of the occulting objects passing in front of KIC 8462852 might be forthcoming from a deeper examination of the cyclic fluctuations recorded in connection with the star. As previously noted, a full cycle of 48.4 days and a half cycle of 24.2 days(5) have been observed to separate various minor and major light dimming episodes. For example, it was noted that the gap between the D792 and D1519 events was 726 days, the equivalent of 13 x 48.4 day cycles, or 26 x 24.2 days, while the gap between the D1519 episode and the D1568 event was approximately 48.4 days, or 2 x 24.2 days(Boyajian et al, 2016).
Jason Wright and Steinn Sigurdsson examined the six deepest dipping events (cited by them as Kepler days 261, 793, 1206, 1496, 1523, and 1568) and observed that they "all fall within a narrow range of phases when folded at a period near 24.2 days, suggesting a close-in orbital period (Wright & Sigurdsson, 2016)." In order to check the statistical probability of these results, 2,000 periods from the Kepler data were evenly sampled in frequency between 10 and 700 days. They then repeated the exercise using 10,000 mock sets of six dips with times randomly drawn from a uniform distribution with the same range as the Kepler time series. Results showed that the apparent periods of 24.2 days between the six deepest dips were without any statistical significance.
Testing the 24.2-day half cycle
check these findings, Rodney Hale used the Kepler data to create a graph with
a time scale of 24.2 days per unit beginning with the first recorded dipping event
on day 140 (D140), a date corresponding to May 21, 2009 (see fig. 4.1). This then
became "day" zero. In this manner a significant number of minor and
major dips can be seen to line up almost perfectly with complete "Dip Days."
More significantly, this trend does not simply apply to the dimming events recorded
in the Kepler data. It is extended beyond the two years between 2013 and 2015,
where no data was available, to embrace two new dimming events, the data for which
coming from Bruce Gary, an astronomer who has been monitoring the star's light
fluctuations since October 2015.(6) The first of these occurred across a course
of several days in May 2017 (the so-called "Elsie" dip), with a maximum
drop of two percent recorded on May 19. The second began on June 13 and reached
a two percent drop in flux on June 17. Of these, only the June 17 event corresponds
to the 24.2-day cycle, falling around one day before Dip Day 122. The Elsie dimming
event in May was askew of Dip Day 121 by approximately 10 days, thus showing no
correlation to the pattern.(7) The June dip has continued at approximately 0.5
percent below normalised flux levels through into the first week of July. This
and further dips will continue to be monitored to see their possible relationship
to the star's 24.2- and 48.4-day periodicities.
Figure 4.1. Graph showing the relationship between KIC 8462852's 24.2-day cycle and all major light dimming events since 2009. The graph starts with the first dip seen in the Kepler data, D140, corresponding to May 21, 2009, which we shall call Dip Day 0. It then counts forward in periods of 24.2 conventional days, i.e., Dip Day 10 would be 242 conventional days later. The graph then continues counting past Kepler's last day, May 11, 2013, to include Bruce Gary's data from May 1, 2017 onwards, which corresponds, sequentially, to Dip Days 121 to 122.
How exactly light dipping events can synchronize so perfectly with periodicities associated with KIC 8462852 is an enigma in itself. Naturally occurring astronomical objects such as swarms of comets, clusters of Trojan asteroids, or trails of dust and debris, are extremely unlikely to order themselves into regular groups that appear on cue at the culmination of cyclic periods of either 24.2 days or 48.4 days. Their appearance would surely display a chaotic randomness that precludes the idea of regular gaps between light dipping episodes. It is unlikely also that we are seeing the same objects coming around and around again on an orbital period of 24.2/48.4 days since their size and appearance differ so greatly from one event to the next.
In addition to this, and as noted in Section 2.2, a clear relationship exists between Tabby's Star's cyclic periodicities of 48.4 and 24.2 days and its 0.88-day fluctuations, the former being exactly 55 cycles of 0.88 days, the latter being 27.5 cycles of 0.88 days. Not only do these figures appear to confirm that the 48.4-day periodicity can be seen as one whole cycle with the 24.2-day periods as half cycles, but they also tell us there is a close relationship between all three of these periodicities, the higher values synchronizing very well with the 0.88-day cycle. Having said this, if the star's 0.88-day drops in flux are indeed rotational in nature, then it seems unlikely that the occulting objects causing the light-dimming events would time their transits to conform to pre-existing 24.2-day and 48.4-day periodicities.
Yet having discounted the idea that the dimming episodes are occurring on the star itself, this leaves us with a puzzling conundrum. What type of objects can cause such carefully spaced light dimming events? Their clear cyclic behaviour makes them seem almost mechanical in nature, like cogs of different sizes turning inside an old clock.
Such surmises lend weight to the possibility of an artificial solution to the light dimming events connected with KIC 8462852. What is more there appears to be something almost contrived about the manner the four main periodicities associated with the star can be shown to synchronize with the earth's solar cycle.
Cyclic Number Sequences
KIC 8462852's recorded periodicity of 0.88 days synchronizes with the earth's solar calendar every 22 days. Its 24.2-day cycle coincides with earth days every 121 days, while its 48.4-day cycle synchronizes with the earth every 242 days. The independent importance of a 242-day cycle seems confirmed in the knowledge that the 726-day period between the star's D792 and D1519 light-dimming episodes is exactly three cycles of 242 days (i.e. 242 x 3 = 726). Almost immediately we can see that each of these synchronizations with earth days are multiples of the number 11 (2 x 11 = 22, 11 x 11 = 121 & 22 x 11 = 242). Remember also that there are 55 cycles of 0.88 days every 48.4 days, with 55 being another multiple of 11 (5 x 11 = 55).
The inter-relationship between KIC 8462852's periodic fluctuations is shown in fig. 5.1. Here we see that the star's 0.88-day periodicity becomes the key to determining the proportional relationship between its other main cyclic values of 48.4 days and 242 days. For example, 242 days is exactly 275 x 0.88 days, while 48.4 days is 55 x 0.88 days. This means that the star's 48.4-day cycle is exactly 1/5th of 242 days, making the time between 48.4 days and 242 days precisely four times this amount. In addition to this, the period between 48.4 days and 242 days is not only 4 x 48.4 days, as well as 4/5th of 242 days, but also 220 x 0.88 days, with 220 being 4 x 55 or 20 x 11 cycles of 0.88 days.
Figure 5.1. The inter-relationship between the 0.88-day, 48.4-day and 242-day periodicities noted in connection with the Kepler light curve for KIC 8462852 (not to scale).
Thus there appears to be two basic cycles seen in connection with Tabby's Star. One lasts a grand total of 242 earth days and can be divided into either five parts of 48.4 days or ten parts of 24.2 days (see fig. 5.2a). The other, based on 0.88 days, coincides with the earth every 22 days, generating 11 points of synchronization over a period of 242 earth days (see fig. 5.2b). Since 25 x 0.88 days equals 22 days a clear relationship can be shown to exist between this cycle and the 24.2-day cycle. The latter creates ten divisions across a 242-day period with the former generating eleven. This means that the rate of expansion of the two cycles bears a 11:10 ratio. This is shown in the fact that 24.2 is 11/10th of 22 (25 x 0.88), 48.4 is 11/10th of 44 (50 x 0.88), 121 is 11/10th of 110 (125 x 0.88), while 242 is 11/10th of 220 (250 x 0.88). Please note also that the expansion rate between the 0.88-day periodicities shown in fig. 5.2c and the 48.4-day cycle seen in fig. 5.2a is 25:22, e.g. 55 to 48.4, 110 to 96.8, 165 to 145.2, and 220 to 193.6.
The relationship between the progression of the three different periodicities, based on their culmination amounts of 220, 242 and 275 can be shown to be 1/5th, e.g. 22 (2 x 11) between 220 and 242 and 33 (3 x 11) between 242 and 275. This reveals a ratio between the three values of 22:33 or 2:3. Adding together 22 and 33 we arrive at 55 (5 x 11). As previously noted, 55 x 0.88 days is 1/5th of 275, the total number of 0.88 periodicities in 242 earth days, while 1/5th of 242 days is 48.4 days, one complete Tabby's Star cycle. Thus we can see that a perfect harmony exists between these three periodicities of 24.2/48.4 days, 22 days and 0.88 days with the numerical values generated by their points of synchronization nearly always being multiples of eleven (the exception being some the figures generated by the 24.2/48.4-day cycle).
5.2a-c. Three calendar rounds showing Tabby's
Star's periodicities. Left, a, the 24.2-day and 48.4-day cycles over a period
of 242 days, with this being the first point of synchronization between the 48.4-day
cycle and earth days. Centre, b, the star's grand cycle of 242 days broken up
into divisions of 22 days defined by the points of synchronization between the
star's 0.88-day cycle and earth days. Right, c, calendar round of 242 earth days
showing periods of 0.88 Tabby's Star orbital periods based on their synchronization
with the star's 48.4-day cycle.
The additional presence of a periodicity of approximately 11 days noted in connection with the star's 0.88-day fluctuations is further evidence that this cycle reflects eleven-fold synchronizations with earth days. The fact that the cycles can also be shown to synchronize with the earth in amounts that are themselves divisible by 11, i.e. 22 days (2 x 11) for the 0.88-day cycle, 121 days (11 x 11) for the 24.2-day cycle, and 242 days (22 x 11) for the 48.4-day cycle, starts to become difficult to explain in normal terms.
5.2. The Power of Eleven
A few general words might be helpful here on the nature of the number eleven and its multiples. It is a prime number. It is the fifth prime, coming after 2, 3, 5, and 7. It is also the first prime in double figures, as well as the first numeric palindrome. The other principal number generated by the 1/5th divisions of the star's 242-day grand cycle into periodicities of 0.88 days is 55, a multiple of 5 and 11 as well as the tenth Fibonacci number (with the interesting fact that the sum of any consecutive sequence of ten Fibonacci numbers will always be divisible by eleven). Values of 11, 55 and 220 feature in Pascal's Triangle, a triangular arrangement of binomial coefficients, which can be used to generate the Fibonacci series. Not only does each of its descending rows consecutively express multiples of eleven (11 squared, 11 cubed, etc.), but the triangle's fourth diagonal contains the values of so-called tetrahedral numbers, each one being the sum of the ascending rows making up a three-dimensional triangle or tetrahedron(known also as the 3-simplex - see below), easily imagined as a triangular stack of cannon balls. They include 220 (4 x 55), which follows 165 (3 x 55). This defines a tetrahedron made up of 220 cells with each of its four triangular faces displaying 55 facets.
Cell values of 11 and 55 feature also in Pascal's Triangle's eleventh row. As in all its descending rows the eleventh defines the numeric expansion of polytopes (a geometric object with flat sides) known as simplexes, in this instance the 10-simplex or henecaxennon. This has 11 vertices, 55 edges, 165 faces, 330 (6 x 55) tetrahedral cells as well as a series of higher dimensional faces. In the knowledge that Pascal's Triangle's row 2 relates to 1D (one dimensionality, or 1-simplex) forms, row 3 to 2D forms (the triangle or 2-simplex), row 4 to 3D forms (the tetrahedron or 3-simplex), row 5 to 4D forms (the pentatope, tetrahedral pyramid or 4-simplex), etc., row 11 (the henecaxennon or 10-simplex) provides the structure for an 11-faceted polytope existing in ten dimensions. Of possible interest here is that it is ten dimensions of space and one of time that defines eleven-dimensional supergravity used to determine the low-energy limit of M-theory in theoretical physics. None of this need be directly related to the mystery of KIC 8462852's strange dipping episodes, although the fact that its cyclic patterns very clearly reflect an interest in the number eleven and its multiples is curious to say the least.
KIC 8462852's periodicities are not simply the product of false data generated
by Kepler between 2009 and 2013, perhaps based on the observation of circumstellar
rings on the edge of our own solar system as is proposed by I. I. Katz (2017),
is it possible that its cyclic patterns expressing an apparent emphasis on the
number eleven and its multiples are generated by a natural process inherent to
the star? Alternately, and somewhat more controversially, could it be possible
that the star's light emissions are being manipulated quite deliberately to convey
meaningful mathematical patterns and formula?
In 2005 French astronomer Luc Arnold proposed that the launch of space telescopes like the future Kepler mission would provide extraterrestrial civilizations with an ideal opportunity to communicate information using what he referred to as "attention-grabbing signals" (Arnold, 2005). In his opinion, this could be achieved by deploying massive solar panels with the express purpose of transiting stars. The resulting light curves could then be used to convey mathematical patterns such as prime number sequences, binary code, and even more complicated formulas. As Jason Wright realised when he first saw the Kepler data for KIC 8462852, this was exactly what Luc Arnold said we should look for in light curves produced by occulting objects transiting stars.(8)
the knowledge that Tabby's Star's periodicities synchronize with the earth's solar
cycle in a manner that generates multiples of the number eleven, a prime number,
it is right to consider the possibility that these cyclic light fluctuations contain
mathematical information of specific interest to life on earth. It is important
also to remember that the inter-relationship between the star's different periodicities
and the mathematical patterns they appear to generate will remain valid even if
a natural explanation is eventually found for its strange light dimming episodes.
Long-term Light Dimming
Understanding the cyclic patterns of KIC 8462852 should also be considered in the knowledge that in addition to the short-term light dips reported in connection with the star a long-term light-dimming trend has been noted. Dr Bradley Schaefer of Louisiana State University has determined from a detailed eyeball examination of photographic plates from the DASCH-Harvard collection that between 1890 and 1989 that the star faded by as much as 20 percent (Schaefer, 2016). Even though this finding has been criticised by two separate teams of astronomers, who failed to find the same trend in either the DASCH-Harvard plates or another similar set of plates in Germany (Hippke et al, 2016; Lund et al, 2016), an examination by Benjamin Montet and Joshua Simon of the so-called Full Frame images taken by Kepler between 2009 and 2013 showed that Boyajian's Star faded by around 3 percent across Kepler's initial four-year mission (Montet and Simon, 2016). A similar "non linear fade" has been reported by Bruce Gary who has been observing the star, initially with a clear filter and afterwards with a V-filter, from October 2015 through to the present day. Although the fade rate fluctuates, Gary notes that the star is currently fading at a rate of approximately 1.4 percent per year.
the American Association of Variable Star Observers (AAVSO) has also noted a clear
dimming trend in connection with KIC 8462852 across a period of 638 days of monitoring
the star's light emissions. As noted in a blog dated June 29, 2017: "You
can see a clear dimming trend. We have the most data in "V" band, and
you can see there the curve is flat for about 286 days (early August 2016), when
it turns downward at a rate of almost 3% per year (0.028 magnitudes/year). Even
by eye, the trend appears to be unmistakable. In "B" the turning point
seems to be coming a bit earlier, but the rate of decline is similar - about 2%
per year. The trends in "R" data are similar."(9) As suggested,
these findings are similar to those obtained by Montet and Simon using the Kepler
Full Frame images from between 2009 and 2013.
clearly, the existence of a long term dimming trend is unlikely to be unconnected
with the star's short-term dimming events. Yet finding a mechanism to suitably
explain both trends has so far proved difficult, and if the long-term trend can
be verified then it could lend weight to an artificial source being behind both
trends. If so, then it would strengthen the idea that the mathematical patterns
detected in connection with KIC 8462852's light fluctuations really do have meaning
and purpose. What is more, if the star's long-term fading continues at its present
rate then there is a possibility that it will cease to exist in its present form
inside a century. Whether or not Boyajian's Star is an old star about to die,
or the long-term fading is being caused, as surmised by Eduard Heindl (2016),
by star-lifting operations or by the gradual construction of a Dyson sphere (Wright
& Sigurdsson, 2016) is currently impossible to determine. What we can surmise
is that the imminent death of a star might well be something of interest to a
nearby alien civilization.
number of solutions have been put forward by a host of authors to explain the
strange light fluctuations experienced by KIC 8462852. Some of these rely on the
assumption that their source comes from the star itself (Metzger et al, 2017).
Others rely on the surmise that they are the result of liberated planetary material
in the interstellar medium (Makarov, 2016), circumsolar rings on the edge of our
own solar system (Katz, 2017), or large groups of objects orbiting the star (e.g.
Boyajian et al, 2016; Ballesteros et al, 2017). Of all these possible solutions
the physical modelling of the light curves from the Kepler data leans firmly towards
the conclusion that the true source of the light dimming events will be found
to be extremely large objects, natural or otherwise, either orbiting or transiting
the star in some manner.
Kepler data suggests also that the occulting objects, which all create light curves
with sharp tips, display elliptical profiles with flat bottoms and tops. If correct,
this indicates that the objects are themselves either ellipses, slim disks or
irregular shards rotating along the line of sight. Indeed, if the obscuring objects
can be shown to be slim disks then a disk's non-isotropic manner of distribution
of its waste heat could help explain why no IR excess has been noted in connection
with the star.
physical modelling does not tell us what these objects are, the one thing it can
do is virtually rule out the idea that the D792 event was caused by a giant-sized
planet. Being round, a planet of any size would provide a distinctive light curve
with a characteristic flat-bottomed profile. The possibility that the obscuring
objects are in fact the dense rings of planets tilted so that they assume an elliptical
profile (and in so doing obscure the true profile of the planet) remains on the
table. However, the fact that three slim ellipses in a line appear to have created
the D1519 event makes the ringed-planet idea inadequate to explain the sheer number
of objects involved. Such a theory cannot also explain the overall shape of the
D792 event. This, as we have seen, showed the presence of incredibly long "wings"
or trails visible during the ingress and egress of the star, while the main object
itself displayed a clear elliptical profile with a flat bottom and top. Together
these two quite separate elements do not add up to a giant-sized planet with dense
rings tilted so as to create an elliptical profile.
the likelihood of the light fluctuations being caused by the transit across the
face of the star by random clusters of comets or asteroids, or by giant-sized
planets, is greatly lessened by the almost contrived manner in which the occulting
objects seem to conform to very specific periodicities, most obviously the 24.2
day half cycle noted above. What is more, the fact that these periodicities reflect
mathematical patterns centered around the prime number eleven, and coincide also
with the earth's own solar cycle in a meaningful manner, only adds to the problem
of finding a single explanation for the star's light dimming episodes whether
periodic or secular, i.e. long term. Indeed, we should not rule out the possibility
that encoded within the Kepler data for KIC 8462852 is specific information manufactured
in some intelligent manner and meaningful to life on earth. It is a proposition
that if proved correct would vindicate the predictions of Luc Arnold who as long
ago as 2005 had one eye on the greater potential of future space missions. This,
of course, included the Kepler space telescope, the very source of the data behind
Tabby's Star's light dimming episodes.
Notes and References
1. A 10.7-day cycle in the Kepler data for days 1322 - 1352 and a 13-day cycle for days 1232 - 1254 are noted here: http://imgur.com/gallery/CRRSG, courtesy of acco.
2. Flux data from http://www.wherestheflux.com/public. Spectrogram using Excel and associated maths software Octave.
3. Gdsacco, "Seeing the forest through the trees," June 10, 2017, https://www.reddit.com/r/KIC8462852/comments/6gim8b/seeing_the_forest_through_the_trees/.
4. Jason Wright during a presentation for the SETI Institute: Science Colloquium: "Frontiers in Artifact SETI: Waste Heat, Alien Megastructures & Tabbys Star - Jason Wright (ST 2016)", uploaded August 12, 2016. https://www.youtube.com/watch?v=XEDR-G2EDRM.
5. Gdsacco, "Seeing the forest through the trees," June 10, 2017, https://www.reddit.com/r/KIC8462852/comments/6gim8b/seeing_the_forest_through_the_trees/.
6. See Bruce L. Gary's webpage on KIC 8462852 at http://www.brucegary.net/KIC846/.
7. Reddit member gdcasso used the existing 24.2-day half cycle to predict a further dimming event after a further dimming episode that peaked at around two percent on May 19, 2017. This did indeed begin on June 13, 2017, with a maximum drop down to two percent occurring on on June 15. Gdsacco, "Seeing the forest through the trees," June 10, 2017, https://www.reddit.com/r/KIC8462852/comments/6gim8b/seeing_the_forest_through_the_trees/.
8. Jason Wright during a presentation for the SETI Institute: Science Colloquium: "Frontiers in Artifact SETI: Waste Heat, Alien Megastructures & Tabbys Star - Jason Wright (ST 2016)", uploaded August 12, 2016. https://www.youtube.com/watch?v=XEDR-G2EDRM.
9. Carr, Paul, Dream of the Open Channel, June 29, 2017, https://disownedsky.blogspot.co.uk/2017/06/more-on-aavso-trends-for-boyajians-star.html?m=1.
(2015), Ross, "The Most Mysterious Star in Our Galaxy," The Atlantic,
October 13, 2015. https://www.theatlantic.com/science/archive/2015/10/the-most-interesting-star-in-our-galaxy/410023/.
Arnold (2005), Luc, "Transit Lightcurve Signatures of Artificial Objects," AJ 627, 534-9, https://arxiv.org/abs/astro-ph/0503580.
Ballesteros (2017), Fernando J., Pablo Arnalte-Mur, Alberto Fernandez-Soto and Vicent J. Mart?nez, "KIC 8462852: Will the Trojans return in 2021?" MNRAS 000, 1-5, https://arxiv.org/pdf/1705.08427.pdf.
Boyajian (2016), T. S., et al. "Planet Hunters IX. KIC 8462852 - where's the flux?" MNRAS 457: 4, 3988-4004. https://arxiv.org/abs/1509.03622.
Hale (2016), R. B., "Thoughts on Star KIC8462852," private circulation only, December 21, 2016.
Heindl (2016), Eduard. "A physically inspired model of Dip d792 and d1519 of the Kepler light curve seen at KIC8462852," https://arxiv.org/abs/1611.08368.
Hippke (2016), Michael, Daniel Angerhausen, Michael B. Lund, Joshua Pepper, and Keivan G. Stassun, "A statistical analysis of the accuracy of the digitized magnitudes of photometric plates on the time scale of decades with an application to the century-long light curve of KIC 8462852," https://arxiv.org/abs/1601.07314.
Katz, I. I (2017). "Can Dips of Boyajian's Star be Explained by Circumsolar Rings?" ArXiv #: 1705.08377, http://harvard.voxcharta.org/tag/quot-boyajians-star-quot-kic-8462852/.
Lund (2016), Michael B., Joshua Pepper, Keivan G. Stassun, Michael Hippke, and Daniel Angerhausen. "The Stability of F-star Brightness on Century Timescales," https://arxiv.org/abs/1605.02760.
Makarov (2016), Valeri V., "Photometric and astrometric vagaries of the enigma star KIC 8462852," https://arxiv.org/abs/1609.04032.
Metzger (2017), Brian D. Ken J. Shen, and Nicholas C. Stone, "Secular Dimming of KIC 8462852 Following its Consumption of a Planet," https://arxiv.org/abs/1612.07332.
Montet (2016), Benjamin T., and Joshua D. Simon, "KIC 8462852 Faded Throughout the Kepler Mission," https://arxiv.org/abs/1608.01316.
Schaefer (2016), Bradley E., "KIC 8462852 Faded at an Average Rate of 0.164+-0.013 Magnitudes Per Century From 1890 To 1989," AJL 822: 2, article id. L34, 6 pp. https://arxiv.org/abs/1601.03256.
Wright (2016), Jason T. and Steinn Sigurd?sson, "Families of Plausible Solutions to the Puzzle of Boyajian's Star," AJL 829: 1, 1-12. http://iopscience.iop.org/article/10.3847/2041-8205/829/1/L3/pdf.
The authors wish to thank Greg Little, Richard Ward, Catherine Hale, and Russell M. Hossain for their help in the preparation of this paper.
All pictures appearing in this paper are the copyright of the authors unless otherwise stated in the accompanying caption. Main opening image is copyright Russell M. Hossain, July 2017.
Download a PDF of the original paper by Andrew Collins and Rodney Hale entitled "KIC 8462852Physical Modelling of its Occulting Objects and the Growing Mystery Surrounding its Cyclic Fluctuations: A New Assessment," published on viXra in June 2017:
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