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Variable Star of the Season: Delta Scuti and the Delta Scuti variables
This summer's Variable Star of the Season is delta Scuti and the
class of variables which carries its name. Because they are low amplitude
variables, they will be challenging to visual and CCD observers alike, but
we hope it's a challenge you will all enjoy! A diverse class of very short
period stars,
the delta Scuti variables have something for everyone. Some have amplitudes
of nearly one magnitude and regular light curves like some of the RR Lyrae
stars and Cepheid variables. Others have complex light curves and multiple
periods with millimagnitude light variations. The delta Scuti stars are
important astrophysically for many reasons. They are some of the best
targets for asteroseismology -- using the pulsations of a star to study
the structure of the interior -- and the high amplitude stars serve as
standard candles
to measure cosmic distances with.
Photograph of the delta Scuti field from a 1781 edition of Flamsteed's Atlas,
with delta Scuti indicated by the red circle (click to see full page).
Flamsteed didn't recognize Scutum as a constellation, and it was considered
part of Aquila. Since Scutum is now one of the 88 recognized constellations, the
variable is now designated delta Scuti. It can be found on page 97 of
the AAVSO Variable Star Atlas. Photo credit: A. Price, AAVSO.
Discovery
Credit for the discovery of the delta Scuti as a variable star goes to
W.W.
Campbell and W.H. Wright of
Lick Observatory. Using the
Mills Spectrograph, the two astronomers measured the radial velocities
of a sample
of moderately bright stars, and found several whose radial velocities varied
with time.
One of these, "2 Scuti",
showed radial velocity variations with amplitudes of several kilometers per
second. More than 30 years later, Edward Fath and Attilio Colacevich
revisited this object, and published short summaries of their findings in
PASP. Fath conducted a photometric study, while
Colacevich used the
Mills Spectrograph to measure the radial velocity amplitude. Both found
periods near 0.1937 day, and Colacevich claimed that it couldn't be a
spectroscopic binary with such a combination of radial velocity amplitude
and period. Fath noted photometric amplitude variations in his 1935 paper,
and in
1937
found multiple periods in the photometric data. In 1938, Theodore Sterne of
Harvard examined whether radial pulsations could be responsible for the
multiple periods observed in this star. Radial pulsations are pulsations where
the star pulsates in a spherically symmetric manner -- all points on the
surface move in and out at the same time with the same period and velocity.
The periods and period ratios of radial modes are fixed by the structure of the
star. Sterne calculated the predicted periods and period ratios for a
reasonable stellar model, and subsequently ruled out radial modes as being
capable of producing all of the observed periods.
By June 1956, four delta Scuti stars were known (Eggen 1956):
delta Scuti, rho Puppis, CC Andromedae, and DQ Cephei. Eggen discovered a
fifth,
delta Delphini,
shortly thereafter, and the number began to climb rapidly
from then on. The dwarf Cepheids or delta Scuti stars soon
became a hot topic in stellar astronomical research. Theoretical
modeling of pulsating variable stars commenced in the early 1960's, as
part of a general effort to use digital computers in stellar astrophysics, and
an understanding of what delta Scuti stars were began to develop. Since that
time,
several hundred delta Scuti stars have been discovered, and our physical
understanding of their pulsations has progressed along with their numbers.
It is now well-understood that multiple periods in delta Scuti stars are due
to pulsation in radial and non-radial modes, and some stars
are now known to have dozens of pulsation modes simultaneously excited.
The discovery of new delta Scuti stars continues as new large-scale
photometric monitoring projects develop and expand. As of 2002, the
number of known delta Scuti stars stood at 636 (Rodriguez et al 2002), but
the number has grown since then.
The delta Scuti bestiary
The delta Scuti stars reside near the point where the instability strip crosses
the main sequence in the HR diagram. Stars in a variety of evolutionary
states -- including pre-main sequence stars -- can lie within the instability
strip, so long as they have spectral types between (roughly) F8 and A2, and
luminosity classes between V (dwarf) and III (subgiant). For stars with
solar metal abundances, this corresponds to masses between about 1.5 and
2.5 solar masses, and between 1.0 and 2.0 solar masses for metal-poor stars.
They are all short period stars, with individual periods lying in the range of
0.03 to 0.3 day.
Light curves for the high-amplitude delta Scuti stars CY Aquarii and
XX Cygni, obtained visually and with a CCD camera, respectively. Although
CY Aquarii is classified as
a high-amplitude star, it has a varying light curve which indicates the
presence of secondary modes.
The primary subclassifications of the delta Scuti stars rise from two things:
the pulsation amplitude, and the metal abundances. High-amplitude delta
Scuti stars (known as "HADS") are defined as those
with amplitudes above 0.1 magnitudes in V, and low-amplitude delta
Scuti stars ("LADS") are those with smaller amplitudes. Though the amplitude
break is somewhat arbitrary, there is a reasonable physical basis for it. The
large-amplitude
stars tend to be those undergoing radial pulsations, and typically
only pulsate in one dominant mode at a time. They also tend to be more
evolved, and lie well off the main sequence in the subgiant branch of the
HR diagram. And it is these stars that are typically used for distance
measurements, because they have well-defined period-luminosity relations
McNamara et al. 2000).
The low-amplitude stars can be pre-main, main, or post-main
sequence stars, and may either be multiperiodic or monoperiodic. However,
it is the multiperiodic LADS that are useful in asteroseismological studies,
and are often the targets of long-duration, multi-site photometric campaigns
designed to detect larger and larger numbers of pulsation periods.
The other subclassification is one of metal abundances. The metal rich,
Population I stars are known as delta Scuti stars, since the class
prototype is a Population I star. The metal-poor stars are also known as
the SX Phoenicis stars, after the class prototype. These stars
pulsate for exactly the same reason as the delta Scuti stars, and are
essentially the same as the high-amplitude delta Scuti stars except for their
metal abundances. The SX Phe
stars are known primarily as globular cluster and galactic halo stars, and
also have a period-luminosity relation.
What makes them tick?
The delta Scuti stars lie on what is known as the instability strip, a
region of the Hertzsprung-Russell diagram where stars may undergo self-excited
oscillations. The instability strip is home to many other types of pulsating
stars that you may be familiar with, including the Cepheids and the RR Lyrae
stars. The driving mechanism behind "self-excited"
oscillations is a special region of the stellar interior
where atoms of either hydrogen or helium transition from partly to completely
ionized. If the star is compressed, the ionization fraction of these regions
increases, raising the opacity of the material and blocking the
luminous energy trying to escape from the interior. The increased heat and
pressure built up in this layer push the outer layers of the
star outward. As these outer layers fall back inward again under
the force of gravity, the ionization region gets compressed again, restarting
the cycle. The variation in brightness is caused by changes in temperature
and radius caused by these motions. For stars on the
instability strip, this important layer lies at just the right depth in the
star for pulsations to be self-sustaining. If it were deeper, the driving
forces would be overwhelmed by convection,
and if it were shallower, the energy would be dissipated in the atmosphere.
In the delta Scuti stars, the ionization layer that drives the pulsations
the most is the second helium ionization zone, where singly-ionized helium
loses a second electron, but both the hydrogen ionization and neutral helium
ionization layers can also contribute to the pulsation driving. The driving
mechanism for the Cepheids and RR Lyrae stars is the same.
A theoretical Hertzsprung-Russell diagram, showing the location of
the Cepheid instability strip. Delta scuti stars can cross the instability
strip early or late in their lives, depending upon their masses. The
Cepheid variables (which are more massive) cross the instability strip
well away from the main sequence. The Sun will never cross the instability
strip prior to becoming a red giant.
Since the delta Scuti stars share the same pulsation mechanism, it's not
surprising that their light curves can look very similar to those of
Cepheids and RR Lyrae stars. Indeed, the high-amplitude delta Scuti stars or
AI Velorum stars are
still considered to be dwarf Cepheids stars by
some, and some have been
given the RR Lyrae designation RRs. But unlike the Cepheids
and the RR Lyrae stars, some delta Scuti stars exhibit very different behavior,
namely non-radial pulsation. The light variations in Cepheids, RR
Lyrae, and the high-amplitude delta Scuti stars come about because of
spherically symmetric variations in radius and surface temperature of the
star, which give rise to a change in luminosity. In some delta Scuti stars,
the surface also undergoes changes in radius and temperature, but in an
asymmetric way. Because the star is a three-dimensional object, there
are a large number of resonant modes which can be excited within the
star, each of which has a unique pulsation period. A few delta Scuti stars
(like FG Virginis and XX Pyxidis) are known to have a dozen or more of these
non-radial modes excited at once, and can be detected via the analysis
of very precise time-series photometry.
The delta Scuti stars aren't the only objects to exhibit such modes. The
pulsating white dwarfs can also have non-radial modes, as do many stars outside
of the instability strip (such as the beta Cepheid and slowly pulsating B
stars, the gamma Doradus variables, and others). Our own Sun has a rich
pulsation spectrum of thousands of radial and non-radial modes. The Sun has
often been compared to a giant bell ringing in space, and several observatories
here on Earth and in space
are devoted to "listening in" to the vibrations our Sun makes. The study of
these modes lets us fine-tune models of the solar interior, much like
the study of earthquakes enabled seismologists to study the interior
of the Earth. The study of vibrations in the Sun is known as
helioseismology, and the study of pulsating stars in general is known
as asteroseismology. (Note the spelling asteroseismology is
the commonly accepted one -- see Gough 1996 for a discussion.)
Observing the delta Scuti stars
The delta Scuti stars have something to offer visual, CCD, and PEP observers
alike, and it is best to choose targets according to one's photometric
capabilities. Many high-amplitude delta Scuti stars will be easily visible
to visual observers, and you can treat them like the RR Lyrae and Cepheid
variables. In fact, there are already a few high-amplitude stars (like VX Hya
and SZ Lyn)
in the
RR Lyrae observing program. The RR Lyrae observing committee has put together
a page for
the RR Lyrae program, and the
observing procedures given there are just as applicable to the high
amplitude delta Scuti stars as to the RR Lyrae stars.
The lower-amplitude stars are beyond the capabilities of visual observers
because the amplitude cutoff between high- and
low-amplitude stars is 0.1 magnitude, the precision limit for visual
observing. However, several low-amplitude, multiperiodic delta Scuti stars
can be observed by CCD and PEP observers. Generally, visual observers should
not try to observe stars whose amplitude is less than 0.5 magnitude.
When observing, it's important to remember that these stars have very short
periods of six hours at most, so you will need to obtain observations once
every fifteen minutes or less to follow the light curve. If you are looking
at a multiperiodic star, you could even try to obtain several consecutive
nights of photometry on a single star.
Delta Scuti itself lies on the boundary between the high- and
low-amplitude stars. It is highly evolved, and has an amplitude of about one
tenth of a magnitude, but it contains at least six independent pulsation
modes, and may contain more. It has an average V magnitude of about
4.75, so CCD observers may need to use very short exposures. Because there
is a secondary period close to the primary one, you should notice the varying
amplitude in the light curve (caused by beating of the two periods). It is
located at α 18h 42m 16.4s, δ -9° 3' 9.2" (J2000), and is
well placed right now for observers in the northern and southern hemispheres.
Some potential targets for the current observing season include the following:
Some seasonal δ Scuti stars in the AAVSO validation file
| Star name | Desig | V | comments
|
| YZ Boo | 1520+37 | 10.6 | Atlas, p.45
| DY Her | 1626+12 | 10.4 | Chart available
| V703 Sco | 1735-32 | 7.8 | Atlas, p.14
| δ Sct | 1836-09 | 4.7 | Atlas, p.97
| | XX Cyg | 2001+58 | 11.7 | Atlas, p.27
| RS Gru | 2136-48 | 8.2 | Atlas, p.164
| CY Aqr | 2232+01 | 10.8 | Chart available
| | | | | |
- The Delta Scuti network in Vienna
has been at the forefront of delta Scuti star research for many years, and
they maintain an extensive website with information for observers and the
general public.
-
Swinburne University presentation on pulsating variables (powerpoint)
- Campbell, W.W. and Wright, W.H., 1900, "A list of nine stars whose velocities in the line of sight are variable", ApJ 12, 254
- Colacevich, A., 1935, "On the variable radial velocity of delta Scuti", PASP 47, 231
- Cox, J.P., 1963, "On second helium ionization as a cause of pulsational instability in stars", ApJ 138, 487
- Eggen, O.J., 1956, "rho Puppis: a new short-period variable star", PASP 68, 238
- Eggen, O.J., 1956, "Two new bright variable stars: delta Delphini and delta Capricorni", PASP 68, 541
- Fath, E.A., 1935, "The variability of delta Scuti", PASP 47, 232
- Fath, E.A., 1937, "The multiple variability of delta Scuti", Lick Obs. Bulletin 487, 77
- Gough, D.O., 1996, "Astereoasteroseismology", The Observatory 116, 313
- Kollath, Zoltan, Konkoly Observatory: "Animations of pulsating variables"
- Laney, C.D. et al., 2003, "HADS, multiple periods, period changes, and the PL relation", in Interplay of Periodic, Cyclic and Stochastic Variability in Selected Areas of the H-R Diagram, edited by C. Sterken, ASP Conf. Proc 292, 203
- McNamara, D.H. et al., 2000, "The distance to the Galactic Center", PASP 112, 768
- Rodriguez, E. et al., 2002, "delta Sct and field SX Phe variables: a new catalogue", in Proceedings of the First Eddington Workshop on Stellar Structure and Habitable Planet Finding, edited by B. Battrick, ESA Publications (ESA SP-485)
- Sterne, T.E., 1938, "The secondary variation of delta Scuti", ApJ 87, 133
- Templeton, M.R. et al., 1997, "A new pulsation spectrum and asteroseismology of delta Scuti", AJ 114, 1592
This month's Variable Star of the Season was prepared by Dr. Matthew Templeton, AAVSO.
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