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Semiregular variable star
Semiregular variable star
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Light curve of semiregular variable star Betelgeuse

In astronomy, a semiregular variable star, a type of variable star, is a giant or supergiant of intermediate and late (cooler) spectral type. It shows considerable periodicity in its light changes, accompanied or sometimes interrupted by various irregularities. Periods lie in the range from 20 to more than 2000 days, while the shapes of the light curves may be rather different and variable with each cycle. The amplitudes may be from several hundredths to several magnitudes (usually 1-2 magnitudes in the V filter).

Classification

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The semiregular variable stars have been sub-divided into four categories for many decades, with a fifth related group defined more recently. The original definitions of the four main groups were formalised in 1958 at the tenth general assembly of the International Astronomical Union (IAU). The General Catalogue of Variable Stars (GCVS) has updated the definitions with some additional information and provided newer reference stars where old examples such as S Vul have been re-classified.

Semiregular variable subtypes
Subtype[1] IAU definition[1] GCVS code[2] GCVS definition[2] Standard
stars
SRa semi-regular variable giants of late spectral classes (M, C and S), which retain periodicity with comparative stability and possess, as a rule, small (less than 2m.5) light-variation amplitudes. Amplitudes and forms of light curves are usually liable to strong variations from period to period. Many of these stars differ from Mira Ceti type stars only owing to the smaller amplitude of light variation. SRA Semiregular late-type (M, C, S or Me, Ce, Se) giants displaying persistent periodicity and usually small (<2.5 mag in V) light amplitudes. Amplitudes and light-curve shapes generally vary and periods are in the range of 35–1200 days. Many of these stars differ from Miras only by showing smaller light amplitudes Z Aqr[1][2]
SRb semi-regular variable giants of late spectral classes (M, C and S) with a poorly expressed periodicity, i.e. with a different duration of individual cycles (which leads to the impossibility of predicting the epochs of maximum and minimum brightness), or with the replacement of periodical changes by slow irregular variations, or even by the constancy of brightness. Some of them are characterised by a certain mean value of the period, given in the catalogue. SRB Semiregular late-type (M, C, S or Me, Ce, Se) giants with poorly defined periodicity (mean cycles in the range of 20 to 2300 days) or with alternating intervals of periodic and slow irregular changes, and even with light constancy intervals. Every star of this type may usually be assigned a certain mean period (cycle), which is the value given in the Catalogue. In a number of cases, the simultaneous presence of two or more periods of light variation is observed AF Cyg[1][2]
RR CrB[1][2]
SRc semi-regular variable super-giants of late spectral classes SRC Spectral-type (M, C, S or Me, Ce, Se) supergiants with amplitudes of about 1 mag and periods of light variation from 30 days to several thousand days. μ Cep[1][2]
RW Cyg[1]
SRd semi-regular variable giants and super-giants belonging to spectral classes F, G, K SRD Semiregular variable giants and supergiants of F, G, or K spectral types, sometimes with emission lines in their spectra. Amplitudes of light variation are in the range from 0.1 to 4 mag, and the range of periods is from 30 to 1100 days S Vul[1]
UU Her[1]
AG Aur[1]
SX Her[2]
SV UMa[2]
SRS Semiregular pulsating red giants with short period (several days to a month), probably high-overtone pulsators AU Ari[2]

Pulsation

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The semiregular variable stars, particularly the SRa and SRb sub-classes, are often grouped with the Mira variables under the long-period variable heading. In other situations, the term is expanded to cover almost all cool pulsating stars. The semi-regular giant stars are closely related to the Mira variables: Mira stars generally pulsate in the fundamental mode; semiregular giants pulsate in one or more overtones.[3]

Photometric studies in the Large Magellanic Cloud looking for gravitational microlensing events have shown that essentially all cool evolved stars are variable, with the coolest stars showing very large amplitudes and warmer stars showing only micro-variations. The semiregular variable stars fall on one of five main period-luminosity relationship sequences identified, differing from the Mira variables only in pulsating in an overtone mode. The closely related OSARG (OGLE small amplitude red giant) variables pulsate in an unknown mode.[4][5]

Many semiregular variables show long secondary periods around ten times the main pulsation period, with amplitudes of a few tenths of a magnitude at visual wavelengths. The cause of the pulsations is not known.[3]

Bright examples

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η Gem is the brightest SRa variable, and also an eclipsing binary. GZ Peg is an SRa variable and S-type star with a maximum magnitude of 4.95. T Cen is listed as the next-brightest SRa example,[2] but it is suggested that it may actually be an RV Tauri variable, which would make it by far the brightest member of that class.[6]

There are numerous naked-eye SRb stars, with third-magnitude L2 Pup being the brightest listed in the GCVS. σ Lib and ρ Per are also third-magnitude SRb stars at maximum brightness. β Gru is a second magnitude star classified as a slow irregular variable by the GCVS, but reported to be of SRb type by later research.[7] These four are all class M giants, although some SRb variables are carbon stars such as UU Aur or S-type stars such as Pi1 Gru.[2]

Catalogued SRc stars are less numerous, but include some of the brightest stars in the sky such as Betelgeuse and α Her. Although SRc stars are defined as being supergiants, a number of them have giant spectral luminosity classes and some such as α Her are known to be asymptotic giant branch stars.[2]

Many SRd stars are extremely luminous hypergiants, including the naked-eye ρ Cas, V509 Cas, and ο1 Cen. Others are classified as giant stars, but the brightest example is the seventh-magnitude LU Aqr.[2]

Most SRS variables have been discovered in deep large-scale surveys, but the naked-eye stars V428 And, AV Ari, and EL Psc are also members.[2]

See also

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References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Semiregular variable stars are giant or stars of intermediate and late types, such as , , and , that exhibit brightness variations with noticeable but often irregular periodicity due to radial pulsations in their extended envelopes. These variations typically have periods ranging from 20 days to more than 2000 days and visual amplitudes of several hundredths to several magnitudes, usually 1–2 magnitudes, with light curves that can differ significantly in shape. The General Catalogue of Variable Stars (GCVS) classifies semiregular variables into several subclasses to account for differences in spectral type, regularity of pulsation, and evolutionary status. SRa stars are late-type giants (, C, S, and their emission-line variants) with persistent periodicity, amplitudes less than 2.5 magnitudes in V, and periods of 35–1200 days; SRb are similar giants but with poorly defined or alternating periodic and irregular changes, periods of 20–2300 days; SRc are late-type supergiants with amplitudes around 1 magnitude and periods from 30 days to several thousand days; SRd encompass , or K giants and supergiants, often with emission lines, amplitudes of 0.1–4 magnitudes, and periods of 30–1100 days; and SRs are short-period (days to a month) red giants likely pulsating in high overtones. These subclasses highlight the diversity within the group, where fundamental-mode pulsations dominate in more regular cases akin to , while multi-periodic or chaotic behavior occurs in others due to overlapping pulsation modes or processes. Notable examples include (α Orionis), a classified as SRc with a primary period of about 400 days and amplitudes up to 1.5 magnitudes, and (α Scorpii), a slow irregular variable (LC) in the Hertzsprung-Russell diagram. Other prominent semiregular variables are L2 Puppis, an SRa star showing complex light curves indicative of evolutionary transitions, and μ Cephei, a with irregular outbursts. Semiregular variables represent a critical phase in the (AGB) evolution of low- to intermediate-mass stars, marking the onset of significant mass loss through stellar winds and providing insights into the dynamical atmospheres of evolved stars. Their pulsations drive dust formation and circumstellar envelopes, influencing galactic chemical enrichment, and while less precise than Miras for distance measurements, they serve as standard candles in nearby galaxies and probes of models.

Overview

Definition

Semiregular variable stars are giant or stars of intermediate and late spectral types, including M, C, and S classes, that display periodic light variations which are not strictly regular. These stars exhibit noticeable periodicity in their brightness changes, often interrupted by intervals of semiregular or irregular fluctuations, setting them apart from other classes. The defining characteristic of semiregular variables is their quasi-periodic or multi-periodic behavior, where light curves show appreciable repetition but lack the precise regularity seen in types like Cepheids. This irregularity arises from complex interactions in their atmospheres and envelopes, leading to variations that can include multiple overlapping cycles. Primarily, semiregular variables consist of stars or red supergiants, representing evolved, cool luminous phases in . Their pulsations, driven by internal thermal instabilities, are the general cause of these light variations.

General Characteristics

Semiregular variable stars exhibit light variations with amplitudes ranging from 0.01 magnitudes to several magnitudes, though commonly 1–2 magnitudes in the V filter. Their periods span from 20 days to over 2000 days, frequently displaying multiple overlapping periods or intervals of irregularity that result in non-repeating light curves suggestive of superimposed pulsation modes. These photometric traits distinguish them from more regular pulsators like , which have larger amplitudes and stricter periodicity. Spectrally, semiregular variables are predominantly giants or supergiants of late spectral types, including , , and S classes, characterized by prominent molecular absorption bands such as (TiO) in M-type giants. Earlier subtypes, like those in F, G, or K classes, may show weaker or occasional TiO features alongside metallic lines. These spectral signatures reflect cool, extended atmospheres conducive to formation. In evolutionary terms, semiregular variables are closely associated with the (AGB) phase of , where stars undergo significant mass loss that forms circumstellar dust envelopes, often detectable through infrared excess or variations. Some reside on the (RGB) or in post-AGB stages, contributing to their observed irregularity as they transition toward formation.

Classification

Subtypes

Semiregular variable stars are classified into subtypes primarily based on their spectral types, pulsation periods, light amplitudes, and the degree of regularity in their light curves, as standardized in the General Catalogue of Variable Stars (GCVS). These subtypes distinguish variations in stability and physical characteristics among giants and supergiants exhibiting semiregular behavior. The SRa subtype consists of late-type giants with spectral classes M, C, or S (or their emission-line variants Me, Ce, Se), featuring persistent single or multiple periodicities, with amplitudes and light-curve shapes that generally vary, periods ranging from 35 to 1200 days and visual amplitudes less than 2.5 magnitudes. In contrast, SRb variables are also late-type giants of similar spectral classes but display poorly defined periods or alternating intervals of periodic and irregular variations, with periods from 20 to 2300 days and possible episodes of near-constancy. SRc subtypes are characterized by late-type supergiants (M, C, S or Me, Ce, Se) with amplitudes around 1 magnitude in the visual band and periods from 30 days to several thousand days. SRd variables encompass giants or supergiants of earlier spectral types , or (occasionally with emission lines), with periods between 30 and 1100 days and amplitudes ranging from 0.1 to 4 magnitudes in the visual. Additionally, the SRs subtype includes short-period semiregular red giants, often pulsating in high overtones with periods of days to about a month. The SRs subtype was introduced in later updates to the GCVS (Name-Lists 67-77 and vol. V).

Relation to Other Variable Stars

Semiregular variable stars share significant similarities with , as both classes consist of long-period pulsating red giants and supergiants on the (AGB) of . Unlike Miras, however, semiregulars exhibit smaller photometric amplitudes, typically less than 2.5 magnitudes in the visual band, and their periods are less strictly regular, often showing multi-periodic or quasi-periodic behavior. This distinction arises from the underlying pulsation modes, where Miras predominantly pulsate in the fundamental mode with high regularity, while semiregulars display a mix of radial and non-radial modes leading to more variable light curves. In contrast to irregular variables such as the Lb subtype, semiregulars demonstrate detectable periodicity in their variations, albeit with some irregularity in amplitude and timing. Lb variables, characterized by slow, non-periodic fluctuations in late-type giants without discernible cycles, often represent insufficiently observed stars that may later reveal semiregular patterns upon extended monitoring. The boundary between these classes is thus somewhat fluid, with many initially classified Lb objects reclassified as semiregular after period analysis confirms underlying pulsations. Semiregular variables of the SRd subtype show overlaps with RV Tauri stars in spectral types, both featuring F to K supergiants with pulsational variability. However, SRd stars differ in their period-amplitude behavior, displaying semiregular pulsations with periods from 30 to 1000 days and amplitudes under 2 magnitudes, whereas RV Tauri stars exhibit characteristic alternating deep and shallow minima on shorter cycles of 30 to 150 days due to binarity and dust effects. This spectral overlap suggests possible evolutionary connections in post-AGB phases, though their morphologies remain distinct. Some semiregular variables exhibit overlaps with symbiotic stars, where the cool giant component undergoes pulsational variability akin to semiregular behavior. In these systems, the primary variability stems from the pulsations of the , with additional photometric changes from accretion onto a hot companion, but the semiregular pulsations dominate the long-term . Such overlaps highlight how pulsational instability in AGB stars can coexist with binary interactions without altering the core . Evolutionarily, late-type semiregular variables (SRa, SRb, SRc) serve as an intermediate stage in the AGB evolution of low- to intermediate-mass stars, between earlier phases and the more evolved, higher-amplitude , reflecting increasing envelope instability and mass loss. SRd variables may relate to different evolutionary stages, potentially post-AGB or in higher-mass progenitors. As AGB stars progress through thermal pulses, semiregular pulsations may transition to the more regular phase. This positioning underscores their role in tracing late-stage .

Pulsation Mechanisms

Physical Processes

Semiregular variable stars exhibit variability primarily through radial pulsations in their extended envelopes, akin to those in but typically involving higher or multiple modes rather than the fundamental mode alone. These pulsations cause periodic expansions and contractions of the stellar surface, leading to changes as the and vary. In (AGB) stars, which comprise most semiregular variables, the envelopes are convective and loosely bound, facilitating these oscillations with periods ranging from tens to hundreds of days. The driving force behind these pulsations is the kappa mechanism, operating in the zones of and within the envelope. During compression, rising temperatures in these partial regions increase opacity (κ), trapping heat and causing further expansion; upon cooling, opacity decreases, releasing energy efficiently. This cyclic modulation of creates a net energy gain for the pulsation, sustaining the instability despite the convective nature of AGB envelopes. Multi-periodicity arises from the superposition of the fundamental mode and higher overtones, resulting in the characteristic semi-regular light curves that lack strict periodicity. Recent 3D radiation hydrodynamics simulations reveal that both radial and non-radial modes can be excited, leading to complex interactions. Observations indicate that most semiregular variables display two or more dominant periods, with ratios suggesting excitation of first and higher overtones rather than solely fundamental and first-overtone combinations. This mode interference produces irregular but quasi-periodic variations, as the amplitudes and phases of individual modes evolve over time. Additionally, stochastic processes and chaotic dynamics can contribute to the observed irregularity, particularly in less stable pulsators, as recent models show a transition from stochastic driving in smaller-amplitude variables to self-excited pulsations in semiregulars. A subset of semiregular variables also exhibit long secondary periods (LSPs), approximately 10 times longer than the primary pulsation period, whose origins remain debated. Possible explanations include binary motion, where a companion induces variations and circumstellar obscuration, or dynamical processes in the stellar envelope, such as radial pulsations in the outer layers or non-radial gravity modes. Pulsations in semiregular variables enhance mass loss by levitating the and enabling -driven winds, where on newly formed grains accelerates outflows. This process becomes prominent when pulsation periods exceed about 60 days, increasing mass-loss rates by factors of up to 10 and producing observable excesses from reprocessed stellar light by circumstellar . In pulsation , the period PP approximates the dynamical timescale, scaling as PR/csP \propto R / c_s, where RR is the stellar radius and csc_s is the sound speed (assumed roughly constant). For AGB stars with similar effective temperatures, luminosity LR2Teff4R2L \propto R^2 T_{\rm eff}^4 \approx R^2, so RLR \propto \sqrt{L}
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