Abstract
The Asymptotic Giant Branch (AGB) is the late stage of the evolution of intermediate and low-mass stars and is of great importance for understanding stellar evolution, nucleosynthesis, and the chemical evolution of galaxies. This paper systematically reviews the methods for identifying AGB stars, from both traditional approaches and machine learning techniques. By integrating multi-wavelength data such as optical and infrared spectra, along with stellar evolution models, we analyze the existing methods and potential directions for improvement. We also explore the possibility of using interpretable machine learning algorithms to discover new features and applying deep learning algorithms to enhance search efficiency. With the advancement of data processing technology and the widespread application of machine learning methods, future AGB star searches will be more accurate and efficient. The increased number of discoveries, enabled by more advanced search methods, will particularly enhance our ability to reveal examples of short-lived late-stage stellar evolutionary processes.
1 Introduction
The Asymptotic Giant Branch (AGB) is a region in the Hertzsprung-Russell diagram characterized by low temperature and high luminosity, representing a stage in the late evolution of all low-to intermediate-mass stars (approximately 0.8–8 ) (; ). At this stage, the stellar core is composed of carbon and oxygen, while the hydrogen and helium shells undergo burning surrounding the carbon-oxygen core. The s-process during the AGB phase produces heavier elements, which, along with carbon, are mixed into the outer envelope during the third dredge-up process. These elements are then released into the interstellar medium through strong stellar winds.
As a result, AGB stars are crucial for understanding stellar evolution, elemental abundance, and chemical evolution within the Milky Way. Additionally, before removing their outer layers to form planetary nebulae and evolving into white dwarfs, AGB stars experience significant mass loss, providing a valuable opportunity to study the formation of interstellar dust and molecular gas (; ). As one of the primary contributors to the recycling of interstellar material, the mass loss process of AGB stars also has a profound impact on the chemical enrichment, dynamics, and structural evolution of the surrounding interstellar medium (). Therefore, the search and study of AGB stars hold a crucial position in the field of astronomy and they serve as a key component in the chemical evolution of galaxies.
AGB stars can be classified in various ways based on their evolutionary stage, surface chemical composition, and variability period. The AGB phase can be divided into the Early Asymptotic Giant Branch (E-AGB) phase and the Thermally Pulsing Asymptotic Giant Branch (TP-AGB) phase. Initially during the E-AGB phase, the helium shell undergoes stable nuclear fusion, and the stellar core consists of inert carbon and oxygen. Over time, the star enters the TP-AGB phase, where it experiences periodic thermal pulses, meaning the helium shell ignites convectively in periodic thermal instabilities, causing significant fluctuations in both the star’s luminosity and mass loss rate (). During the TP-AGB phase, the nucleosynthesis process coupled with mixing episodes leads to significant changes in surface chemical composition, especially an increase in carbon content, with AGB stars within a certain mass range evolving into carbon stars at this stage. Moreover, the large-scale mass loss during the TP-AGB phase ultimately determines whether the star can form a planetary nebula and evolve into a white dwarf ().
Another common basis for classification is the surface chemical composition, which mainly divides AGB stars into oxygen-rich AGB stars (O-rich AGB) and carbon-rich AGB stars (C-rich AGB). Oxygen-rich AGB stars, whose spectral types include M-type and S-type, are characterized by a C/O ratio less than 1, with TiO as their primary molecular absorption line; these stars are usually in the earlier stages of AGB evolution (). As the nucleosynthesis processes proceed, stars of about 2–3 gradually evolve into carbon-rich stars, whose spectral type is classified as C-type, and they are characterized by a C/O ratio greater than 1. Their main absorption lines are carbon-based molecules such as and CN, and these stars are typically in the later stages of AGB evolution.
AGB stars can also be classified based on their photometric periods. As soon as stars enter the TP-AGB phase,the majority of them exhibit variability in their luminosity due to thermal pulses. These variable stars are further divided into Mira variables, Semi-Regular Variables (SRVs), and Irregular variables. The distinctive features are the regularity of light curves, their amplitude and their period (; ; ).
Methods for searching for AGB stars have evolved progressively from traditional manual feature construction to modern machine learning algorithms. Traditional approaches primarily rely on astronomers’ expertise, identifying AGB stars through specific features such as spectral characteristics and photometric variability (; ). In the optical wavelength range, the low surface temperatures of AGB stars cause their spectra to exhibit prominent absorption lines of oxide molecules (e.g., TiO and VO) or carbon-based molecules (e.g., and CN). These features are used to distinguish oxygen-rich AGB stars from carbon-rich stars ().
Infrared search methods are also particularly important because AGB stars form extensive dust shells due to intense mass loss, leading to significantly enhanced infrared emission. Consequently, infrared survey projects such as 2MASS (Two Micron All Sky Survey) and WISE (Wide-field Infrared Survey Explorer) have become essential resources for identifying AGB stars (; Wright et al., 2010). Similarly, sub-millimeter and radio observations provide a route to penetrate obscuration using molecular lines and masers. Observations in the radio band primarily rely on molecular gases produced during the mass-loss processes of AGB stars, such as OH molecular lines (), or masers like OH, O and SiO masers (; ; ; ).
Additionally, since AGB stars are typically variable, they can be effectively identified through the characteristics of their light curves. Survey projects such as OGLE (Optical Gravitational Lensing Experiment) and ASAS-SN (All-Sky Automated Survey for Supernovae) have extensively utilized this identification method in their searches (; ).
With the growth of data volume and the rapid advancement of computer technology, machine learning has gradually become an effective tool for searching AGB stars. Compared to traditional methods of manual feature extraction and visual inspection, machine learning enables the identification of complex patterns in high-dimensional survey data such as spectra. Researchers have employed various machine learning techniques, including Support Vector Machines (SVM), XGBoost, and Convolutional Neural Networks (CNNs), among others (; ; ; ; ; ; Ye et al., 2025; ), to classify AGB stars with greater accuracy. These methods have been especially effective in identifying carbon-rich (C-type) and S-type AGB stars, which exhibit characteristic molecular bands (e.g., , CN, or ZrO) in their spectra. For example, SVM and ensemble methods (like XGBoost) have been used to distinguish S-type stars based on ZrO band indices (; ), while CNN-based models have achieved high accuracy in classifying carbon stars from large spectroscopic datasets (; Ye et al., 2025). However, due to the spectral overlap between oxygen-rich AGB stars and other red giants, current machine learning applications for O-rich AGB identification remain limited. Expanding the use of interpretable algorithms and multimodal data fusion is expected to further enhance the efficiency and precision of machine learning in AGB star searches.
2 Characteristics of AGB stars
Observationally, AGB stars appear as bright red giants, with luminosities reaching several thousand times that of the Sun.
2.1 Structure and evolution of AGB stars
An AGB star can be described as consisting of six parts (see Figure 1): (i) a degenerate C/O core, (ii) a He burning shell, (iii) a H burning shell, (iv) a large and cold convective stellar envelope, (v) a tenuous dynamical atmosphere, and (vi) a very large, very diluted, and cold circumstellar envelope.
FIGURE 1
Thus, an AGB star covers more than 10 orders of magnitude in size scale, 30 orders of magnitude in density scale, and seven orders of magnitude in temperature scale. Specifically, the temperature range of AGB stars is approximately 10 K to K, with the temperature gradually decreasing from the inside to the outside. The temperature of the He-burning region is about K, while the temperature of the outermost circumstellar envelope is below 10 K (e.g., ; ; ).
The evolution of the AGB phase can be broadly divided into two stages: E-AGB and TP-AGB. During the E-AGB phase, the helium shell burns while the hydrogen shell is extinguished. Toward the end of the E-AGB phase, the hydrogen shell contracts and heats up until it reignites. As the intershell region accumulates additional helium produced by the hydrogen-burning shell above, the He shell reaches the conditions necessary for unstable ignition. This marks the onset of the TP-AGB phase, characterized by the thermally unstable He-burning shell undergoing periodic thermal pulses. After the onset of the TP-AGB phase, as helium shell burning proceeds, the He-rich intershell region expands, causing the temperature in the hydrogen shell to decrease and hydrogen burning to be extinguished. Expansion and cooling of the intershell region can also lead to a deeper penetration of the outer convective envelope. In some cases, convection can penetrate beyond the now extinct H-burning shell, such that material from the intershell region is mixed into the outer envelope. This phenomenon is called third dredge-up (TDU). Then, as the star contracts again under gravity, the hydrogen shell region heats up, hydrogen burning restarts and the He-burning shell becomes inactive. A long phase of stable H-shell burning follows in which the mass of the intershell region grows until the next thermal pulse occurs.
During the TP-AGB phase, the third dredge-up episode mixes carbon from the intershell region into the stellar envelope. Whether an AGB star evolves into a carbon star depends on several factors, including metallicity, initial stellar mass, mass loss rate, the dredge-up efficiency, the occurrence of Hot Bottom Burning (HBB), and extra mixing (e.g., ; ; ; ). For example, both sufficient thermal pulses and adequate dredge-up efficiency are required to accumulate enough carbon for the C/O ratio to exceed 1, since typically increases with successive pulses (). The 12C-enrichment by TDU is partly compensated by its destruction in extra-mixing processing during the interpulse stages (). In addition, a sudden massive ejection event may terminate the AGB phase of the central source in advance, preventing its transformation into a carbon star ().
The third dredge-up also brings elements synthesized via the slow neutron-capture process (s-process) into the stellar envelope. In the AGB stars the s-process occurs in the He rich layers of the stars, during both the interpulse period (the H-shell is burning) thanks to the neutrons delivered by the 13C (,n)16O reaction and the thermal pulses thanks to the neutrons from 22Ne (,n)25Mg. In the most of the AGBs the 13C (,n)16O is the main source of neutrons for the s-process. These neutrons are captured by seed nuclei, producing heavier elements through a sequence of slow neutron captures and -decays. Typical s-process elements include light-s elements such as Sr, Y, and Zr, as well as heavy-s elements such as Ba, La, and Pb. This nucleosynthetic pathway is a hallmark of AGB stars confirmed by . The TP-AGB phase is characterized by the simultaneous action of internal nucleosynthesis, convective mixing and a strong stellar wind. This leads to them to significantly contribute to the chemical enrichment of galaxies as well as up to 40 per cent of interstellar medium dust (e.g., ; ).
2.2 Observational characteristics of AGB stars
Features in the optical band. AGB stars are classified based on the C/O ratio in their atmospheres, with oxygen-rich AGB stars having C/O < 1 and carbon-rich AGB stars having C/O > 1. Alternatively, they can be classified by spectral type (; ): M-type (C/O < 0.5), S-type (0.5 < C/O < 1), C-type (C/O > 1), and the intermediate MS and SC type. Optical observational characteristics of AGB stars include: M-type stars have spectra dominated by TiO molecular bands (and VO for very cool stars); the spectra of S-type stars are characterized by enhanced bands of molecules involving s-process elements (like Sr, Y, Zr, Ba, La, Ce, Nd, Sm, Tc, and Pb), such as ZrO, YO and LaO (); and C-type stars have spectra dominated by and CN molecular bands (as shown in Figure 2). The MS type is a transitional type between M-type and S-type stars, containing strong YO, TiO and weak ZrO molecules, while the SC type is a transitional type between S-type and C-type stars, containing weak ZrO, , and strong Na I D-lines (; ; ). In addition, recent studies suggest that a small number of S-type stars also exhibit the CN characteristics of C-type stars. The possible reason is that the external ultraviolet radiation field of these stars may, in certain cases, effectively promote the photodissociation of HCN, thereby increasing the abundance of CN ().
FIGURE 2
Molecular line features in the infrared and radio band. In the infrared band, O-rich AGB stars exhibit oxygen-rich molecular bands such as SiO, and O, while C-rich AGB stars display carbon-rich molecular bands such as and HCN () (as shown in Figure 3). In the radio band, common molecular spectral lines in C-rich AGB stars include H, H, N (). And in O-rich AGB stars, the main molecular lines are OH lines ().
FIGURE 3
Dust features. Oxygen-rich AGB stars with amorphous silicate in the dust envelop exhibit either absorption or emission features at around 10 and 18 m, depending on the optical depth and mass-loss rate (
FIGURE 4

ISO spectra of several O-rich AGB stars in the 6–200 m region are ordered by their 10 m optical depth, with stars having higher mass loss rates generally showing deeper silicate absorption at 10 m. Credit:
Masers features. Masers in the circumstellar envelopes of oxygen-rich stars include OH masers at 1612, 1665 and 1667 MHz (
Variability features. The TP-AGB phase is characterized by variability in brightness. Mira stars are a type of prominent variable stars located in the TP-AGB phase, and their light curves have obvious features of large amplitudes ( mag, mag, mag, and mag) and long periods (–1000 days) (
3 Traditional methods for searching AGB stars
In practical observations and data analysis, the identification of AGB stars relies on various observational indicators and methods. Since AGB stars exhibit distinct characteristics in terms of spectral features, color, magnitude, and maser distribution, the search for AGB stars typically involves a multidimensional approach for comprehensive analysis. This section will discuss in detail the identification methods and current applications of AGB stars from four perspectives: color and magnitude, light curves, infrared spectra, and radio masers. By utilizing different observational techniques, we can capture the prominent features of AGB stars across multiple wavelengths, thereby improving the identification rate and classification accuracy of AGB stars.
3.1 Search methods using color and magnitude criteria
Color-Color Diagrams and Color-Magnitude Diagrams are commonly used tools in astronomy for classifying and studying stellar types, and they are also applicable for identifying AGB stars. Among them, the color-magnitude diagram is essentially the observational version of the Hertzsprung-Russell diagram (HR diagram).
The color of a star is closely related to its surface temperature. Stars with higher temperatures emit more blue light, appearing bluer, while stars with lower temperatures appear redder. AGB stars are generally cooler stars with lower temperatures, so they are positioned redder on Color-Color Diagrams and Color-Magnitude Diagrams, showing a higher degree of redness. AGB stars are giant stars with large radii and high luminosities, so they are typically located in the high-luminosity, redder regions of the color-magnitude diagram.
The color-color diagrams or color-magnitude diagrams currently used to search for AGB stars are essentially linear separation methods. The commonly used color diagram methods are shown in Table 1.
TABLE 1
| Data sources | Methods | References |
|---|---|---|
| 2MASS/UKIRT | ||
| Wiśniewski et al. (2011) | ||
| (H-K, J-H) Color-Color Diagram | ||
| (J-K, K) Color-Magnitude Diagram | ||
| DENIS | (J-K, I-J) Color-Color Diagram | |
| Strömgren | (b, b-y) Color-Magnitude Diagram | |
| (y, v-y) Color-Magnitude Diagram | ||
| Subaru Suprime-Cam | (V-I, I)Color-Magnitude Diagram | |
| CFHT V and I, TiO and CN filters | (V-I, I) Color-Magnitude Diagram | |
| Du Pont R and I, TiO and CN filters | (R-I, CN-TiO) Color-Color Diagram | |
| NOT V and i, TiO and CN filters | (V-i/I, CN-TiO) Color-Color Diagram | |
| WISE | (W1-W2, W3-W4) Color-Color Diagram | |
| Wu et al. (2018) | ||
| WISE and 2MASS | (J-Ks, Ks-W3) Color-Color Diagram | |
| MSX and 2MASS | [A]-[D], [A]-[E] and [C]-[E] color index | |
| (K-A, J-K) and (K-A, H-K) Color-Color Diagram | ||
| Spitzer IRAC/MIPS | ([3.6]-[8.0], [8.0]) Color-Magnitude Diagram | |
| ([8.0]-[24], [5.8]-[8.0]) Color-Color Diagram | ||
| Spitzer IRAC and 2MASS | (J-[3.6], [3.6]) Color-Magnitude Diagram | |
| IRAS and/or 2MASS | ([12]-[25], [25]-[60]) Color-Color Diagram | |
| (K-[12], [12]-[25]) Color-Color Diagram | ||
| IRTS | ([2.30–3.77], [2.20–2.30]) Color-Color Diagram | |
| IRTS Team et al. (1997) | ||
| SDSS | (g-r, g-i) Color-Color Diagram |
Traditional AGB star search methods based on color diagrams.
For example, the (-W3, J-) color-color diagram based on WISE and 2MASS is shown in Figure 5 (
FIGURE 5

J-Ks versus Ks-W3 color-color diagram of the known C-rich and O-rich stars (blue: C-rich AGB stars; green: AGB stars; red: O-rich stars). Picture reproduced from
For 0.35 < ( - W3) < 1.45:
for ( - W3) > 1.45:and,
The (J-, ) color-magnitude diagram based on 2MASS JHK photometry is shown in Figure 6 (
FIGURE 6

J - vs. color-magnitude diagram showing the separation of carbon-rich and oxygen-rich AGB stars in the Small Magellanic Cloud, with the selection of C-rich AGB (pink), O-rich AGB (blue), RSG (red),and RGB (white) stars shown in contours. The x-AGB stars (heavily extinguished “extreme” stars with a thick dust envelope), are also plotted in green. Picture reproduced from
The three solid lines in the figure correspond to Equations 7–9:The (TiO CN, V i) color-color diagram based on the V and i filters is shown in Figure 7, which indicate effective temperature, and the TiO and CN filters, which distinguish between O-rich AGB and C-rich AGB characteristics (
FIGURE 7

Color-color diagram and the selection areas for O-rich and C-rich stars. Synthetic photometry is plotted as well (M-stars with open circles, C-stars with asterisks). Credit:
For O-rich AGB stars:
For C-rich AGB stars:
3.2 Search methods based on light curves
Since E-AGB stars have not exhibited obvious variability characteristics in studies to date, they cannot yet be detected through light curves. However, TP-AGB stars typically exhibit various forms of variability: many are Long Period Variables (LPVs) with large amplitude variations, known as Mira variables, while others show semiregular or irregular pulsations. The large-amplitude variations characteristic of Mira variables allow TP-AGB star samples to be identified from variable star catalogs based on light curve amplitude criteria (
3.3 Search methods based on infrared spectra
Currently, the search for AGB stars based on infrared spectroscopy primarily revolves around infrared spectral data from IRAS and ISO (
3.4 Search methods based on radio masers
Masers (Microwave Amplification by Stimulated Emission of Radiation) occur in the outer atmosphere of AGB stars, particularly near the circumstellar envelope. Examples include SiO, O, OH, HCN and SiS masers. The search methods are divided into two types. One is blind searches, where all stars in a specified region of the sky are checked for maser emission. The other is targeted searches, which use cataloged right ascension and declination data of cold giant stars obtained from previous surveys or databases. These positional data serve as the basis for the detection of maser emission from cold giant stars. Maser radiation appears as narrow and intense spectral lines, distinct from thermal emission from other astrophysical sources. Radio interferometry provides high-resolution imaging that enables precise astrometric and kinematic measurements of AGB masers (e.g.,
4 Machine-learning-based methods for searching AGB stars
Identifying AGB stars in large volumes of observational data is a complex task, and traditional methods relying on manually constructed features face limitations in both efficiency and accuracy. The introduction of machine learning techniques can significantly enhance the speed and precision of AGB star identification. Currently, machine learning-based methods have been primarily applied to identify specific AGB star subtypes: S-type stars and carbon stars. For the majority of oxygen-rich AGB stars (M-type stars), due to their relatively indistinct characteristics, they are easily confused with stars in adjacent evolutionary stages (especially oxygen-rich red giants). Therefore, effective machine learning-based methods for specifically targeting this most common type of AGB star are still lacking. Given these constraints, the following sections will focus on the two AGB subtypes where machine learning approaches have shown practical success: the identification of S-type stars and C-rich AGB stars in detail.
4.1 Search methods for S-type stars based on machine learning
The methods for searching S-type stars have undergone significant historical development across different techniques. In the past, researchers have used spectra to identify S-type stars through visual inspection, initially focusing on ZrO spectral bands (
The machine learning-based search for S-type stars currently has two main papers (
In the first paper,
FIGURE 8

Location of the sample of low-temperature giants in the Hertzsprung-Russell diagram, from
Then, they calculated the ZrO band strength for S-type and M-type giant stars, using the criterion to preliminarily distinguish between S-type and M giants. This criterion was applied to the spectra of low-temperature giant stars. The band strength index was calculated using Equation 16:
where is the observed flux within the wavelength range , is the continuum window, is the ZrO molecular band window, and their definitions are listed in Table 2.
TABLE 2
| Band | ||||
|---|---|---|---|---|
| 6345.0 | 6352.0 | 6464.0 | 6472.0 | |
| 6378.0 | 6382.0 | 6464.0 | 6472.0 | |
| 6474.0 | 6479.0 | 6464.0 | 6472.0 | |
| 6508.0 | 6512.0 | 6464.0 | 6472.0 |
Boundaries of the continuum and ZrO molecular band window used in the computation of the band indices (
After the above steps, a sample of S-type star candidates was obtained, and then the authors used the SVM algorithm to further distinguish S-type stars from non-S-type stars among the obtained candidates. The input features were four ZrO bands with specific wavelengths listed in Table 2. Subsequently, the authors used absolute bolometric magnitudes to further distinguish between S-type stars and red supergiant stars (RSGs) to obtain a reliable set of S-type stars. The reliability of the classification results was verified by the stars’ positions on the color-magnitude diagram and their C/O ratios.
In subsequent research,
The application of these machine learning methods significantly improved the efficiency and accuracy of S-type star identification, providing valuable scientific insights into the evolution of AGB stars.
4.2 Search methods for carbon stars based on machine learning
Traditionally, the search for carbon stars is mainly carried out through feature engineering (manual extraction of features) for preliminary selection and linear division, followed by visual inspection. The extracted features primarily include the.
Molecular band indices of and CN, light curve characteristics, and color and luminosity features (
With the increasing volume of spectra from large-scale surveys, traditional methods that rely on linear division techniques using band indices and other extracted features have proven insufficient in terms of efficiency and accuracy, often missing many carbon star spectra. To improve the effectiveness of carbon star searches, subsequent studies have increasingly utilized more efficient machine learning algorithms.
Traditional machine learning methods for carbon star search require experienced experts to spend a lot of time on feature engineering, which plays a crucial role in machine learning. In contrast, deep learning is an end-to-end approach that reduces the reliance on manually constructed features. As the sample size of carbon stars increases, deep learning algorithms have also been introduced to carbon star searches.
Ye et al. (2025) propose a classification model named ‘GaiaNet’, an improved one-dimensional convolutional neural network specifically designed for handling Gaia’s XP spectra, and obtained 451 new candidate carbon stars. In this study, the SHAP interpretability method was utilized to enhance the interpretability of spectral features.
FIGURE 9

The convolutional neural network-based model architecture proposed by
In summary, with the continuous development of machine learning algorithms, from traditional spectral indices and linear division to machine learning models and deep learning models, the efficiency and accuracy of carbon star identification have been significantly improved. These studies provide important references for large-scale data processing of carbon stars in astronomy and offer well-prepared samples to further understand the properties and evolution of carbon stars.
5 Challenges and prospects
In the search for AGB stars, although machine learning and deep learning techniques have been introduced in recent years, significant challenges remain in handling complex observational data and achieving accurate identification. With the increasing volume of observational data and growing identification requirements, overcoming current technical bottlenecks and fully utilizing advanced algorithmic approaches have become key to enhancing the efficiency and accuracy of AGB star searches. This section will explore in detail the challenges and future directions in the search for AGB stars, with the aim of providing reference and inspiration for future research.
(1) Limitation of Data Sample Size and Algorithm Selection. Due to the scarcity of observational data on AGB stars, selecting an appropriate algorithm poses a major challenge. Deep learning models have an advantage in recognizing subtle differences in features, but they require a large amount of data. However, observational data on AGB stars are often scarce and difficult to obtain. In such cases, traditional feature engineering or machine learning methods may be more advantageous when working with limited samples. Therefore, future research should choose suitable algorithms based on specific data volume and feature requirements to improve identification accuracy and efficiency.
(2) Imbalanced Sample Problem. The scarcity of AGB star observational data, especially the imbalance between positive and negative samples, can affect the training performance of models. In the future, generative models (e.g., autoencoders and diffusion models) can be used to generate synthetic samples to compensate for the lack of real data. Balancing and generating samples is one of the key directions for improving the recognition performance of machine learning models.
(3) Multi-modal Data Fusion. The fusion of multi-modal data and the construction of multi-modal models for AGB stars is also a future research direction. By integrating multi-band observational data, researchers can more comprehensively characterize the physical properties of AGB stars. Using multi-modal data fusion techniques, such as contrastive learning methods or cross-modal attention mechanisms, can achieve effective integration of multiple data sources, thereby improving classification accuracy and model generalization ability. This provides an important direction for future research in the search for AGB stars.
(4) Challenges in Algorithm Interpretability. Current deep learning algorithms can achieve good classification results, but their “black box” nature makes them difficult for scientists to accept. To address this issue, future research can introduce interpretability tools such as SHAP to reveal the model’s focus on specific features and improve algorithm interpretability. For example, applying interpretative analysis to models like XGBoost, SVM, and CNN can help understand the influence of different spectral features on AGB star classification, thereby optimizing the feature selection process and enhancing the overall performance and interpretability of the model. This is also significant for theoretical validation and feature discovery in scientific research.
In conclusion, research on AGB star searches is gradually shifting from traditional methods to those based on machine learning and deep learning. In the future, with the collaborative application of various methods such as multi-modal data fusion, generative models, and interpretability tools, the identification and classification of AGB stars are expected to achieve higher precision and efficiency. This will not only enrich the AGB star sample library but also provide more solid data support for stellar evolution and cosmological research.
6 Conclusion
The search methods for AGB (Asymptotic Giant Branch) stars have evolved from traditional manual feature engineering and visual inspection to the gradual development of modern machine learning approaches. Early searches primarily relied on astronomers’ expertise to identify AGB stars based on their spectral features, photometry data and variability characteristics. However, with the increase in observational data and the application of multi-wavelength techniques such as infrared and radio, researchers have progressively incorporated more diverse observational methods, such as using enhanced infrared emission and maser radiation characteristics for detection. In recent years, machine learning and deep learning-based methods have become mainstream, significantly improving the efficiency and accuracy of AGB star searches.
Nevertheless, the search for AGB stars still faces numerous challenges. First, observational data are sparse and unevenly distributed, with a substantial imbalance between positive and negative samples, which poses difficulties for training machine learning models. Additionally, the “black box” nature of current deep learning models limits their widespread application in scientific research, as scientists find it challenging to understand the basis of the models’ decisions.
In the future, with the accumulation of observational data and the application of new technologies, the search and identification of AGB stars are expected to enter a new phase. The application of generative models, interpretability tools, and multimodal data fusion will further enhance the accuracy of AGB star identification and the interpretability of models. By integrating multi-wavelength data, scientists will be able to more comprehensively characterize the physical properties of AGB stars, providing robust theoretical and data support for stellar evolution and cosmological research. The field of AGB star searches will continue to achieve breakthroughs in both precision and efficiency, offering valuable insights into the late evolutionary processes of stars and the cycle of interstellar matter.
Statements
Author contributions
H-LL: Writing – original draft, Writing – review and editing. Y-BL: Writing – review and editing. A-LL: Resources, Writing – review and editing. Z-QZ: Writing – review and editing. X-MK: Writing – review and editing. Z-PY: Writing – review and editing. HJ: Writing – review and editing, Validation, Investigation. J-CL: Formal Analysis, Software, Writing – review and editing. SL: Formal Analysis, Software, Writing – review and editing.
Funding
The author(s) declare that financial support was received for the research and/or publication of this article. This work is supported by the National Natural Science Foundation of China (12273078, 12411530071, 12273075, 12473104, 12261141689), National Astronomical Observatories of the Chinese Academy of Sciences (No. E4ZR0516), and the Royal Society (IEC/NSFC/233140).
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Generative AI statement
The author(s) declare that Generative AI was used in the creation of this manuscript. Solely for literature search and language polishing.
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Summary
Keywords
asymptotic giant branch stars, late-type stars, stars evolution, Hertzsprung–Russell and colour–magnitude diagrams, machine learning
Citation
Lu H-L, Li Y-B, Luo A-L, Zou Z-Q, Kong X-M, Yi Z-P, Jones HRA, Liang J-C and Li S (2025) A review of the search for AGB stars. Front. Astron. Space Sci. 12:1587415. doi: 10.3389/fspas.2025.1587415
Received
04 March 2025
Accepted
16 June 2025
Published
24 July 2025
Volume
12 - 2025
Edited by
Maurizio Maria Busso, University of Perugia, Italy
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Copyright
© 2025 Lu, Li, Luo, Zou, Kong, Yi, Jones, Liang and Li.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Yin-Bi Li, ybli@bao.ac.cn; A-Li Luo, lal@nao.cas.cn
ORCID: Hai-Ling Lu, orcid.org/0000-0002-8252-8743; Yin-Bi Li, orcid.org/0000-0001-7607-2666; A-Li Luo, orcid.org/0000-0001-7865-2648; Zhi-Qiang Zou, orcid.org/0000-0003-2828-8491; Xiao-Ming Kong, orcid.org/0000-0002-4764-4749; Zhen-Ping Yi, orcid.org/0000-0001-8590-4110; Hugh R. A. Jones, orcid.org/0000-0003-0433-3665; Jun-Chao Liang, orcid.org/0009-0001-9085-8718; Shuo Li, orcid.org/0000-0002-8913-3605
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