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REVIEW 2 major objections 6 minor 73 references

Symbiotic novae

T0 review · 2 major / 6 minor · reviewed 2026-08-10 · deepseek-v4-flash

Pith's one-line read This review proposes a single 3D geometry for symbiotic novae, placing hard X-rays, radio synchrotron, and permitted lines at the equatorial wind-enhancement interface and forbidden lines in polar lobes.

desk verdict A useful review with a new catalog and a clear 3D synthesis, but the quantitative argument placing Hα and hard X-rays at the DEOP interface rests on a shaky FWHM-to-distance conversion. read the letter →

arxiv 2412.20499 v1 pith:DWSVGURD submitted 2024-12-29 astro-ph.SR astro-ph.HE

classification astro-ph.SRastro-ph.HE
keywords symbioticnovaeRSOphiuchiV407CygniDEOPredgiantwindnovaeruptionradiosynchrotronTCoronaeBorealis
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

Symbiotic novae are ordinary novae that erupt inside a binary where the white dwarf accretes from a red giant. The paper argues that the red giant's slow wind, gravitationally focused by the white dwarf, creates a dense equatorial structure (DEOP) that shapes everything we see. Based on the well-observed eruptions of RS Oph and V407 Cyg, the claim is that most hard X-rays, the central radio-synchrotron source, and the permitted optical lines all come from the shock interface between the ejecta and this DEOP, while the forbidden lines form in the inner regions of the bipolar lobes that escape along the poles. If correct, this gives a unified multi-wavelength map of a symbiotic nova and explains why the light curves at different wavelengths track each other so closely.

What carries the argument

The central object is the DEOP (Density Enhancement on the Orbital Plane): the dense, equatorial concentration of the red giant's wind created by the white dwarf's gravitational pull. The paper uses this structure as the organizing element of the whole multi-wavelength phenomenology; it sets the deceleration profile of the ejecta, determines where the hard X-ray and permitted-line shocks occur, and absorbs the radio emission from the far lobe. A second essential element is the measured contrast in deceleration: RS Oph's radio lobes maintain ~8150 km/s to day 64 while the H-alpha-emitting ejecta travel only ~15 AU in 100 days, showing that the permitted-line region is distinct from the fast polar outflow.

What would settle it

Very long baseline interferometry of RS Oph at late epochs (years after outburst) could image the central radio component: if it is found to move outward with the speed of the polar lobes rather than staying stationary near the binary position, the DEOP/ejecta interface would not be the source of the compact radio emission.

Watch

Extended reading notes

Core claim

The paper establishes a 3D picture of a symbiotic nova in which the ejecta from the white dwarf interact with the pre-existing circumstellar material in two distinct locations. Close to the binary, the ejecta slam into the DEOP, a density enhancement on the orbital plane formed when the white dwarf's gravity deflects the red giant's wind away from the poles. This DEOP/ejecta interface is where most of the hard X-rays, the compact radio-synchrotron component, and the permitted optical emission lines originate, and probably also the early gamma-ray emission. Toward the poles, where the density is much lower, the ejecta keep moving at thousands of km/s and form wide bipolar lobes whose inner regions host the forbidden lines, while the shocked outer edges are the site of the radio synchrotron lobes. The same model also explains the free-free absorption of the receding radio lobe by the ionized DEOP seen in RS Oph.

Load-bearing premise

The entire 3D picture rests on the assumption that the red giant's wind is efficiently deflected into a dense equatorial plane (DEOP) by the white dwarf's gravity, leaving the polar directions relatively empty; if this focusing is weaker than assumed, the assigned emission sites would have to be revised.

Editorial extensions

If this is right

  • The next outburst of T CrB, expected around 2025-2026, should show a prompt free-free radio flash from the UV-ionized red giant wind within 1-2 days, before synchrotron emission from shocked ejecta takes over.
  • If the 3D geometry is generic, then for any symbiotic nova the hard X-ray and H-alpha light curves should evolve identically and smoothly, as observed in RS Oph in both 2006 and 2021.
  • The DEOP/ejecta interface should remain a compact, unresolved radio source near the binary position, not expanding with the polar lobes, a prediction that VLBI can test.
  • Forbidden-line profiles should stay narrow and decouple from the broad permitted lines, tracing the slowly moving inner cavity of the bipolar lobes.
  • The recurrence timescale of symbiotic novae depends on how quickly the red giant wind refills the cavity blown by the previous eruption; RS Oph data suggest refilling is complete within about 9 years.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The DEOP wind-focusing mechanism implies that the mass-loss geometry of the red giant directly controls the nova's multi-wavelength visibility; an observer looking down the orbital poles would see a very different light curve than one looking through the orbital plane.
  • If the permitted lines and hard X-rays are co-spatial, then high-resolution spectroscopy during the first days could measure the density and temperature structure of the very inner DEOP, which is otherwise inaccessible.
  • The 'K' radio blob in V407 Cyg suggests that super-active accretion phases before eruption can eject collimated mass; searching for similar blobs in T CrB's pre-eruption data might reveal a common pre-nova ejection mechanism.
  • The paper's catalog of symbiotic novae, selected by M(K) from 2MASS and Gaia, could be extended to fainter or more reddened objects by using mid-infrared colors or variability, which would test whether the bimodal M(K) distribution is complete.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

2 major / 6 minor

Summary. The manuscript is an invited review of symbiotic novae, defined as thermonuclear runaways occurring in symbiotic binaries. It presents a revised catalog of Galactic symbiotic novae based on Gaia DR3 astrometry and 2MASS K-band photometry, then uses the well-observed 2006/2021 outbursts of RS Oph and the 2010 outburst of V407 Cyg to propose a three-dimensional model of the outburst structure. In this model, the gravitational focusing of the red-giant wind creates a dense equatorial structure (DEOP); the DEOP/ejecta interface is claimed to be the site of the hard X-rays, the central radio-synchrotron component, and the permitted optical lines, while forbidden lines form in the inner regions of the bipolar lobes. The review also discusses the UV-flash ionization of the red-giant wind, the prompt radio emission, and the expected imminent eruption of T CrB.

Significance. The paper is a valuable synthesis of multi-wavelength observations of two rare and closely monitored symbiotic novae, and the revised catalog is a useful community resource built on public data with explicit astrometric vetting. The proposed 3D model is physically motivated and makes specific, testable predictions (e.g., the spatial coincidence of Hα and hard X-rays, the DEOP as a free-free absorber, and the expected behavior of the upcoming T CrB outburst). The manuscript is also notable for explicitly integrating VLBI lobe kinematics, X-ray light curves, and optical line profiles into a single geometric picture.

major comments (2)
  1. [§3.2] The 14–15 AU distance traveled by the Hα-emitting ejecta is derived by integrating v_exp(t) = FWHM_Hα(t)/2.355, which assumes that the Gaussian line width directly measures the bulk expansion velocity of the emitting gas. This assumption is not uniquely justified: in an optically thick, velocity-stratified ejecta the line width can shrink as the photosphere recedes into slower material even if the ejecta coast at constant velocity, and in a radiative shock Hα can be emitted by decelerated post-shock gas whose width does not track the spatial displacement of the emitting region. The observed smooth FWHM ∝ t^(−0.6/−0.7) decline is equally compatible with a smooth radial density/velocity gradient in a no-deceleration flow. Because this conversion is the only quantitative estimate of the size of the Hα-emitting region, the statement in §3.4 that 'the DEOP/ejecta interface is the location from where originates most of the hard X-rays, the central radio-synchrotron component, and the permitted optical emission lines' is stronger than the current evidence supports. The authors should either provide an independent check (e.g., resolved line-profile constraints, light-echo bounds, or model comparison) or rephrase this conclusion as a working hypothesis to be tested by future observations.
  2. [§3.4] The model is presented as a '3D picture of RS Oph (serving also as a guideline for symbiotic novae in general)', but the two systems used to construct the model have qualitatively different deceleration behaviors: the radio lobes of RS Oph expand at constant 8150 km/s after day 14, while those of V407 Cyg decelerate from 6000 to 2800 km/s over days 20–91, a difference attributed to a factor of ~20 in orbital separation (§3.2). It is therefore not self-evident that a single geometric assignment (Hα and hard X-rays always at the DEOP interface, forbidden lines always in the inner lobes) applies to all symbiotic novae, including systems like T CrB that have not yet been observed in a comparable multi-wavelength campaign. The authors should state explicitly the conditions under which the model applies and what observations would falsify it for a particular system.
minor comments (6)
  1. [Abstract] The word 'syncrothron' appears in the abstract; it should be 'synchrotron'.
  2. [§1] In the sentence beginning 'Unbind from the system', the intended word is 'Unbound' rather than 'Unbind'.
  3. [§3.4] In the first paragraph of Section 3.4, 'lunched' should be 'launched'.
  4. [§4] In the final paragraph, 'will results is' should be 'will result in', and 'particoular' should be 'particular'.
  5. [Table 1] V5581 Sgr is listed with a negative Gaia DR3 parallax (π = −0.04, σ(π) = 0.145); the text mentions that some systems use literature distances, but it is not clear which rows use that approach and how the adopted distance for V5581 Sgr was determined, so a clarifying note would be helpful.
  6. [§3.2] The recombination e-folding times, derived electron densities, and FWHM power-law slopes are quoted without uncertainties; adding error bars or a systematic-uncertainty statement would strengthen the quantitative comparisons in Figures 2 and 4.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the 3D model is an interpretive synthesis of independent multi-wavelength data, and no derived quantity reduces by construction to a fitted input or to a self-citation chain.

full rationale

The paper is an invited review whose central contribution is a 3D interpretive model for symbiotic novae. The model locates hard X-rays, permitted lines, and the central radio-synchrotron source at the DEOP/ejecta interface, and forbidden lines in the inner bipolar lobes, using converging but independent evidence: VLBI radio-lobe kinematics, free-free absorption geometry, H-alpha FWHM evolution, Swift X-ray light curves, and nebular line behavior. No equation in the paper defines a derived quantity in terms of an earlier fitted quantity in a way that makes the conclusion true by construction. The H-alpha FWHM-to-distance conversion (FWHM/2.355 integrated over time) is an interpretive assumption about what the line width measures, not a circular reduction: it is not the case that the distance traveled is inserted into the same formula that produces the FWHM, nor is the DEOP location imposed as an input and then recovered as an output. Similarly, the matching time dependence of H-alpha and hard X-ray fluxes is cited as empirical support for co-spatiality, but co-spatiality is not used to define either light curve. The heavy reliance on the author's own earlier papers is for observational data (spectra, VLBI maps, X-ray decompositions) and catalog work; these are external empirical measurements, and the central conclusion does not rest on an unverified self-citation or on a uniqueness theorem imported from the author's prior work. The DEOP concept itself is grounded in cited external wind-focusing models and in direct radio evidence of bipolar lobes and free-free absorption. Potential weaknesses such as the degeneracy between line-width shrinking and optical-depth/velocity-stratification effects are modeling uncertainties, not circularities. Accordingly, the derivation chain is self-contained against external benchmarks and the circularity score is 0.

Assumptions & free parameters 6 free parameters · 4 assumptions · 0 invented entities

The paper introduces no new physical entities. It adopts the DEOP concept from prior work and renames the old 'symbiotic nova' phenomenon as SETE. The free parameters are fits to observed light curves and a classification threshold.

free parameters (6)
  • Recombination e-folding time for V407 Cyg 2010 = 100 hours
    Fitted to the decline of the narrow Hα component in Fig. 2; used to derive electron density 6.6e6 cm^-3.
  • Recombination e-folding time for RS Oph 2021 = 60 hours
    Fitted to the narrow Hα decline in Fig. 2; used to derive electron density 1.1e7 cm^-3.
  • Recombination e-folding time for V3890 Sgr 2019 = 13 hours
    Fitted to narrow Hα and continuum decline in Fig. 2; used to derive electron density 5.0e7 cm^-3.
  • FWHM power-law slope for V407 Cyg Hα = -0.59
    Fit to FWHM evolution in Fig. 4; used to infer continuous deceleration of ejecta.
  • FWHM power-law slope for RS Oph Hα = -0.73
    Fit to FWHM evolution in Fig. 4; used to infer continuous deceleration of ejecta.
  • M(K) cutoff for symbiotic novae = -4.0 mag
    Chosen to separate the two peaks in Fig. 1; used to define the catalog in Table 1.
assumptions (4)
  • domain assumption The ejecta are decelerated by sweeping up the red giant wind, with kinetic energy converted to radiation.
    Section 3.2; standard nova-in-symbiotic model.
  • domain assumption The red giant wind is gravitationally focused by the WD into a density enhancement on the orbital plane (DEOP).
    Section 3.2, DEOP paragraph; based on Mohamed & Podsiadlowski 2012 and Skopal & Cariková 2015.
  • standard math The recombination timescale formula t_rec = 0.66 T_e^0.8 n_e^-1 (Ferland 2003) applies to the flashed wind.
    Section 3.1, used to convert recombination e-folding times to electron densities.
  • domain assumption The WD in symbiotic novae undergoes the same thermonuclear runaway as in classical novae.
    Section 1, adopted definition.

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Cite this review

Pith. "Pith review of Symbiotic novae." pith.science (2026). https://pith.science/paper/DWSVGURD

@misc{pith2026241220499,
  author       = {Pith},
  title        = {Pith review of: Symbiotic novae},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/DWSVGURD}},
  note         = {Machine review of arXiv:2412.20499}
}
read the original abstract

(Invited Review) According to modern definition, a symbiotic nova is an otherwise normal nova (i.e. powered by explosive thermonuclear burning) that erupts within a symbiotic star, which is a binary where a WD accretes from a cool giant companion. Guided primarily by the very well observed eruptions of RS Oph in 2006 and 2021, and that of V407 Cyg in 2010, we investigate the main multi-wavelength properties of symbiotic novae and their relation to classical novae, and propose a 3D model structure that identifies the emitting source location for hard and supersoft X-rays, radio syncrothron and thermal, permitted and forbidden emission lines. Very few symbiotic novae are known in the Galaxy, and we compile a revised catalog based on firm astrometric identification. The exciting prospect of an imminent new outburst of T CrB is also discussed.

Figures

Figures reproduced from arXiv: 2412.20499 by the authors.

Figure 1
Figure 1. Distribution in absolute M(K) magnitude of all validated thermonuclear runaway novae with an accurate astrometric identification. Those containing a red giant (M(K)≤−4 mag) are listed in Tab. 1. As a final step, the Gaia DR3 parallax was adopted to compute the absolute magnitude of novae in the K band (2.2 µm), which resulted in the distribution of [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. High-resolution Hα profiles covering the first days for the outburst of three symbiotic novae, to highlight the sharp component from the recombining flashed-wind of the RG and the broad one from the expanding ejecta. For comparison, the early photometric evolution of V3890 Sgr is deconvolved into the same two components (data from Munari et al., 2011; Munari & Valisa, 2021, F. Walter private comm.) [PITH_FULL_IMAGE… view at source ↗
Figure 3
Figure 3. Top: VLBI high resolution radio maps of the 2010 and 2021 outbursts of the symbiotic novae V407 Cyg and RS Oph. The red cross marks the astrometric position from Gaia. Bottom right: cartoon highlighting the location of DEOP and the extinction it excerpts on the receding lobe of RS Oph (compare with panel directly above). Bottom left: the radial dependence of density within DEOP of RS Oph (data from Giroletti et al.,… view at source ↗
Figures from the paper (3 more)
Figure 4
Figure 4. Figure 4: Comparing the evolution of the FWHM of Balmer and [OIII] emission lines (left) and the space velocity of the radio bipolar jets (right) for V407 Cyg and RS Oph (data from Munari et al., 2011; Giroletti et al., 2020; Munari & Valisa, 2022; Lico et al., 2024). synchrotro…
Figure 5
Figure 5. Figure 5: Comparing the evolution in flux for the 2006 and 2021 outbursts of RS Oph for hard X-rays, super-soft X-rays, permitted and coronal emission lines (data from Page et al., 2022; Munari & Valisa, 2022). The fluxes of optical emission lines are in erg cm−2 s −1 . Supersof…
Figure 6
Figure 6. Figure 6: Artistic impression showing the location of key emission features in RS Oph around day +35 of the outburst (drawing not to scale). The WD + RG binary is at the center, DEOP (density enhancement on the orbital plane) is seen edge-on, and the polar directions run vertica…

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Works this paper leans on

73 extracted references · 27 canonical work pages

  1. [1]

    , " * write output.state after.block = add.period write newline

    ENTRY address archiveprefix author booktitle chapter edition editor howpublished institution eprint journal key month note number organization pages publisher school series title type volume year doi label extra.label sort.label short.list INTEGERS output.state before.all mid.sentence after.sentence after.block FUNCTION init.state.consts #0 'before.all :=...

  2. [2]

    write newline

    " write newline "" before.all 'output.state := FUNCTION n.dashify 't := "" t empty not t #1 #1 substring "-" = t #1 #2 substring "--" = not "--" * t #2 global.max substring 't := t #1 #1 substring "-" = "-" * t #2 global.max substring 't := while if t #1 #1 substring * t #2 global.max substring 't := if while FUNCTION word.in bbl.in " " * FUNCTION format....

  3. [3]

    A., Ackermann , M., Ajello , M., et al

    Abdo , A. A., Ackermann , M., Ajello , M., et al. , Gamma-Ray Emission Concurrent with the Nova in the Symbiotic Binary V407 Cygni . 2010, Science , 329 , 817, DOI: 10.1126/science.1192537

  4. [4]

    A., Ansoldi , S., Antonelli , L

    Acciari , V. A., Ansoldi , S., Antonelli , L. A., et al. , Proton acceleration in thermonuclear nova explosions revealed by gamma rays . 2022, Nature Astronomy , 6 , 689, DOI: 10.1038/s41550-022-01640-z

  5. [5]

    A., On the late-type components of slow novae and symbiotic stars

    Allen , D. A., On the late-type components of slow novae and symbiotic stars. 1980, , 192 , 521, DOI: 10.1093/mnras/192.3.521

  6. [6]

    , Measuring the Mass Radius Relation of White Dwarfs Using Wide Binaries

    Arseneau , S., Chandra , V., Hwang , H.-C., et al. , Measuring the Mass Radius Relation of White Dwarfs Using Wide Binaries . 2024, , 963 , 17, DOI: 10.3847/1538-4357/ad2168

  7. [7]

    Banerjee , D. P. K., Joshi , V., Venkataraman , V., et al. , Near-IR Studies of Recurrent Nova V745 Scorpii during its 2014 Outburst . 2014, , 785 , L11, DOI: 10.1088/2041-8205/785/1/L11

  8. [8]

    Bode , M. F. & Evans , A., eds. 1989, Classical novae (John Wiley & Sons)

Show all 73 references
  1. [9]

    Bode , M. F. & Evans , A., eds. 2008, Classical Novae (Cambridge Univ. Press)

  2. [10]

    E., & Garc \' a , L

    Brandi , E., Quiroga , C., Miko ajewska , J., Ferrer , O. E., & Garc \' a , L. G., Spectroscopic orbits and variations of RS Ophiuchi . 2009, , 497 , 815, DOI: 10.1051/0004-6361/200811417

  3. [11]

    2004, ESA Special Publication, Vol

    Cassatella , A., Gonz \'a lez-Riestra , R., & Selvelli , P., eds. 2004, ESA Special Publication, Vol. 1283 , INES Access Guide No. 3 - Classical Novae

  4. [12]

    L., Gilmozzi , R., Bianchini , A., & Friedjung , M., IUE observations of faint old novae

    Cassatella , A., Selvelli , P. L., Gilmozzi , R., Bianchini , A., & Friedjung , M., IUE observations of faint old novae. 1990, in Accretion-Powered Compact Binaries , ed. C. W. Mauche (Cambridge Univ. Press), 373--376

  5. [13]

    & Viotti , R., eds

    Cassatella , A. & Viotti , R., eds. 1990, Lecture Notes in Physics, Vol. 369 , Physics of Classical Novae (Springer-Verlag)

  6. [14]

    F., & Shara , M

    Downes , R., Webbink , R. F., & Shara , M. M., A Catalog and Atlas of Cataclysmic Variables-Second Edition . 1997, , 109 , 345, DOI: 10.1086/133900

  7. [15]

    Downes , R. A. & Shara , M. M., A Catalog of Cataclysmic Variables . 1993, , 105 , 127, DOI: 10.1086/133139

  8. [16]

    A., Webbink , R

    Downes , R. A., Webbink , R. F., Shara , M. M., et al. , A Catalog and Atlas of Cataclysmic Variables: The Living Edition . 2001, , 113 , 764, DOI: 10.1086/320802

  9. [17]

    Duerbeck , H. W. 1987, A reference catalogue and atlas of galactic novae (D. Reidel Publ.)

  10. [18]

    F., O'Brien , T

    Evans , A., Bode , M. F., O'Brien , T. J., & Darnley , M. J., eds. 2008, Astronomical Society of the Pacific Conference Series, Vol. 401 , RS Ophiuchi (2006) and the Recurrent Nova Phenomenon

  11. [19]

    J., Quantitative Spectroscopy of Photoionized Clouds

    Ferland , G. J., Quantitative Spectroscopy of Photoionized Clouds . 2003, , 41 , 517, DOI: 10.1146/annurev.astro.41.011802.094836

  12. [20]

    Y., A Theory of Hydrogen Shell Flashes on Accreting White Dwarfs - Part Two - the Stable Shell Burning and the Recurrence Period of Shell Flashes

    Fujimoto , M. Y., A Theory of Hydrogen Shell Flashes on Accreting White Dwarfs - Part Two - the Stable Shell Burning and the Recurrence Period of Shell Flashes . 1982 a , , 257 , 767, DOI: 10.1086/160030

  13. [21]

    Y., A theory of hydrogen shell flashes on accreting white dwarfs

    Fujimoto , M. Y., A theory of hydrogen shell flashes on accreting white dwarfs. I - Their progress and the expansion of the envelope. II - The stable shell burning and the recurrence period of shell flashes . 1982 b , , 257 , 752, DOI: 10.1086/160029

  14. [22]

    2016, , 595 , A1, DOI: 10.1051/0004-6361/201629272

    Gaia Collaboration , The Gaia mission . 2016, , 595 , A1, DOI: 10.1051/0004-6361/201629272

  15. [23]

    Summary of the content and survey properties

    Gaia Collaboration , Gaia Data Release 3. Summary of the content and survey properties . 2023, , 674 , A1, DOI: 10.1051/0004-6361/202243940

  16. [24]

    Gaposchkin , C. H. P. 1957, The Galactic Novae (Dover Pub.)

  17. [25]

    , Very long baseline interferometry imaging of the advancing ejecta in the first gamma-ray nova V407 Cygni

    Giroletti , M., Munari , U., K \"o rding , E., et al. , Very long baseline interferometry imaging of the advancing ejecta in the first gamma-ray nova V407 Cygni . 2020, , 638 , A130, DOI: 10.1051/0004-6361/202038142

  18. [26]

    H. E. S. S. Collaboration , Aharonian , F., Ait Benkhali , F., et al. , Time-resolved hadronic particle acceleration in the recurrent nova RS Ophiuchi . 2022, Science , 376 , 77, DOI: 10.1126/science.abn0567

  19. [27]

    & Jos \'e , J., eds

    Hernanz , M. & Jos \'e , J., eds. 2002, American Institute of Physics Conference Series, Vol. 637 , Classical Nova Explosions (AIP)

  20. [28]

    H., Fekel , F

    Hinkle , K. H., Fekel , F. C., Joyce , R. R., & Wood , P., Infrared Spectroscopy of Symbiotic Stars. IX. D-type Symbiotic Novae . 2013, , 770 , 28, DOI: 10.1088/0004-637X/770/1/28

  21. [29]

    1982, , 259 , 244, DOI: 10.1086/160164

    Iben , I., J., Hot accreting white dwarfs in the quasi-static approximation . 1982, , 259 , 244, DOI: 10.1086/160164

  22. [30]

    Kenyon , S. J. 1986, The symbiotic stars (Cambridge Univ. Press)

  23. [31]

    Kenyon , S. J. & Truran , J. W., The outbursts of symbiotic novae. 1983, , 273 , 280, DOI: 10.1086/161367

  24. [32]

    A., Shenavrin , V

    Kolotilov , E. A., Shenavrin , V. I., Shugarov , S. Y., & Yudin , B. F., UBVJHKLM photometry of the symbiotic Mira V407 Cyg in 1998 2002 . 2003, Astronomy Reports , 47 , 777, DOI: 10.1134/1.1611218

  25. [33]

    , High-resolution imaging of the evolving bipolar outflows in symbiotic novae: The case of the RS Ophiuchi 2021 nova outburst

    Lico , R., Giroletti , M., Munari , U., et al. , High-resolution imaging of the evolving bipolar outflows in symbiotic novae: The case of the RS Ophiuchi 2021 nova outburst . 2024, , 692 , A107, DOI: 10.1051/0004-6361/202451364

  26. [34]

    Liimets , T., Corradi , R. L. M., Santander-Garc \' a , M., et al. , A Three-dimensional View of the Remnant of Nova Persei 1901 (GK Per) . 2012, , 761 , 34, DOI: 10.1088/0004-637X/761/1/34

  27. [35]

    & Podsiadlowski , P., Mass Transfer in Mira-type Binaries

    Mohamed , S. & Podsiadlowski , P., Mass Transfer in Mira-type Binaries . 2012, Baltic Astronomy , 21 , 88, DOI: 10.1515/astro-2017-0362

  28. [36]

    D., et al

    Molina , I., Chomiuk , L., Linford , J. D., et al. , The symbiotic recurrent nova V745 Sco at radio wavelengths . 2024, , 534 , 1227, DOI: 10.1093/mnras/stae2093

  29. [37]

    Montez , R., Luna , G. J. M., Mukai , K., Sokoloski , J. L., & Kastner , J. H., Expanding Bipolar X-Ray Structure After the 2006 Eruption of RS Oph . 2022, , 926 , 100, DOI: 10.3847/1538-4357/ac4583

  30. [38]

    2019, in The Impact of Binary Stars on Stellar Evolution , ed

    Munari , U., The Symbiotic Stars . 2019, in The Impact of Binary Stars on Stellar Evolution , ed. G. Beccari & H. Boffin , arXiv:1909.01389

  31. [39]

    2016, , 47 , 7, DOI: 10.1016/j.newast.2016.01.002

    Munari , U., Dallaporta , S., & Cherini , G., The 2015 super-active state of recurrent nova T CrB and the long term evolution after the 1946 outburst . 2016, , 47 , 7, DOI: 10.1016/j.newast.2016.01.002

  32. [40]

    , Radio interferometric imaging of RS Oph bipolar ejecta for the 2021 nova outburst

    Munari , U., Giroletti , M., Marcote , B., et al. , Radio interferometric imaging of RS Oph bipolar ejecta for the 2021 nova outburst . 2022, , 666 , L6, DOI: 10.1051/0004-6361/202244821

  33. [41]

    H., Ashok , N

    Munari , U., Joshi , V. H., Ashok , N. M., et al. , The 2010 nova outburst of the symbiotic Mira V407 Cyg . 2011, , 410 , L52, DOI: 10.1111/j.1745-3933.2010.00979.x

  34. [42]

    & Tabacco , F., Flickering Returns as RS Oph Reestablishes Quiescent Conditions Following its 2021 Nova Outburst

    Munari , U. & Tabacco , F., Flickering Returns as RS Oph Reestablishes Quiescent Conditions Following its 2021 Nova Outburst . 2022, Research Notes of the American Astronomical Society , 6 , 103, DOI: 10.3847/2515-5172/ac72ae

  35. [43]

    , The GALAH survey and symbiotic stars - I

    Munari , U., Traven , G., Masetti , N., et al. , The GALAH survey and symbiotic stars - I. Discovery and follow-up of 33 candidate accreting-only systems . 2021, , 505 , 6121, DOI: 10.1093/mnras/stab1620

  36. [44]

    & Valisa , P., The 2021 outburst of RS Oph

    Munari , U. & Valisa , P., The 2021 outburst of RS Oph. A pictorial atlas of the spectroscopic evolution: the first 18 days . 2021, arXiv e-prints , arXiv:2109.01101, DOI: 10.48550/arXiv.2109.01101

  37. [45]

    & Valisa , P., The 2021 outburst of RS Oph: a pictorial atlas of the spectroscopic evolution

    Munari , U. & Valisa , P., The 2021 outburst of RS Oph: a pictorial atlas of the spectroscopic evolution. II. From day 19 to 102 (solar conjunction) . 2022, arXiv e-prints , arXiv:2203.01378, DOI: 10.48550/arXiv.2203.01378

  38. [46]

    U., Beardmore , A

    Ness , J. U., Beardmore , A. P., Bode , M. F., et al. , High-resolution X-ray spectra of RS Ophiuchi (2006 and 2021): Revealing the cause of SSS variability . 2023, , 670 , A131, DOI: 10.1051/0004-6361/202245269

  39. [47]

    M., Linford , J

    Nyamai , M. M., Linford , J. D., Allison , J. R., et al. , Synchrotron emission from double-peaked radio light curves of the symbiotic recurrent nova V3890 Sgr . 2023, , 523 , 1661, DOI: 10.1093/mnras/stad1534

  40. [48]

    & Bode , M., Resolved nebular remnants

    O'Brien , T. & Bode , M., Resolved nebular remnants . 2008, in Classical Novae , ed. M. F. Bode & A. Evans (Cabridge Univ. Press), 285--305

  41. [49]

    P., Page , K

    Osborne , J. P., Page , K. L., Beardmore , A. P., et al. , The Supersoft X-ray Phase of Nova RS Ophiuchi 2006 . 2011, , 727 , 124, DOI: 10.1088/0004-637X/727/2/124

  42. [50]

    L., Beardmore , A

    Page , K. L., Beardmore , A. P., Osborne , J. P., et al. , The 2021 outburst of the recurrent nova RS Ophiuchi observed in X-rays by the Neil Gehrels Swift Observatory: a comparative study . 2022, , 514 , 1557, DOI: 10.1093/mnras/stac1295

  43. [51]

    & Wright , F

    Payne-Gaposchkin , C. & Wright , F. W., The Photographic Light-Curve of T Coronae Borealis. 1946, , 104 , 75, DOI: 10.1086/144834

  44. [52]

    Ribeiro , V. A. R. M., Bode , M. F., Darnley , M. J., et al. , The Expanding Nebular Remnant of the Recurrent Nova RS Ophiuchi (2006). II. Modeling of Combined Hubble Space Telescope Imaging and Ground-based Spectroscopy . 2009, , 703 , 1955, DOI: 10.1088/0004-637X/703/2/1955

  45. [53]

    Saikia , D. F. & Anupama , G. C., eds. 2012, Bull. Astr. Soc. India, Vol. 40 , Novae from radio to gamma rays (Astron. Soc. India)

  46. [54]

    Schaefer , B. E., The B & V light curves for recurrent nova T CrB from 1842-2022, the unique pre- and post-eruption high-states, the complex period changes, and the upcoming eruption in 2025.5 1.3 . 2023, , 524 , 3146, DOI: 10.1093/mnras/stad735

  47. [55]

    J., Ness , J.-U., Osborne , J

    Schwarz , G. J., Ness , J.-U., Osborne , J. P., et al. , Swift X-Ray Observations of Classical Novae. II. The Super Soft Source Sample . 2011, , 197 , 31, DOI: 10.1088/0067-0049/197/2/31

  48. [56]

    R., Krogulec , M., & Taylor , A

    Seaquist , E. R., Krogulec , M., & Taylor , A. R., A Highly Sensitive Radio Survey of Symbiotic Stars at 3.6 Centimeters . 1993, , 410 , 260, DOI: 10.1086/172742

  49. [57]

    Seaquist , E. R. & Taylor , A. R., The Collective Radio Properties of Symbiotic Stars . 1990, , 349 , 313, DOI: 10.1086/168315

  50. [58]

    R., Taylor , A

    Seaquist , E. R., Taylor , A. R., & Button , S., A Radio Survey of Symbiotic Stars . 1984, , 284 , 202, DOI: 10.1086/162399

  51. [59]

    N., Wahlgren , G

    Shore , S. N., Wahlgren , G. M., Augusteijn , T., et al. , The spectroscopic evolution of the symbiotic-like recurrent nova V407 Cygni during its 2010 outburst. I. The shock and its evolution . 2011, , 527 , A98, DOI: 10.1051/0004-6361/201015901

  52. [60]

    & Carikov \'a , Z., Wind mass transfer in S-type symbiotic binaries

    Skopal , A. & Carikov \'a , Z., Wind mass transfer in S-type symbiotic binaries. I. Focusing by the wind compression model . 2015, , 573 , A8, DOI: 10.1051/0004-6361/201424779

  53. [61]

    Y., Munari , U., et al

    Skopal , A., Shugarov , S. Y., Munari , U., et al. , The path to Z And-type outbursts: The case of V426 Sagittae (HBHA 1704-05) . 2020, , 636 , A77, DOI: 10.1051/0004-6361/201937199

  54. [62]

    F., Cutri , R

    Skrutskie , M. F., Cutri , R. M., Stiening , R., et al. , The Two Micron All Sky Survey (2MASS) . 2006, , 131 , 1163, DOI: 10.1086/498708

  55. [63]

    L., Rupen , M

    Sokoloski , J. L., Rupen , M. P., & Mioduszewski , A. J., Uncovering the Nature of Nova Jets: A Radio Image of Highly Collimated Outflows from RS Ophiuchi . 2008, , 685 , L137, DOI: 10.1086/592602

  56. [64]

    , VLA observations of the 2021 eruption of RS Oph

    Sokolovsky , K., Aydi , E., Chomiuk , L., et al. , VLA observations of the 2021 eruption of RS Oph . 2021, The Astronomer's Telegram , 14886 , 1

  57. [65]

    1989, in Classical Novae , ed

    Starrfield , S., Thermonuclear processes and the classical nova outburst. 1989, in Classical Novae , ed. M. F. Bode & A. Evans (John Wiley & Sons), 39--60

  58. [66]

    R., Thermonuclear processes

    Starrfield , S., Iliadis , C., & Hix , W. R., Thermonuclear processes . 2008, in Classical Novae , ed. M. F. Bode & A. Evans (Cambridge Univ. Press), 77--101

  59. [67]

    A., Marrese , P

    Tatarnikova , A. A., Marrese , P. M., Munari , U., Tomov , T., & Yudin , B. F., Spectral observations of the symbiotic Mira variable V407 Cyg in 1993 2002 . 2003, Astronomy Reports , 47 , 889, DOI: 10.1134/1.1626192

  60. [68]

    Taylor , A. R. & Seaquist , E. R., Radio emission from symbiotic stars : a binary model. 1984, , 286 , 263, DOI: 10.1086/162594

  61. [69]

    V., Stoyanov , K

    Tomov , T. V., Stoyanov , K. A., & Zamanov , R. K., AG Pegasi - now a classical symbiotic star in outburst? 2016, , 462 , 4435, DOI: 10.1093/mnras/stw2012

  62. [70]

    Cataclysmic variable stars , , Vol

    Warner , B. Cataclysmic variable stars , , Vol. 28 (Cambridge Univ. Press)

  63. [71]

    , AMI-LA, e-MERLIN and MeerKAT radio detections of RS Oph in outburst

    Williams , D., O'Brien , T., Woudt , P., et al. , AMI-LA, e-MERLIN and MeerKAT radio detections of RS Oph in outburst . 2021, The Astronomer's Telegram , 14849 , 1

  64. [72]

    Woudt , P. A. & Ribeiro , V. A. R. M., eds. 2014, Astronomical Society of the Pacific Conference Series, Vol. 490 , Stella Novae: Past and Future Decades

  65. [73]

    Y., et al

    Zamanov , R., Boeva , S., Latev , G. Y., et al. , Accretion in the recurrent nova T CrB: Linking the superactive state to the predicted outburst . 2023, , 680 , L18, DOI: 10.1051/0004-6361/202348372

Pith tools

Reviewed August 10, 2026 · model on record in the stance chip above.