Igor I. Zinchenko
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Igor I. Zinchenko has a total of 344 co-authors. Here are the top co-authors by number of shared publications:
- Lokesh Kumar Dewangan
Physical Research Laboratory
15 shared publications - Peter M. Zemlyanukha
Russian Academy of Sciences
15 shared publications - Devendra K. Ojha
Department of Astronomy and Astrophysics, Tata Institute of Fundamental Research, Mumbai 400005, India
12 shared publications - Sheng-Yuan Liu
Institute of Astronomy and Astrophysics
10 shared publications A. M. Sobolev
Astronomical Observatory Ural Federal University 51, Lenin ave. 620000 Ekaterinburg Russia
7 shared publicationsD. K. Ojha
Tata Institute of Fundamental Research, 400 005 Mumbai, India
7 shared publications
Latest Publications
- 1 November 2026
- Published by Special Astrophysical Observatory of the Russian Academy of Sciences
Evolution of Low-Frequency Radio Emission of the Ionised Gas around S255IR\,NIRS3 after the Accretion Luminosity Burst
We present the results of analyzing the radio variability of the source S255IR\,NIRS3 following an accretion event. The source was observed at two epochs: in January$-$March 2017 at frequencies of $0.3\!-\!10$ GHz and in March 2019 at $1.32\!-\!1.42$ GHz using the GMRT and VLA observatories. The 2017 data show that the spectrum is well described by a power-law dependence, $F_{\nu}\sim\nu^{0.50\pm0.02}$, over the entire frequency range. Such a spectral index is typically attributed to a combination of thermal bremsstrahlung emission from the ionized gas with both optically thick and optically thin components. No evidence for nonthermal emission or emission solely from an optically thick component is found at the low-frequency end of the spectrum. In contrast, the 2019 observations in the range of $1.32\!-\!1.42$ GHz yield a spectral index of $1.58 \pm 0.03$, which is characteristic of predominantly optically thick thermal emission from the ionized gas. This change in behavior may be explained by a transition from jet-dominated emission in 2017 to emission dominated by an ultracompact H II region in 2019. The observed flux density is $3.93\pm0.10$ mJy in 2017 (at $1.42$ GHz) and $3.58\pm0.16$ mJy in 2019 ($1.37$ GHz). The emission measured in 2017 is $EM\gtrsim 3\times 10^8$ pc cm$^{-6}$.- 1 November 2026
- Published by Special Astrophysical Observatory of the Russian Academy of Sciences
Evolution of Low-Frequency Radio Emission of the Ionised Gas around S255IR\,NIRS3 after the Accretion Luminosity Burst
We present the results of analyzing the radio variability of the source S255IR\,NIRS3 following an accretion event. The source was observed at two epochs: in January$-$March 2017 at frequencies of $0.3\!-\!10$ GHz and in March 2019 at $1.32\!-\!1.42$ GHz using the GMRT and VLA observatories. The 2017 data show that the spectrum is well described by a power-law dependence, $F_{\nu}\sim\nu^{0.50\pm0.02}$, over the entire frequency range. Such a spectral index is typically attributed to a combination of thermal bremsstrahlung emission from the ionized gas with both optically thick and optically thin components. No evidence for nonthermal emission or emission solely from an optically thick component is found at the low-frequency end of the spectrum. In contrast, the 2019 observations in the range of $1.32\!-\!1.42$ GHz yield a spectral index of $1.58 \pm 0.03$, which is characteristic of predominantly optically thick thermal emission from the ionized gas. This change in behavior may be explained by a transition from jet-dominated emission in 2017 to emission dominated by an ultracompact H II region in 2019. The observed flux density is $3.93\pm0.10$ mJy in 2017 (at $1.42$ GHz) and $3.58\pm0.16$ mJy in 2019 ($1.37$ GHz). The emission measured in 2017 is $EM\gtrsim 3\times 10^8$ pc cm$^{-6}$.- Open Access
- 20 October 2026
- Published by EDP Sciences in Astronomy & Astrophysics
- Vol. 714, A257
Southern eROSITA bubble as a forward shock and the low-metallicity circumgalactic medium
Unlike the complicated X-ray and radio structure observed in the North Polar Spur area, the southeastern part of the eROSITA bubbles can be reasonably well described as a propagating forward shock, plausibly created by the transient energy release at the Galactic center. In this model, the physical radius of the bubble is R b ∼ 7–8 kpc, and the age of the outburst is t age ∼ 5–8 Myr. The latter quantity is plausibly a lower limit on the true age. The visible segment of the shock front (located at a distance of ∼10–12 kpc above the Galactic disk and at a similar distance from the Sun) is currently expanding with a velocity of ∼700 km s −1 through gas with a density of n e ∼ 3×10 −4 cm −3 . Moreover, the abundance of heavy elements in this gas is low, Z ∼ 0.1–0.2× Z ⊙ (depending on the adopted reference solar abundances). Unlike the constraints derived from the line-of-sight-integrated quantities, these are effectively in situ measurements of the properties of the circumgalactic medium. Given the simplifying assumptions used in deriving the density and abundance, we assigned a systematic uncertainty of factor of 2 to the final estimates. An eventual decisive test for the shock properties can be provided by the velocity measurements of the X-ray-emitting gas with soft X-ray bolometers. The extended forward shock propagating through low-metallicity gas is a favorable site to accelerate very high-energy cosmic rays, which might contribute to the recently discovered proton-rich Galactic cosmic ray component at PeV energies impinging on the Earth’s atmosphere.
- 20 October 2026
- Published by EDP Sciences in Astronomy & Astrophysics
- Vol. 714, A257
Open AccessSouthern eROSITA bubble as a forward shock and the low-metallicity circumgalactic medium
Unlike the complicated X-ray and radio structure observed in the North Polar Spur area, the southeastern part of the eROSITA bubbles can be reasonably well described as a propagating forward shock, plausibly created by the transient energy release at the Galactic center. In this model, the physical radius of the bubble is R b ∼ 7–8 kpc, and the age of the outburst is t age ∼ 5–8 Myr. The latter quantity is plausibly a lower limit on the true age. The visible segment of the shock front (located at a distance of ∼10–12 kpc above the Galactic disk and at a similar distance from the Sun) is currently expanding with a velocity of ∼700 km s −1 through gas with a density of n e ∼ 3×10 −4 cm −3 . Moreover, the abundance of heavy elements in this gas is low, Z ∼ 0.1–0.2× Z ⊙ (depending on the adopted reference solar abundances). Unlike the constraints derived from the line-of-sight-integrated quantities, these are effectively in situ measurements of the properties of the circumgalactic medium. Given the simplifying assumptions used in deriving the density and abundance, we assigned a systematic uncertainty of factor of 2 to the final estimates. An eventual decisive test for the shock properties can be provided by the velocity measurements of the X-ray-emitting gas with soft X-ray bolometers. The extended forward shock propagating through low-metallicity gas is a favorable site to accelerate very high-energy cosmic rays, which might contribute to the recently discovered proton-rich Galactic cosmic ray component at PeV energies impinging on the Earth’s atmosphere.
- 28 July 2026
- Published by Special Astrophysical Observatory of the Russian Academy of Sciences
The BTA Optical Telescope as an Instrument for Millimeter Astronomy: Scientific Objectives
During the period 2023$-$2026, the Special Astrophysical Observatory of the Russian Academy of Sciences (SAO RAS) is implementing a project to create a millimeter-wave observatory based on the BTA optical telescope. The project involves the installation of sub-terahertz receivers at the Nasmyth focus and the performance of test observations. This paper discusses the scientific objectives that can be addressed both at the initial stage of the project using bolometric receivers for continuum observations and, in the future, using receiver systems based on HEMT and SIS technologies for molecular line observations.
- 28 July 2026
- Published by Special Astrophysical Observatory of the Russian Academy of Sciences
The BTA Optical Telescope as an Instrument for Millimeter Astronomy: Scientific Objectives
During the period 2023$-$2026, the Special Astrophysical Observatory of the Russian Academy of Sciences (SAO RAS) is implementing a project to create a millimeter-wave observatory based on the BTA optical telescope. The project involves the installation of sub-terahertz receivers at the Nasmyth focus and the performance of test observations. This paper discusses the scientific objectives that can be addressed both at the initial stage of the project using bolometric receivers for continuum observations and, in the future, using receiver systems based on HEMT and SIS technologies for molecular line observations.
- Open Access
- 19 March 2026
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society
- Vol. 548 (1)
Unveiling an hourglass-shaped magnetic field toward IRDC G351.77–0.53
We present the SOFIA/HAWC+ 214 μm polarimetric observations toward the infrared dark cloud G351.77-0.53 (hereafter G351), complemented by existing multi-wavelength data sets. Infrared excess from the embedded sources indicate ongoing star formation activity in the cloud. The G351 cloud hosts two prominent star-forming clumps, i.e., c1 and c2. The plane-of-the-sky magnetic field lines from Planck observations are predominantly oriented perpendicular to the filament’s major axis. Magnetic field orientations from SOFIA/HAWC+ 214 μm observations reveal distinct hourglass-shaped field configuration toward c1, while the field lines remain perpendicular to the rest of the filament. Using the Davis-Chandrasekhar-Fermi method, we estimate a mean plane-of-the-sky magnetic field strength of ~147 ± 60 μG in the G351 filament, with values reaching ~0.8 mG toward c1. The mass-to-flux ratio analysis indicates that the filament is magnetically transcritical, where the gravitational and magnetic field energies are comparable. The hourglass-shaped magnetic field observed toward c1 could result from magnetically regulated gravitational collapse, the alignment of converging sub-filaments with the magnetic field, or a combination of both processes. The energy budget analysis further indicates that magnetic fields play an important role in governing the cloud’s gas dynamics, followed by contributions from turbulence and gravity.
- 19 March 2026
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society
- Vol. 548 (1)
Open AccessUnveiling an hourglass-shaped magnetic field toward IRDC G351.77–0.53
We present the SOFIA/HAWC+ 214 μm polarimetric observations toward the infrared dark cloud G351.77-0.53 (hereafter G351), complemented by existing multi-wavelength data sets. Infrared excess from the embedded sources indicate ongoing star formation activity in the cloud. The G351 cloud hosts two prominent star-forming clumps, i.e., c1 and c2. The plane-of-the-sky magnetic field lines from Planck observations are predominantly oriented perpendicular to the filament’s major axis. Magnetic field orientations from SOFIA/HAWC+ 214 μm observations reveal distinct hourglass-shaped field configuration toward c1, while the field lines remain perpendicular to the rest of the filament. Using the Davis-Chandrasekhar-Fermi method, we estimate a mean plane-of-the-sky magnetic field strength of ~147 ± 60 μG in the G351 filament, with values reaching ~0.8 mG toward c1. The mass-to-flux ratio analysis indicates that the filament is magnetically transcritical, where the gravitational and magnetic field energies are comparable. The hourglass-shaped magnetic field observed toward c1 could result from magnetically regulated gravitational collapse, the alignment of converging sub-filaments with the magnetic field, or a combination of both processes. The energy budget analysis further indicates that magnetic fields play an important role in governing the cloud’s gas dynamics, followed by contributions from turbulence and gravity.
- 1 March 2026
- Published by Pleiades Publishing Ltd in Astrophysical Bulletin
- Vol. 81 (1) , 107-115
BTA Optical Telescope as Instrument for Millimeter Astronomy: Scientific Objectives
During the period of 2023–2026, the scientists of the Special Astrophysical Observatory of the Russian Academy of Sciences (SAO RAS) are implementing a project to create a millimeter-wave observatory based on the BTA optical telescope. The project involves the installation of subterahertz receivers at the Nasmyth focus and the performance of test observations. This paper discusses scientific objectives that can be addressed both at the initial stage of the project using bolometric receivers for continuum observations and, in the future, using receiver systems based on HEMT and SIS technologies for molecular line observations.
- 1 March 2026
- Published by Pleiades Publishing Ltd in Astrophysical Bulletin
- Vol. 81 (1) , 107-115
BTA Optical Telescope as Instrument for Millimeter Astronomy: Scientific Objectives
During the period of 2023–2026, the scientists of the Special Astrophysical Observatory of the Russian Academy of Sciences (SAO RAS) are implementing a project to create a millimeter-wave observatory based on the BTA optical telescope. The project involves the installation of subterahertz receivers at the Nasmyth focus and the performance of test observations. This paper discusses scientific objectives that can be addressed both at the initial stage of the project using bolometric receivers for continuum observations and, in the future, using receiver systems based on HEMT and SIS technologies for molecular line observations.
- 1 September 2025
- Published by Springer Nature in Radiophysics and Quantum Electronics
- Vol. 68 (4) , 300-305
On Determination of the Atmospheric Optical Thickness from Absolute Measurements of Sky Brightness Temperature in the Millimeter Wavelength Range
- 1 September 2025
- Published by Springer Nature in Radiophysics and Quantum Electronics
- Vol. 68 (4) , 300-305
On Determination of the Atmospheric Optical Thickness from Absolute Measurements of Sky Brightness Temperature in the Millimeter Wavelength Range
- Open Access
- 4 August 2025
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society: Letters
- Vol. 543 (1) , L9-L13
Submillimetre Class II methanol masers near the massive protostar S255IR NIRS 3: evolution and excitation of the J1 − J0 A−+ series and a new maser line at 345.919 GHz
We present the results of a further investigation of the Class II methanol maser emission in the $14_1 - 14_0$ A$^{-+}$ transition at 349.1 GHz discovered in 2016 in the remarkable core S255IR-SMA1, which harbours a $\sim$20-M$_{\odot }$ protostar NIRS 3 that exhibited a disc-mediated accretion burst in 2015. The present study is based on observations of this object with Atacama Large Millimeter/submillimeter Array in Band 7 at the largest baselines, which provide an angular resolution of $\sim$15 mas. We estimated the physical conditions in the region where the maser emission comes from, and in the surroundings, using the presumably quasi-thermal methanol lines in our bands and the CH$_3$CN $19_\mathrm{K} - 18_\mathrm{K}$ line series. The total flux density in the $14_1 - 14_0$ A$^{-+}$ line in 2021 is about two times higher than in 2019. A maser emission of about the same intensity in 2021 is detected for the first time in the $12_1 - 12_0$ A$^{-+}$ transition at 336.9 GHz. The physical conditions in the masering and non-masering regions are similar. The masers are apparently excited by the radiation of the central source. Unfortunately, the existing models cannot adequately take into account this radiation. The $18_{-3}-17_{-4}$ E transition at 345.919 GHz also shows characteristics of maser emission.- 4 August 2025
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society: Letters
- Vol. 543 (1) , L9-L13
Open AccessSubmillimetre Class II methanol masers near the massive protostar S255IR NIRS 3: evolution and excitation of the J1 − J0 A−+ series and a new maser line at 345.919 GHz
We present the results of a further investigation of the Class II methanol maser emission in the $14_1 - 14_0$ A$^{-+}$ transition at 349.1 GHz discovered in 2016 in the remarkable core S255IR-SMA1, which harbours a $\sim$20-M$_{\odot }$ protostar NIRS 3 that exhibited a disc-mediated accretion burst in 2015. The present study is based on observations of this object with Atacama Large Millimeter/submillimeter Array in Band 7 at the largest baselines, which provide an angular resolution of $\sim$15 mas. We estimated the physical conditions in the region where the maser emission comes from, and in the surroundings, using the presumably quasi-thermal methanol lines in our bands and the CH$_3$CN $19_\mathrm{K} - 18_\mathrm{K}$ line series. The total flux density in the $14_1 - 14_0$ A$^{-+}$ line in 2021 is about two times higher than in 2019. A maser emission of about the same intensity in 2021 is detected for the first time in the $12_1 - 12_0$ A$^{-+}$ transition at 336.9 GHz. The physical conditions in the masering and non-masering regions are similar. The masers are apparently excited by the radiation of the central source. Unfortunately, the existing models cannot adequately take into account this radiation. The $18_{-3}-17_{-4}$ E transition at 345.919 GHz also shows characteristics of maser emission. - Open AccessSubmillimeter Class II methanol masers near the massive protostar S255IR NIRS3: evolution and excitation of the $J_1 -J_0$ A$^{-+}$ series and a new maser line at 345.919 GHzWe present the results of the further investigation of the Class II methanol maser emission in the $14_1 - 14_0$ A$^{-+}$ transition at 349.1 GHz discovered in 2016 in the remarkable core S255IR-SMA1, harboring a $\sim$20 M$_\odot$ protostar NIRS3, which exhibited a disk-mediated accretion burst in 2015. The present study is based on the observations of this object with ALMA in Band 7 at the largest baselines, which provide the angular resolution of $\sim$15 mas. We estimated physical conditions in the region from which comes the maser emission, and in the surroundings, using the presumably quasi-thermal methanol lines in our bands and the CH$_3$CN $19_\mathrm{K} - 18_\mathrm{K}$ line series. The total flux density in the $14_1 - 14_0$ A$^{-+}$ line in 2021 is about two times higher than in 2019. A maser emission of about the same intensity in 2021 is detected for the first time in the $12_1 - 12_0$ A$^{-+}$ transition at 336.9 GHz. The physical conditions in the masering and non-masering regions are similar. The masers are apparently excited by the radiation of the central source. Unfortunately, the existing models cannot adequately take into account this radiation. The $18_{-3}-17_{-4}$ E transition at 345.919 GHz shows characteristics of maser emission, too.Open AccessSubmillimeter Class II methanol masers near the massive protostar S255IR NIRS3: evolution and excitation of the $J_1 -J_0$ A$^{-+}$ series and a new maser line at 345.919 GHzWe present the results of the further investigation of the Class II methanol maser emission in the $14_1 - 14_0$ A$^{-+}$ transition at 349.1 GHz discovered in 2016 in the remarkable core S255IR-SMA1, harboring a $\sim$20 M$_\odot$ protostar NIRS3, which exhibited a disk-mediated accretion burst in 2015. The present study is based on the observations of this object with ALMA in Band 7 at the largest baselines, which provide the angular resolution of $\sim$15 mas. We estimated physical conditions in the region from which comes the maser emission, and in the surroundings, using the presumably quasi-thermal methanol lines in our bands and the CH$_3$CN $19_\mathrm{K} - 18_\mathrm{K}$ line series. The total flux density in the $14_1 - 14_0$ A$^{-+}$ line in 2021 is about two times higher than in 2019. A maser emission of about the same intensity in 2021 is detected for the first time in the $12_1 - 12_0$ A$^{-+}$ transition at 336.9 GHz. The physical conditions in the masering and non-masering regions are similar. The masers are apparently excited by the radiation of the central source. Unfortunately, the existing models cannot adequately take into account this radiation. The $18_{-3}-17_{-4}$ E transition at 345.919 GHz shows characteristics of maser emission, too.
- 1 March 2025
- Published by Pleiades Publishing Ltd in Astrophysical Bulletin
- Vol. 80 (1) , 140-161
Possibilities for Studying Star-Formation Processes at IRAO ‘‘Suffa’’: Objects and Tasks
We describe the general remaining unclear issues of the star-formation process that could be studied using the millimeter radio telescope on the Suffa plateau (Uzbekistan). A description of possible objects of study is given. The possibilities of solving scientific problems in studying these objects using various instruments are assessed: the 70-m RT-70 radio telescope, a smaller-diameter antenna (15–20 m), and an antenna array consisting of small (3–8 m) antennas.
- 1 March 2025
- Published by Pleiades Publishing Ltd in Astrophysical Bulletin
- Vol. 80 (1) , 140-161
Possibilities for Studying Star-Formation Processes at IRAO ‘‘Suffa’’: Objects and Tasks
We describe the general remaining unclear issues of the star-formation process that could be studied using the millimeter radio telescope on the Suffa plateau (Uzbekistan). A description of possible objects of study is given. The possibilities of solving scientific problems in studying these objects using various instruments are assessed: the 70-m RT-70 radio telescope, a smaller-diameter antenna (15–20 m), and an antenna array consisting of small (3–8 m) antennas.
- 1 February 2025
- Published by Pleiades Publishing Ltd in Astronomy Reports
- Vol. 69 (2) , 87-102
Study of the Physical and Chemical Properties of Dense Clumps at Different Evolutionary Stages in Several Regions of Massive Star and Stellar Cluster Formation
Massive stars play an important role in the Universe. Unlike low-mass stars, the formation of these objects located at great distances is still unclear. It is expected to be governed by some combination of self-gravity, turbulence, and magnetic fields. Our aim is to study the chemical and physical conditions of dense clumps at different evolutionary stages. We performed observations towards 5 regions of massive star and stellar cluster formation (L1287, S187, S231, DR 21(OH), NGC 7538) with the IRAM-30m telescope. We covered the 2 and 3–4 mm wavelength bands and analyzed the lines of HCN, HNC, HCO+, HC3N, HNCO, OCS, CS, SiO, SO2, and SO. Using astrodendro algorithm on the 850 µm dust emission data from the SCUBA Legacy catalog, we determined the masses, H2 column densities, and sizes of the clumps. Furthermore, the kinetic temperatures, molecular abundances, and dynamical state were obtained. The Red Midcourse Space Experiment Source survey (RMS) was used to determine the clump types. A total of 20 clumps were identified. Three clumps were found to be associated with the H II regions, 10 with young stellar objects (YSOs), and 7 with submillimeter emission. The clumps have typical sizes of about 0.2 pc and masses ranging from 1 to 102\({{M}_{ \odot }}\), kinetic temperatures ranging from 20 to 40 K and line widths of H13CO+ (1–0) approximately 2 km s–1. We found no significant correlation in the “line width–size” and the “line width–mass” relationships. However, a strong correlation is observed in “mass–size” relationships. The virial analysis indicated that three clumps are gravitationally bound. Furthermore, we suggested that significant magnetic fields of about 1 mG provide additional support for clump stability. The molecular abundances (relative to H2) are approximately 10–10–10–8.- 1 February 2025
- Published by Pleiades Publishing Ltd in Astronomy Reports
- Vol. 69 (2) , 87-102
Study of the Physical and Chemical Properties of Dense Clumps at Different Evolutionary Stages in Several Regions of Massive Star and Stellar Cluster Formation
Massive stars play an important role in the Universe. Unlike low-mass stars, the formation of these objects located at great distances is still unclear. It is expected to be governed by some combination of self-gravity, turbulence, and magnetic fields. Our aim is to study the chemical and physical conditions of dense clumps at different evolutionary stages. We performed observations towards 5 regions of massive star and stellar cluster formation (L1287, S187, S231, DR 21(OH), NGC 7538) with the IRAM-30m telescope. We covered the 2 and 3–4 mm wavelength bands and analyzed the lines of HCN, HNC, HCO+, HC3N, HNCO, OCS, CS, SiO, SO2, and SO. Using astrodendro algorithm on the 850 µm dust emission data from the SCUBA Legacy catalog, we determined the masses, H2 column densities, and sizes of the clumps. Furthermore, the kinetic temperatures, molecular abundances, and dynamical state were obtained. The Red Midcourse Space Experiment Source survey (RMS) was used to determine the clump types. A total of 20 clumps were identified. Three clumps were found to be associated with the H II regions, 10 with young stellar objects (YSOs), and 7 with submillimeter emission. The clumps have typical sizes of about 0.2 pc and masses ranging from 1 to 102\({{M}_{ \odot }}\), kinetic temperatures ranging from 20 to 40 K and line widths of H13CO+ (1–0) approximately 2 km s–1. We found no significant correlation in the “line width–size” and the “line width–mass” relationships. However, a strong correlation is observed in “mass–size” relationships. The virial analysis indicated that three clumps are gravitationally bound. Furthermore, we suggested that significant magnetic fields of about 1 mG provide additional support for clump stability. The molecular abundances (relative to H2) are approximately 10–10–10–8.