183 research outputs found
PACS and SPIRE range spectroscopy of cool, evolved stars
Context: At the end of their lives AGB stars are prolific producers of dust
and gas. The details of this mass-loss process are still not understood very
well. Herschel PACS and SPIRE spectra offer a unique way of investigating
properties of AGB stars in general and the mass-loss process in particular.
Methods: The HIPE software with the latest calibration is used to process the
available PACS and SPIRE spectra of 40 evolved stars. The spectra are convolved
with the response curves of the PACS and SPIRE bolometers and compared to the
fluxes measured in imaging data of these sources. Custom software is used to
identify lines in the spectra, and to determine the central wavelengths and
line intensities. Standard molecular line databases are used to associate the
observed lines. Because of the limited spectral resolution of the spectrometers
several known lines are typically potential counterparts to any observed line.
To help identifications the relative contributions in line intensity of the
potential counterpart lines are listed for three characteristic temperatures
based on LTE calculations and assuming optically thin emission. Result: The
following data products are released: the reduced spectra, the lines that are
measured in the spectra with wavelength, intensity, potential identifications,
and the continuum spectra, i.e. the full spectra with all identified lines
removed. As simple examples of how this data can be used in future studies we
have fitted the continuum spectra with three power laws and find that the few
OH/IR stars seem to have significantly steeper slopes than the other oxygen-
and carbon-rich objects in the sample. As another example we constructed
rotational diagrams for CO and fitted a two-component model to derive
rotational temperatures.Comment: A&A accepte
An ALMA view of CS and SiS around oxygen-rich AGB stars
We aim to determine the distributions of molecular SiS and CS in the
circumstellar envelopes of oxygen-rich asymptotic giant branch stars and how
these distributions differ between stars that lose mass at different rates. In
this study we analyse ALMA observations of SiS and CS emission lines for three
oxygen-rich galactic AGB stars: IK Tau, with a moderately high mass-loss rate
of M yr, and W Hya and R Dor with low mass loss
rates of M yr. These molecules are usually
more abundant in carbon stars but the high sensitivity of ALMA allows us to
detect their faint emission in the low mass-loss rate AGB stars. The high
spatial resolution of ALMA also allows us to precisely determine the spatial
distribution of these molecules in the circumstellar envelopes. We run
radiative transfer models to calculate the molecular abundances and abundance
distributions for each star. We find a spread of peak SiS abundances with
for R Dor, for W Hya, and for
IK Tau relative to H. We find lower peak CS abundances of
for R Dor, for W Hya and
for IK Tau, with some stratifications in the abundance
distributions. For IK Tau we also calculate abundances for the detected
isotopologues: CS, SiS, SiS, SiS, SiS,
SiS, and SiS. Overall the isotopic ratios we derive
for IK Tau suggest a lower metallicity than solar.Comment: 16 page
The unusual 3D distribution of NaCl around the AGB star IK Tau
NaCl is a diatomic molecule with a large dipole moment, which allows for its
detection even at relatively small abundances. It has been detected towards
several evolved stars, among which is the AGB star IK Tau, around which it is
distributed in several clumps that lie off-center from the star. We aim to
study the three-dimensional distribution of NaCl around the AGB star IK Tau,
and to obtain the abundance of NaCl relative to H for each of the clumps.
First, a new value for the maximum expansion velocity is determined. The
observed ALMA channel maps are then deprojected to create a three-dimensional
model of the distribution of NaCl. This model is then used as input for the
radiative transfer modelling code magritte, which is used to obtain the NaCl
abundances of each of the clumps by comparing the observations with the results
of the magritte simulations. Additionally, the rotational temperature of the
clumps is determined using population diagrams. We derive an updated value for
the maximum expansion velocity of IK Tau = 28.4 km/s. A
spiral-like shape can be discerned in our three-dimensional distribution model
of the NaCl. This spiral lies more or less in the plane of the sky. The
distribution is also flatter in the line-of-sight direction than in the plane
of the sky. We find clump abundances between and relative to H, where the relative abundance is typically lower for
clumps closer to the star. For the first time, we used deprojection to
understand the three-dimensional environment of an AGB star and calculated the
fractional abundance of NaCl in clumps surrounding the star.Comment: Accepted for publication in A&
New observations and models of circumstellar CO line emission of AGB stars in the Herschel SUCCESS programme
CONTEXT: Asymptotic giant branch (AGB) stars are in one of the latest
evolutionary stages of low to intermediate-mass stars. Their vigorous mass loss
has a significant effect on the stellar evolution, and is a significant source
of heavy elements and dust grains for the interstellar medium. The mass-loss
rate can be well traced by carbon monoxide (CO) line emission.
AIMS: We present new Herschel HIFI and IRAM 30m telescope CO line data for a
sample of 53 galactic AGB stars. The lines cover a fairly large range of
excitation energy from the line to the line, and even the
line in a few cases. We perform radiative transfer modelling for 38
of these sources to estimate their mass-loss rates.
METHODS: We used a radiative transfer code based on the Monte Carlo method to
model the CO line emission. We assume spherically symmetric circumstellar
envelopes that are formed by a constant mass-loss rate through a smoothly
accelerating wind.
RESULTS: We find models that are consistent across a broad range of CO lines
for most of the stars in our sample, i.e., a large number of the circumstellar
envelopes can be described with a constant mass-loss rate. We also find that an
accelerating wind is required to fit, in particular, the higher-J lines and
that a velocity law will have a significant effect on the model line
intensities. The results cover a wide range of mass-loss rates (
to ) and gas expansion
velocities (2 to km s), and include M-, S-, and C-type AGB stars.
Our results generally agree with those of earlier studies, although we tend to
find slightly lower mass-loss rates by about 40%, on average. We also present
"bonus" lines detected during our CO observations.Comment: 36 page
An ALMA view of SO and SO around oxygen-rich AGB stars
We present and analyse SO and SO, recently observed with high angular
resolution and sensitivity in a spectral line survey with ALMA, for two
oxygen-rich AGB stars: the low mass-loss rate R Dor and high mass-loss rate IK
Tau. We analyse 8 lines of SO detected towards both stars, 78 lines of
SOdetected towards R Dor and 52 lines of SO detected towards IK Tau. We
detect several lines of SO, SO and SO towards both
stars, and tentatively SO towards R Dor, and hence derive isotopic
ratios for these species. The spatially resolved observations show us that the
two sulphur oxides are co-located towards R Dor and trace out the same wind
structures in the circumstellar envelope (CSE). Much of the emission is well
reproduced with a Gaussian abundance distribution spatially centred on the
star. Emission from the higher energy levels of SO and SO towards R Dor
provide evidence in support of a rotating inner region of gas identified in
earlier work. The new observations allow us to refine the abundance
distribution of SO in IK Tau derived from prior observations with single
antennas, and confirm the distribution is shell-like with the peak in the
fractional abundance not centred on the star. The confirmation of different
types of SO abundance distributions will help fine-tune chemical models and
allows for an additional method to discriminate between low and high mass-loss
rates for oxygen-rich AGB stars.Comment: Accepted for publication in MNRA
Rotational spectra of vibrationally excited AlO and TiO in oxygen rich stars
Rotational transitions in vibrationally excited AlO and TiO -- two possible
precursors of dust -- were observed in the 300 GHz range (1 mm wavelength)
towards the oxygen rich AGB stars R Dor and IK Tau with ALMA, and vibrationally
excited AlO was observed towards the red supergiant VY CMa with the SMA. The
transition of TiO in the levels, and the transition in the level of AlO were identified towards R Dor;
the line of TiO was identified in the level towards IK Tau;
and two transitions in the levels of AlO were identified
towards VY CMa. The newly-derived high vibrational temperature of TiO and AlO
in R Dor of K, and prior measurements of the angular extent
confirm that the majority of the emission is from a region within
of the central star. A full radiative transfer analysis of
AlO in R Dor yielded a fractional abundance of 3% of the solar abundance
of Al. From a similar analysis of TiO a fractional abundance of % of
the solar abundance of Ti was found. The observations provide indirect evidence
that TiO is present in a rotating disk close to the star. Further observations
in the ground and excited vibrational levels are needed to determine whether
AlO, TiO, and TiO are seeds of the AlO dust in R Dor, and perhaps
in the gravitationally bound dust shells in other AGB stars with low mass loss
rates.Comment: Accepted for publication in Ap
ΠΡΠ΄Π°Π»Π΅Π½Π½ΡΠ΅ ΠΈΡΡ ΠΎΠ΄Ρ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΈ ΠΌΠΎΠ·Π³Π° ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ ΡΡΠ΅ΡΠΊΠΎΠΆΠ½ΡΡ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ² ΠΈ ΠΊΠ°ΡΠΎΡΠΈΠ΄Π½ΠΎΠΉ ΡΠ½Π΄Π°ΡΡΠ΅ΡΡΠΊΡΠΎΠΌΠΈΠΈ Π² Π³ΠΈΠ±ΡΠΈΠ΄Π½ΠΎΠΌ ΠΈ ΠΏΠΎΡΡΠ°ΠΏΠ½ΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
Aim To evaluate in-hospital and long-term outcomes of myocardial and cerebral revascularization with combined or staged PCI and carotid endarterectomy.Methods.263 myocardial and cerebral revascularizations with PCI and CEA in patients with combined cerebral and coronary artery lesions in the period from 2011 to 2017 were performed. Patients were divided into two groups depending on the surgical strategy. Patient (n = 133) who underwent a staged intervention (CEA and PCI) were included in Group 1, whereas patients (n = 130) who underwent a hybrid intervention (CEE+PCI CA) were included in Group 2. The mean follow-up was 3.5 years.Results.100% of patients in Group 2 underwent coronary and internal carotid revascularization according to the results of in-hospital and long-term follow-up. 81.35% of patient in Group 1 underwent PCI and CEA, whereas 3.01% of patients underwent only PCI and 6.77% of patients β CEA. 1.5% of patients in Group 1 did not receive any surgical treatment. The most common causes of incomplete revascularization were the subsequent change of the initially defined treatment for myocardial (6.02%) or cerebral revascularization (0.75%). The rest refused the second stage, or it was associated with extremely high risk and the strategy was switched to the conservative therapy.Conclusion.100% of patients received hybrid myocardial and cerebral revascularization during one hospitalization. It allowed reducing mortality from MI and stroke during the waiting period for the next stage of the treatment in Group 1 (almost 5%). Hybrid interventions can be used in patients with high risk for open-heart surgery, severe comorbidities (obesity, diabetes, renal dysfunction), significant coronary and cerebral artery lesions with high risk of MI and stroke. However, hybrid approach was associated with high rate (almost 7%) of non-fatal MI in the long-term follow-up.Π¦Π΅Π»Ρ.ΠΡΠ΅Π½ΠΊΠ° Π³ΠΎΡΠΏΠΈΡΠ°Π»ΡΠ½ΡΡ
ΠΈ ΠΎΡΠ΄Π°Π»Π΅Π½Π½ΡΡ
ΠΈΡΡ
ΠΎΠ΄ΠΎΠ² ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° ΠΈ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ ΡΡΠ΅ΡΠΊΠΎΠΆΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΠΎΠ³ΠΎ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° (Π§ΠΠ) ΠΈ ΠΊΠ°ΡΠΎΡΠΈΠ΄Π½ΠΎΠΉ ΡΠ½Π΄Π°ΡΡΠ΅ΡΡΠΊΡΠΎΠΌΠΈΠΈ (ΠΠΠ) Π² ΠΏΠΎΡΡΠ°ΠΏΠ½ΠΎΠΌ ΠΈ Π³ΠΈΠ±ΡΠΈΠ΄Π½ΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
.ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ.Π‘ 2011 ΠΏΠΎ 2017 Π³. Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΎ 263 ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π§ΠΠ ΠΈ ΠΠΠ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΌΡΠ»ΡΡΠΈΡΠΎΠΊΠ°Π»ΡΠ½ΡΠΌ Π°ΡΠ΅ΡΠΎΡΠΊΠ»Π΅ΡΠΎΠ·ΠΎΠΌ Ρ ΡΠΎΡΠ΅ΡΠ°Π½Π½ΡΠΌ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΡΠ΅Π±ΡΠ°Π»ΡΠ½ΡΡ
ΠΈ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ. Π Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π²ΡΠ±ΡΠ°Π½Π½ΡΡ
ΡΡΡΠ°ΡΠ΅Π³ΠΈΠΉ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° Π΄Π²Π΅ Π³ΡΡΠΏΠΏΡ: 1-Ρ Π³ΡΡΠΏΠΏΠ° (n = 133) β ΠΏΠΎΡΡΠ°ΠΏΠ½ΡΠ΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° (ΠΠΠ ΠΈ Π§ΠΠ); 2-Ρ Π³ΡΡΠΏΠΏΠ° (n = 130) β Π³ΠΈΠ±ΡΠΈΠ΄Π½ΡΠ΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° (ΠΠΠ + Π§ΠΠ). Π‘ΡΠ΅Π΄Π½ΠΈΠΉ ΠΏΠ΅ΡΠΈΠΎΠ΄ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ ΡΠΎΡΡΠ°Π²ΠΈΠ» 3,5 Π³ΠΎΠ΄Π°.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ.Π Π³ΡΡΠΏΠΏΠ΅ Π³ΠΈΠ±ΡΠΈΠ΄Π½ΡΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΡ Π΄Π²ΡΡ
ΡΠΎΡΡΠ΄ΠΈΡΡΡΡ
Π±Π°ΡΡΠ΅ΠΉΠ½ΠΎΠ² (ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ
ΠΈ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΡ
ΡΠΎΠ½Π½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ) Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π° Π² 100% ΡΠ»ΡΡΠ°Π΅Π². Π Π³ΡΡΠΏΠΏΠ΅ ΠΏΠΎΡΡΠ°ΠΏΠ½ΠΎΠΉ ΡΠ°ΠΊΡΠΈΠΊΠΈ ΠΏΠΎΠ»Π½ΡΠΉ ΠΎΠ±ΡΠ΅ΠΌ Π·Π°ΠΏΠ»Π°Π½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ»ΠΈ Π»ΠΈΡΡ 81,35% ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΡΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ Π² 3,01% ΡΠ»ΡΡΠ°Π΅Π² Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΎ ΡΠΎΠ»ΡΠΊΠΎ Π§ΠΠ, Π² 6,77% ΡΠ»ΡΡΠ°Π΅Π² β ΡΠΎΠ»ΡΠΊΠΎ ΠΠΠ, Π° Π² 1,5% β Π½Π΅ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ Π½ΠΈ ΠΎΠ΄ΠΈΠ½ ΡΡΠ°ΠΏ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ. Π‘Π°ΠΌΡΠΌΠΈ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΡΠΌΠΈ ΠΏΡΠΈΡΠΈΠ½Π°ΠΌΠΈ Π½Π΅ΠΏΠΎΠ»Π½ΠΎΠΉ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠ²ΠΈΠ»ΠΈΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ°ΠΊΡΠΈΠΊΠΈ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° (6,02%) ΠΈΠ»ΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° (0,75%), Π² ΠΎΡΡΠ°Π²ΡΠΈΡ
ΡΡ ΡΠ»ΡΡΠ°ΡΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΡ Π½Π΅ ΡΠ²Π»ΡΠ»ΠΈΡΡ Π½Π° Π²ΡΠΎΡΠΎΠΉ ΡΡΠ°ΠΏ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠΎ ΡΡΠ±ΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΌ ΠΏΡΠΈΡΠΈΠ½Π°ΠΌ ΠΈΠ»ΠΈ Π΅Π³ΠΎ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΠ΅ Π±ΡΠ»ΠΎ ΡΠΎΠΏΡΡΠΆΠ΅Π½ΠΎ Ρ ΠΊΡΠ°ΠΉΠ½Π΅ Π²ΡΡΠΎΠΊΠΈΠΌ ΡΠΈΡΠΊΠΎΠΌ, Π² ΡΠ²ΡΠ·ΠΈ Ρ ΡΠ΅ΠΌ ΡΠ°ΠΊΡΠΈΠΊΠ° Π±ΡΠ»Π° ΠΏΠ΅ΡΠ΅ΡΠΌΠΎΡΡΠ΅Π½Π° Π² ΠΏΠΎΠ»ΡΠ·Ρ ΠΊΠΎΠ½ΡΠ΅ΡΠ²Π°ΡΠΈΠ²Π½ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ.ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅.ΠΠΈΠ±ΡΠΈΠ΄Π½ΡΠ΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π»ΠΈ 100% Π΄ΠΎΡΡΡΠΏΠ½ΠΎΡΡΡ ΡΠ΅Π²Π°ΡΠΊΡΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΈ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΎΠ΄Π½ΠΎΠΉ Π³ΠΎΡΠΏΠΈΡΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ, ΡΡΠΎ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠΎΠΊΡΠ°ΡΠ°Π»ΠΎ Π»Π΅ΡΠ°Π»ΡΠ½ΠΎΡΡΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΎΡ ΠΈΠ½ΡΠ°ΡΠΊΡΠ° ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΈ ΠΎΡΡΡΠΎΠ³ΠΎ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠ³ΠΎ ΠΊΡΠΎΠ²ΠΎΠΎΠ±ΡΠ°ΡΠ΅Π½ΠΈΡ Π² ΠΏΠ΅ΡΠΈΠΎΠ΄ ΠΎΠΆΠΈΠ΄Π°Π½ΠΈΡ ΡΠ»Π΅Π΄ΡΡΡΠ΅Π³ΠΎ ΡΡΠ°ΠΏΠ° Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΈ ΠΏΠΎΡΡΠ°ΠΏΠ½ΠΎΠΉ ΡΡΡΠ°ΡΠ΅Π³ΠΈΠΈ (ΠΏΠΎΡΡΠΈ Π½Π° 5%). ΠΠΈΠ±ΡΠΈΠ΄Π½ΡΠ΅ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° ΠΌΠΎΠ³ΡΡ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡΡΡ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ Π²ΡΡΠΎΠΊΠΈΠΌ ΡΠΈΡΠΊΠΎΠΌ Β«ΠΎΡΠΊΡΡΡΡΡ
Β» ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ Π½Π° ΡΠ΅ΡΠ΄ΡΠ΅, ΡΡΠΆΠ΅Π»ΠΎΠΉ ΡΠΎΠΏΡΡΡΡΠ²ΡΡΡΠ΅ΠΉ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠ΅ΠΉ (ΠΎΠΆΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ, ΡΠ°Ρ
Π°ΡΠ½ΡΠΌ Π΄ΠΈΠ°Π±Π΅ΡΠΎΠΌ, Π½Π°ΡΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΡΠ½ΠΊΡΠΈΠΈ ΠΏΠΎΡΠ΅ΠΊ), Π·Π½Π°ΡΠΈΠΌΡΠΌ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ
ΠΈ ΡΠ΅ΡΠ΅Π±ΡΠ°Π»ΡΠ½ΡΠΉ Π°ΡΡΠ΅ΡΠΈΠΉ Ρ Π²ΡΡΠΎΠΊΠΈΠΌ ΡΠΈΡΠΊΠΎΠΌ ΠΈΠ½ΡΠ°ΡΠΊΡΠ° ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° ΠΈ ΠΎΡΡΡΠΎΠ³ΠΎ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠ³ΠΎ ΠΊΡΠΎΠ²ΠΎΠΎΠ±ΡΠ°ΡΠ΅Π½ΠΈΡ. ΠΠ΅Π΄ΠΎΡΡΠ°ΡΠΊΠΎΠΌ Π³ΠΈΠ±ΡΠΈΠ΄Π½ΠΎΠΉ ΡΡΡΠ°ΡΠ΅Π³ΠΈΠΈ ΡΠ²ΠΈΠ»Π°ΡΡ Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠΎΠΊΠ°Ρ ΡΠ°ΡΡΠΎΡΠ° (ΠΏΠΎΡΡΠΈ Π½Π° 7%) Π½Π΅ΡΠ°ΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ½ΡΠ°ΡΠΊΡΠ° ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° Π² ΠΎΡΠ΄Π°Π»Π΅Π½Π½ΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ
Morphology and optical properties of aluminum oxide formed into oxalic electrolyte with addition surface active agents
The article discusses the results of investigations of porous films of alumina, formed into oxalic electrolyte with addition surface active agents, in particular, ordering structure, roughness of a surface, the optical transparency of the electrolyte concentration and surface active agents. Also discusses the features of the formation of porous films of temperature and IR radiation
SYNTHESIS OF NONSTOCHIOMETRIC NANO-NBC AND ITS ELECTROCHEMICAL PERFORMANCE
This work was supported by the Russian Science Foundation (RNF grant No. 19-73-20012)
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