21 results on '"D. Pogosyan"'
Search Results
2. [Translated article] Immunophenotypic Characteristics of Dermal Macrophages in Experimental Sepsis
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G. Demyashkin, E. Shapovalova, M. Malanichev, D. Pogosyan, I. Zorin, V. Shchekin, and M. Zatsepina
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Dermatology ,RL1-803 ,Internal medicine ,RC31-1245 - Published
- 2022
- Full Text
- View/download PDF
3. Non-saccular aneurysms: pathogenesis, clinic and methods of treatment (review)
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A. D. Pogosyan and L. Ya. Kravets
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medicine.medical_specialty ,business.industry ,Geography, Planning and Development ,Clinical course ,Fusiform Aneurysm ,Management, Monitoring, Policy and Law ,medicine.disease ,Treatment review ,030218 nuclear medicine & medical imaging ,Saccular aneurysm ,Clinical Practice ,Pathogenesis ,03 medical and health sciences ,Dissection ,0302 clinical medicine ,cardiovascular system ,Medicine ,cardiovascular diseases ,Radiology ,business ,Stroke ,030217 neurology & neurosurgery - Abstract
In clinical practice, we use the term “fusiform aneurysm” for local expansion of artery. Under this generic term specialists understand heterogeneous arterial pathology, which is very important for diagnosis and choosing the treatment. We conducted an analysis of scientific literature published in 1987–2019, including 63 foreign and 4 Russian sources devoted to pathogenesis and types of non-saccular aneurysms. Among non-saccular aneurysms, dolichoectatic aneurysms are distinguished, rather of genetically or non-atherosclerotic origin and fusiform aneurysm acquired due to dissection processes. Features of mechanisms of their formation, variants of clinical course and methods of treatment are presented.
- Published
- 2020
4. Forecasts for WEAVE-QSO: 3D clustering and connectivity of critical points with Lyman-α tomography
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K Kraljic, C Laigle, C Pichon, S Peirani, S Codis, J Shim, C Cadiou, D Pogosyan, S Arnouts, M Pieri, V Iršič, S S Morrison, J Oñorbe, I Pérez-Ràfols, G Dalton, Laboratoire d'Astrophysique de Marseille (LAM), Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), Institut d'Astrophysique de Paris (IAP), Institut national des sciences de l'Univers (INSU - CNRS)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Théorique - UMR CNRS 3681 (IPHT), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Joseph Louis LAGRANGE (LAGRANGE), Université Nice Sophia Antipolis (1965 - 2019) (UNS), COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de la Côte d'Azur, COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Université Côte d'Azur (UCA)-Université Côte d'Azur (UCA)-Centre National de la Recherche Scientifique (CNRS), Observatoire de la Côte d'Azur (OCA), Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), Korea Institute for Advanced Study (KIAS), Department of Physics and Astronomy [UCL London], University College of London [London] (UCL), Department of Physics, University of Alberta, Kavli Institute for Cosmology [Cambridge] (KICC), University of Cambridge [UK] (CAM), Cavendish Laboratory, Department of Astronomy, University of Illinois, Faculty of Physics [Sevilla University] | Facultad de Física [Universidad de Sevilla], Universidad de Sevilla / University of Sevilla, Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE (UMR_7585)), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Department of Physics [Oxford], University of Oxford, ANR-18-CE31-0009,SPHERES,Modéliser les grandes structures de l'Univers dans le régime non-linéaire(2018), and ANR-19-CE31-0023,DEEPDIP,Apprentissage profond pour les grands programmes d'imagerie(2019)
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Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,surveys ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,FOS: Physical sciences ,galaxies: formation ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,galaxies: evolution ,[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph] ,Astrophysics - Astrophysics of Galaxies ,cosmology: large-scale structure of Universe ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
The upcoming WEAVE-QSO survey will target a high density of quasars over a large area, enabling the reconstruction of the 3D density field through Lyman-$\alpha$ tomography over unprecedented volumes smoothed on intermediate scales ($\approx$ 16 Mpc/$h$). We produce mocks of the Lyman-$\alpha$ forest using LyMAS, and reconstruct the 3D density field between sightlines through Wiener filtering in a configuration compatible with the future WEAVE-QSO observations. The fidelity of the reconstruction is assessed by measuring one- and two-point statistics from the distribution of critical points in the cosmic web. In addition, initial Lagrangian statistics are predicted from first principles, and measurements of the connectivity of the cosmic web are performed. The reconstruction captures well the expected features in the auto- and cross-correlations of the critical points. This remains true after a realistic noise is added to the synthetic spectra, even though sparsity of sightlines introduces systematics, especially in the cross-correlations of points with mixed signature. Specifically, for walls and filaments, the most striking clustering features could be measured with up to 4 sigma of significance with a WEAVE-QSO-like survey. Moreover, the connectivity of each peak identified in the reconstructed field is globally consistent with its counterpart in the original field, indicating that the reconstruction preserves the geometry of the density field not only statistically, but also locally. Hence the critical points relative positions within the tomographic reconstruction could be used as standard rulers for dark energy by WEAVE-QSO and similar surveys., Comment: 26 pages, 22 figures, submitted to MNRAS
- Published
- 2022
5. Production of olefins by the conjugated oxidation of light hydrocarbons
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L. A. Tavadyan, L. N. Strekova, M. D. Pogosyan, Vladimir S. Arutyunov, O.V. Shapovalova, and N. M. Pogosyan
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Ethylene ,General Chemical Engineering ,02 engineering and technology ,General Chemistry ,Oxidative pyrolysis ,Conjugated system ,010402 general chemistry ,021001 nanoscience & nanotechnology ,Photochemistry ,01 natural sciences ,Industrial and Manufacturing Engineering ,Methane ,0104 chemical sciences ,Light hydrocarbons ,chemistry.chemical_compound ,chemistry ,Propane ,Yield (chemistry) ,Environmental Chemistry ,Organic chemistry ,0210 nano-technology - Abstract
A number of possibilities to increase the yield of propylene in the processing of light gaseous hydrocarbons are considered, including the oxidative pyrolysis of propane, conjugated oxidation of propane and ethylene, conjugated oxidation of ethylene and methane, and introduction of methane into the products of a rich methane flame. The principal possibility of production of olefins in non-catalytic gas-phase processes from light gaseous hydrocarbons, including methane, is demonstrated.
- Published
- 2017
6. Oxidative pyrolysis of propane with an admixture of ethylene
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Vladimir S. Arutyunov, N. M. Pogosyan, L. N. Strekova, M. D. Pogosyan, S. D. Arsentiev, and L. A. Tavadyan
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Ethylene ,General Chemical Engineering ,Energy Engineering and Power Technology ,General Chemistry ,Oxidative pyrolysis ,010402 general chemistry ,01 natural sciences ,010406 physical chemistry ,0104 chemical sciences ,Catalysis ,chemistry.chemical_compound ,Fuel Technology ,chemistry ,Geochemistry and Petrology ,Propane ,Scientific method ,Organic chemistry - Abstract
It has been shown that in the case of noncatalytic oxidative pyrolysis of propane, the admixture of ethylene in the reactants significantly increases the concentration of propylene in the products. This process can be arranged in such a manner that the ethylene will not be noticeably consumed, i.e., will actually act as a propylene formation catalyst. This arrangement opens up a possibility to design a selective process for producing propylene directly from propane.
- Published
- 2016
7. On the onset of stochasticity in Λ cold dark matter cosmological simulations
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Jerome Thiebaut, Christophe Pichon, D. Pogosyan, Thierry Sousbie, and Simon Prunet
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Physics ,Velocity dispersion ,Astronomy and Astrophysics ,Observable ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Lambda ,01 natural sciences ,Upper and lower bounds ,Amplitude ,Space and Planetary Science ,0103 physical sciences ,Dark energy ,Statistical physics ,Halo ,010306 general physics ,010303 astronomy & astrophysics ,Scaling - Abstract
The onset of stochasticity is measured in $\Lambda$CDM cosmological simulations using a set of classical observables. It is quantified as the local derivative of the logarithm of the dispersion of a given observable (within a set of different simulations differing weakly through their initial realization), with respect to the cosmic growth factor. In an Eulerian framework, it is shown here that chaos appears at small scales, where dynamic is non-linear, while it vanishes at larger scales, allowing the computation of a critical transition scale corresponding to ~ 3.5 Mpc/h. This picture is confirmed by Lagrangian measurements which show that the distribution of substructures within clusters is partially sensitive to initial conditions, with a critical mass upper bound scaling roughly like the perturbation's amplitude to the power 0.15. The corresponding characteristic mass, $M_{\rm crit}=2 10^{13} M_{\odot}$, is roughly of the order of the critical mass of non linearities at z=1 and accounts for the decoupling induced by the dark energy triggered acceleration. The sensitivity to detailed initial conditions spills to some of the overall physical properties of the host halo (spin and velocity dispersion tensor orientation) while other "global" properties are quite robust and show no chaos (mass, spin parameter, connexity and center of mass position). This apparent discrepancy may reflect the fact that quantities which are integrals over particles rapidly average out details of difference in orbits, while the other observables are more sensitive to the detailed environment of forming halos and reflect the non-linear scale coupling characterizing the environments of halos.
- Published
- 2008
8. Velocity Modification of the Power Spectrum from an Absorbing Medium
- Author
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D. Pogosyan and A. Lazarian
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Physics ,Spectral index ,010504 meteorology & atmospheric sciences ,Turbulence ,Spectral density ,Astronomy and Astrophysics ,Astrophysics ,01 natural sciences ,Spectral line ,Computational physics ,Space and Planetary Science ,0103 physical sciences ,Absorption (electromagnetic radiation) ,010303 astronomy & astrophysics ,Scaling ,Intensity (heat transfer) ,0105 earth and related environmental sciences ,Line (formation) - Abstract
Quantitative description of the statistics of intensity fluctuations within spectral line data cubes introduced in our earlier work is extended to the absorbing media. A possibility of extracting 3D velocity and density statistics from both integrated line intensity as well as from the individual channel maps is analyzed. We find that absorption enables the velocity effects to be seen even if the spectral line is integrated over frequencies. This regime that is frequently employed in observations is characterized by a non-trivial relation between the spectral index of velocities and the spectral index of intensity fluctuations. For instance when density is dominated by fluctuations at large scales, i.e. when correlations scale as r^{-\gamma}, \gamma 0, the resulting spectrum of the integrated lines depends on the scaling of the underlying density and scales as K^{-3+\gamma}. We show that if we take the spectral line slices that are sufficiently thin we recover our earlier results for thin slice data without absorption. As the result we extend the Velocity Channel Analysis (VCA) technique to optically thick lines enabling studies of turbulence in molecular clouds. In addition, the developed mathematical machinery enables a quantitative approach to solving other problems that involved statistical description of turbulence within emitting and absorbing gas.
- Published
- 2004
9. Estimates of Cosmological Parameters Using the Cosmic Microwave Background Angular Power Spectrum of ACBAR
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M. D. Daub, C. Cantalupo, M. Newcomb, J. B. Peterson, J. E. Ruhl, D. Pogosyan, E. Torbet, Andrew E. Lange, Chao-Lin Kuo, P. A. R. Ade, James J. Bock, M. C. Runyan, W. L. Holzapfel, M. Lueker, J. R. Bond, Carlo R. Contaldi, and J. H. Goldstein
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Physics ,Cold dark matter ,010308 nuclear & particles physics ,Cosmic microwave background ,Spectral density ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Lambda ,01 natural sciences ,Omega ,symbols.namesake ,Supernova ,Amplitude ,13. Climate action ,Space and Planetary Science ,0103 physical sciences ,symbols ,010303 astronomy & astrophysics ,Hubble's law - Abstract
We report an investigation of cosmological parameters based on the measurements of anisotropy in the cosmic microwave background radiation (CMB) made by ACBAR. We use the ACBAR data in concert with other recent CMB measurements to derive Bayesian estimates of parameters in inflation-motivated adiabatic cold dark matter models. We apply a series of additional cosmological constraints on the shape and amplitude of the density power spectrum, the Hubble parameter and from supernovae to further refine our parameter estimates. Previous estimates of parameters are confirmed, with sensitive measurements of the power spectrum now ranging from \ell \sim 3 to 2800. Comparing individual best model fits, we find that the addition of \Omega_\Lambda as a parameter dramatically improves the fits. We also use the high-\ell data of ACBAR, along with similar data from CBI and BIMA, to investigate potential secondary anisotropies from the Sunyaev-Zeldovich effect. We show that the results from the three experiments are consistent under this interpretation, and use the data, combined and individually, to estimate \sigma_8 from the Sunyaev-Zeldovich component.
- Published
- 2003
10. Noise Estimation in CMB Time-Streams and Fast Iterative Map-Making
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S. Prunet, P. A. R. Ade, J. J. Bock, J. R. Bond, J. Borrill, A. Boscaleri, K. Coble, B. P. Crill, P. de Bernardis, G. De Gasperis, G. De Troia, P. C. Farese, P. G. Ferreira, K. Ganga, M. Giacometti, E. Hivon, V. V. Hristov, A. Iacoangeli, A. H. Jaffe, A. E. Lange, L. Martinis, S. Masi, P. Mason, P. D. Mauskopf, A. Melchiorri, L. Miglio, T. Montroy, C. B. Netterfield, E. Pascale, F. Piacentini, D. Pogosyan, F. Pongetti, S. Rao, G. Romeo, J. E. Ruhl, F. Scaramuzzi, D. Sforna, and N. Vittorio
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Physics ,Noise estimation ,Noise power spectrum ,Robustness (computer science) ,Iterative method ,Cosmic microwave background ,Statistics ,Map making ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Algorithm - Abstract
We describe here an iterative method for jointly estimating the noise power spectrum from a CMB experiment's time-ordered data, together with the maximum-likelihood map. We test the robustness of this method on simulated Boomerang datasets with realistic noise.
- Published
- 2006
11. A Measurement of the CMB Spectrum from the 2003 Flight of BOOMERANG
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J. Borrill, F. Piacentini, Alessandro Melchiorri, A. de Oliveira-Costa, Theodore Kisner, P. Cabella, Calvin B. Netterfield, J. E. Ruhl, E. Hivon, Enzo Pascale, T. E. Montroy, D. Pogosyan, G. Romeo, S. Ricciardi, P. D. Mauskopf, Carlo R. Contaldi, P. A. R. Ade, Simon Prunet, J. R. Bond, P. Natoli, W. C. Jones, Max Tegmark, C. J. MacTavish, B. P. Crill, J. J. Bock, M. Veneziani, G. De Troia, G. de Gasperis, Nicola Vittorio, P. de Bernardis, Andrew E. Lange, G. Di Stefano, G. Polenta, Andrew H. Jaffe, Paola Santini, Silvia Masi, and A. Boscaleri
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media_common.quotation_subject ,Cosmic microwave background ,FOS: Physical sciences ,Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,01 natural sciences ,Spectral line ,Cosmology ,law.invention ,Settore FIS/05 - Astronomia e Astrofisica ,law ,0103 physical sciences ,Adiabatic process ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics ,media_common ,Physics ,010308 nuclear & particles physics ,Bolometer ,Detector ,Astrophysics (astro-ph) ,Astrophysics::Instrumentation and Methods for Astrophysics ,Astronomy and Astrophysics ,Cosmology: Cosmic Microwave Background ,Polarization (waves) ,Cosmology: Cosmic Microwave Background, Instrumentation: Detectors ,Instrumentation: Detectors ,Space and Planetary Science ,Sky - Abstract
We report measurements of the CMB polarization power spectra from the January 2003 Antarctic flight of BOOMERANG. The primary results come from six days of observation of a patch covering 0.22% of the sky centered near R.A. = 82.5 deg., Dec= -45 deg. The observations were made using four pairs of polarization sensitive bolometers operating in bands centered at 145 GHz. Using two independent analysis pipelines, we measure a non-zero signal in the range 100< l contribution, and a 2-sigma upper limit of 7.0 uK^2 for the spectrum. Estimates of foreground intensity fluctuations and the non-detection of and signals rule out any significant contribution from galactic foregrounds. The results are consistent with a Lambda-CDM cosmology seeded by adiabatic perturbations. We note that this is the first detection of CMB polarization with bolometric detectors., Comment: Submitted to Astrophysical Journal
- Published
- 2005
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12. Recent results from the cosmic microwave background radiation
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Carlo R. Contaldi, M. Giacometti, P. C. Farese, D. Pogosyan, F. Pongetti, V. V. Hristov, A. Iacoangeli, Calvin B. Netterfield, K. Coble, F. Piacentini, Paul Mason, B. P. Crill, J. E. Ruhl, Francesco Scaramuzzi, Andrew E. Lange, Ken Ganga, A. Boscaleri, P. de Bernardis, T. E. Montroy, Enzo Pascale, J. R. Bond, Julian Borrill, J. J. Bock, G. Romeo, P. D. Mauskopf, Andrew H. Jaffe, W. C. Jones, Simon Prunet, E. Hivon, Alessandro Melchiorri, Silvia Masi, Peter A. R. Ade, and L. Martinis
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Physics ,Cosmic microwave background ,Astronomy - Published
- 2001
13. SPECTRUM AND ANISOTROPY OF TURBULENCE FROM MULTI-FREQUENCY MEASUREMENT OF SYNCHROTRON POLARIZATION.
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A. Lazarian and D. Pogosyan
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ANISOTROPY , *MATHEMATICAL models , *PROPERTIES of matter , *TURBULENT heat transfer , *BURGERS' equation , *FLUID dynamics - Abstract
We consider turbulent synchrotron-emitting media that also exhibit Faraday rotation and provide a statistical description of synchrotron polarization fluctuations. In particular, we consider these fluctuations as a function of the spatial separation of the direction of the measurements and as a function of wavelength for the same line of sight. On the basis of our general analytical approach, we introduce several measures that can be used to obtain the spectral slopes and correlation scales of both the underlying magnetic turbulence responsible for emission and the spectrum of the Faraday rotation fluctuations. We show the synergetic nature of these measures and discuss how the study can be performed using sparsely sampled interferometric data. We also discuss how additional characteristics of turbulence can be obtained, including the turbulence anisotropy and the three-dimensional direction of the mean magnetic field. In addition, we consider the cases when the synchrotron emission and Faraday rotation regions are spatially separated. Appealing to our earlier study, we explain that our new results are applicable to a wide range of spectral indexes of relativistic electrons responsible for synchrotron emission. We expect wide application of our techniques, both with existing synchrotron data sets and with big forthcoming data sets from LOFAR and SKA. [ABSTRACT FROM AUTHOR]
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- 2016
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14. PRINCIPAL COMPONENT ANALYSIS STUDIES OF TURBULENCE IN OPTICALLY THICK GAS.
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C. Correia, A. Lazarian, B. Burkhart, D. Pogosyan, and J. R. De Medeiros
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BROWNIAN motion ,INTERSTELLAR medium ,RADIATIVE transfer ,ACOUSTIC transients ,AERODYNAMICS - Abstract
In this work we investigate the sensitivity of principal component analysis (PCA) to the velocity power spectrum in high-opacity regimes of the interstellar medium (ISM). For our analysis we use synthetic position–position–velocity (PPV) cubes of fractional Brownian motion and magnetohydrodynamics (MHD) simulations, post-processed to include radiative transfer effects from CO. We find that PCA analysis is very different from the tools based on the traditional power spectrum of PPV data cubes. Our major finding is that PCA is also sensitive to the phase information of PPV cubes and this allows PCA to detect the changes of the underlying velocity and density spectra at high opacities, where the spectral analysis of the maps provides the universal −3 spectrum in accordance with the predictions of the Lazarian & Pogosyan theory. This makes PCA a potentially valuable tool for studies of turbulence at high opacities, provided that proper gauging of the PCA index is made. However, we found the latter to not be easy, as the PCA results change in an irregular way for data with high sonic Mach numbers. This is in contrast to synthetic Brownian noise data used for velocity and density fields that show monotonic PCA behavior. We attribute this difference to the PCA's sensitivity to Fourier phase information. [ABSTRACT FROM AUTHOR]
- Published
- 2016
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15. STUDYING THE INTERSTELLAR MAGNETIC FIELD FROM ANISOTROPIES IN VELOCITY CHANNELS.
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A. Esquivel, A. Lazarian, and D. Pogosyan
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INTERSTELLAR medium ,MAGNETIC fields ,TURBULENCE ,ANISOTROPY ,PROPERTIES of matter - Abstract
Turbulence in the interstellar medium is anisotropic due to the ubiquitous magnetic fields. This anisotropy depends on the strength of the magnetic field and leaves an imprint on observations of spectral line maps. We use a grid of ideal magnetohydrodynamic simulations of driven turbulence and produce synthetic position–position–velocity maps to study the turbulence anisotropy in velocity channels of various resolutions. We found that the average structure function of velocity channels is aligned with the projection of the magnetic field on the plane of the sky. We also found that the degree of such anisotropy increases with the magnitude of the magnetic field. For thick velocity channels (low velocity resolution), the anisotropy is dominated by density, and the degree of anisotropy in these maps allows one to distinguish sub-Alfvénic and super-Alfvénic turbulence regimes, but it also depends strongly on the sonic Mach number. For thin channels (high velocity resolution), we find that the anisotropy depends less on the sonic Mach number. An important limitation of this technique is that it only gives a lower limit on the magnetic field strength because the anisotropy is related only to the magnetic field component on the plane of the sky. It can, and should, be used in combination with other techniques to estimate the magnetic field, such as the Fermi-Chandrasekhar method, anisotropies in centroids, Faraday rotation measurements, or direct line-of-sight determinations of the field from Zeeman effect observations. [ABSTRACT FROM AUTHOR]
- Published
- 2015
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16. Systematic review of artificial intelligence tack in preventive orthopaedics: is the land coming soon?
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Korneev A, Lipina M, Lychagin A, Timashev P, Kon E, Telyshev D, Goncharuk Y, Vyazankin I, Elizarov M, Murdalov E, Pogosyan D, Zhidkov S, Bindeeva A, Liang XJ, Lasovskiy V, Grinin V, Anosov A, and Kalinsky E
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- Humans, Artificial Intelligence, Hip Joint, Software, Orthopedic Procedures, Orthopedics
- Abstract
Purpose: This study aims to describe and assess the current stage of the artificial intelligence (AI) technology integration in preventive orthopaedics of the knee and hip joints., Materials and Methods: The study was conducted in strict compliance with the Preferred Reporting Items for Systematic Reviews and Meta-Analysis (PRISMA) statement. Literature databases were searched for articles describing the development and validation of AI models aimed at diagnosing knee or hip joint pathologies or predicting their development or course in patients. The quality of the included articles was assessed using the Quality Assessment of Diagnostic Accuracy Studies (QUADAS-2) and QUADAS-AI tools., Results: 56 articles were found that meet all the inclusion criteria. We identified two problems that block the full integration of AI into the routine of an orthopaedic physician. The first of them is related to the insufficient amount, variety and quality of data for training, and validation and testing of AI models. The second problem is the rarity of rational evaluation of models, which is why their real quality cannot always be evaluated., Conclusion: The vastness and relevance of the studied topic are beyond doubt. Qualitative and optimally validated models exist in all four scopes considered. Additional optimization and confirmation of the models' quality on various datasets are the last technical stumbling blocks for creating usable software and integrating them into the routine of an orthopaedic physician., (© 2022. The Author(s) under exclusive licence to SICOT aisbl.)
- Published
- 2023
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17. Immunophenotypic Characteristics of Dermal Macrophages in Experimental Sepsis.
- Author
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Demyashkin G, Shapovalova E, Malanichev M, Pogosyan D, Zorin I, Shchekin V, and Zatsepina M
- Subjects
- Humans, Immunophenotyping, Macrophages, Sepsis
- Published
- 2022
- Full Text
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18. Polarization observations with the Cosmic Background Imager.
- Author
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Readhead AC, Myers ST, Pearson TJ, Sievers JL, Mason BS, Contaldi CR, Bond JR, Bustos R, Altamirano P, Achermann C, Bronfman L, Carlstrom JE, Cartwright JK, Casassus S, Dickinson C, Holzapfel WL, Kovac JM, Leitch EM, May J, Padin S, Pogosyan D, Pospieszalski M, Pryke C, Reeves R, Shepherd MC, and Torres S
- Abstract
Polarization observations of the cosmic microwave background with the Cosmic Background Imager from September 2002 to May 2004 provide a significant detection of the E-mode polarization and reveal an angular power spectrum of polarized emission showing peaks and valleys that are shifted in phase by half a cycle relative to those of the total intensity spectrum. This key agreement between the phase of the observed polarization spectrum and that predicted on the basis of the total intensity spectrum provides support for the standard model of cosmology, in which dark matter and dark energy are the dominant constituents, the geometry is close to flat, and primordial density fluctuations are predominantly adiabatic with a matter power spectrum commensurate with inflationary cosmological models.
- Published
- 2004
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19. Cosmic microwave background snapshots: pre-WMAP and post-WMAP.
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Bond JR, Contaldi C, and Pogosyan D
- Abstract
We highlight the remarkable evolution in the cosmic microwave background (CMB) power spectrum C(l) as a function of multipole l over the past few years, and in the cosmological parameters for minimal inflation models derived from it: from anisotropy results before 2000; in 2000 and 2001 from Boomerang, Maxima and the Degree Angular Scale Interferometer (DASI), extending l to approximately 1000; and in 2002 from the Cosmic Background Imager (CBI), Very Small Array (VSA), ARCHEOPS and Arcminute Cosmology Bolometer Array Receiver (ACBAR), extending l to approximately 3000, with more from Boomerang and DASI as well. Pre-WMAP (pre-Wilkinson Microwave Anisotropy Probe) optimal band powers are in good agreement with each other and with the exquisite one-year WMAP results, unveiled in February 2003, which now dominate the l less, similar 600 bands. These CMB experiments significantly increased the case for accelerated expansion in the early Universe (the inflationary paradigm) and at the current epoch (dark energy dominance) when they were combined with "prior" probabilities on the parameters. The minimal inflation parameter set, [omega(b), omega(cdm), Omega(tot), Omega(Lambda), n(s), tau(C), sigma(8)], is applied in the same way to the evolving data. C(l) database and Monte Carlo Markov Chain (MCMC) methods are shown to give similar values, which are highly stable over time and for different prior choices, with the increasing precision best characterized by decreasing errors on uncorrelated "parameter eigenmodes". Priors applied range from weak ones to stronger constraints from the expansion rate (HST-h), from cosmic acceleration from supernovae (SN1) and from galaxy clustering, gravitational lensing and local cluster abundance (LSS). After marginalizing over the other cosmic and experimental variables for the weak + LSS prior, the pre-WMAP data of January 2003 compared with the post-WMAP data of March 2003 give Omega(tot) = 1.03(-0.04)(+0.05) compared with 1.02(-0.03)(+0.04), consistent with (non-Baroque) inflation theory. Adding the flat Omega(tot) = 1 prior, we find a nearly scale-invariant spectrum, n(s) = 0.95(-0.04)(+0.07) compared with 0.97(-0.02)(+0.02). The evidence for a logarithmic variation of the spectral tilt is less than or approximately 2sigma. The densities are for: baryons, omega(b) identical with Omega(b)h(2) = 0.0217(-0.002)(+0.002) (compared with 0.0228(-0.001)(+0.001)), near the Big Bang nucleosynthesis (BBN) estimate of 0.0214 +/- 0.002; CDM, omega(cdm) = Omega(cdm)h(2) = 0.126(-0.012)(+0.012) (compared with 0.121(-0.010)(+0.010)); the substantial dark (unclustered) energy, Omega(Lambda) approximately 0.66(-0.09)(+0.07) (compared with 0.70(-0.05)(+0.05)). The dark energy pressure-to-density ratio w(Q) is not well constrained by our weak + LSS prior, but adding SN1 gives w(Q) less than or approximately -0.7 for January 2003 and March 2003, consistent with the w(Q) = -1 cosmological constant case. We find sigma(8) = 0.89(-0.07)(+0.06) (compared with 0.86(-0.04)(+0.04)), implying a sizable Sunyaev-Zel'dovich (SZ) effect from clusters and groups; the high-l power found in the January 2003 data suggest sigma(8) approximately 0.94(-0.16)(+0.08) is needed to be SZ-compatible.
- Published
- 2003
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20. Cosmology from MAXIMA-1, BOOMERANG, and COBE DMR cosmic microwave background observations.
- Author
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Jaffe AH, Ade PA, Balbi A, Bock JJ, Bond JR, Borrill J, Boscaleri A, Coble K, Crill BP, de Bernardis P, Farese P, Ferreira PG, Ganga K, Giacometti M, Hanany S, Hivon E, Hristov VV, Iacoangeli A, Lange AE, Lee AT, Martinis L, Masi S, Mauskopf PD, Melchiorri A, Montroy T, Netterfield CB, Oh S, Pascale E, Piacentini F, Pogosyan D, Prunet S, Rabii B, Rao S, Richards PL, Romeo G, Ruhl JE, Scaramuzzi F, Sforna D, Smoot GF, Stompor R, Winant CD, and Wu JH
- Abstract
Recent results from BOOMERANG-98 and MAXIMA-1, taken together with COBE DMR, provide consistent and high signal-to-noise measurements of the cosmic microwave background power spectrum at spherical harmonic multipole bands over 2
- Published
- 2001
- Full Text
- View/download PDF
21. Tree structure of a percolating Universe.
- Author
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Colombi S, Pogosyan D, and Souradeep T
- Abstract
We present a numerical study of topological descriptors of initially Gaussian and scale-free density perturbations evolving via gravitational instability in an expanding Universe. The measured Euler number of the excursion set at the percolation threshold, delta(c), is positive and nearly equal to the number of isolated components, suggesting that these structures are trees. Our study of critical point counts reconciles the clumpy appearance of the density field at delta(c) with measured filamentary local curvature. In the Gaussian limit, we measure delta(c)>sigma, where sigma2 is the variance of the density field.
- Published
- 2000
- Full Text
- View/download PDF
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