59 research outputs found
MC-128: current commutator for silicon strip detector tests
The MC-128 is a CAMAC module designed to simplify routine tests of multichannel semiconductor detectors. It was developed at Budker Institute of Nuclear Physics (BINP) Novosibirsk in collaboration with RD2 as part of the ATLAS SCT development program. The module provides 128 channels, offering sequential measurements of the currents flowing grom detector strips to a grounded Common Bus. Each input stays virtually connected to the Common Bus independently on whether its current is measured or not. Eight inputs are permanently connected to the Common Bus, allowing the connection of additional elements like guard ring structures. The total detector current can be measured as the current flowing through the Common Bus. Measurements are accessible via a CAMAC bus and in analog form via a front panel detector. Optionally, the MC 128 allows the measurement of the capacitance between each strip and the common (high voltage) electrode of the detector at 10 kHz frequency
ΠΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠ΅ Ρ Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ Π»ΡΡΠ΅Π²ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ Ρ ΠΎΠ½ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΡΠΈ Π»ΡΡΠ΅Π²ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ Π΄Π°Π½Π½ΡΡ Π ΠΠ’
Objective. Comparison of the magnitude of the change in the density of lung tissue and the volume of these changes after radiation therapy over time based on the data obtained using the new method of quantitative analysis developed by us and with the usual visual assessment of the CT data.Materials and methods. We used the data of dynamic observation of 90 patients who underwent RT for the tumors of thoracic localization during the period from 2014 to 2021 at the Federal Institution βRussian Scientific Center of Roentgenoradiologyβ. These patients had CT examinations performed before and after RT. Control CT studies were performed 1β237 days after RT (mean control interval 96 Β± 64.3 days). A total of 238 CT studies of these patients were analyzed, with an average number of RCT studies per patient of 2.6. Among the selected patients, there were 36 (40%) men and 54 (60%) women aged 23 to 86 years (the average age was 51.9 Β± 15.6 years).Results. Radiation damage in the lungs using the method of quantitative analysis of CT data is detected starting from the value of ΞHU = 20 and volume from 3.2% for the early period (15β35 days) after the end of treatment. Starting from 15β25 to 50 days after the end of RT, quantitative analysis reveals primary changes in the lung tissue, incl. and undetectable visually (from 20 to 80 HU), and to suggest further dynamics of these changes depending on the characteristics of the performed RT. From 50 to 80 days β reveals the real volume of radiation pulmonitis by taking into account the changes invisible during visual analysis in the lung tissue irradiated at a dose of 20 Gy to 30 Gy. From 80 to 120 days β allows you to assess the presence and dynamics of changes in the lung tissue with the threshold radiation dose in the lung tissue 30β35 Gy. From 120 onwards, quantitative analysis of CT data, as well as visual assessment, reveals damage in areas of the lungs with the dose of more than 30β35 Gy, which is caused by post-radiation pneumofibrosis. On the basis of the obtained quantitative data on radiation lung damage, the mathematical regularities of the development of this process were calculated, taking into account the time and dose factors.Conclusions. Quantitative assessment of changes in lung density according to CT data in dynamics, carried out using the technique developed by us, is a radiomic indicator of their radiation damage during therapeutic irradiation in cancer patients, which, in combination with the presented mathematical model, can be used for diagnostic purposes to quantify the severity and predicting the dynamics of radiation damage to the lungs in general, as well as identifying individual radiosensitivity.The results obtained can be presented not only in the form of graphs, but also in the form of color maps with preservation of anatomical landmarks, which is convenient for use in clinical practice to support medical decision-making on patient management.Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ: ΡΠΎΠΏΠΎΡΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ ΠΈ ΠΎΠ±ΡΠ΅ΠΌΠΎΠ² ΡΡΠΈΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ ΠΏΠΎΡΠ»Π΅ Π»ΡΡΠ΅Π²ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ (ΠΠ’) Ρ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ΠΌ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ Π΄Π°Π½Π½ΡΡ
, ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌΡΡ
Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠΉ Π½Π°ΠΌΠΈ Π½ΠΎΠ²ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ ΠΏΡΠΈ ΠΎΠ±ΡΡΠ½ΠΎΠΉ Π²ΠΈΠ·ΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΎΡΠ΅Π½ΠΊΠ΅ Π΄Π°Π½Π½ΡΡ
Π ΠΠ’.ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈΡΡ Π΄Π°Π½Π½ΡΠ΅ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ 90 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠΌ Π±ΡΠ»Π° ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π° ΠΠ’ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρ ΠΎΠΏΡΡ
ΠΎΠ»Π΅ΠΉ ΡΠΎΡΠ°ΠΊΠ°Π»ΡΠ½ΠΎΠΉ Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°ΡΠΈΠΈ Π·Π° ΠΏΠ΅ΡΠΈΠΎΠ΄ Ρ 2014 ΠΏΠΎ 2021 Π³. Π² Π€ΠΠΠ£ βΠ ΠΎΡΡΠΈΠΉΡΠΊΠΈΠΉ Π½Π°ΡΡΠ½ΡΠΉ ΡΠ΅Π½ΡΡ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈβ. Π£ Π²ΡΠ΅Ρ
ΡΡΠΈΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΈΠΌΠ΅Π»ΠΈΡΡ Π ΠΠ’-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ, Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΡΠ΅ Π΄ΠΎ ΠΈ ΠΏΠΎΡΠ»Π΅ ΠΠ’. ΠΠΎΠ½ΡΡΠΎΠ»ΡΠ½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π²ΡΠΏΠΎΠ»Π½ΡΠ»ΠΈΡΡ ΡΠ΅ΡΠ΅Π· 1β237 ΡΡΡ ΠΏΠΎΡΠ»Π΅ ΠΠ’ (ΡΡΠ΅Π΄Π½ΠΈΠΉ ΠΈΠ½ΡΠ΅ΡΠ²Π°Π» ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ 96 Β± 64,3 ΡΡΡ). ΠΡΠ΅Π³ΠΎ Π±ΡΠ»ΠΎ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½ΠΎ 238 Π ΠΠ’-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΡΠΎ ΡΡΠ΅Π΄Π½ΠΈΠΌ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎΠΌ Π ΠΠ’-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π° ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° 2,6. Π‘ΡΠ΅Π΄ΠΈ ΠΎΡΠΎΠ±ΡΠ°Π½Π½ΡΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π±ΡΠ»ΠΎ 36 (40,0%) ΠΌΡΠΆΡΠΈΠ½ ΠΈ 54 (60,0%) ΠΆΠ΅Π½ΡΠΈΠ½Ρ Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ ΠΎΡ 23 Π΄ΠΎ 86 Π»Π΅Ρ (ΡΡΠ΅Π΄Π½ΠΈΠΉ Π²ΠΎΠ·ΡΠ°ΡΡ 51,9 Β± 15,6 Π³ΠΎΠ΄Π°).Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΠ΅Π΄Π»Π°Π³Π°Π΅ΠΌΠ°Ρ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Π΄Π°Π½Π½ΡΡ
Π ΠΠ’ Π²ΡΡΠ²Π»ΡΠ΅Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ ΠΎΠ±Π»ΡΡΠ΅Π½Π½ΡΡ
ΡΡΠ°ΡΡΠΊΠΎΠ² Π»Π΅Π³ΠΊΠΎΠ³ΠΎ Π½Π°ΡΠΈΠ½Π°Ρ Ρ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΠΎΡ 20 HU ΠΈ ΠΎΠ±ΡΠ΅ΠΌΠ° ΠΎΡ 3,2% Π΄Π»Ρ ΡΠ°Π½Π½Π΅Π³ΠΎ ΠΏΠ΅ΡΠΈΠΎΠ΄Π° (15β35 ΡΡΡ) ΠΏΠΎΡΠ»Π΅ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΡ ΠΠ’. ΠΠ°ΡΠΈΠ½Π°Ρ Ρ 25-Ρ
ΠΏΠΎ 50-Π΅ ΡΡΡΠΊΠΈ ΠΏΠΎΡΠ»Π΅ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΡ ΠΠ’ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ Π²ΡΡΠ²ΠΈΡΡ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΡΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ Π² Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΈ Π½Π΅ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΠΌΡΠ΅ Π²ΠΈΠ·ΡΠ°Π»ΡΠ½ΠΎ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΡΡ ΠΎΡ 20 Π΄ΠΎ 80 HU, ΠΈ ΠΏΡΠ΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠΈΡΡ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΡΡ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΡ ΡΡΠΈΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠΉ ΠΠ’. Π‘ 50-Ρ
ΠΏΠΎ 80-Π΅ ΡΡΡΠΊΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Π²ΡΡΠ²Π»ΡΠ΅Ρ ΡΠ΅Π°Π»ΡΠ½ΡΠΉ ΠΎΠ±ΡΠ΅ΠΌ Π»ΡΡΠ΅Π²ΠΎΠ³ΠΎ ΠΏΡΠ»ΡΠΌΠΎΠ½ΠΈΡΠ° Π·Π° ΡΡΠ΅Ρ ΡΡΠ΅ΡΠ° Π½Π΅Π²ΠΈΠ΄ΠΈΠΌΡΡ
ΠΏΡΠΈ Π²ΠΈΠ·ΡΠ°Π»ΡΠ½ΠΎΠΌ Π°Π½Π°Π»ΠΈΠ·Π΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ, ΠΎΠ±Π»ΡΡΠ΅Π½Π½ΠΎΠΉ Π² Π΄ΠΎΠ·Π΅ ΠΎΡ 20 Π΄ΠΎ 30 ΠΡ. Π‘ 80-Ρ
ΠΏΠΎ 120-Π΅ ΡΡΡΠΊΠΈ β ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΎΡΠ΅Π½ΠΈΡΡ Π½Π°Π»ΠΈΡΠΈΠ΅ ΠΈ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Π² Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ, ΠΎΠ±Π»ΡΡΠ΅Π½Π½ΠΎΠΉ Π² Π΄ΠΎΠ·Π΅ Π±ΠΎΠ»Π΅Π΅ 30β35 ΠΡ. ΠΠ°ΡΠΈΠ½Π°Ρ ΡΠΎ 120-Ρ
ΡΡΡΠΎΠΊ ΠΈ Π΄Π°Π»Π΅Π΅ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Π ΠΠ’ Π΄Π°Π½Π½ΡΡ
, ΠΊΠ°ΠΊ ΠΈ Π²ΠΈΠ·ΡΠ°Π»ΡΠ½Π°Ρ ΠΎΡΠ΅Π½ΠΊΠ°, Π²ΡΡΠ²Π»ΡΠ΅Ρ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΡΠΎΠΉΠΊΠΎΠ³ΠΎ ΠΏΠΎΡΡΠ»ΡΡΠ΅Π²ΠΎΠ³ΠΎ ΠΏΠ½Π΅Π²ΠΌΠΎΡΠΈΠ±ΡΠΎΠ·Π° Π² ΡΡΠ°ΡΡΠΊΠ°Ρ
Π»Π΅Π³ΠΊΠΈΡ
, ΠΎΠ±Π»ΡΡΠ΅Π½Π½ΡΡ
Π² Π΄ΠΎΠ·Π΅ Π±ΠΎΠ»Π΅Π΅ 30β35 ΠΡ. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
Π΄Π°Π½Π½ΡΡ
ΠΎ Π»ΡΡΠ΅Π²ΠΎΠΌ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠΈ Π»Π΅Π³ΠΎΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ Π±ΡΠ»Π° ΡΠ°ΡΡΡΠΈΡΠ°Π½Π° ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠ°Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΡΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡΠ° Ρ ΡΡΠ΅ΡΠΎΠΌ Π²ΡΠ΅ΠΌΠ΅Π½Π½FΠΎΠ³ΠΎ ΠΈ Π΄ΠΎΠ·ΠΎΠ²ΡΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ².ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½Π°Ρ ΠΎΡΠ΅Π½ΠΊΠ° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ Π»Π΅Π³ΠΊΠΈΡ
ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ Π ΠΠ’ Π² Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ ΠΏΠΎ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠΉ Π½Π°ΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠ°Π΄ΠΈΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΌ ΠΈΡ
Π»ΡΡΠ΅Π²ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ ΠΏΡΠΈ ΡΠ΅ΡΠ°ΠΏΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΎΠ±Π»ΡΡΠ΅Π½ΠΈΠΈ ΠΎΠ½ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠΉ Π² ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΠΈ Ρ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΠΎΠΉ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΡΡ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ Π² Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅Π»ΡΡ
Π΄Π»Ρ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ ΡΡΠΆΠ΅ΡΡΠΈ ΠΈ ΠΏΡΠΎΠ³Π½ΠΎΠ·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ Π»ΡΡΠ΅Π²ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ Π»Π΅Π³ΠΊΠΈΡ
Π² ΡΠ΅Π»ΠΎΠΌ, Π° ΡΠ°ΠΊΠΆΠ΅ Π²ΡΡΠ²Π»Π΅Π½ΠΈΡ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ°Π΄ΠΈΠΎΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ.ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π½Π΅ ΡΠΎΠ»ΡΠΊΠΎ Π² Π²ΠΈΠ΄Π΅ Π³ΡΠ°ΡΠΈΠΊΠΎΠ², Π½ΠΎ ΠΈ Π² Π²ΠΈΠ΄Π΅ ΡΠ²Π΅ΡΠΎΠ²ΡΡ
ΠΊΠ°ΡΡ Ρ ΡΠΎΡ
ΡΠ°Π½Π΅Π½ΠΈΠ΅ΠΌ Π°Π½Π°ΡΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠΈΠ΅Π½ΡΠΈΡΠΎΠ², ΡΡΠΎ ΡΠ΄ΠΎΠ±Π½ΠΎ Π΄Π»Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅ Ρ ΡΠ΅Π»ΡΡ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠΊΠΈ ΠΏΡΠΈΠ½ΡΡΠΈΡ Π²ΡΠ°ΡΠ΅Π±Π½ΡΡ
ΡΠ΅ΡΠ΅Π½ΠΈΠΉ ΠΏΠΎ Π²Π΅Π΄Π΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ²
Discovery of new colonies by Sentinel2 reveals good and bad news for emperor
The distribution of emperor penguins is circumpolar, with 54 colony locations currently reported of which 50 are currently extant as of 2019. Here we report on eight newly discovered colonies and confirm the rediscovery of three breeding sites, only previously reported in the era before Very High Resolution satellite imagery was available, making a total of 61 breeding locations. This represents an increase of ~20% in the number of breeding sites, but, as most of the colonies appear to be small, they may only increase the total population by around 5β10%. The discoveries have been facilitated by the use of Sentinel2 satellite imagery, which has a higher resolution and more efficient search mechanism than the Landsat data previously used to search for colonies. The small size of these new colonies indicates that considerations of reproductive output in relation to metabolic rate during huddling is likely to be of interest. Some of the colonies exist in offshore habitats, something not previously reported for emperor penguins. Comparison with recent modelling results show that the geographic locations of all the newly found colonies are in areas likely to be highly vulnerable under businessβasβusual greenhouse gas emissions scenarios, suggesting that population decreases for the species will be greater than previously thought
NESTOR: A neutrino particle astrophysics underwater laboratory for the Mediterranean
Abstract An underwater neutrino astrophysics laboratory, to be located in the international waters off the Southwest of Greece, near the town of Pylos is now under construction. In the last two years a group of physicists from Greece and Russia have carried out two demonstration experiments in 4km deep water, counting muons and verifying the adequacy of the deep sea site. Plans are presented for a 100, 000 m 2 high energy neutrino detector composed of a hexagon of hexagonal towers, with 1176 optical detector units. A progress report is given and the physics potential of a siggle tower with 168 phototubes (currently under construction) is described
THE EXPRESSIONISM OF L.ANDREEVβS PROSE IN CINEMA
The article considers the issue of the cinematic potential of some prosaic expressionistic works written by L. Andreev. In βThe Letters On Theatreβ (1912-1913) the writer expressed his views on the problems of interaction between theatre, cinema and literature, emphasized the great role of cinematograph and predicted the phenomenon of the film script. Moreover, his close collaboration with the domestic cinema producers had influenced the poetics of his artistic works and therefore provoked future multiple screening of them. Despite the fact that all film scripts made by L. Andreev were based only on his dramas, the majority of film directors turned to his prose for screening - eager to find cinematic equivalents and analogies to his expressionist style. The primary subjects of the paper are film adaptations of Andreevβs literary legacy and the patterns of intermediality used by film directors to embody their interpretations of the original texts
High-frequency waves in the solar coronal plasma
We derived numerical solutions of a dispersion equation in order to analyze the effect of
finite plasma temperature on the high-frequency wave dispersion characteristics in conditions of hot
magnetized plasma in the solar corona. Spectra of the high-frequency eigen modes of these plasma
were determined in conditions when the electron gyrofrequency is lower than the plasma one and when the
eigen modes frequencies are higher than the electron gyrofrequency. The longitudinal wave mode is shown to
turn to the Z-mode at refractive index . At refractive index , the longitudinal wave frequency
increases when n grows, and these waves go to strongly damped ones with an anomalous dispersion. We interpret
some spectral features of type II and IV radio bursts in the solar corona.
High-frequency waves in solar and stellar coronae
On the basis of a numerical solution of dispersion equation we analyze characteristics of
low-damping high-frequency waves in hot magnetized solar and stellar coronal plasmas in conditions when the
electron gyrofrequency is equal or higher than the electron plasma frequency. It is shown that branches that
correspond to Z-mode and ordinary waves approach each other when the magnetic field increases and become
practically indistinguishable in a broad region of frequencies at all angles between the wave vector and the
magnetic field. At angles between the wave vector and the magnetic field close toΒ 90\degr, a wave branch with an
anomalous dispersion may occur. On the basis of the obtained results we suggest a new interpretation of such
events in solar and stellar radio emission as broadband pulsations and spikes
Polarization changes in solar radio emission caused by scattering from high-frequency plasma turbulence
This paper deals with the scattering of electromagnetic radiation during
propagation through a plasma layer with developed Langmuir
turbulence. The ordinary component is slightly lowered, while the
extraordinary component undergoes the most effective scattering.
This leads to a change in the polarization characteristics of the
original radiation, namely: the extraordinarily polarized
emission can undergo a substantial decrease and even the
polarization sign can be changed. AsΒ aΒ consequence the radiation
increases its polarization degree in the ordinary mode.β©We performed calculations of the polarization of the radio
emission propagating through a layer of turbulent plasma and
examined the complex event that occurred on July 14, 2000;
specifically, this event showed long-lasting emissions and the
polarization varied both in time and in frequency range. Assuming
that the variation of the polarization degree during the lifetime
of the phenomenon is determined by the scattering from Langmuir
turbulence, we obtained an estimate of the level of turbulence and
of the magnetic field intensity in the emission region
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