24 research outputs found
Low-energy optical conductivity of TaP : comparison of theory and experiment
The ab-plane optical conductivity of the Weyl semimetal TaP is calculated from the band structure and compared to the experimental data. The overall agreement between theory and experiment is found to be best when the Fermi level is slightly (20 to 60 meV) shifted upwards in the calculations. This confirms a small unintentional doping of TaP, reported earlier, and allows a natural explanation of the strong low-energy (50 meV) peak seen in the experimental ab-plane optical conductivity: this peak originates from transitions between the almost parallel non-degenerate electronic bands split by spin-orbit coupling. The temperature evolution of the peak can be reasonably well reproduce by calculations using an analog of the Mott formula.Deutsche Forschungsgemeinschaf
Fractional power-law intraband optical conductivity in the low-dimensional Dirac material CaMnBi2
We studied the broadband optical conductivity of CaMnBi2, a material with two-dimensional Dirac electronic bands, and found that both components of the intraband conductivity follow a universal power law as a function of frequency at low temperatures. This conductivity scaling differs from the Drude(-like) behavior, generally expected for free carriers, but matches the predictions for the intraband response of an electronic system in a quantum critical region. Since no other indications of quantum criticality are reported for CaMnBi2 so far, the cause of the observed unusual scaling remains an open question.Deutsche Forschungsgemeinschaf
Boxnep - ΠΌΠΎΠ΄ΡΠ»ΡΠ½ΡΠΉ ΠΏΠΎΠ΄Π²ΠΎΠ΄Π½ΡΠΉ ΡΠΎΠ±ΠΎΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ ΡΠ΅Ρ Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ
The article discusses the relevance of the underwater vehicles are able to solve a wide range of problems. The decision puts in a basis of the research is designing a modular underwater robot. It allows to make a mounting of various equipment and testing it in the water medium. The paper deals with the concept of the robot and its characteristics
ΠΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΏΠΎΠ·ΠΈΡΡΠΎΠ½Π½ΠΎΠΉ ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΠΈ, ΡΠΎΠ²ΠΌΠ΅ΡΠ΅Π½Π½ΠΎΠΉ Ρ ΠΊΠΎΠΌΠΏΡΡΡΠ΅ΡΠ½ΠΎΠΉ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΠ΅ΠΉ, Ρ 18F-Π€ΠΠ Π² Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ΅ ΠΏΠΎΡΠ΅ΡΠ½ΠΎ-ΠΊΠ»Π΅ΡΠΎΡΠ½ΠΎΠ³ΠΎ ΡΠ°ΠΊΠ°
Positron emission tomography combined with computed tomography (PET/CT) is a method, capable of evaluation of not only structural, but also metabolic alterations in organs and tissues. 18F-fluorodeoxyglucose (18F-PDG) PET/CT is widely used in diagnostics of various malignant tumors, but its role in renal cell carcinoma (RCC) remains obscure.Despite its limited effectiveness in primary and differential diagnosis of RCC, PET/CT can be used to determine the grade of malignancy and the histological type of tumor. According to various authors, 18F-FDG standardized uptake value (SUV) of a renal neoplasm can serve as an independent prognostic factor of overall survival.18F-FDG PET/CT is widely used to detect local recurrence and metastatic lesions in various neoplastic processes. Numerous studies confirm the high efficiency of PET/CT in detection of metastases and recurrence discernment for RCC.The ability to assess the metabolic activity of neoplastic foci using PET/CT may allow for evaluation of RCC therapy effectiveness, which is confirmed by clinical studies of various targeted therapy agents, such as tyrosine kinase inhibitors, mammalian target of rapamycin inhibitors, and monoclonal antibodies.Thus, there is growing evidence that 18F-FDG PET/CT is a useful tool in diagnostics of RCC.ΠΠΎΠ·ΠΈΡΡΠΎΠ½Π½Π°Ρ ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½Π°Ρ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΡ, ΡΠΎΠ²ΠΌΠ΅ΡΠ΅Π½Π½Π°Ρ Ρ ΠΊΠΎΠΌΠΏΡΡΡΠ΅ΡΠ½ΠΎΠΉ ΡΠΎΠΌΠΎΠ³ΡΠ°ΡΠΈΠ΅ΠΉ (ΠΠΠ’/ΠΠ’), ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΎΡΠ΅Π½ΠΊΠΈ Π½Π΅ ΡΠΎΠ»ΡΠΊΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
, Π½ΠΎ ΠΈ ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Π² ΠΎΡΠ³Π°Π½Π°Ρ
ΠΈ ΡΠΊΠ°Π½ΡΡ
. ΠΠΠ’/ΠΠ’ Ρ 18F-ΡΡΠΎΡΠ΄Π΅Π·ΠΎΠΊΡΠΈΠ³Π»ΡΠΊΠΎΠ·ΠΎΠΉ (18F-Π€ΠΠ) ΡΠΈΡΠΎΠΊΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΡΡΡ Π² Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ΅ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΎΠΏΡΡ
ΠΎΠ»Π΅ΠΉ, ΠΎΠ΄Π½Π°ΠΊΠΎ ΡΠΎΠ»Ρ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΏΡΠΈ ΠΏΠΎΡΠ΅ΡΠ½ΠΎ-ΠΊΠ»Π΅ΡΠΎΡΠ½ΠΎΠΌ ΡΠ°ΠΊΠ΅ (ΠΠΠ ) ΠΎΡΡΠ°Π΅ΡΡΡ Π½Π΅ΡΡΠ½ΠΎΠΉ.ΠΠ΅ΡΠΌΠΎΡΡΡ Π½Π° ΠΎΠ³ΡΠ°Π½ΠΈΡΠ΅Π½Π½ΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ Π² ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΠΎΠΉ ΠΈ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎΠΉ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ΅ ΠΠΠ , ΠΠΠ’/ΠΠ’ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Π° Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΡΡΠΈ ΠΈ Π³ΠΈΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΈΠΏΠ° ΠΎΠΏΡΡ
ΠΎΠ»ΠΈ. ΠΡΠΎΠΌΠ΅ ΡΡΠΎΠ³ΠΎ, ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π°Π²ΡΠΎΡΠΎΠ², ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΡΡΠ°Π½Π΄Π°ΡΡΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΠΏΠΎΠ³Π»ΠΎΡΠ΅Π½ΠΈΡ (standardized uptake value, SUV) 18F-Π€ΠΠ Π½Π΅ΠΎΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ°Π³Π° ΠΏΡΠΈ ΠΠΠ ΠΌΠΎΠΆΠ΅Ρ ΡΠ»ΡΠΆΠΈΡΡ Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΠΌ ΠΏΡΠΎΠ³Π½ΠΎΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠ°ΠΊΡΠΎΡΠΎΠΌ ΠΎΠ±ΡΠ΅ΠΉ Π²ΡΠΆΠΈΠ²Π°Π΅ΠΌΠΎΡΡΠΈ.ΠΠΠ’/ΠΠ’ Ρ 18F-Π€ΠΠ ΡΠΈΡΠΎΠΊΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΡΡΡ Π΄Π»Ρ Π²ΡΡΠ²Π»Π΅Π½ΠΈΡ ΠΌΠ΅ΡΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΡΠΈΠ΄ΠΈΠ²Π° ΠΈ ΠΌΠ΅ΡΠ°ΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π΄ΠΈΡΡΠ΅ΠΌΠΈΠ½Π°ΡΠΈΠΈ ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π½Π΅ΠΎΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ΅ΡΡΠ°Ρ
. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΌΠ½ΠΎΠ³ΠΎΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°ΡΡ Π²ΡΡΠΎΠΊΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΠΠ’/ΠΠ’ Π² ΠΎΡΠ΅Π½ΠΊΠ΅ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΠΎΡΡΠΈ ΠΈ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ΅ ΡΠ΅ΡΠΈΠ΄ΠΈΠ²Π° ΠΠΠ .ΠΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π½Π΅ΠΎΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ°Π³ΠΎΠ² Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΠΠ’/ΠΠ’ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ ΡΡΠΎΡ ΠΌΠ΅ΡΠΎΠ΄ Π΄Π»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΠΠ , ΡΡΠΎ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°Π΅ΡΡΡ Π΄Π°Π½Π½ΡΠΌΠΈ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ°ΡΠ³Π΅ΡΠ½ΡΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ², ΡΠ°ΠΊΠΈΡ
ΠΊΠ°ΠΊ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΡ ΡΠΈΡΠΎΠ·ΠΈΠ½ΠΊΠΈΠ½Π°Π·Ρ, ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΡ ΠΌΠΈΡΠ΅Π½ΠΈ ΡΠ°ΠΏΠ°ΠΌΠΈΡΠΈΠ½Π° ΠΌΠ»Π΅ΠΊΠΎΠΏΠΈΡΠ°ΡΡΠΈΡ
ΠΈ ΠΌΠΎΠ½ΠΎΠΊΠ»ΠΎΠ½Π°Π»ΡΠ½ΡΠ΅ Π°Π½ΡΠΈΡΠ΅Π»Π°.Π’Π°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, Π²ΡΠ΅ Π±ΠΎΠ»ΡΡΠ΅ Π΄Π°Π½Π½ΡΡ
ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΠ΅Ρ Π² ΠΏΠΎΠ»ΡΠ·Ρ ΡΠΎΠ³ΠΎ, ΡΡΠΎ ΠΠΠ’/ΠΠ’ Ρ 18F-Π€ΠΠ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΏΠΎΠ»Π΅Π·Π½ΡΠΌ ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠΎΠΌ Π² Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ΅ ΠΠΠ .
Rotational coherence of encapsulated ortho and para water in fullerene-C60 revealed by time-domain terahertz spectroscopy
We resolve the real-time coherent rotational motion of isolated water molecules encapsulated in fullerene-C60 cages by time-domain terahertz (THz) spectroscopy. We employ single-cycle THz pulses to excite the low-frequency rotational motion of water and measure the subsequent coherent emission of electromagnetic waves by water molecules. At temperatures belowβ~β100Β K, C60 lattice vibrational damping is mitigated and the quantum dynamics of confined water are resolved with a markedly long rotational coherence, extended beyond 10Β ps. The observed rotational transitions agree well with low-frequency rotational dynamics of single water molecules in the gas phase. However, some additional spectral features with their major contribution atβ~2.26 THz are also observed which may indicate interaction between water rotation and the C60 lattice phonons. We also resolve the real-time change of the emission pattern of water after a sudden cooling to 4Β K, signifying the conversion of ortho-water to para-water over the course of 10s hours. The observed long coherent rotational dynamics of isolated water molecules confined in C60 makes this system an attractive candidate for future quantum technology.Deutsche ForschungsgemeinschaftEPSRC-UKProjekt DEA
Advances in Topological Materials
Materials with electronic bands that possess nontrivial topology have remained a focal point of condensed matter physics since 2005, when topological insulators were theoretically discovered by Kane and Mele [...
Low-Energy Optical Conductivity of TaP: Comparison of Theory and Experiment
The ab-plane optical conductivity of the Weyl semimetal TaP is calculated from the band structure and compared to the experimental data. The overall agreement between theory and experiment is found to be best when the Fermi level is slightly (20 to 60 meV) shifted upwards in the calculations. This confirms a small unintentional doping of TaP, reported earlier, and allows a natural explanation of the strong low-energy (50 meV) peak seen in the experimental ab-plane optical conductivity: this peak originates from transitions between the almost parallel non-degenerate electronic bands split by spin-orbit coupling. The temperature evolution of the peak can be reasonably well reproduce by calculations using an analog of the Mott formula