42 research outputs found
Anharmonic theory of superconductivity in the high-pressure materials
Electron-phonon superconductors at high pressures have displayed the highest
values of critical superconducting temperature on record, now rapidly
approaching room temperature. Despite the importance of high-
superconductivity in the quest for room-temperature superconductors, a
mechanistic understanding of the effect of pressure and its complex interplay
with phonon anharmonicity and superconductivity is missing, as numerical
simulations can only bring system-specific details clouding out key players
controlling the physics. Here we develop a minimal model of electron-phonon
superconductivity under an applied pressure which takes into account the
anharmonic decoherence of the optical phonons. We find that behaves
non-monotonically as a function of the ratio , where
is the optical phonon damping and the optical phonon energy at zero
pressure and momentum. Optimal pairing occurs for a critical ratio
when the phonons are on the verge of decoherence
("diffuson-like" limit). Our framework gives insights into recent experimental
observations of as a function of pressure in the complex BCS material
TlInTe
A Unified Understanding of minimum lattice thermal conductivity
We propose a first-principles model of minimum lattice thermal conductivity based on a unified theoretical treatment of thermal transport in crystals and glasses
The Effect of Na Atom on TlInSe2 and TlInTe2 Compounds
Thermoelectric materials have widely used applications in technological areas such as electronic devices and data storage. TlInSe2 and TlInTe2 compounds are among these thermoelectric materials. In this study, while the structural, electronic, and optical properties of TlInSe2, TlInTe2, Tl0.75Na0.25InSe2 and Tl0.75Na0.25InTe2 compounds have been examined with the WIEN2k program based on DFT, their thermoelectric properties have been calculated with another program BoltzTrap. The electronic calculations show that, all compounds exhibit indirect band gap properties. In addition, the band gap energy of Tl0.75Na0.25InSe2 is shifted in the electromagnetic spectrum. The optical properties are found to change depending on the direction for all compounds. Finally, the thermoelectric parameters have been calculated depending on temperature. It is thought that especially the results for Na-doped compounds will be a leading reference for experimental studies
Ab initio study of NaSrSb and NaBaSb as potential thermoelectric prospects
Zintl phases are excellent thermoelectric prospects to put the waste heat to
good use. In the quest of the same, using first-principles methods combined
with Boltzmann transport theory, we explored two recent phases NaSrSb and
NaBaSb. We found low lattice thermal conductivity of 1.9 and 1.3 W m
K at 300~K for NaSrSb and NaBaSb, respectively, which are of the same
order as other potential Zintl phases such as SrAlSb and BaCuSb. We
account for such low values to short phonon lifetimes, small phonon group
velocities, and lattice anharmonicity in the crystal structure. The calculated
electrical transport parameters based on acoustic deformation potential,
ionized impurity, and polar optical phonon scattering mechanisms reveal large
Seebeck coefficients for both materials. Further, we obtain a high figure of
merit of ZT2.0 at 900~K for \textit{n}-type NaSrSb. On the other hand,
the figure of merit of \textit{n}-type NaBaSb surpasses the unity. We are
optimistic about our findings and believe our work would set a basis for future
experimental investigations.Comment: 10 figures, 1 tabl
Current-voltage characteristic of InGaTe?
Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ: ΠΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ ΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΎΠ»ΡΡΠ°ΠΌΠΏΠ΅ΡΠ½ΠΎΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΠΌΠΎΠ½ΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² ΠΈ ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΡ InGaTe2 Π² ΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
, ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
ΠΈ ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΏΠ»ΠΎΡΠ°Π΄ΡΡ
ΠΊΠΎΠ½ΡΠ°ΠΊΡΠΎΠ². ΠΠ΅ΡΠΎΠ΄Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΠΎΠ½ΠΎΠΊΡΠΈΡΡΠ°Π»Π»Ρ InGaTe? Π±ΡΠ»ΠΈ Π²ΡΡΠ°ΡΠ΅Π½Ρ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΡΠΈΠ΄ΠΆΠΌΠ΅Π½Π°-Π‘ΡΠΎΠΊΠ±Π°ΡΠ³Π΅ΡΠ°, Π° ΡΠΎΠ½ΠΊΠΈΠ΅ ΠΏΠ»Π΅Π½ΠΊΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΊΠΎΠ½Π΄Π΅Π½ΡΠ°ΡΠΈΠΈ ΠΈΠ· ΠΏΠ°ΡΠΎΠ²ΠΎΠΉ ΡΠ°Π·Ρ. Π Π΅Π½ΡΠ³Π΅Π½ΠΎΠ³ΡΠ°ΠΌΠΌΡ InGaTe? ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ Π½Π° Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠΌΠ΅ΡΡΠ΅ ΠΠ ΠΠ-2 Π² CuKa ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠΈ (l=1,54178C). ΠΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½ΠΎΠΉ ΡΡΠ΅ΠΉΠΊΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΠ»ΠΈ Ρ ΡΠΎΡΠ½ΠΎΡΡΡΡ 0,005C. ΠΠΎΠ»ΡΡΠ°ΠΌΠΏΠ΅ΡΠ½Π°Ρ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° Π½Π° ΠΎΠ±ΡΠ°Π·ΡΠ°Ρ
ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΠΎΠΉ ΡΠΎΡΠΌΡ ΡΠ°Π·ΠΌΠ΅ΡΠ°ΠΌΠΈ 7?1?1 ΠΌΠΌΡ . ΠΠΎΠ½ΡΠ°ΠΊΡΠ°ΠΌΠΈ ΡΠ»ΡΠΆΠΈΠ»ΠΈ I. n ΠΈ Cu. Π’ΠΎΠΊ, ΡΠ½Π°Π±ΠΆΠ°ΡΡΠΈΠΉ ΠΊΠΎΠ½ΡΡ ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·ΡΠΎΠ², ΠΎΡΠΈΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ ΡΠ°ΠΊ, ΡΡΠΎ ΡΠΎΠΊ ΡΠ΅ΡΠ΅Π· ΠΎΠ±ΡΠ°Π·Π΅Ρ ΠΏΡΠΎΡΠ΅ΠΊΠ°Π΅Ρ Π²Π΄ΠΎΠ»Ρ ΠΏΠΎ ΠΎΡΠΈ c6 ΠΌΠΎΠ½ΠΎΠΊΡΠΈΡΡΠ°Π»Π»Π° InGaTe?. ΠΠΎΠ»ΡΡΠ°ΠΌΠΏΠ΅ΡΠ½Π°Ρ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»Π°ΡΡ Π½Π° ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠΌ ΡΠΎΠΊΠ΅ Π² ΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ: Π Π΅Π½ΡΠ³Π΅Π½ΠΎΡΠ°Π·ΠΎΠ²ΡΠΌ Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ Π²ΡΡΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠ΅ InGaTe2 ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΠ·ΡΠ΅ΡΡΡ Π² ΡΠ΅ΡΡΠ°Π³ΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ ΡΠΈΠ½Π³ΠΎΠ½ΠΈΠΈ Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ ΡΠ΅ΡΠ΅ΡΠΊΠΈ Π°=8,463C; Ρ=6,981C. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈΡΡ ΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΈ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ Π²ΠΎΠ»ΡΡΠ°ΠΌΠΏΠ΅ΡΠ½ΡΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ InGaTe2 ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΎΡΡΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ, Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΎΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ, Π²ΠΎΠ»ΡΡΠ°ΠΌΠΏΠ΅ΡΠ½Π°Ρ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ° ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ InGaTe2 ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΏΠ»ΠΎΡΠ°Π΄ΡΡ
ΠΊΠΎΠ½ΡΠ°ΠΊΡΠΎΠ². ΠΡΡΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄Π°Π½Π½Π°Ρ ΡΠ°Π·Π° ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ°ΡΡΠΈΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ Ρ ΠΏΠ°ΠΌΡΡΡΡ ΠΈ Ρ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ Π²Π΅Π»ΠΈΡΠΈΠ½Π° ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π΅ΡΡΡ, Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ S-ΠΎΠ±ΡΠ°Π·Π½Π°Ρ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ° ΡΡΠ°Π½ΠΎΠ²ΠΈΡΡΡ ΡΡΠΊΠΎ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠΉ. ΠΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½ΠΎ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈΡΡ ΠΠΠ₯ ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΠΏΠ»ΠΎΡΠ°Π΄ΠΈ ΠΈ ΠΎΡ ΡΠ°Π·ΠΌΠ΅ΡΠ° ΡΠ°ΠΌΠΎΠΉ ΠΏΠ»Π΅Π½ΠΊΠΈ. ΠΡΡΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΏΠ»Π΅Π½ΠΊΠΈ ΡΠ°ΠΊΠΆΠ΅ ΠΎΠ±Π»Π°Π΄Π°ΡΡ ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ°ΡΡΠΈΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ ΠΈ Ρ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠ»ΠΎΡΠ°Π΄ΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠΎΠ² Π²Π΅Π»ΠΈΡΠΈΠ½Π° ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΠΎΠΌ ΠΏΡΠΎΠΈΡΡ
ΠΎΠ΄ΠΈΡ ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅, ΡΠΌΠ΅Π½ΡΡΠ°Π΅ΡΡΡ. Π ΡΠ°ΠΊΠΆΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΈ ΠΏΠ»ΠΎΡΠ°Π΄ΠΈ ΠΊΠΎΠ½ΡΠ°ΠΊΡΠΎΠ² ΡΠΏΡΠ°Π²Π»ΡΠ΅ΡΡΡ Π²Π΅Π»ΠΈΡΠΈΠ½Π° ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ. Π ΡΡΠΎ ΠΎΠ·Π½Π°ΡΠ°Π΅Ρ, ΡΡΠΎ Π΄Π°Π½Π½Π°Ρ ΡΠ°Π·Π° ΠΌΠΎΠΆΠ΅Ρ ΡΡΠΏΠ΅ΡΠ½ΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡΡΡ ΠΏΡΠΈ ΡΠΎΠ·Π΄Π°Π½ΠΈΠΈ Π±ΡΡΡΡΠΎΠ΄Π΅ΠΉΡΡΠ²ΡΡΡΠΈΡ
ΠΈ Π²ΡΡΠΎΠΊΠΎΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΏΡΠΈΠ±ΠΎΡΠΎΠ².The main aim of the research is to prepare and study the current-voltage characteristics of single crystals and thin films of InGaTe2 compound in static and dynamic modes at different temperatures and for different contact area. Methods: InGaTe? single crystals were grown by the Bridgman- Stockbarger, and thin films were prepared by the method of physical vapor deposition. InGaTe2 radiographs were obtained on a DRON-2 CuKa radiation (l=1,54178C). The unit cell parameters were determined with an accuracy 0,005C. The current-voltage characteristics was investigated on rectangular samples with dimensions 7?1?1 mmΡ . In and Cu served as contacts. Current supplying the ends of rectangular samples is oriented in the way that current flows through the sample along a single crystal axis c6 of InGaTe?monocrystal. The current-voltage characteristics were examined for constant current in static and dynamic modes. Results. X-ray analysis revealed that InGaTe2 compound crystallizes in tetragonal syngony with lattice parameters a=8,463C; a=6,981C. The authors have investigated the static and dynamic current-voltage characteristics of InGaTe4 at different temperatures, change in the samples temperature in the region of negative differential resistance, dependence of the threshold voltage on the temperature, current-voltage characteristics of InGaTe2 thin films at different contact area. It was ascertained that this phase has switching properties with memory. The threshold voltage increases at temperature decreas. The S-pattern becomes clearly expressed. The authors analyzed the change in the threshold voltage at temperature change. The CVC of thin films were investigated depending on the area and the size of the film itself. It was revealed that the films also exhibit switching properties and decreasing contact area with the magnitude of the threshold voltage at which the switching is reduced. The threshold voltage value is controlled by the changes in temperature and contact area. This means that this phase can be successfully used in the design of fast and highly sensitive instrumentation
Electronic Structure of a Chain-like Compound: TlSe
An ab-initio pseudopotential calculation using density functional theory
within the local density approximation has been performed to investigate the
electronic properties of TlSe which is of chain-like crystal geometry. The
energy bands and effective masses along high symmetry directions, the density
of states and valence charge density distributions cut through various planes
are presented. The results have been discussed in terms of previously existing
experimental and theoretical data, and comparisons with similar compounds have
been made.Comment: 7 page
Upgrade of the MARI spectrometer at ISIS
The MARI direct geometry time-of-flight neutron spectrometer at ISIS has been
upgraded with an supermirror guide and new detector electronics. This has
resulted in a flux gain of at {\AA}, and
improvements on discriminating electrical noise, allowing MARI to continue to
deliver a high quality science program well into its fourth decade of life
Upgrade of the MARI spectrometer at ISIS
The MARI direct geometry time-of-flight neutron spectrometer at ISIS has been upgraded with an m = 3 supermirror guide and new detector electronics. This has resulted in a flux gain of approximate to 6x at lambda = 1.8 angstrom, and improvements on discriminating electrical noise, allowing MARI to continue to deliver a high quality science program well into its fourth decade of life