28 research outputs found
Momentum alignment and the optical valley Hall effect in low-dimensional Dirac materials
We study the momentum alignment phenomenon and the optical control of valley
population in gapless and gapped graphene-like materials. We show that the
trigonal warping effect allows for the spatial separation of carriers belonging
to different valleys via the application of linearly polarized light. Valley
separation in gapped materials can be detected by measuring the degree of
circular polarization of band-edge photoluminescence at different sides of the
sample or light spot (optical valley Hall effect). We also show that the
momentum alignment phenomenon leads to the giant enhancement of near-band-edge
interband optical transitions in narrow-gap carbon nanotubes and graphene
nanoribbons independent of the mechanism of the gap formation. A detection
scheme to observe these giant interband transitions is proposed which opens a
route for creating novel terahertz radiation emitters.Comment: 28 pages, 9 figure
Tuning terahertz transitions in a double-gated quantum ring
We theoretically investigate the optical functionality of a semiconducting
quantum ring manipulated by two electrostatic lateral gates used to induce a
double quantum well along the ring. The well parameters and corresponding
inter-level spacings, which lie in the THz range, are highly sensitive to the
gate voltages. Our analysis shows that selection rules for inter-level dipole
transitions, caused by linearly polarized excitations, depend on the
polarization angle with respect to the gates. In striking difference from the
conventional symmetric double well potential, the ring geometry permits
polarization-dependent transitions between the ground and second excited
states, allowing the use of this structure in a three-level lasing scheme.Comment: 7 pages, 6 figure
Electro-absorption of silicene and bilayer graphene quantum dots
We study numerically the optical properties of low-buckled silicene and
AB-stacked bilayer graphene quantum dots subjected to an external electric
field, which is normal to their surface. Within the tight-binding model, the
optical absorption is calculated for quantum dots, of triangular and hexagonal
shapes, with zigzag and armchair edge terminations. We show that in triangular
silicene clusters with zigzag edges a rich and widely tunable infrared
absorption peak structure originates from transitions involving zero energy
states. The edge of absorption in silicene quantum dots undergoes red shift in
the external electric field for triangular clusters, whereas blue shift takes
place for hexagonal ones. In small clusters of bilayer graphene with zigzag
edges the edge of absorption undergoes blue/red shift for triangular/hexagonal
geometry. In armchair clusters of silicene blue shift of the absorption edge
takes place for both cluster shapes, while red shift is inherent for both
shapes of the bilayer graphene quantum dots.Comment: 7 pages, 7 figure
2N+4-rule and an atlas of bulk optical resonances of zigzag graphene nanoribbons
Development of on-chip integrated carbon-based optoelectronic nanocircuits requires fast and non-invasive structural characterization of their building blocks. Recent advances in synthesis of single wall carbon nanotubes and graphene nanoribbons allow for their use as atomically precise building blocks. However, while cataloged experimental data are available for the structural characterization of carbon nanotubes, such an atlas is absent for graphene nanoribbons. Here we theoretically investigate the optical absorption resonances of armchair carbon nanotubes and zigzag graphene nanoribbons continuously spanning the tube (ribbon) transverse sizes from 0.5(0.4) nm to 8.1(12.8) nm. We show that the linear mapping is guaranteed between the tube and ribbon bulk resonance when the number of atoms in the tube unit cell is 2 N+ 4 , where N is the number of atoms in the ribbon unit cell. Thus, an atlas of carbon nanotubes optical transitions can be mapped to an atlas of zigzag graphene nanoribbons
Dynamics of Cryogenic Jets: Non-Rayleigh Breakup and Onset of Nonaxisymmetric Motions
We report development of generators for periodic, satellite-free fluxes of
mono-disperse drops with diameters down to 10 mikrometers from cryogenic
liquids like H_2, N_2, Ar and Xe (and, as reference fluid, water). While the
breakup of water jets can well be described by Rayleigh's linear theory, we
find jet regimes for H_2 and N_2 which reveal deviations from this behavior.
Thus, Rayleigh's theory is inappropriate for thin jets that exchange energy
and/or mass with the surrounding medium. Moreover, at high evaporation rates,
axial symmetry of the dynamics is lost. When the drops pass into vacuum, frozen
pellets form due to surface evaporation. The narrow width of the pellet flux
paves the way towards various industrial and scientific applications.Comment: 4 pages, 4 figures, 1 table; final version to appear in Phys.Rev.Lett
(minor changes with respect to v1
Adenosine thiamine triphosphate and adenosine thiamine triphosphate hydrolase activity in animal tissues
Adenosine thiamine triphosphate (AThTP), a vitamin B1 containing nucleotide with unknown biochemiΒcal role, was found previously to be present in various biological objects including bacteria, yeast, some human, rat and mouse tissues, as well as plant roots. In this study we quantify AThTP in mouse, rat, bovine and chicks. We also show that in animal tissues the hydrolysis of AThTP is catalyzed by a membrane-bound enzyme seemingly of microsomal origin as established for rat liver, which exhibits an alkaline pH optimum of 8.0-8.5 and requires no Mg2+ ions for activity. In liver homogenates, AThTP hydrolase obeys Michaelis-Menten kinetics with apparent Km values of 84.4 Β± 9.4 and 54.6 Β± 13.1 Β΅Π as estimated from the Hanes plots for rat and chicken enzymes, respectively. The hydrolysis of AThTP has been found to occur in all samples examined from rat, chicken and bovine tissues, with liver and kidney beingΒ the most abundant in enzyme activity. In rat liver, the activity of AThTP hydrolase depends on the age of animals
Π Π°Π±ΠΎΡΠ° ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ ΡΠΎ ΡΡΡΡΠΊΡΡΡΠΎΠΉ p+βpβn+ Π² ΡΠ΅ΠΆΠΈΠΌΠ΅ ΠΎΠ΄Π½ΠΎΠΊΠ²Π°Π½ΡΠΎΠ²ΠΎΠΉ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ
The conditions for realizing the single-quantum detection mode for silicon photomultiplier tubes with the p+βpβn+ structure are studied and data on their characteristics in this mode are obtained. The structure of the experimental setup and the research technique are presented. Measurements of the counting characteristics of the photodetectors, such as the dependences of the counting rate of single-photon pulses, the speed of dark pulses, and the signal-to-noise ratio, have beenΒ performed. The dependences of the counting rate of one-photon pulses on the intensity of optical radiation recorded by a silicon photomultiplier tube are presented. It was found that these dependences had a linear section, the length of which increased with increasing overvoltage of silicon photomultiplier tubes. Also, with an increase in overvoltage, the angle of inclination of the linear section increased. The dependences of the count rate of one-photon and dark pulses, as well as the signal-to-noise ratio on overvoltage, are given. It was found that the counting rate of dark pulses increased with increasing overvoltage. It was found that the dependence of the signal-to-noise ratio on the overvoltage for these silicon photomultiplier tubes has a maximum. To obtain the maximum sensitivity of the studied silicon photomultiplier tubes, it is necessary to select the overvoltage corresponding to this maximum. As a result of comparing the sensitivity of the investigated silicon photomultiplier tubes and avalanche photodiodes, it was found that silicon photomultiplier tubes operating in the single-quantum detection mode have a higher sensitivity compared to avalanche photodiodes in the same operating mode. With a decrease in temperature, this superiority persisted. Also, a decrease in temperature led to a decrease in the minimum value of the intensity of the recorded optical radiation. Thus, the possibility of operation of silicon photomultiplier tubes in the single-quantum registration mode has been proved. These results can be applied in quantum cryptography systems when receiving an optical signal.ΠΠ·ΡΡΠ΅Π½Ρ ΡΡΠ»ΠΎΠ²ΠΈΡ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΡΠ΅ΠΆΠΈΠΌΠ° ΠΎΠ΄Π½ΠΎΠΊΠ²Π°Π½ΡΠΎΠ²ΠΎΠΉ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ Π΄Π»Ρ ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ ΡΠΎ ΡΡΡΡΠΊΡΡΡΠΎΠΉ p+βpβn+ ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ Π΄Π°Π½Π½ΡΠ΅ ΠΎΠ± ΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°Ρ
Π² ΡΡΠΎΠΌ ΡΠ΅ΠΆΠΈΠΌΠ΅. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΡΡΡΠΊΡΡΡΠ° ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ. ΠΡΠΏΠΎΠ»Π½Π΅Π½Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠ΅ΡΠ½ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠΎΡΠΎΠΏΡΠΈΠ΅ΠΌΠ½ΠΈΠΊΠΎΠ², ΡΠ°ΠΊΠΈΡ
ΠΊΠ°ΠΊ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΡΠΊΠΎΡΠΎΡΡΠΈ ΡΡΠ΅ΡΠ° ΠΎΠ΄Π½ΠΎΡΠΎΡΠΎΠ½Π½ΡΡ
ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ², ΡΠΊΠΎΡΠΎΡΡΠΈ ΡΠ΅ΠΌΠ½ΠΎΠ²ΡΡ
ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² ΠΈ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΡ ΡΠΈΠ³Π½Π°Π»/ΡΡΠΌ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΡΠΊΠΎΡΠΎΡΡΠΈ ΡΡΠ΅ΡΠ° ΠΎΠ΄Π½ΠΎΡΠΎΡΠΎΠ½Π½ΡΡ
ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² ΠΎΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ, ΡΠ΅Π³ΠΈΡΡΡΠΈΡΡΠ΅ΠΌΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΠΌ ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠΌ ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΌ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄Π°Π½Π½ΡΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΈΠΌΠ΅ΡΡ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΠΉ ΡΡΠ°ΡΡΠΎΠΊ, Π΄Π»ΠΈΠ½Π° ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π΅ΡΡΡ Ρ ΡΠΎΡΡΠΎΠΌ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ. Π’Π°ΠΊΠΆΠ΅ Ρ ΡΠΎΡΡΠΎΠΌ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π΅ΡΡΡ ΡΠ³ΠΎΠ» Π½Π°ΠΊΠ»ΠΎΠ½Π° Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠ³ΠΎ ΡΡΠ°ΡΡΠΊΠ°. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΡΠΊΠΎΡΠΎΡΡΠΈ ΡΡΠ΅ΡΠ° ΠΎΠ΄Π½ΠΎΡΠΎΡΠΎΠ½Π½ΡΡ
ΠΈ ΡΠ΅ΠΌΠ½ΠΎΠ²ΡΡ
ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ², Π° ΡΠ°ΠΊΠΆΠ΅ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΡ ΡΠΈΠ³Π½Π°Π»/ΡΡΠΌ ΠΎΡ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ. ΠΠΎΠ»ΡΡΠ΅Π½ΠΎ, ΡΡΠΎ ΡΠΊΠΎΡΠΎΡΡΡ ΡΡΠ΅ΡΠ° ΡΠ΅ΠΌΠ½ΠΎΠ²ΡΡ
ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² Π²ΠΎΠ·ΡΠ°ΡΡΠ°Π΅Ρ Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΡ ΡΠΈΠ³Π½Π°Π»/ΡΡΠΌ ΠΎΡ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ ΡΡΠΈΡ
ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ ΠΈΠΌΠ΅Π΅Ρ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌ. ΠΠ»Ρ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΡ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠΉ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π½ΡΡ
ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ Π²ΡΠ±ΠΈΡΠ°ΡΡ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠ΅, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠ΅Π΅ ΡΡΠΎΠΌΡ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌΡ. Π ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΡΡ
ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ ΠΈ Π»Π°Π²ΠΈΠ½Π½ΡΡ
ΡΠΎΡΠΎΠ΄ΠΈΠΎΠ΄ΠΎΠ² ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΠ΅ ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠ΅ ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»ΠΈ, ΡΠ°Π±ΠΎΡΠ°ΡΡΠΈΠ΅ Π² ΡΠ΅ΠΆΠΈΠΌΠ΅ ΠΎΠ΄Π½ΠΎΠΊΠ²Π°Π½ΡΠΎΠ²ΠΎΠΉ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ, ΠΈΠΌΠ΅ΡΡ Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠΎΠΊΡΡ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ Π»Π°Π²ΠΈΠ½Π½ΡΠΌΠΈ ΡΠΎΡΠΎΠ΄ΠΈΠΎΠ΄Π°ΠΌΠΈ Π² ΡΡΠΎΠΌ ΠΆΠ΅ ΡΠ΅ΠΆΠΈΠΌΠ΅ ΡΠ°Π±ΠΎΡΡ. Π‘ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ Π΄Π°Π½Π½ΠΎΠ΅ ΠΏΡΠ΅Π²ΠΎΡΡ
ΠΎΠ΄ΡΡΠ²ΠΎ ΡΠΎΡ
ΡΠ°Π½ΡΠ΅ΡΡΡ. Π’Π°ΠΊΠΆΠ΅ ΠΏΠΎΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠ΅Π³ΠΈΡΡΡΠΈΡΡΠ΅ΠΌΠΎΠ³ΠΎ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ. Π’Π΅ΠΌ ΡΠ°ΠΌΡΠΌ Π΄ΠΎΠΊΠ°Π·Π°Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΠ°Π±ΠΎΡΡ ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΡ
ΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ Π² ΡΠ΅ΠΆΠΈΠΌΠ΅ ΠΎΠ΄Π½ΠΎΠΊΠ²Π°Π½ΡΠΎΠ²ΠΎΠΉ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ. ΠΠ°Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΌΠΎΠ³ΡΡ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡΡΡ Π² ΡΠΈΡΡΠ΅ΠΌΠ°Ρ
ΠΊΠ²Π°Π½ΡΠΎΠ²ΠΎΠΉ ΠΊΡΠΈΠΏΡΠΎΠ³ΡΠ°ΡΠΈΠΈ ΠΏΡΠΈ ΠΏΡΠΈΠ΅ΠΌΠ΅ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°
ΠΠ΅ΡΠ΅ΠΊΡΠΎΡ ΡΡΠ΅Π΄Π½Π΅Π³ΠΎ ΠΈ Π΄Π°Π»ΡΠ½Π΅Π³ΠΎ ΠΠ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠ»ΠΎΡΠΊΠΈΡ ΠΌΠ°ΡΡΠΈΠ²ΠΎΠ² Π³ΡΠ°ΡΠ΅Π½ΠΎΠ²ΡΡ Π½Π°Π½ΠΎΠ»Π΅Π½Ρ
A concept of a middle- and far-infrared detector has been proposed. The detector is built as a planar collection of parallel graphene strips of different length and width. The feature of the detector scheme is the concurrent utilization of two different detection mechanisms: excitation in the given frequency range of low-frequency interband transitions inherent in armchair graphene strips and antenna resonances of strongly slowed-down surface waves (plasmon polaritons). It has been shown that matching these two resonances results in the essential detector signal amplification, thus providing an alternative way how to solve the problem of the low efficiency of resonant graphene antennas. An approach is proposed to analyze the design of such detectors, as well as to discuss the ways of tuning the both mechanisms.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π° ΠΏΡΠΈΠ½ΡΠΈΠΏΠΈΠ°Π»ΡΠ½Π°Ρ ΡΡ
Π΅ΠΌΠ° Π΄Π΅ΡΠ΅ΠΊΡΠΎΡΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΡΡ
Π²ΠΎΠ»Π½ ΡΡΠ΅Π΄Π½Π΅Π³ΠΎ ΠΈ Π΄Π°Π»ΡΠ½Π΅Π³ΠΎ ΠΠ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° ΡΠ°ΡΡΠΎΡ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½Π°Ρ Π½Π° ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΠ»ΠΎΡΠΊΠΈΡ
ΠΌΠ°ΡΡΠΈΠ²ΠΎΠ² Π³ΡΠ°ΡΠ΅Π½ΠΎΠ²ΡΡ
Π½Π°Π½ΠΎΠ»Π΅Π½Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠΉ ΡΠΈΡΠΈΠ½Ρ ΠΈ Π΄Π»ΠΈΠ½Ρ. ΠΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΡ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΠΌΠΎΠΉ ΡΡ
Π΅ΠΌΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ Π΄Π»Ρ Π΄Π΅ΡΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π΄Π²ΡΡ
ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ²: Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΌΠ΅ΠΆΠ·ΠΎΠ½Π½ΡΡ
ΠΏΠ΅ΡΠ΅Ρ
ΠΎΠ΄ΠΎΠ², ΠΏΡΠΈΡΡΡΠΈΡ
Π³ΡΠ°ΡΠ΅Π½ΠΎΠ²ΡΠΌ Π»Π΅Π½ΡΠ°ΠΌ ΡΠΈΠΏΠ° Β«armchairΒ» Π² Π΄Π°Π½Π½ΠΎΠΉ ΡΠ°ΡΡΠΎΡΠ½ΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ, ΠΈ Π°Π½ΡΠ΅Π½Π½ΡΡ
ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠΎΠ² ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΡΡ
Π²ΠΎΠ»Π½ (ΠΏΠ»Π°Π·ΠΌΠΎΠ½-ΠΏΠΎΠ»ΡΡΠΈΡΠΎΠ½ΠΎΠ²). ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΠΎΠ²ΠΏΠ°Π΄Π΅Π½ΠΈΠ΅ Π΄Π²ΡΡ
ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠΎΠ², Π΄ΠΎΡΡΠΈΠ³Π°Π΅ΠΌΠΎΠ΅ ΠΏΡΡΠ΅ΠΌ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠ΅Π³ΠΎ ΠΏΠΎΠ΄Π±ΠΎΡΠ° Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π½Π°Π½ΠΎΠ»Π΅Π½Ρ ΠΈ Π½Π°ΡΡΡΠΎΠΉΠΊΠΈ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π° Π³ΡΠ°ΡΠ΅Π½Π°, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΡΡΠΈΠ»ΠΈΡΡ ΡΠΈΠ³Π½Π°Π», ΡΠ΅ΠΌ ΡΠ°ΠΌΡΠΌ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Ρ Π°Π»ΡΡΠ΅ΡΠ½Π°ΡΠΈΠ²Π½ΠΎΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ Π½ΠΈΠ·ΠΊΠΎΠΉ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠ½ΡΡ
Π³ΡΠ°ΡΠ΅Π½ΠΎΠ²ΡΡ
Π°Π½ΡΠ΅Π½Π½. Π ΡΠ°Π±ΠΎΡΠ΅ ΠΏΡΠ΅Π΄Π»Π°Π³Π°Π΅ΡΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠΉ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ ΠΊ ΠΏΡΠΎΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ Π°Π½Π°Π»ΠΈΠ·Ρ ΡΠ°ΠΊΠΈΡ
Π΄Π΅ΡΠ΅ΠΊΡΠΎΡΠΎΠ², Π° ΡΠ°ΠΊΠΆΠ΅ ΠΎΠ±ΡΡΠΆΠ΄Π°ΡΡΡΡ ΡΠΏΠΎΡΠΎΠ±Ρ Π½Π°ΡΡΡΠΎΠΉΠΊΠΈ ΠΎΠ±ΠΎΠΈΡ
ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ²
ΠΠ°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Ρ Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ ΡΠΎΡΠΎΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ ΠΎΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ
The characteristics dependence on the ambient temperature for three types of silicon photoelectronic multipliers have been studied in this research. The prototypes of Si-photoelectronic multipliers with a p+βpβn+ structure produced by JSC Integral (Republic of Belarus), serially produced silicon photoelectronic multipliers KETEK Π Π3325 and ON Semi FC 30035 have been used as objects of research. We present the setup diagram and research technique. Measurements of the photocurrent magnitude versus the illumination intensity, calculations of the critical and threshold intensities, and the dynamic range have been performed. We also present the photocurrent dependences on the illumination intensity at different ambient temperatures. As it was found, these dependences have a linear section, the length of which characterizes the critical intensity value, and the inclination angle of the linear section to the intensity axis characterizes the photodetector sensitivity to optical radiation. It has been determined that the temperature increase leads to an increase in the critical intensity value and to a decrease in the sensitivity value. We present the dependences of the threshold intensity on the overvoltage at different ambient temperatures. The dependence of the threshold intensity on overvoltage is most strongly pronounced when the supply voltage is below the breakdown voltage. It was found that the threshold intensity is increased with the temperature increase and the threshold intensity dependence on the temperature is the same for all investigated photodetectors. It was found that the dynamic range value is decreased with the temperature increase, which is caused by a more significant change in the threshold intensity as compared to the critical one. The results given in this article can be applied when developing and designing the tools and devices for recording optical radiation based on silicon photoelectronic multipliers.ΠΠ·ΡΡΠ΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΎΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΎΠΊΡΡΠΆΠ°ΡΡΠ΅ΠΉ ΡΡΠ΅Π΄Ρ ΡΡΠ΅Ρ
ΡΠΈΠΏΠΎΠ² ΠΊΡΠ΅ΠΌΠ½ΠΈΠ΅Π²ΡΡ
ΡΠΎΡΠΎΡΠΌΠ½ΠΎΠΆΠΈΡΠ΅Π»Π΅ΠΉ. Π ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ² ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈΡΡ ΠΎΠΏΡΡΠ½ΡΠ΅ ΠΎΠ±ΡΠ°Π·ΡΡ Si-Π€ΠΠ£ ΡΠΎ ΡΡΡΡΠΊΡΡΡΠΎΠΉ p+βpβn+ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π° ΠΠΠ Β«ΠΠ½ΡΠ΅Π³ΡΠ°Π»Β» (Π Π΅ΡΠΏΡΠ±Π»ΠΈΠΊΠ° ΠΠ΅Π»Π°ΡΡΡΡ), ΡΠ΅ΡΠΈΠΉΠ½ΠΎ Π²ΡΠΏΡΡΠΊΠ°Π΅ΠΌΡΠ΅ Si-Π€ΠΠ£ KETEK Π Π3325 ΠΈ ON Semi FC 30035. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΡΡ
Π΅ΠΌΠ° ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. ΠΡΠΏΠΎΠ»Π½Π΅Π½Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΡΠΎΡΠΎΡΠΎΠΊΠ° ΠΎΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ Π·Π°ΡΠ²Π΅ΡΠΊΠΈ, ΡΠ°ΡΡΠ΅ΡΡ ΠΊΡΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ, Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° ΡΠ΅Π³ΠΈΡΡΡΠΈΡΡΠ΅ΠΌΠΎΠ³ΠΎ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΡΠΎΡΠΎΡΠΎΠΊΠ° ΠΎΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ Π·Π°ΡΠ²Π΅ΡΠΊΠΈ ΠΏΡΠΈ ΡΠ°Π·Π½ΡΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
ΠΎΠΊΡΡΠΆΠ°ΡΡΠ΅ΠΉ ΡΡΠ΅Π΄Ρ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄Π°Π½Π½ΡΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΈΠΌΠ΅ΡΡ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΠΉ ΡΡΠ°ΡΡΠΎΠΊ, Π΄Π»ΠΈΠ½Π° ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ ΠΊΡΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ, Π° ΡΠ³ΠΎΠ» Π½Π°ΠΊΠ»ΠΎΠ½Π° Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠ³ΠΎ ΡΡΠ°ΡΡΠΊΠ° ΠΊ ΠΎΡΠΈ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ β ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ Si-Π€ΠΠ£ ΠΊ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ. ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΠΎΡΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠΎ- ΡΡΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ ΠΊΡΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΎΡ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΈ ΡΠ°Π·Π½ΡΡ
ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ°Ρ
ΠΎΠΊΡΡΠΆΠ°ΡΡΠ΅ΠΉ ΡΡΠ΅Π΄Ρ. ΠΠ°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠΈΠ»ΡΠ½ΠΎ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΎΡ ΠΏΠ΅ΡΠ΅Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΎΡΠ²Π»ΡΠ΅ΡΡΡ ΠΏΡΠΈ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΈ ΠΏΠΈΡΠ°Π½ΠΈΡ Π½ΠΈΠΆΠ΅ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ±ΠΎΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΏΠΎΡΠΎΠ³ΠΎΠ²Π°Ρ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΠΎΠ²ΡΡΠ°Π΅ΡΡΡ Ρ ΡΠΎΡΡΠΎΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΈ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΎΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²Π° Π΄Π»Ρ Π²ΡΠ΅Ρ
ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΡΡ
Si-Π€ΠΠ£. ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΎ, ΡΡΠΎ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° Ρ ΡΠΎΡΡΠΎΠΌ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΡΠΌΠ΅Π½ΡΡΠ°Π΅ΡΡΡ, ΡΡΠΎ Π²ΡΠ·Π²Π°Π½ΠΎ Π±ΠΎΠ»Π΅Π΅ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠΌ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΡΠΎΠ³ΠΎΠ²ΠΎΠΉ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΊΡΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΉ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΌΠΎΠ³ΡΡ Π½Π°ΠΉΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΡΠΈ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ΅ ΠΈ ΠΊΠΎΠ½ΡΡΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΡΠΈΠ±ΠΎΡΠΎΠ² ΠΈ ΡΡΡΡΠΎΠΉΡΡΠ² Π΄Π»Ρ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Si-Π€ΠΠ£