93 research outputs found
Ultrafast dynamic conductivity and scattering rate saturation of photoexcited charge carriers in silicon investigated with a midinfrared continuum probe
We employ ultra-broadband terahertz-midinfrared probe pulses to characterize
the optical response of photoinduced charge-carrier plasmas in high-resistivity
silicon in a reflection geometry, over a wide range of excitation densities
(10^{15}-10^{19} cm^{-3}) at room temperature. In contrast to conventional
terahertz spectroscopy studies, this enables one to directly cover the
frequency range encompassing the resultant plasma frequencies. The intensity
reflection spectra of the thermalized plasma, measured using sum-frequency
(up-conversion) detection of the probe pulses, can be modeled well by a
standard Drude model with a density-dependent momentum scattering time of
approx. 200 fs at low densities, reaching approx. 20 fs for densities of
approx. 10^{19} cm^{-3}, where the increase of the scattering rate saturates.
This behavior can be reproduced well with theoretical results based on the
generalized Drude approach for the electron-hole scattering rate, where the
saturation occurs due to phase-space restrictions as the plasma becomes
degenerate. We also study the initial sub-picosecond temporal development of
the Drude response, and discuss the observed rise in the scattering time in
terms of initial charge-carrier relaxation, as well as the optical response of
the photoexcited sample as predicted by finite-difference time-domain
simulations.Comment: 9 pages, 4 figure
600-GHz Fourier Imaging Based on Heterodyne Detection at the 2nd Sub-harmonic
Fourier imaging is an indirect imaging method which records the diffraction
pattern of the object scene coherently in the focal plane of the imaging system
and reconstructs the image using computational resources. The spatial
resolution, which can be reached, depends on one hand on the wavelength of the
radiation, but also on the capability to measure - in the focal plane - Fourier
components with high spatial wave-vectors. This leads to a conflicting
situation at THz frequencies, because choosing a shorter wavelength for better
resolution usually comes at the cost of less radiation power, concomitant with
a loss of dynamic range, which limits the detection of higher Fourier
components. Here, aiming at maintaining a high dynamic range and limiting the
system costs, we adopt heterodyne detection at the 2nd sub-harmonic, working
with continuous-wave (CW) radiation for object illumination at 600 GHz and
local-oscillator (LO) radiation at 300 GHz. The detector is a single-pixel
broad-band Si CMOS TeraFET equipped with substrate lenses on both the front-
and backside for separate in-coupling of the waves. The entire scene is
illuminated by the object wave, and the Fourier spectrum is recorded by raster
scanning of the single detector unit through the focal plane. With only 56 uW
of power of the 600-GHz radiation, a dynamic range of 60 dB is reached,
sufficient to detect the entire accessible Fourier space spectrum in the test
measurements. A lateral spatial resolution of better than 0.5 mm, at the
diffraction limit, is reached
Π Π°Π·Π²ΠΈΡΠΈΠ΅ ΡΠΈΡΡΠ΅ΠΌΡ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΡΠ°ΡΠ»ΡΡ Π² ΡΠ΅Π³ΠΈΠΎΠ½Π΅
ΠΠ±ΡΠ΅ΠΊΡΠΎΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²Π»ΡΠ΅ΡΡΡ β ΡΠΈΡΡΠ΅ΠΌΠ° ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΡΠ°ΡΠ»ΡΡ Π² ΡΠ΅Π³ΠΈΠΎΠ½Π΅. Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ - ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ΠΎΠ² ΠΊ Π²ΡΡΠ²Π»Π΅Π½ΠΈΡ, Π°Π½Π°Π»ΠΈΠ·Ρ ΠΈ ΡΠ°Π·ΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌ, ΠΏΡΠ΅ΠΏΡΡΡΡΠ²ΡΡΡΠΈΡ
ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠΌΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠΈΡΡΠ΅ΠΌΡ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π² ΡΠ΅ΠΏΠ»ΠΎΡΠ½Π΅ΡΠ³Π΅ΡΠΈΠΊΠ΅. Π ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΡΡ Π°Π½Π°Π»ΠΈΠ· Π·Π°ΡΡΠ±Π΅ΠΆΠ½ΡΡ
ΠΈ ΠΎΡΠ΅ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΡΠΈΡΡΠ΅ΠΌ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΠΏΡΡΠ° ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π² ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΡΠ΅ΠΏΠ»ΠΎΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΡΠ°ΡΠ»ΠΈ.The object of study is the control system of thermal power industry in the region. The aim of this work is to develop approaches to the identification, analysis and resolution of problems impeding the effective development of the management system in power. In the process of investigation the analysis of foreign and domestic control systems and practical experience in the implementation of management models in the energy and power industry
Terahertz Nano-Imaging with s-SNOM
Spectroscopy and imaging with terahertz radiation propagating in free space suffer from the poor spatial resolution which is a consequence of the comparatively large wavelength of the radiation (300Β ΞΌm at 1 THz in vacuum) in combination with the Abbe diffraction limit of focusing. A way to overcome this limitation is the application of near-field techniques. In this chapter, we focus on one of them, scattering-type Scanning Near-field Optical Microscopy (s-SNOM) which β due to its versatility β has come to prominence in recent years. This technique enables a spatial resolution on the sub-100-nm length scale independent of the wavelength. We provide an overview of the state-of-the-art of this imaging and spectroscopy modality, and describe a few selected application examples in more detail
Combined investigation of collective amplitude and phase modes in a quasi-one-dimensional charge-density-wave system over a wide spectral range
We investigate experimentally both the amplitude and phase channels of the
collective modes in the quasi-1D charge-density-wave (CDW) system, K0.3MoO3, by
combining (i) optical impulsive-Raman pump-probe and (ii) terahertz time-domain
spectroscopy (THz-TDS), with high resolution and a detailed analysis of the
full complex-valued spectra in both cases. This allows an unequivocal
assignment of the observed bands to CDW modes across the THz range up to 9 THz.
We revise and extend a time-dependent Ginzburg-Landau model to account for the
observed temperature dependence of the modes, where the combination of both
amplitude and phase modes allows one to robustly determine the bare-phonon and
electron-phonon coupling parameters. While the coupling is indeed strongest for
the lowest-energy phonon, dropping sharply for the immediately subsequent
phonons, it grows back significantly for the higher-energy phonons,
demonstrating their important role in driving the CDW formation. We also
include a reassessment of our previous analysis of the lowest-lying phase
modes, whereby assuming weaker electronic damping for the phase channel results
in a qualitative picture more consistent with quantum-mechanical treatments of
the collective modes, with a strongly coupled amplitudon and phason as the
lowest modes
Strong coupling of plasmonic bright and dark modes with two eigenmodes of a photonic crystal cavity
Dark modes represent a class of forbidden transitions or transitions with
weak dipole moments between energy states. Due to their low transition
probability, it is difficult to realize their interaction with light, let alone
achieve the strong interaction of the modes with the photons in a cavity.
However, by mutual coupling with a bright mode, the strong interaction of dark
modes with photons is possible. This type of mediated interaction is widely
investigated in the metamaterials community and is known under the term
electromagnetically induced transparency (EIT). Here, we report strong coupling
between a plasmonic dark mode of an EIT-like metamaterial with the photons of a
1D photonic crystal cavity in the terahertz frequency range. The coupling
between the dark mode and the cavity photons is mediated by a plasmonic bright
mode, which is proven by the observation of a frequency splitting which depends
on the strength of the inductive interaction between the plasmon bright and
dark modes of the EIT-like metamaterial. In addition, since the plasmonic dark
mode strongly couples with the cavity dark mode, we observes four polariton
modes. The frequency splitting by interaction of the four modes (plasmonic
bright and dark mode and the two eigenmodes of the photonic cavity) can be
reproduced in the framework of a model of four coupled harmonic oscillators
ΠΠ±ΠΎΠ³Π°ΡΠ΅Π½ΠΈΠ΅ ΡΠ³Π»Π΅ΠΉ Π³ΡΠ°Π²ΠΈΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π½Π° Π£ΠΠ€, Π³. ΠΠ½Π³ΡΠ΅Π½
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠΏΡΡΡ ΠΏΠΎ ΠΎΠ±ΠΎΠ³Π°ΡΠ΅Π½ΠΈΡ ΡΠ³Π»Ρ Π³ΡΠ°Π²ΠΈΡΠ°ΡΠΈΠΎΠ½Π½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ.Research experiments on coal preparation by gravitational method
High-power even- and odd mode emission from linear arrays of resonant-tunneling-diode (RTD) oscillators in the 0.4- to 0.8-THz frequency range
Resonant tunneling diode (RTD) oscillators possess the highest oscillation
frequency among all electronic THz emitters. However, the emitted power from
RTDs remains limited. Here, we propose linear RTD-oscillator arrays capable of
supporting coherent emission from both odd and even coupled modes. Both modes
exhibit constructive interference in the far field, enabling high power
emission. Experimental demonstrations of coherent emission from
11-RTD-oscillator linear arrays are presented. The odd mode oscillates at
approximately 450 GHz, emitting about 0.5 mW, while the even mode oscillates at
around 750 GHz, emitting about 1 mW. Moreover, certain RTD-oscillator arrays
demonstrate dual-band oscillation under different biases, allowing for
controllable switching between two coupled modes. In addition, during bias
sweeping in both directions, a notable hysteresis feature is observed in the
switching bias for the odd and even modes. Our linear RTD-oscillator array
represents a significant step forward in the realization of high-power large
RTD-oscillator arrays and enables large-scale applications of RTD devices.Comment: 7 pages, 6 figure
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