Optoelectromechanical systems offer a promising route towards frequency conversion between microwaves and light and towards building quantum networks of superconducting circuits. Current theoretical and experimental efforts focus on approaches based on either optomechanically induced transparency or adiabatic passage. The former has the advantage of working with time-independent control but only in a limited bandwidth (typically much smaller than the cavity linewidth); the latter can, in principle, be used to increase the bandwidth but at the expense of working with time-dependent control fields and with strong optomechanical coupling. In my presentation, I will show that an array of optoelectromechanical transducers can overcome this limitation and reach a bandwidth that is larger than the cavity linewidth. The coupling rates are varied in space throughout the array so that a mechanically dark mode of the propagating fields adiabatically changes from microwave to optical or vice versa. This strategy also leads to significantly reduced thermal noise with the collective optomechanical cooperativity being the relevant figure of merit. I will also demonstrate that, remarkably, the bandwidth enhancement per transducer element is largest for small arrays. With these features the scheme is particularly relevant for improving the conversion bandwidth in state-of-the-art experimental setups.
Measurement of the Lifetime of the 59.5keV excited State of 237Np from the Al...theijes
The International Journal of Engineering & Science is aimed at providing a platform for researchers, engineers, scientists, or educators to publish their original research results, to exchange new ideas, to disseminate information in innovative designs, engineering experiences and technological skills. It is also the Journal's objective to promote engineering and technology education. All papers submitted to the Journal will be blind peer-reviewed. Only original articles will be published.
Measurement of the Lifetime of the 59.5keV excited State of 237Np from the Al...theijes
The International Journal of Engineering & Science is aimed at providing a platform for researchers, engineers, scientists, or educators to publish their original research results, to exchange new ideas, to disseminate information in innovative designs, engineering experiences and technological skills. It is also the Journal's objective to promote engineering and technology education. All papers submitted to the Journal will be blind peer-reviewed. Only original articles will be published.
First-principles computations of phonon-limited carrier mobilities in semiconductors have recently gained popularity. Such calculations are indeed crucial for the discovery and development of new functional materials.
In state-of-the-art approaches, Fourier-based interpolation schemes are used to obtain the electron-phonon matrix elements on the very dense wavevector grids needed to converge carrier lifetimes and mobilities. In polar semiconductors, the long-range electrostatic interactions lead to a divergence of the matrix elements, rendering their interpolation unstable. For this reason, ab initio methods have been recently developed to model the non-analytical behavior of the matrix elements for q→0 [1].
Most of the studies performed so far have focused on this Fröhlich divergence generated by dynamical dipoles. However, additional non-analytical terms are present in the q→0 limit [2]. In this work, we analyze the role played by the dynamical quadrupoles and show that an accurate interpolation is obtained only when both dipolar and quadrupolar fields are taken into account. We discuss their impact on the accuracy and on the convergence of carrier mobilities both in polar and non-polar semiconductors.
[1] Phys. Rev. Lett. 115, 176401 (2015)
[2] Phys. Rev. B 13, 694 (1976)
https://arxiv.org/abs/2002.00628
https://arxiv.org/abs/2002.00630
Transmission spectra of single ring coupled-waveguide resonator configuration...TELKOMNIKA JOURNAL
Development of optical waveguide resonators have greatly expanded and continues to grow since they have kinds potential applications such as wavelength filtering, switching, coupling and multiplexing. One of resonators, coupled waveguides, ring resonators are designed and operated using various coupling configurations. Ring resonators can be particularly used as wavelength filter if the wavelength can fit a whole multiple time in the circumference of the ring. This article proposes to investigate the transmission spectra from the power source and amplify it in linearized ring resonator configurations and varies the input amplitude on five different wavelengths. With finite difference time domain method, the geometry and power source are simulated to obtain the better result and configuration. The results show the intensity phenomena of filtering in optical circuit.
Study of conductivity, optical constants and solid state parameters of thiour...eSAT Journals
Abstract In the present paper single crystals of Thiourea Zinc Sulphate (TZS) have been subjected to conductivity studies, determination of optical constants and fundamental parameters. The dielectric constant and dielectric loss were used to calculate the AC conductivity of the grown crystals over a frequency range 50 Hz to 5 MHz at temperatures 313 K, 323 K and 333 K respectively. The activation energies for the conduction process were determined from the Arrhenius plots for different frequencies. The optical constants such as refractive index, reflectance and susceptibility of the TZS single crystals were evaluated from the Ultra violet-Visible (UV-Vis) spectrum data. The Plasma energy, Penn gap energy, Fermi energy and polarizability of the grown crystals were estimated theoretically using the single crystal X- ray diffraction (XRD) data. Keywords: Conductivity, Activation energy, Refractive index, Penn energy, Polarizability.
Pseudoperiodic waveguides with selection of spatial harmonics and modesVictor Solntsev
A principle of selection of modes and their spatial harmonics in periodic waveguides and, in particular, in spatially developed slowing systems for multibeam traveling-wave tubes (TWTs) is elaborated. The essence of the principle is in the following: varying along the length of the system its period and at least one more parameter that determines the phase shift per period, one can provide constant phase velocity of one spatial harmonic and destroy other spatial harmonics, i.e., reduce their amplitudes substantially. In this case, variations of the period may be significant, and the slowing system becomes nonuniform, or pseudoperiodic; namely, one of the spatial harmonics remains the same as in the initial periodic structure. Relationships are derived for the amplitudes of the spatial-wave harmonics, interaction coefficient, and coupling impedance of the pseudoperiodic system. The possibility of the mode selection in pseudoperiodic slowing systems when the synchronism condition is satisfied for the spatial harmonic of one mode is investigated. The efficiency of suppressing spurious spatial harmonics and modes for linear and abrupt variation of spacing is estimated. The elaborated principle of selection of spatial harmonics and modes is illustrated by an example of a two-section helical-waveguide slowing system.
First-principles computations of phonon-limited carrier mobilities in semiconductors have recently gained popularity. Such calculations are indeed crucial for the discovery and development of new functional materials.
In state-of-the-art approaches, Fourier-based interpolation schemes are used to obtain the electron-phonon matrix elements on the very dense wavevector grids needed to converge carrier lifetimes and mobilities. In polar semiconductors, the long-range electrostatic interactions lead to a divergence of the matrix elements, rendering their interpolation unstable. For this reason, ab initio methods have been recently developed to model the non-analytical behavior of the matrix elements for q→0 [1].
Most of the studies performed so far have focused on this Fröhlich divergence generated by dynamical dipoles. However, additional non-analytical terms are present in the q→0 limit [2]. In this work, we analyze the role played by the dynamical quadrupoles and show that an accurate interpolation is obtained only when both dipolar and quadrupolar fields are taken into account. We discuss their impact on the accuracy and on the convergence of carrier mobilities both in polar and non-polar semiconductors.
[1] Phys. Rev. Lett. 115, 176401 (2015)
[2] Phys. Rev. B 13, 694 (1976)
https://arxiv.org/abs/2002.00628
https://arxiv.org/abs/2002.00630
Transmission spectra of single ring coupled-waveguide resonator configuration...TELKOMNIKA JOURNAL
Development of optical waveguide resonators have greatly expanded and continues to grow since they have kinds potential applications such as wavelength filtering, switching, coupling and multiplexing. One of resonators, coupled waveguides, ring resonators are designed and operated using various coupling configurations. Ring resonators can be particularly used as wavelength filter if the wavelength can fit a whole multiple time in the circumference of the ring. This article proposes to investigate the transmission spectra from the power source and amplify it in linearized ring resonator configurations and varies the input amplitude on five different wavelengths. With finite difference time domain method, the geometry and power source are simulated to obtain the better result and configuration. The results show the intensity phenomena of filtering in optical circuit.
Study of conductivity, optical constants and solid state parameters of thiour...eSAT Journals
Abstract In the present paper single crystals of Thiourea Zinc Sulphate (TZS) have been subjected to conductivity studies, determination of optical constants and fundamental parameters. The dielectric constant and dielectric loss were used to calculate the AC conductivity of the grown crystals over a frequency range 50 Hz to 5 MHz at temperatures 313 K, 323 K and 333 K respectively. The activation energies for the conduction process were determined from the Arrhenius plots for different frequencies. The optical constants such as refractive index, reflectance and susceptibility of the TZS single crystals were evaluated from the Ultra violet-Visible (UV-Vis) spectrum data. The Plasma energy, Penn gap energy, Fermi energy and polarizability of the grown crystals were estimated theoretically using the single crystal X- ray diffraction (XRD) data. Keywords: Conductivity, Activation energy, Refractive index, Penn energy, Polarizability.
Pseudoperiodic waveguides with selection of spatial harmonics and modesVictor Solntsev
A principle of selection of modes and their spatial harmonics in periodic waveguides and, in particular, in spatially developed slowing systems for multibeam traveling-wave tubes (TWTs) is elaborated. The essence of the principle is in the following: varying along the length of the system its period and at least one more parameter that determines the phase shift per period, one can provide constant phase velocity of one spatial harmonic and destroy other spatial harmonics, i.e., reduce their amplitudes substantially. In this case, variations of the period may be significant, and the slowing system becomes nonuniform, or pseudoperiodic; namely, one of the spatial harmonics remains the same as in the initial periodic structure. Relationships are derived for the amplitudes of the spatial-wave harmonics, interaction coefficient, and coupling impedance of the pseudoperiodic system. The possibility of the mode selection in pseudoperiodic slowing systems when the synchronism condition is satisfied for the spatial harmonic of one mode is investigated. The efficiency of suppressing spurious spatial harmonics and modes for linear and abrupt variation of spacing is estimated. The elaborated principle of selection of spatial harmonics and modes is illustrated by an example of a two-section helical-waveguide slowing system.
Attosecond pulses produced by using HHG in gases, it is possible to make a few simple statements: attosecond pulses are unique tools for the investigation of ultrafast electronic processes in atoms, molecules, nano structures and solids. Impressive progress has been demonstrated from the technological point of view, with the possibility to routinely generate attosecond pulses in perfectly reproducible ways.
The objective of this paper is to study how the selection of the coil and the frequency affects the received modes in
guided Lamb waves, with the objective of analyzing the best configuration for determining the depth of a given
defect in a metallic pipe with the minimum error. Studies of the size of the damages with all the extracted
parameters are then used to propose estimators of the residual thickness, considering amplitude and phase
information in one or several modes. Results demonstrate the suitability of the proposal, improving the estimation of
the residual thickness when two simultaneous modes are used, as well as the range of possibilities that the coil and
frequency selection offers.
the paper focuses on the fabrication and characterization of heterostructures using transition metal dichalcogenide (TMDC) monolayers. The authors describe the process of mechanical exfoliation to obtain thin flakes of TMDC material, which are then placed on a viscoelastic polydimethylsiloxane film. These monolayers are subsequently stamped onto a silicon wafer covered with thermal oxide to create heterobilayers .
The paper also discusses the use of ultrafast optical-pump/terahertz-probe near-field microscopy to study these heterostructures. The authors explain that this technique allows them to investigate the electric near fields and scattered fields of the emitted waveforms, as well as the photo-induced polarizability .
The experimental setup involves a high-average-power, low-noise Yb:YAG thin-disc oscillator, which generates terahertz probe pulses through optical rectification of 200-fs-long pulses. These pulses are centered at a wavelength of 1,030 nm and are generated in a gallium phosphide crystal .
The paper likely includes additional details on the experimental procedures, data analysis, and results obtained from the terahertz near-field microscopy experiments. It may also discuss the potential applications and implications of the findings
Directional Spreading Effect on a Wave Energy ConverterElliot Song
The results demonstrate the importance of tuning the WEC system for specific wave environments to harvest most energy and to avoid potential capsize due to hurricanes etc.
Presentation in the Franhoufer IIS about my thesis: A wavelet transform based...Pedro Cerón Colás
Presentation in the Franhoufer IIS about my thesis: A wavelet transform based application for seismic waves. Analysis of the performance. Code made in Matlab.
Luigi Giubbolini | Time/Space-Probing Interferometer for Plasma DiagnosticsLuigi Giubbolini
By Luigi Giubbolini Published article about Rapid progress in plasma applications requires new instrumentation. Luigi Giubbolini has engineering experience in industrial, government laboratory & academic environments.
Microwave Planar Sensor for Determination of the Permittivity of Dielectric M...journalBEEI
This paper proposed a single port rectangular microwave resonator sensor. This sensor operates at the resonance frequency of 4GHz. The sensor consists of micro-strip transmission line and applied the enhancement method. The enhancement method is able to improve the return loss of the sensor, respectively. Plus, the proposed sensor is designed and fabricated on Roger 5880 substrate. Based on the results, the percentage of error for the proposed rectangular sensor is 0.2% to 8%. The Q-factor of the sensor is 174.
Simulation of Nonstationary Processes in Backward-Wave Tube with the Self-Mod...Victor Solntsev
The equations that describe nonlinear nonstationary processes in carcinotrode (backward- wave tube with the emission modulation in the presence of the field of the output signal fed to the cathode via a feedback loop) are derived. An algorithm and the corresponding code are developed to solve the equations with allowance for the modulation of emission using nonuniform (with respect to time) large particles (electrons of equal charge) ejected from the cathode. The effect of the feedback parameter on the intensity and shape of the carcinotrode oscillations is analyzed. It is demonstrated that the carcinotrode efficiency can be increased to about 50% upon the generation of harmonic oscil- lations. A more significant increase in the efficiency to 70% is possible in the regime of the weak self- modulation of oscillations upon an increase in the feedback coefficient in the feedback loop involving the slow-wave structure and the cathode and a decrease in the cathode–grid static field.
Gaussian control and readout of levitated nanoparticles via coherent scatteringOndrej Cernotik
Optically levitated nanoparticles present an attractive optomechanical platform owing to their lack of clamping losses. The most promising approach to control the state of nanoparticle motion is coherent scattering of tweezer photons into a cavity mode. Originally proposed as a technique for cooling the motion of atoms and ions, this mechanism has recently been used to cool the motion of a nanoparticle to its quantum ground state for the first time. In my presentation, I will discuss how coherent scattering can be used to create and measure complex motional states of levitated nanoparticles. Coherent scattering gives us access to the same basic types of interaction as the more usual radiation-pressure interaction (of the beam-splitter and two-mode-squeezing type) allowing the same protocols to be realized. An important distinction—relevant particularly for quantum nondemolition readout of nanoparticle motion—is that coherent scattering can be accompanied by additional effects modifying the free nanoparticle evolution. I will discuss these differences and address the consequences they have for controlling and measuring nanoparticle motion in the quantum regime.
Transformations of continuous-variable entangled states of lightOndrej Cernotik
Gaussian states and Gaussian transformations represent an interesting counterpart to two-level photonic systems in the field of quantum information processing. On the theoretical side, Gaussian states are easily described using first and second moments of the quadrature operators; from the experimental point of view, Gaussian operations can be implemented using linear optics and optical parametric amplifiers. The biggest advantage compared to two-level photonic systems, is deterministic generation of entangled states in parametric amplifiers and highly efficient homodyne detection. In this presentation, we propose new protocols for manipulation of entanglement of Gaussian states.
Firstly, we study entanglement concentration of split single-mode squeezed vacuum states by photon subtraction enhanced by local coherent displacements. These states can be obtained by mixing a single-mode squeezed vacuum state with vacuum on a beam splitter and are, therefore, generated more easily than two-mode squeezed vacuum states. We show that performing local coherent displacements prior to photon subtraction can lead to an enhancement of the output entanglement. This is seen in weak-squeezing approximation where destructive quantum interference of dominant Fock states occurs, while for arbitrarily squeezed input states, we analyze a realistic scenario, including limited transmittance of tap-off beam splitters and limited efficiency of heralding detectors.
Next, motivated by results obtained for bipartite Gaussian states, we study symmetrization of multipartite Gaussian states by local Gaussian operations. Namely, we analyze strategies based on addition of correlated noise and on quantum non-demolition interaction. We use fidelity of assisted quantum teleportation as a figure of merit to characterize entanglement of the state before and after the symmetrization procedure. Analyzing the teleportation protocol and considering more general transformations of multipartite Gaussian states, we show that the fidelity can be improved significantly.
In this tutorial, I will give an overview of hybrid quantum systems and their applications in quantum technologies. I will start by reviewing their individual components, focusing primarily on the theory of superconducting circuits, cavity optomechanics, and electromechanics. Afterwards, I will discuss a few applications of hybrid systems composed of these components. In particular, I will explain how opto-electro-mechanical systems can be used to achieve frequency conversion between microwaves and light and how electromechanical systems can be used to couple mechanical motion to superconducting quantum bits.
Measurement-induced long-distance entanglement with optomechanical transducersOndrej Cernotik
Although superconducting systems provide a promising platform for quantum computing, their networking poses a challenge as they cannot be interfaced to light---the medium used to send quantum signals through channels at room temperature. We show that mechanical oscillators can mediated such coupling and light can be used to measure the joint state of two distant qubits. The measurement provides information on the total spin of the two qubits such that entangled qubit states can be postselected. Entanglement generation is possible without ground-state cooling of the mechanical oscillators for systems with optomechanical cooperativity moderately larger than unity; in addition, our setup tolerates a substantial transmission loss. The approach is scalable to generation of multipartite entanglement and represents a crucial step towards quantum networks with superconducting circuits.
Quantum force sensing with optomechanical transducersOndrej Cernotik
Optomechanical force sensing is an established measurement technique that can reach remarkable precision. In most applications, the system exerting the force on the mechanical oscillator is treated classically and we are not interested in any coherence between states of the system that give rise to different forces. A full quantum treatment, however, enables richer physics since measuring more such systems can lead to interference effects.
In this talk, I will show that the coherence can survive the measurement and can be used for quantum-technological applications. I will consider a model example of spin readout in superconducting qubits. Coupling two transmon qubits to mechanical oscillators and reading out the mechanical positions using a single beam of light provides information on the total spin of the qubits. It is thus possible to conditionally generate entanglement between the two qubits. The system represents a basic quantum network with superconducting circuits. The scheme has modest requirements on the system parameters; it does not require ground-state cooling or resolved-sideband regime and can work with quantum cooperativity moderately larger than unity.
Afterwards, I will consider another scheme, namely nondestructive detection of a single photon using an optomechanical transducer. The basic idea is similar to spin readout; the photon exerts a force on a mechanical oscillator and the the force is measured optically. I will argue that such a measurement is subject to a quantum limit due to backaction of the transducer on the dynamics of the photon and that this result also applies to other techniques of nondestructive photon detection, such as methods using Kerr interaction between the single photon and a meter beam. Finally, I will show numerically that measurement backaction can be evaded when the measurement rate is suitably modulated.
Quantum networks with superconducting circuits and optomechanical transducersOndrej Cernotik
Connecting distant chips in a quantum network is one of biggest challenges for superconducting quantum computers. Superconducting systems operate at microwave frequencies; transmission of microwave signals through room-temperature quantum channels is impossible due to the omnipresent thermal noise. I will show how two well-known experimental techniques—parity measurements on superconducting systems and optomechanical force sensing—can be combined to generate entanglement between two superconducting qubits through a room-temperature environment. An optomechanical transducer acting as a force sensor can be used to determine the state of a superconducting qubit. A joint readout of two qubits and postselection can lead to entanglement between the qubits. From a conceptual perspective, the transducer senses force exerted by a quantum object, entering a new paradigm in force sensing. In a typical scenario, the force sensed by an optomechanical system is classical. I will argue that the coherence between different states of the qubit (which give rise to different values of the force) can be preserved during the measurement, making it an important resource for quantum communication.
Novel approaches to optomechanical transductionOndrej Cernotik
Optomechanical systems offer a promising route towards frequency conversion between microwaves and light. Current theoretical and experimental efforts focus on approaches based on either optomechanically induced transparency (suffering from limited conversion bandwidth) or adiabatic passage (requiring time-dependent control). In my talk, I will present two alternative strategies for optomechanical transduction that avoid these limitations. In the first one, entanglement between two superconducting qubits is generated by using transducers as force sensors; jointly measuring the force with which the qubits act on the transducers leads to conditional generation of entanglement between the qubits. The other device uses spatially adiabatic frequency conversion in an array of optomechanical transducers, allowing for large conversion bandwidth with time-independent control.
Improved optomechanical interactions for quantum technologiesOndrej Cernotik
Cavity optomechanics reached remarkable success in coupling optical and mechanical degrees of freedom. The standard mechanism relies on dispersive interaction wherein a cavity mode acquires a frequency shift proportional to the mechanical displacement. Efficient coupling is, however, often impeded by large cavity decay rates or strong heating of the mechanical element by optical absorption. In this talk, I will present two strategies to circumvent this problem. In the first one, a membrane doped with an ensemble of two-level emitters or patterned with a photonic-crystal structure is used as a mechanical element. The hybridization of the cavity mode with the membrane’s internal resonance leads to a modified response, resulting in an effective narrow cavity linewidth. I will show how such systems can be described quantum mechanically and discuss how optomechanical sideband cooling can be improved by the presence of the internal resonance. Second, I will discuss optomechanics with levitated particles and show how coherent scattering can be used to generate strong mechanical squeezing. In this system, the standard dispersive interaction is replaced by scattering of the trapping beam into an empty cavity mode. This process can result in strong, controllable coupling between the cavity mode and the motion of the particle with minimal absorption heating. I will also briefly outline how this type of interaction can be used to engineer coupling between different center-of-mass modes of the particle allowing, in principle, full optomechanical control of the particle motion.
Improved optomechanical interactions for quantum technologiesOndrej Cernotik
Cavity optomechanics reached remarkable success in coupling optical and mechanical degrees of freedom. The standard mechanism relies on dispersive interaction wherein a cavity mode acquires a frequency shift proportional to the mechanical displacement. Efficient coupling is, however, often impeded by large cavity decay rates or strong heating of the mechanical element by optical absorption. In this talk, I will present two strategies to circumvent this problem. In the first one, a membrane doped with an ensemble of two-level emitters or patterned with a photonic-crystal structure is used as a mechanical element. The hybridization of the cavity mode with the membrane’s internal resonance leads to a modified response, resulting in an effective narrow cavity linewidth. I will show how such systems can be described quantum mechanically and discuss how optomechanical sideband cooling can be improved by the presence of the internal resonance. Second, I will discuss optomechanics with levitated particles and show how coherent scattering can be used to generate strong mechanical squeezing. In this system, the standard dispersive interaction is replaced by scattering of the trapping beam into an empty cavity mode. This process can result in strong, controllable coupling between the cavity mode and the motion of the particle with minimal absorption heating. I will also briefly outline how this type of interaction can be used to engineer coupling between different center-of-mass modes of the particle allowing, in principle, full optomechanical control of the particle motion.
Entangling distant superconducting qubits using nanomechanical transducersOndrej Cernotik
Optical fields are ideal for transmission of quantum information due to low losses and high repetition rates. Microwave fields, on the other hand, can be used to manipulate superconducting systems that belong among the most promising candidates for quantum computing architecture. A device enabling conversion between electromagnetic fields of such distinct frequencies would thus represent a basic building block of future quantum computer networks. Nanomechanical oscillators represent an extremely suitable platform for this task as they can couple to both optical and microwave fields. The electromechanical interaction is achieved through capacitance of an LC circuit, where the change of voltage couples to the position of a mechanical membrane forming one plate of the capacitor, while coupling to the visible light is due to radiation pressure from light reflected off the membrane.
Here we study how such nanomechanical transducers can be employed to generate entanglement between two superconducting qubits placed on two separate chips. Our protocol is based on continuous Bell measurement of the outgoing light fields and applying feedback on the qubits. With such a setup, it is, in principle, possible to generate entanglement between qubits deterministically in the steady state.
Measurement-induced long-distance entanglement of superconducting qubits usin...Ondrej Cernotik
Although superconducting systems provide a promising platform for quantum computing, their networking poses a challenge as they cannot be interfaced to light---the medium used to send quantum signals through channels at room temperature. We show that mechanical oscillators can mediated such coupling and light can be used to measure the joint state of two distant qubits. The measurement provides information on the total spin of the two qubits such that entangled qubit states can be postselected. Entanglement generation is possible without ground-state cooling of the mechanical oscillators for systems with optomechanical cooperativity moderately larger than unity; in addition, our setup tolerates a substantial transmission loss. The approach is scalable to generation of multipartite entanglement and represents a crucial step towards quantum networks with superconducting circuits.
Measurement-induced long-distance entanglement of superconducting qubits usin...Ondrej Cernotik
Although superconducting systems provide a promising platform for quantum computing, their networking poses a challenge as they cannot be interfaced to light---the medium used to send quantum signals through channels at room temperature. We show that mechanical oscillators can mediated such coupling and light can be used to measure the joint state of two distant qubits. The measurement provides information on the total spin of the two qubits such that entangled qubit states can be postselected. Entanglement generation is possible without ground-state cooling of the mechanical oscillators for systems with optomechanical cooperativity moderately larger than unity; in addition, our setup tolerates a substantial transmission loss. The approach is scalable to generation of multipartite entanglement and represents a crucial step towards quantum networks with superconducting circuits.
Measurement-induced long-distance entanglement of superconducting qubits usin...Ondrej Cernotik
Although superconducting systems provide a promising platform for quantum computing, their networking poses a challenge as they cannot be interfaced to light---the medium used to send quantum signals through channels at room temperature. We show that mechanical oscillators can mediated such coupling and light can be used to measure the joint state of two distant qubits. The measurement provides information on the total spin of the two qubits such that entangled qubit states can be postselected. Entanglement generation is possible without ground-state cooling of the mechanical oscillators for systems with optomechanical cooperativity moderately larger than unity; in addition, our setup tolerates a substantial transmission loss. The approach is scalable to generation of multipartite entanglement and represents a crucial step towards quantum networks with superconducting circuits.
Measurement-induced long-distance entanglement of superconducting qubits usin...Ondrej Cernotik
Although superconducting systems provide a promising platform for quantum computing, their networking poses a challenge as they cannot be interfaced to light—the medium used to send quantum signals through channels at room temperature. We show that mechanical oscillators can mediate such coupling and light can be used to measure the joint state of two distant qubits. The measurement provides information on the total spin of the two qubits such that entangled qubit states can be postselected.
Our scheme works in analogy to experimental technique already established in the microwave domain but employs an optical channel at room temperature. The use of light greatly enhances the distance over which the qubits can become entangled. The generalization to the optical domain—although relatively straightforward from the experimental point of view—is highly nontrivial and requires a systematic investigation of new sources of decoherence; thermal mechanical noise and optical transmission loss have to be analysed. Such an analysis requires adiabatic elimination of the complex transducer dynamics since the Hilbert space dimension is too large to allow numerical simulations.
Compared to earlier proposals of optomechanical transducers, our strategy requires no time-dependent control. This simplicity leads to modest requirements on the system parameters; optomechanical cooperativity moderately larger than unity is sufficient and large transmission losses can be tolerated. The approach is scalable to generation of multipartite entanglement and represents a crucial step towards quantum networks with superconducting circuits.
Novel approaches to optomechanical transductionOndrej Cernotik
In recent years, mechanical oscillators received attention as a promising tool for frequency conversion between microwaves and light. A general, bi-directional transducer with high efficiency is still far from reach of current technology; finding new strategies for optomechanical transduction allows us to relax the requirements and bring these systems closer to an experimental realization. An interesting example is generation of entanglement between two superconducting qubits using measurement and postselection. Here, the mechanical oscillators interacts directly with the superconducting transmon qubit in such a way that it feels a qubit-state dependent force. This force can then be read out using a cavity field; reading out two such systems sequentially realizes an effective total spin measurement. Starting from a suitable initial state and employing postselection, entanglement can be generated. Another interesting approach is to use an array of optomechanical transducers in which the output fields of one transducer are fed into the input of the next. The periodicity of the array results in a joint dispersion relation for the propagating microwave and optical fields. The resulting structure can be used to control the conversion bandwidth and forward and backward scattering.
Interference effects in cavity optomechanics with hybridized membranesOndrej Cernotik
Radiation pressure forces in cavity optomechanics allow for efficient cooling of motion, the manipulation of photonic and phononic quantum states, as well as generation of optomechanical entanglement. The standard mechanism relies on the cavity photons directly modifying the state of the mechanical resonator. Hybrid cavity optomechanics provides an alternative approach by coupling mechanical objects to quantum emitters, either directly or indirectly via the common interaction with a cavity field mode. In these systems, the interference between forces from the cavity field and the emitters can give rise to novel optomechanical phenomena. We analyze two such hybrid optomechanical systems where a vibrating membrane is doped by quantum emitters or patterned with a photonic crystal structure. In particular, we demonstrate that, in the former system, a three-body interaction between the cavity field, emitters, and mechanical motion can be used to improve cooling of the mechanical motion. Second, we show that, when a photonic crystal structure in the membrane strongly modifies the membrane reflectivity, the cavity linewidth can be significantly reduced and the system can reach the sideband resolved regime.
We study entanglement concentration of continuous variable Gaussian states by local photon subtractions enhanced by coherent displacements. Instead of the previously considered symmetric two-mode squeezed vacuum states, we investigate the protocol for input states in the form of split single-mode squeezed vacuum, i.e., states obtained by mixing a single-mode squeezed vacuum with a vacuum state on a beam splitter, which is an experimentally highly relevant configuration. We analyze two scenarios in which the displacement-enhanced photon subtraction is performed either only on one, or on both of the modes and show that local displacements can lead to improved performance of the concentration protocol.
Synthetic Fiber Construction in lab .pptxPavel ( NSTU)
Synthetic fiber production is a fascinating and complex field that blends chemistry, engineering, and environmental science. By understanding these aspects, students can gain a comprehensive view of synthetic fiber production, its impact on society and the environment, and the potential for future innovations. Synthetic fibers play a crucial role in modern society, impacting various aspects of daily life, industry, and the environment. ynthetic fibers are integral to modern life, offering a range of benefits from cost-effectiveness and versatility to innovative applications and performance characteristics. While they pose environmental challenges, ongoing research and development aim to create more sustainable and eco-friendly alternatives. Understanding the importance of synthetic fibers helps in appreciating their role in the economy, industry, and daily life, while also emphasizing the need for sustainable practices and innovation.
Palestine last event orientationfvgnh .pptxRaedMohamed3
An EFL lesson about the current events in Palestine. It is intended to be for intermediate students who wish to increase their listening skills through a short lesson in power point.
Read| The latest issue of The Challenger is here! We are thrilled to announce that our school paper has qualified for the NATIONAL SCHOOLS PRESS CONFERENCE (NSPC) 2024. Thank you for your unwavering support and trust. Dive into the stories that made us stand out!
Ethnobotany and Ethnopharmacology:
Ethnobotany in herbal drug evaluation,
Impact of Ethnobotany in traditional medicine,
New development in herbals,
Bio-prospecting tools for drug discovery,
Role of Ethnopharmacology in drug evaluation,
Reverse Pharmacology.
2024.06.01 Introducing a competency framework for languag learning materials ...Sandy Millin
http://sandymillin.wordpress.com/iateflwebinar2024
Published classroom materials form the basis of syllabuses, drive teacher professional development, and have a potentially huge influence on learners, teachers and education systems. All teachers also create their own materials, whether a few sentences on a blackboard, a highly-structured fully-realised online course, or anything in between. Despite this, the knowledge and skills needed to create effective language learning materials are rarely part of teacher training, and are mostly learnt by trial and error.
Knowledge and skills frameworks, generally called competency frameworks, for ELT teachers, trainers and managers have existed for a few years now. However, until I created one for my MA dissertation, there wasn’t one drawing together what we need to know and do to be able to effectively produce language learning materials.
This webinar will introduce you to my framework, highlighting the key competencies I identified from my research. It will also show how anybody involved in language teaching (any language, not just English!), teacher training, managing schools or developing language learning materials can benefit from using the framework.
The Roman Empire A Historical Colossus.pdfkaushalkr1407
The Roman Empire, a vast and enduring power, stands as one of history's most remarkable civilizations, leaving an indelible imprint on the world. It emerged from the Roman Republic, transitioning into an imperial powerhouse under the leadership of Augustus Caesar in 27 BCE. This transformation marked the beginning of an era defined by unprecedented territorial expansion, architectural marvels, and profound cultural influence.
The empire's roots lie in the city of Rome, founded, according to legend, by Romulus in 753 BCE. Over centuries, Rome evolved from a small settlement to a formidable republic, characterized by a complex political system with elected officials and checks on power. However, internal strife, class conflicts, and military ambitions paved the way for the end of the Republic. Julius Caesar’s dictatorship and subsequent assassination in 44 BCE created a power vacuum, leading to a civil war. Octavian, later Augustus, emerged victorious, heralding the Roman Empire’s birth.
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Spatially adiabatic frequency conversion in opto-electro-mechanical arrays
1. Time
Coupling
Spatially adiabatic frequency conversion
in opto-electro-mechanical arrays
Ondřej Černotík,1,2
Sahand Mahmoodian,1
and Klemens Hammerer1
1
Institute for Theoretical Physics, Institute for Gravitational Physics (Albert Einstein Institute), Leibniz University Hannover, Germany
2
Max Planck Institute for the Science of Light, Erlangen, Germany
References Acknowledgements
This work was supported by the European Comission
(FP-7 Programme) through iQUOEMS (Grant Agreement
No. 323924). We gratefully acknowledge support by DFG
through QUEST and by the cluster system team at the
Leibniz University Hannover.
[1] OČ et al., arXiv:1707.03339.
[2] R. Andrews et al., Nature Physics 10, 321 (2014).
[3] L. Tian, Phys. Rev. Lett. 108, 153604 (2012).
[4] Y.-D. Wang and A. Clerk, Phys. Rev. Lett. 108, 153603 (2012).
Email: ondrej.cernotik@mpl.mpg.de
Summary
Optomechanical transduction
We show that an array of opto-electro-mechanical transducers can be used to enhance
the bandwidth of frequency conversion between microwaves and light [1]. In the array,
a mechanically dark mode of the propagating fields adiabatically changes from
microwave to optical or vice versa. Apart from the enhanced conversion bandwidth,
this strategy also leads to significantly reduced thermal noise. Remarkably, the
bandwidth enhancement per transducer element is largest for small arrays.
Conversion of itinerant fields Adiabatic passage
Transducer arrays
Losses and noise
Electromagnetic losses Thermal mechanical noise
0
1
2
3
Addednoise(unitsofshotnoise)
(a)
0.2 0.1 0.0 0.1 0.2
Frequency /
0.0
0.1
0.2
(b)
Bright mode
Dark mode
Cavity opto- and electromechanics
In a standard optomechanical system, the
motion of a mechanical oscillator modifies the
resonance of a cavity mode. The dynamics
can be described by the Hamiltonian
The weak dispersive interaction can be linearized around a strong
laser drive. When the drive frequency is detuned from the cavity
resonance by the mechanical frequency, , the cavity
field and the mechanical oscillator exchange excitations (provided
the system is in the resolved sideband regime ),
M. Aspelmeyer et al., RMP 86, 1391 (2014).
The same effects can also be observed in
electromechanical systems where the motion
of a capacitor plave couples to the field of an
LC circuit.
Conversion of propagating fields is possible in an
impedance-matched transducer, [2]. Such
a device can convert arbitrary input signals within the
bandwidth . Thermal mechanical noise is
suppressed for strong optomechanical cooperativity,
[3,4].
By coupling a mechanical oscillator to an optical cavity and
a microwave resonator, we can build a system for
converting signals between the two frequency domains [2].
The total interaction Hamiltonian is
Better bandwidth (equal to the cavity
linewidth) is possible with adiabatic
passage [3,4]. The signal is stored in one of
the cavities and the coupling rates are
varied so the signal remains in the
mechanically dark mode, .
Advantages of both approaches can be
combined in an array of optomechanical
transducers. The coupling rates are varied
adiabatically in space, enabling conversion of
arbitrary signals over a large bandwidth.
100
101
102
103
Array size N
0.0
0.2
0.4
0.6
0.8
1.0
Conversion|T21()|2
(a)
0.00 0.05 0.10 0.15 0.20
Frequency / R
(b)
Direct loss (on resonance) Backscattering
1.0 0.5 0.0 0.5 1.0
Frequency /
0.0
0.2
0.4
0.6
0.8
1.0
Conversion|T21()|2
(a)
100
101
102
103
Array size N
0.1
1
Bandwidth/
(b)
/ /
15
15
Phase
Far off resonance, the probability of converting a photon is
small, . In an array, it is enhanced -
fold, . We can therefore expect the bandwidth to
grow with the cubic root of the array size. A rigorous
derivation shows that for large arrays [1]
Conversion in small arrays (with ) can be
numerically optimized showing that bandwidth
enhancement is possible also in this regime.
Transfer matrix formalism
The dynamics of a single transducer is described
by the Heisenberg–Langevin equations which we
write in the matrix form
The equations can be solved in the frequency
domain. The effect of the transducer is described
by the scattering matrix
Signal propagation through the array can be
obtained by multiplying the scattering matrices of
individual transducers,
When the cavities decay through both ports, the
relationship between the scattering and transfer
matrices is more complicated. A transformation
between the two can, however, be found.
…
The transfer matrix formalism can also be used to
include free propagation between two transducers,
including propagation loss. Mechanical noise can be
added as a source term in the scattering
process, .
The electromagnetic fields can decay via two distinct
processes: direct loss (during propagation or in cavities)
and backscattering at mirrors. The latter has no
analogue in the usual adiabatic passage and leads to
interference between the incoming and reflected
signals.
Overall, the noise density is suppressed by the
collective cooperativity [1].
For small arrays, one can evaluate the added noise
numerically and show that it is also reduced
compared to using a single transducer.
To quantify the noise from the mechanical
reservoirs, we evaluate the associated spectral
density,
independent reservoirs
adiabaticitysingle transducer