### 5219 results for qubit oscillator frequency

Contributors: Eugene Grichuk, Margarita Kuzmina, Eduard Manykin

Date: 2010-09-26

**qubit** simulates the behavior of electric field of
polarized light beam...**qubit** model has been designed as a
stochastic **oscillator** formed by a pair...**qubits** that is
exploited as a computation resource in one-way quantum
...**oscillators** is
proposed for modeling of a cluster of entangled **qubits** ...**oscillators** with chaotically modulated limit cycle radii and
**frequencies**...one-**qubit**
gates are suggested. Changing of cluster entanglement degree...**qubit** cluster, is designed, and system of equations for
network dynamics...**oscillators**...**qubit** model has been designed as a
stochastic oscillator formed by a pair ... A network of coupled stochastic **oscillators** is
proposed for modeling of a cluster of entangled **qubits** that is
exploited as a computation resource in one-way quantum
computation schemes. A **qubit** model has been designed as a
stochastic **oscillator** formed by a pair of coupled limit cycle
**oscillators** with chaotically modulated limit cycle radii and
**frequencies**. The **qubit** simulates the behavior of electric field of
polarized light beam and adequately imitates the states of two-level
quantum system. A cluster of entangled **qubits** can be associated
with a beam of polarized light, light polarization degree being
directly related to cluster entanglement degree. Oscillatory network,
imitating **qubit** cluster, is designed, and system of equations for
network dynamics has been written. The constructions of one-**qubit**
gates are suggested. Changing of cluster entanglement degree caused
by measurements can be exactly calculated.

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Contributors: Tim Byrnes

Date: 2012-03-24

**qubit** gate operations that can be performed at a time reduced by a factor...**qubits** made of two component Bose-Einstein condensates (BECs) is analyzed...**qubit**. We illustrate the scheme by an application to Deutsch-s and Grover-s ... Quantum computation using **qubits** made of two component Bose-Einstein condensates (BECs) is analyzed. We construct a general framework for quantum algorithms to be executed using the collective states of the BECs. The use of BECs allows for an increase of energy scales via bosonic enhancement, resulting in two **qubit** gate operations that can be performed at a time reduced by a factor of N, where N is the number of bosons per **qubit**. We illustrate the scheme by an application to Deutsch-s and Grover-s algorithms, and discuss possible experimental implementations. Decoherence effects are analyzed under both general conditions and for the experimental implementation proposed.

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Contributors: Goldner, Philippe

Date: 2018-12-02

**Qubits**
in Rare Earth Doped Nanoparticles ... This presentation was given as an invited seminar at the Department of Applied Physics and Materials Science, Caltech, USA, on May 2, 2018, during a visit to the group of Prof. Andrei Faraon. It gives an overview of the current developments on rare earth based nanoscale systems for quantum technologies, focusing on results obtained within the NanOQTech project.

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Contributors: Duddell, William

Date: 1908-10-31

... n/a

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Contributors: Abdul-Niby, M., Alameen, M., Baitie, H.

Date: 2016-12-18

**frequency** synthesis, quadrature signal generation and phase locked loops...**oscillator** (ILO) of 35MHz **frequency**. Phase shifters at high **frequencies**...**oscillator**...**Oscillating** systems, locking of the **oscillators** can take place for injected...**frequency** to nth harmonics of the free-running **frequency**. In this paper ... In Self **Oscillating** systems, locking of the **oscillators** can take place for injected signals close in **frequency** to nth harmonics of the free-running **frequency**. In this paper, we present a simple design for digital phase shift control by using a harmonically injection locked **oscillator** (ILO) of 35MHz **frequency**. Phase shifters at high **frequencies** are essential in many communication system applications such as **frequency** synthesis, quadrature signal generation and phase locked loops (PLLs).

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Contributors: Georgiadis, Apostolos, Collado, Ana, Niotaki, Kyriaki

Date: 2015-05-01

**frequency** of the **oscillator**, while the output section is designed to maximize...**frequency** divide-by-3 circuit is presented based on an injection locked...**oscillator**. Substrate integrated waveguide (SIW) technology is used to...**oscillator**...**frequency** divider...**oscillator** circuit. A prototype is fabricated presenting a measured DC-RF...**frequency** with 3.7 dBm output power. An injection locking bandwidth of ... A 22.8 GHz analog **frequency** divide-by-3 circuit is presented based on an injection locked **oscillator**. Substrate integrated waveguide (SIW) technology is used to implement the input and output sections of the **frequency** divider circuit. The input SIW section at the gate of the active device permits the introduction of the injection signal at the third harmonic **frequency** of the **oscillator**, while the output section is designed to maximize the DC-RF conversion efficiency of the **oscillator** circuit. A prototype is fabricated presenting a measured DC-RF efficiency of 38.5% at 7.603 GHz output **frequency** with 3.7 dBm output power. An injection locking bandwidth of 301.4 MHz was obtained for a 1.5 dBm input injection signal at 22.8 GHz.

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Contributors: Lubich, L.

Date: 2018-02-20

**oscillator** outputs to the square waves obtained is calculated ignoring...**oscillator** phase noise spectrum. In this paper, accurate expressions are...**Oscillators** are often followed by square wave forming circuits and **frequency**...**oscillators**. The phase noise power spectral densities are calculated in...**oscillator**...**frequency** divider ... **Oscillators** are often followed by square wave forming circuits and **frequency** dividers. Traditionally, the level of the phase noise, transferred from the **oscillator** outputs to the square waves obtained is calculated ignoring the correlations in the **oscillator** phase noise spectrum. In this paper, accurate expressions are derived, taking into account the phase noise mechanisms in the **oscillators**. The phase noise power spectral densities are calculated in both the traditional way and by using the proposed expressions and they are compared. The situations where the proposed expressions can be useful are identified.

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Contributors: Meng Hu, Lili Wang

Date: 2012-08-26

**frequency** formulation...**oscillator** with fractional potential. By calculation and computer simulations...**oscillator**...**frequency** formulation is used to obtain a periodic solution for a nonlinear ... In this paper, He-s amplitude **frequency** formulation is used to obtain a periodic solution for a nonlinear **oscillator** with fractional potential. By calculation and computer simulations, compared with the exact solution shows that the result obtained is of high accuracy.

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Contributors: Walls, Fred L., Stein, Samuel R.

Date: 1978-01-01

**frequency** lock a spectrally pure quartz crystal **oscillator** to an independent...**oscillators** employing these resonators Several problem areas common to ... The intrinsic noise of the best quartz crystal resonators is significantly less than the noise observed in **oscillators** employing these resonators Several problem areas common to traditional designs are pointed out and a new approach is suggested for their solution. Two circuits are described which **frequency** lock a spectrally pure quartz crystal **oscillator** to an independent quartz crystal resonator. The performance of the composite system is predicted based on the measured performance of its components.

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Contributors: Puissant, Stéphane, Lee, Young June

Date: 2016-12-31

**oscillations** and the second echeme with high amplitude **oscillations**. C...**oscillations** showing a dominant **frequency** marked by F3. B, Detailed oscillogram...**oscillations** showing dominant **frequencies** marked by F1 and F2....**frequency** spectrum represented with overlay of 71 spectra computed from...**frequency** spectrum represented with overlay of 52 spectra computed from ... FIGURE 6. Hyalessa maculaticollis. Echemes structure. A, Power **frequency** spectrum represented with overlay of 52 spectra computed from echemes with high amplitude **oscillations** showing a dominant **frequency** marked by F3. B, Detailed oscillogram showing the first echeme with low amplitude **oscillations** and the second echeme with high amplitude **oscillations**. C, Power **frequency** spectrum represented with overlay of 71 spectra computed from echemes with low amplitude **oscillations** showing dominant **frequencies** marked by F1 and F2.

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