### 63152 results for qubit oscillator frequency

Contributors: Wallquist, M., Shumeiko, V. S., Wendin, G.

Date: 2006-08-09

**qubit** 1, and Hadamard gates H are applied to the second **qubit**....**oscillator** is entangled with **qubit** 1, at the next resonance the **oscillator**...**qubits** at their optimal points with respect to decoherence during the ...**qubit** states is achieved by sweeping the cavity frequency through the **qubit**-cavity resonances. The circuit is scalable, and allows to keep the...**qubit**-**qubit** coupling and simple gate operations. Tunable **qubit**-cavity ...**oscillator** with variable **frequency**. Our goal in this section will be to...**the** **qubit**-**qubit** coupling strength is smaller than **the** on-resonance coupling...**frequency** is sequentially swept through resonances with both **qubits**; at...**the** **qubit**-cavity resonances compared to **the** differences in **the** **qubit** frequencies...**qubit** coupling to a distributed **oscillator** - stripline cavity possesses...**qubit** states is achieved by sweeping the cavity **frequency** through the **qubit**-cavity resonances. The circuit is scalable, and allows to keep the...non-interacting qubits, and projecting on the qubit eigenbasis, | g | ...**the** qubits. Selective addressing of a **particular** **qubit** is achieved by ...**qubit**-cavity resonances compared to the differences in the **qubit** **frequencies**...two-**qubit**-cavity system, and analyze appropriate circuit parameters. We...**oscillators** represents the stripline cavity, φ 1 and φ N are superconducting... both qubits; at the first resonance the oscillator is entangled** with** ...**qubits** via tunable stripline cavity...**qubits** **frequency** asymmetry and the coupling **frequency**. Recent suggestions... to qubit 1, and Hadamard gates H are applied to the second qubit....**with **qubit 2 before swapping its state back **onto **qubit 1; free evolution...**two**-**qubit** operation. **The** qubits coupled to **the** cavity must have different... 1 , qubit 1 swaps its state **onto **the oscillator, then the oscillator ...**qubit** 1 swaps its state onto the **oscillator**, then the **oscillator** interacts...**qubits** mediated by a superconducting stripline cavity with a tunable resonance...**oscillator** through resonance with both **qubits** performing π -pulse swaps...**frequency**. The **frequency** control is provided by a flux biased dc-SQUID ... We theoretically investigate selective coupling of superconducting charge **qubits** mediated by a superconducting stripline cavity with a tunable resonance **frequency**. The **frequency** control is provided by a flux biased dc-SQUID attached to the cavity. Selective entanglement of the **qubit** states is achieved by sweeping the cavity **frequency** through the **qubit**-cavity resonances. The circuit is scalable, and allows to keep the **qubits** at their optimal points with respect to decoherence during the whole operation. We derive an effective quantum Hamiltonian for the basic, two-**qubit**-cavity system, and analyze appropriate circuit parameters. We present a protocol for performing Bell inequality measurements, and discuss a composite pulse sequence generating a universal control-phase gate.

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Contributors: Chirolli, Luca, Burkard, Guido

Date: 2009-06-04

**qubit** in the state "0" vs driving time τ 1 and τ 2 , at Rabi **frequency**...**qubit** states $|0>$ and $|1>$ during measurements. Our theory can be applied...**qubit** state is extracted from the **oscillator** measurement outcomes, and...**qubit**-shifted **frequencies**, Δ ω ≈ ± g . For weak driving amplitude f , ...**oscillator** **frequency** ω h o , the state of the **qubit** is encoded in the ...**oscillator** driving amplitude is f / 2 π = 20 ~ G H z and a damping rate...**qubit** in the state | 0 0 | . Correction in Δ t are up to second order....**qubit** current states is made small compared to the **qubit** gap E = ϵ 2 +...**qubit** is coupled to a harmonic oscillator which undergoes a projective...**qubit** states | 0 and | 1 , are represented for illustrative purposes by...**qubit**-dependent "position" x s are shown in the top panel. Fig2... the **qubit** QND measurement is studied in** the **regime of strong projective ...**qubit**-split **frequencies**, that is enhanced when the driving strength f ...**frequency** ϵ 2 + Δ 2 , before and between two measurements prepare the ...**qubit**-shifted **frequency**....**qubit** state is extracted from the oscillator measurement outcomes, and...**qubit** measurement. Two mechanisms lead to deviations from a perfect QND...**oscillator** to a **qubit**-dependent state. c) Perfect QND: conditional probability...**qubit** turns out to be quadratic. The **qubit** Hamiltonian is H S = ϵ σ Z ...**qubit** is coupled to a harmonic **oscillator** which undergoes a projective...**oscillator** is driven at resonance with the bare harmonic **frequency** and...**qubit** relaxation time T 1 = 10 ~ n s is assumed. Fig1...**qubit**) and quantify the degree to which such a **qubit** measurement has a...two **qubit** states produce opposite magnetic field that translate into **a qub**...**qubit**-shifted **frequencies**, the probability has a two-peak structure whose...**qubits** coupled to a circuit **oscillator**....**oscillator**, and (ii) quantum tunneling between the **qubit** states $|0>$ ...**qubit** driving time τ 1 and τ 2 starting with the **qubit** in the state | ...**qubit** coupled to a harmonic oscillator...the effect of **qubit** relaxation and **qubit** tunneling on** the **conditional ... We theoretically describe the weak measurement of a two-level system (**qubit**) and quantify the degree to which such a **qubit** measurement has a quantum non-demolition (QND) character. The **qubit** is coupled to a harmonic **oscillator** which undergoes a projective measurement. Information on the **qubit** state is extracted from the **oscillator** measurement outcomes, and the QND character of the measurement is inferred by the result of subsequent measurements of the **oscillator**. We use the positive operator valued measure (POVM) formalism to describe the **qubit** measurement. Two mechanisms lead to deviations from a perfect QND measurement: (i) the quantum fluctuations of the **oscillator**, and (ii) quantum tunneling between the **qubit** states $|0>$ and $|1>$ during measurements. Our theory can be applied to QND measurements performed on superconducting **qubits** coupled to a circuit **oscillator**.

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Contributors: Cooper, K. B., Steffen, Matthias, McDermott, R., Simmonds, R. W., Oh, Seongshik, Hite, D. A., Pappas, D. P., Martinis, John M.

Date: 2004-05-31

**qubit** in state | 0 (solid circles) and in an equal mixture of states |...**oscillations** is consistent with the spectroscopic splittings observed ...**qubits** and microscopic critical-current fluctuators by implementing a ...**qubit**'s resonant frequency. The results point to a possible mechanism ...**oscillation** periods are observed to correspond to the spectroscopic splittings...the **qubit** with strength h S / 2 . On resonance, the **qubit**-fluctuator eigenstates...**qubit** circuitry. For the **qubit** used in Fig. 2, the Josephson critical-current...**qubit**'s resonant **frequency**. The results point to a possible mechanism ... **qubit** circuitry. For the **qubit** used in Fig. 2, the Josephson critical-current...**oscillations** between Josephson phase **qubits** and microscopic critical-current...**qubit** and a microscopic resonator using fast readout...**qubit** probability amplitude first moves to state | 1 g and then **oscillates**...**qubit** with strength h S / 2 . On resonance, the **qubit**-fluctuator eigenstates... **qubit** well is much shallower and state | 1 rapidly tunnels to the right...**qubits** and demonstrate the means to measure two-**qubit** interactions in ...the **qubit** spectroscopy near Δ U / ℏ ω p = 3.55 , showing splittings of...**qubit** spectroscopy near Δ U / ℏ ω p = 3.55 , showing splittings of strengths ... We have detected coherent quantum **oscillations** between Josephson phase **qubits** and microscopic critical-current fluctuators by implementing a new state readout technique that is an order of magnitude faster than previous methods. The period of the **oscillations** is consistent with the spectroscopic splittings observed in the **qubit**'s resonant **frequency**. The results point to a possible mechanism for decoherence and reduced measurement fidelity in superconducting **qubits** and demonstrate the means to measure two-**qubit** interactions in the time domain.

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Contributors: Saiko, A. P., Fedaruk, R.

Date: 2010-12-10

**qubits** arises at double resonance in a bichromatic field when the **frequency**...**frequency** equals the Larmor **frequency** of the initial **qubit**. We show that...**Qubits** in a Doubly Resonant Bichromatic Field...**qubit** operations in the strong-field regime, the counter-rotating component...radio-**frequency** (rf) field is close to that of the Rabi **oscillation** in...**qubit** and transitions created by a bichromatic field at double resonance...**qubits** can be selected by the choice of both the rotating frame and the...**qubits** arises at double resonance in a bichromatic field when the frequency...**qubit**. We show that the operational multiphoton transitions of dressed ... Multiplication of spin **qubits** arises at double resonance in a bichromatic field when the **frequency** of the radio-**frequency** (rf) field is close to that of the Rabi **oscillation** in the microwave field, provided its **frequency** equals the Larmor **frequency** of the initial **qubit**. We show that the operational multiphoton transitions of dressed **qubits** can be selected by the choice of both the rotating frame and the rf phase. In order to enhance the precision of dressed **qubit** operations in the strong-field regime, the counter-rotating component of the rf field is taken into account.

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Contributors: Murch, K. W., Ginossar, E., Weber, S. J., Vijay, R., Girvin, S. M., Siddiqi, I.

Date: 2012-08-22

**qubit**-cavity detuning for the **qubit** prepared in the ground state in the...**qubit**, both the effective nonlinearity and the threshold become a non-trivial...**oscillator** Q....**the** **qubit**-oscillator model with N l = 7 show **the** avoided crossings in ...**qubit**-**oscillator** model with N l = 7 show the avoided crossings in the ...and **qubit** junctions (lower and upper insets)....**qubit** junctions (lower and upper insets)....**qubit** and may be used to realize a high fidelity, latching readout whose...**qubit**-**oscillator** detuning. Moreover, the autoresonant threshold is sensitive...**oscillator** is strongly coupled to a quantized superconducting **qubit**, both...**qubit** state. (a) Color plot shows S | 1 versus **qubit** detuning. The dashed... **qubit** state. (a) Color plot shows S | 1 versus **qubit** detuning. The dashed...**qubit**-cavity detuning for **the** **qubit** prepared in **the** ground state in **the**...**frequency** chirped excitation is applied to a classical high-Q nonlinear...**qubit**-oscillator detuning. Moreover, the autoresonant threshold is sensitive...**oscillators** (red) are shown. The arrows indicate the locations of avoided...**the** **qubit** energy levels were modeled as a Duffing nonlinearity. ... When a **frequency** chirped excitation is applied to a classical high-Q nonlinear **oscillator**, its motion becomes dynamically synchronized to the drive and large oscillation amplitude is observed, provided the drive strength exceeds the critical threshold for autoresonance. We demonstrate that when such an **oscillator** is strongly coupled to a quantized superconducting **qubit**, both the effective nonlinearity and the threshold become a non-trivial function of the **qubit**-**oscillator** detuning. Moreover, the autoresonant threshold is sensitive to the quantum state of the **qubit** and may be used to realize a high fidelity, latching readout whose speed is not limited by the **oscillator** Q.

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Contributors: Bertet, P., Chiorescu, I., Harmans, C. J. P. M, Mooij, J. E.

Date: 2005-07-13

**frequency** in the figure). The dashed line indicates the phase-noise insensitive...**qubit** dephasing time as a function of $\delta \nu_0$. We discuss the specific...**oscillator** variables coming from the flux-dependence of the SQUID Josephson...**qubits** is known to arise because of a variety of environmental degrees... the **qubit** when ϵ = 0 , since at that point** the **average flux generated...(a)...**qubit**. Because of the coupling, the **qubit** frequency is shifted by an amount...mode-**qubit** interaction hamiltonian which, in addition to the usual Jaynes-Cummings...flux-**qubit** coupled to the plasma mode of its DC-SQUID detector. We first...**qubit** biased by Φ x and SQUID biased by current I b . (b) Simplified electrical...**Qubit** **frequency** ν q as a function of the bias ϵ for Δ = 5.5 G H z (minimum...flux-**qubit** coupled to a harmonic oscillator...**qubit** is biased at ϵ = 0 (dashed line in figure fig:nuq), it is insensitive...qubit_hamiltonian yields a **qubit** transition frequency ν q = Δ 2 + ϵ 2 ...**SQUID**-qubit system is seen as an inductance L J connected to the shunct...**frequency** shift now depends on ϵ . Since g 2 is negative (see figure fig...high-**frequency** noise from the dissipative impedance. The SQUID is threaded...lines)....0...the **qubit** is effectively decoupled from its measuring circuit. The ϵ m...flux-**qubit** is a superconducting loop containing three Josephson junctions...**qubit**. Because of the coupling, the **qubit** **frequency** is shifted by an amount...flux-**qubit** is the loop in red containing the three junctions of phases...**Frequency** shift per photon δ ν 0 as a function of I b and ϵ . The white...SQUID-**qubit** system is seen as an inductance L J connected to the shunct...the **qubit** is insensitive to** the **thermal fluctuations of** the **plasma mode...**qubit** transition **frequency** ν q = Δ 2 + ϵ 2 . The corresponding dependence ... Decoherence in superconducting **qubits** is known to arise because of a variety of environmental degrees of freedom. In this article, we focus on the influence of thermal fluctuations in a weakly damped circuit resonance coupled to the **qubit**. Because of the coupling, the **qubit** **frequency** is shifted by an amount $n \delta \nu_0$ if the resonator contains $n$ energy quanta. Thermal fluctuations induce temporal variations $n(t)$ and thus dephasing. We give an approximate formula for the **qubit** dephasing time as a function of $\delta \nu_0$. We discuss the specific case of a flux-**qubit** coupled to the plasma mode of its DC-SQUID detector. We first derive a plasma mode-**qubit** interaction hamiltonian which, in addition to the usual Jaynes-Cummings term, has a coupling term quadratic in the **oscillator** variables coming from the flux-dependence of the SQUID Josephson inductance. Our model predicts that $\delta \nu_0$ cancels in certain non-trivial bias conditions for which dephasing due to thermal fluctuations should be suppressed.

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Contributors: Strauch, F. W., Dutta, S. K., Paik, Hanhee, Palomaki, T. A., Mitra, K., Cooper, B. K., Lewis, R. M., Anderson, J. R., Dragt, A. J., Lobb, C. J.

Date: 2007-03-02

**frequency**, and two-photon Rabi **frequency** are compared to measurements ...**frequency** Ω R , 01 of the one-photon 0 1 transition as function of microwave...**qubit**, scanned in **frequency** (vertical) and bias current (horizontal). ...**qubit** (current-biased Josephson junction) at high microwave drive power...**qubit** with Nb/AlOx/Nb tunnel junctions. Good agreement is found between...**oscillations** of the escape rate for I a c = 16.5 nA....**oscillations** have been observed in many superconducting devices, and represent...**oscillation** **frequency** Ω ̄ R , 01 as a function of the level spacing ω ...**qubit**...**qubits**) in a quantum computer. We use a three-level multiphoton analysis...phase qubit, scanned in frequency (vertical) and bias current (horizontal ... Rabi **oscillations** have been observed in many superconducting devices, and represent prototypical logic operations for quantum bits (**qubits**) in a quantum computer. We use a three-level multiphoton analysis to understand the behavior of the superconducting phase **qubit** (current-biased Josephson junction) at high microwave drive power. Analytical and numerical results for the ac Stark shift, single-photon Rabi **frequency**, and two-photon Rabi **frequency** are compared to measurements made on a dc SQUID phase **qubit** with Nb/AlOx/Nb tunnel junctions. Good agreement is found between theory and experiment.

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Contributors: Dial, O. E., Shulman, M. D., Harvey, S. P., Bluhm, H., Umansky, V., Yacoby, A.

Date: 2012-08-09

**qubit** loses its quantum information due to interactions with its noisy...**frequencies** in the device....**qubit** and gives good contrast over a wide range of J . b, Exchange **oscillations**...**frequency** **oscillations** and small d J / d ϵ , a region of large **frequency**...**qubit** with an integrated RF sensing dot. a The detuning ϵ is the voltage...**qubit** is loaded and measured, and the 0 2 region where J is large but ...**qubit** during exchange oscillations. Using free evolution and Hahn echo... the **qubit** along** the **y -axis (Fig. t2stara, Fig. S1). Fig. t2starb shows ...**oscillations** and large d J / d ϵ , and a region where **oscillations** are...**qubits** are typically operated, the transitional region where J and d J...**qubit** **oscillations** to decay and setting a limit on the fidelity of quantum...**frequencies** are small, allowing the **qubit** to be used as a charge sensor...**qubit** and gives good contrast over a wide range of J . b, Exchange oscillations...single **qubit** rotations in S - T 0 and exchange-only qubits and is the ...**qubit** oscillations to decay and limits** the **fidelity of quantum control...**oscillations**. f, Charge **oscillations** measured in 0 2 . This figure portrays...**qubit**,and in metrology the **frequency** of the precession provides a sensitive...**oscillations**) of these FID **oscillations**, Q ≡ J T 2 * / 2 π ∼ J d J / d...**oscillations** in 0 2 are also primarily dephased by low **frequency** voltage...**qubit** during exchange **oscillations**. Using free evolution and Hahn echo...two-**qubit** operations in single spin, S - T 0 , and exchange-only qubits...**qubit**-based measurements. Understanding how the **qubit** couples to its environment...**qubit** **oscillations** to decay and limits the fidelity of quantum control...**frequency** and high **frequency** environmental fluctuations, respectively....**qubit**,and in metrology the frequency of the precession provides a sensitive...**qubit** to be used as a charge sensor with a sensitivity of $2 \times 10...**qubits**, a particular realization of spin **qubits** , which store quantum ...Singlet-Triplet-**Qubit**...**qubit** are grayed out. d, J ϵ and d J / d ϵ in three regions; the 1 1 region ... Two level systems that can be reliably controlled and measured hold promise in both metrology and as qubits for quantum information science (QIS). When prepared in a superposition of two states and allowed to evolve freely, the state of the system precesses with a **frequency** proportional to the splitting between the states. In QIS,this precession forms the basis for universal control of the **qubit**,and in metrology the **frequency** of the precession provides a sensitive measurement of the splitting. However, on a timescale of the coherence time, $T_2$, the **qubit** loses its quantum information due to interactions with its noisy environment, causing **qubit** **oscillations** to decay and setting a limit on the fidelity of quantum control and the precision of **qubit**-based measurements. Understanding how the **qubit** couples to its environment and the dynamics of the noise in the environment are therefore key to effective QIS experiments and metrology. Here we show measurements of the level splitting and dephasing due to voltage noise of a GaAs singlet-triplet **qubit** during exchange **oscillations**. Using free evolution and Hahn echo experiments we probe the low **frequency** and high **frequency** environmental fluctuations, respectively. The measured fluctuations at high **frequencies** are small, allowing the **qubit** to be used as a charge sensor with a sensitivity of $2 \times 10^{-8} e/\sqrt{\mathrm{Hz}}$, two orders of magnitude better than the quantum limit for an RF single electron transistor (RF-SET). We find that the dephasing is due to non-Markovian voltage fluctuations in both regimes and exhibits an unexpected temperature dependence. Based on these measurements we provide recommendations for improving $T_2$ in future experiments, allowing for higher fidelity operations and improved charge sensitivity.

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Contributors: Averin, D. V.

Date: 2002-02-05

**qubit**, σ z and σ y , as required in the QND Hamiltonian ( 2). For discussion...**oscillations** avoiding the detector-induced dephasing that affects the ... **qubit**. The oscillations are represented as a spin rotation in the z -...**frequency** Δ . QND measurement is realized if the measurement frame (dashed...**qubit** structure that enables measurements of the two non-commuting observables...**oscillations** in an individual two-state system. Such a measurement enables...**frequency** Ω ≃ Δ ....**qubits** which combine flux and charge dynamics....**qubit**...**oscillations** of a **qubit**. The **oscillations** are represented as a spin rotation ... The concept of quantum nondemolition (QND) measurement is extended to coherent **oscillations** in an individual two-state system. Such a measurement enables direct observation of intrinsic spectrum of these **oscillations** avoiding the detector-induced dephasing that affects the standard (non-QND) measurements. The suggested scheme can be realized in Josephson-junction **qubits** which combine flux and charge dynamics.

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Contributors: Mandip Singh

Date: 2015-07-14

flux-**qubit** in the form of a cantilever. The net magnetic flux threading...superconducting-loop-**oscillator** when the intrinsic **frequency** is 10 kHz...flux-**qubit** and the mechanical degrees of freedom of the cantilever are...flux-**qubit**-cantilever turns out to be an entangled quantum state, where...superconducting-loop-**oscillator** with its axis of rotation along the z-axis... flux-qubit and the cantilever. An additional magnetic** flux** threading ...**frequency** (E/h) is ∼4×1011 Hz.
... flux-qubit-cantilever. A part of the** flux**-qubit (larger loop) is projected...**oscillator** is proposed, which consists of a flux-**qubit** in the form of ...flux-**qubit**-cantilever without a Josephson junction, is also discussed....flux-**qubit**-cantilever. A part of the flux-**qubit** (larger loop) is projected...**qubit**...**frequency** (E/h) is ∼3.9×1011 Hz.
... In this paper a macroscopic quantum **oscillator** is proposed, which consists of a flux-**qubit** in the form of a cantilever. The net magnetic flux threading through the flux-**qubit** and the mechanical degrees of freedom of the cantilever are naturally coupled. The coupling between the cantilever and the magnetic flux is controlled through an external magnetic field. The ground state of the flux-**qubit**-cantilever turns out to be an entangled quantum state, where the cantilever deflection and the magnetic flux are the entangled degrees of freedom. A variant, which is a special case of the flux-**qubit**-cantilever without a Josephson junction, is also discussed.

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