CN110120799A - A kind of insulation shortcut method of high-fidelity population inversion in two-level energy system - Google Patents

A kind of insulation shortcut method of high-fidelity population inversion in two-level energy system Download PDF

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Publication number
CN110120799A
CN110120799A CN201910306592.2A CN201910306592A CN110120799A CN 110120799 A CN110120799 A CN 110120799A CN 201910306592 A CN201910306592 A CN 201910306592A CN 110120799 A CN110120799 A CN 110120799A
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fidelity
energy system
level energy
hamiltonian
pulse signal
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班玥
周俊
陈玺
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University of Shanghai for Science and Technology
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University of Shanghai for Science and Technology
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    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/11Complex mathematical operations for solving equations, e.g. nonlinear equations, general mathematical optimization problems
    • G06F17/13Differential equations
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/15Correlation function computation including computation of convolution operations
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06NCOMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
    • G06N10/00Quantum computing, i.e. information processing based on quantum-mechanical phenomena
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K5/00Manipulating of pulses not covered by one of the other main groups of this subclass
    • H03K5/22Circuits having more than one input and one output for comparing pulses or pulse trains with each other according to input signal characteristics, e.g. slope, integral
    • H03K5/26Circuits having more than one input and one output for comparing pulses or pulse trains with each other according to input signal characteristics, e.g. slope, integral the characteristic being duration, interval, position, frequency, or sequence

Abstract

The invention discloses a kind of insulation shortcut methods of high-fidelity population inversion in two-level energy system, using the revertive control method based on Lewis-Riesenfeld quantum invariant, the time-dependent Schrodinger equation of Converse solved two-level energy system, building is able to achieve the set of pulses signal of two-level energy system population inversion, using Arbitrary Waveform Generator generate pulse signal, thus within shorter action time high-fidelity realization population inversion.The pulse signal that the present invention generates can realize the reversion of two-level energy system i on population under the premise of Rabi frequency is no more than 15GHz within the action time of 1ns, fidelity under the influence of phase noise and decoherence not less than 92%, toFrequency detuning within the scope of, fidelity be not less than 99.85%.

Description

A kind of insulation shortcut method of high-fidelity population inversion in two-level energy system
Technical field
The invention belongs to quantum calculation fields, and in particular to the insulation of high-fidelity population inversion in a kind of two-level energy system Shortcut method.
Background technique
Under applied field containing when, the main target that quantum state is always people's research is effectively manipulated and prepares, and And has and be extremely widely applied.Such as the diffraction of nuclear magnetic resonance and relevant frequency spectrum technical aspect, interference and at present rapidly In terms of the quantum information of development and quantum calculation, very important application and researching value are suffered from.
In these above-mentioned fields, two-level energy system model is generally existing basic model, is to constitute that other are more complex Multilevel system basic structural unit, manipulation to two-level energy system quantum state namely realize that its population inversion is one Very important quantum state manipulation.This manipulation request speed is fast, and fidelity is high, and to stablize, not vulnerable to outside noise and The influence of system perturbation, and to have feasibility in practice.
Currently, many scholars propose many methods for realizing population inversion, and such as: Adiabatic Fast Passage technology, π Impulse method, composite pulse method, optimized control method, excited Raman are insulated passage technology and its deriving method etc..However, these Method have the shortcomings that it is respective, such as: π impulse method speed quickly, but the poor robustness when considering systematic error.Quickly absolutely Passage of heat technology is a kind of effective and simple and easy control method, and phylogeny is slowly to guarantee not occur to appoint during being somebody's turn to do What quantum leap, but the evolution time for needing to grow very much, this will lead to the generation of quantum decoherence, to influence fidelity.Most Optimal control method can obtain optimization scheme according to different physical limits, but it often solution is complicated, and as one Black box allows people to be unable to control parameter, while it is also possible to cannot get analytic solutions.Therefore it is desirable to obtain being easy manipulation and Shandong The high nonadiabatic quantum of stick manipulates scheme.
Summary of the invention
It is an object of the invention to solve evolution overlong time, poor robustness, a kind of two energy level systems are provided The insulation shortcut method of high-fidelity population inversion in system.This method generates set of pulses signal, and the group pulse signal is by two Duration is equal, and the two is applied on quantum dot Two-level system by the different pulse composition of amplitude, phase and frequency simultaneously, can Population inversion is completed to manipulate the Two-level system.
Pulse signal generated have the following characteristics that 1) the pulse signal effect time it is short, pulse signal Rabi frequency not Under the premise of 15GHz, action time is no more than 1ns;2) realize that the fidelity of population inversion is not less than 99.85%;3) Consider the fidelity when having phase noise and decoherence influences not less than 92%.
In order to achieve the purpose that foregoing invention, The technical solution adopted by the invention is as follows:
A kind of insulation shortcut method of high-fidelity population inversion in two-level energy system, comprising the following steps:
A. in a two-level energy system, using the revertive control method based on Lewis-Riesenfeld quantum invariant, Converse solved Schrodinger equation:
Two-level energy system Hamiltonian are as follows:
Wherein Δ and Ω are the detuning and Rabi frequency containing when respectively;Hamiltonian eigenstate meets H (t) | ψ±(t) >=ε± (t)|ψ±(t) >, define the lower one group of orthogonal basic vector of the systemThe then instantaneous eigenvector of Hamiltonian It indicates are as follows:
The following differential equation is obtained according to dynamics invariant condition for such two-level energy system:
Wherein, θ and β is respectively polar angle and azimuth on Bloch ball.In order to make the instantaneous eigenstate of Hamiltonian from first When state t=0 | 1 > it is inverted to final states t=tfWhen | 2 >, go out to meet boundary condition using multinomial or other Function Fittings θ and β, to solve Δ and Ω according to Hamiltonian system differential equation is counter;
B. Δ obtained in step a and Ω are input in Arbitrary Waveform Generator, generating has obtained in above-mentioned steps The pulse signal of phase and amplitude;
C. the pulse signal generated in step b is applied on GaAs/Aluminum gallium arsenide's hetero-junctions wafer electrode, pulse The reversion of i on population is realized in signal and semiconductor-quantum-point interaction.
In the step a, in order to be in Hamiltonian initial state | 1 >, reversion is completed when final states to be in | 2 >, it is necessary to it is full Sufficient boundary condition: θ (0)=0, θ (tf)=π.In order to enable Hamiltonian to be smoothly inverted to final states by initial state, and obtain steady Fixed eigenstate, also needs to meet boundary condition:
Compared with prior art, advantages of the present invention is mainly reflected in:
As long as the present invention theoretically Rabi frequency is sufficiently large, the duration of the pulse signal of generation theoretically can be any It is short.The present invention realizes that the fidelity of population inversion is higher, and the phylogeny time is short, and to the robustness of noise and decoherence It is good.Different Evolution Paths can be chosen by different Function Fitting θ and β in the present invention, namely can according to need life At the pulse signal of different performance.
Detailed description of the invention
Fig. 1 is the image that the pulse signal Δ and Ω of the reversion of two ionic fractional abundances are realized in the embodiment of the present invention one.
Fig. 2 is that pulse signal is drilled at any time with i on population in quantum two-level system mechanism in the embodiment of the present invention one The image of change.
Fig. 3 is system in pulse signal in the embodiment of the present invention one and quantum two-level system mechanism in Bloch ball On evolutional path.
Fig. 4 is the image that the pulse signal Δ and Ω of the reversion of two ionic fractional abundances are realized in the embodiment of the present invention two.
Fig. 5 is that pulse signal is drilled at any time with i on population in quantum two-level system mechanism in the embodiment of the present invention two The image of change.
Fig. 6 is system in pulse signal in the embodiment of the present invention two and quantum two-level system mechanism in Bloch ball On evolutional path.
Fig. 7 is decoherence rate γ=7 × 10 in the embodiment of the present invention three6s-1When, pulse signal and quantum two-level system Evolutional path of the system on Bloch ball in mechanism.
Fig. 8 is fidelity F in pulse signal in the embodiment of the present invention three and quantum two-level system mechanism with dephasign The variation relation figure of dry rate γ.
Fig. 9 is pulse signal in the embodiment of the present invention four and there are the interactions of the quantum two-level system of frequency detuning When, realize the objective quantum state that population inversion generates | ψ (tf) > fidelity F with frequency detuning δ variation relation figure.
Specific embodiment
Above scheme is described further with reference to the accompanying drawings and embodiments, the preferred embodiment of the present invention is described in detail such as Under:
Embodiment one:
A kind of insulation shortcut method of high-fidelity population inversion in two-level energy system, according to the initial state of system And final statesUsing multinomialIt is fitted θ and β:
θ (t)=a0+a1t+a2t2+a3t3,
β (t)=b0+b1t+b2t2+b3t3,
Wherein θ is in [0, π] range, β value in [0,2 π] range.Using based on Lewis-Riesenfeld quantum not The time-dependent Schrodinger equation of the Converse solved two-level energy system of insulation shortcut technology of variable theory obtains pulse signal.By what is obtained Pulse signal is input to Arbitrary Waveform Generator generation pulse and is applied on GaAs/Aluminum gallium arsenide's hetero-junctions wafer electrode.
It is the image of pulse signal Δ and Ω that the technical solution generates as shown in Figure 1.It can be seen that curve from image It is smooth readily available in an experiment enough.Pulse operating time only 1ns short enough.
It is the image of i on population Temporal Evolution as shown in Figure 2.It can see this method by the Evolution maps of i on population Make the i on population of two-level energy system from initial stateDevelop to final statesSuccessfully realize the anti-of i on population Turn.
It is evolutional path of the system on Bloch ball as shown in Figure 3, completes system from initial state to last State evolution, correspond to Evolutional path on to Bloch ball is to develop from the arctic of Bloch ball to the South Pole.
Fidelity F=| < -1 | ψ (tf) > |, wherein | ψ (tfThe quantum state that two energy level coupled differential of) > be to solve for obtains | ψ (t) > in t=tfThe state function at moment.The fidelity F=1 of generation objective quantum state in the present embodiment, but the pulse signal It is only applicable to the quantized system there is no frequency detuning and phase noise.
Embodiment two:
The present embodiment is basically the same as the first embodiment, and is particular in that in the present embodiment using trigonometric function and is fitted θ And β:
β (t)=ArcCot (0.1tfθ'(t))
Referring to fig. 4, Fig. 4 can be seen that curve is smooth readily available in an experiment enough to the pulse signal of generation.Pulse is made It is still 1ns with the time.
It is the image of i on population Temporal Evolution as shown in Figure 5.It can see this method by the Evolution maps of i on population Make the i on population of two-level energy system from initial stateDevelop to final statesSuccessfully realize the anti-of i on population Turn.
It is evolutional path of the system on Bloch ball as shown in Figure 6.By comparison diagram 3, we are it can be found that by making It is fitted θ and β with different functions, we have obtained realization can be with the different phylogeny tracks of population inversion.
Embodiment three:
The present embodiment is on the basis of example 1, it is contemplated that the influence of two energy level phase noises and decoherence.System Master equation utilize Lindblad equation form indicate are as follows:
Wherein γ is decoherence rate, ρ and σiRespectively density matrix and Pauli matrices.
Just as referring to Fig. 1 in the pulse signal and embodiment one used in the present embodiment.
Fidelity F=| < -1 | ψ (tf)>|.In decoherence rate γ=7 × 106s-1When, fidelity F=94.56%.System Evolutional path on Bloch ball is referring to Fig. 7, it will be seen that system is still drilled from the arctic of Bloch ball from Fig. 7 Change to the South Pole, namely realize the reversion of i on population, but due to the influence of phase noise and decoherence, there is no drill completely Change at the Geophysical South Pole (0,0, -1) on Bloch ball.
It is to generate objective quantum state as shown in Figure 8 | ψ (tf) > fidelity F with decoherence rate γ variation relation figure, protect True degree reduces with the increase of decoherence rate, but in γ > 107s-1When, fidelity F > 92%.
Example IV:
The present embodiment is that on the basis of example 1, detection realizes the fidelity of population inversion with frequency detuning Variation relation.The pulse signal that the present embodiment uses is identical with embodiment one, and referring to Fig. 1, pulse operating time is still 1ns。
It is that the pulse signal generated in the present embodiment and the quantum two-level system there are frequency detuning are mutual as shown in Figure 9 When effect, the objective quantum state that population inversion generates is realized | ψ (tf) > fidelity F with frequency detuning δ variation relation Figure.When there is no frequency detuning, i.e. δ=0, fidelity 1;Within the scope of Rabi frequency immediate vicinity ± 300MHz, fidelity F > 99.85% shows stronger robustness to existing frequency detuning, and this point is there are the quantum systems of frequency detuning The key element of quantum calculation is realized in system.

Claims (3)

1. a kind of insulation shortcut method of high-fidelity population inversion in two-level energy system, which comprises the following steps:
A. in a two-level energy system, using the revertive control method based on Lewis-Riesenfeld quantum invariant, inversely Solve Schrodinger equation:
Two-level energy system Hamiltonian are as follows:
Wherein Δ and Ω are the detuning and Rabi frequency containing when respectively;Hamiltonian eigenstate meets H (t) | ψ±(t) >=ε±(t)| ψ±(t) >, define the lower one group of orthogonal basic vector of the systemThen the instantaneous eigenvector of Hamiltonian indicates Are as follows:
The following differential equation is obtained according to dynamics invariant condition for such two-level energy system:
Wherein, θ and β is respectively polar angle and azimuth on Bloch ball;In order to make the instantaneous eigenstate of Hamiltonian from initial state t= When 0 | 1 > it is inverted to final states t=tfWhen | 2 >, using multinomial or other Function Fittings go out to meet boundary condition θ and β, to solve Δ and Ω according to Hamiltonian system differential equation is counter;
B. Δ obtained in step a and Ω are input in Arbitrary Waveform Generator, generating has phase obtained in above-mentioned steps With the pulse signal of amplitude;
C. the pulse signal generated in step b is applied on GaAs/Aluminum gallium arsenide's hetero-junctions wafer electrode, pulse signal It interacts with semiconductor-quantum-point and realizes the reversion of i on population.
2. the insulation shortcut method of high-fidelity population inversion, feature exist in two-level energy system according to claim 1 In in the step a, in order to be in Hamiltonian initial state | 1 >, reversion is completed when final states to be in | 2 >, it is necessary to meet boundary Condition: θ (0)=0, θ (tf)=π.
3. the insulation shortcut method of high-fidelity population inversion, feature exist in two-level energy system according to claim 1 In in order to enable Hamiltonian to be smoothly inverted to final states by initial state, and obtaining stable eigenstate, also need to meet perimeter strip Part:
CN201910306592.2A 2019-04-17 2019-04-17 A kind of insulation shortcut method of high-fidelity population inversion in two-level energy system Pending CN110120799A (en)

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Cited By (1)

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Publication number Priority date Publication date Assignee Title
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