CN112532320B - A method for generating low-speed stable optical solitons in weak light - Google Patents

A method for generating low-speed stable optical solitons in weak light Download PDF

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CN112532320B
CN112532320B CN202011411546.8A CN202011411546A CN112532320B CN 112532320 B CN112532320 B CN 112532320B CN 202011411546 A CN202011411546 A CN 202011411546A CN 112532320 B CN112532320 B CN 112532320B
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徐四六
王可畏
薛丽
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Hubei University of Science and Technology
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Abstract

本发明公开了一种产生弱光低速稳定光孤子的方法，通过非相干泵浦光Γ21作用于寿命加宽的四能级倒Y型里德堡冷原子系统，利用控制光诱导的原子量子态之间的干涉来消除共振介质对光强较弱的入射光的吸收，获得较大的非线性效应，得到稳定PT对称光孤子。本发明简单易懂、实现方便，实用性强，可根据实际情况进行相关参数的调整，为光孤子在光通信技术领域的深入应用和发展提供了有力支持。

Figure 202011411546

The invention discloses a method for generating low-speed stable optical solitons in weak light. Incoherent pump light Γ 21 acts on a four-level inverted Y-type Rydberg cold atom system with extended lifetime, and utilizes controlled light-induced atomic quantum The interference between the states can eliminate the absorption of the incident light with weak light intensity by the resonant medium, obtain a large nonlinear effect, and obtain a stable PT symmetrical optical soliton. The invention is simple and easy to understand, easy to implement, and has strong practicability, and can adjust relevant parameters according to actual conditions, and provides strong support for the in-depth application and development of optical soliton in the field of optical communication technology.

Figure 202011411546

Description

Method for generating weak light low-speed stable light solitons
Technical Field
The invention belongs to the technical field of optical communication, relates to a method for generating a low-light low-speed stable optical soliton, and particularly relates to a method for generating a low-light low-speed stable PT symmetrical optical soliton by utilizing a cold atom EIT (atomic energy exchange) of a Reidberg.
Background
Optical soliton/optical bullets (light bullets, LBs) are a special form of ultrashort optical pulses formed by the combined effects of group velocity dispersion and self-phase modulation in the optical medium. The optical soliton is not diffused in space and time, so that the time domain waveform and the spectrum shape can be kept unchanged in the transmission process, the optical soliton has the advantages of large transmission capacity, low error rate, strong anti-interference capability and the like, and has wide application prospect in the technical field of optical soliton communication. Due to the physical characteristics of optical solitons and the technical application thereof, many researchers have conducted theoretical and experimental research on optical solitons in recent years.
With the development of all-optical communication and all-optical computation, the requirements for stable optical solitons based on information transmission and signal processing of optical chips are increasing day by day, and the stable optical solitons can be directly used as carriers of binary information and meet the requirements for signal processing in all-optical systems due to the property that the optical solitons are not diffused in space. However, optical solitons generally have instability and can only propagate over a very short diffraction length. The classical method for obtaining stable optical solitons is to adopt nonlinear materials with adjustable dispersion and diffraction properties, generate nonlinear self-phase adjustment compensation dispersion by utilizing nonlinear self-focusing compensation space diffraction effect through nonlinear action of light and materials, and obtain the spatial and temporal local area of light waves so as to realize the optical solitons.
Although optical solitons can be realized using nonlinear materials, the optical solitons obtained from nonlinear materials are energy dependent and there is an energy threshold below which the soliton propagation will be divergent. In addition, the nonlinear mechanism strongly depends on nonlinear materials, but the number of nonlinear materials which can be practically used is not large, and the generation of stable optical solitons is also greatly limited by the dependence. Therefore, it is necessary to search for a new method for generating a stable optical soliton.
Disclosure of Invention
In order to solve the technical problem, the invention provides a method for generating a low-light low-speed stable light soliton.
The technical scheme adopted by the invention is as follows: a method for generating low-speed stable optical solitons of weak light by optically detecting the incoherent pumping light gamma of field gain21The method is applied to an inverted Y-shaped four-energy-level Reedberg cold atom system with a prolonged service life, the interference between atom quantum states induced by control light with larger light intensity is utilized to eliminate the absorption of a resonant medium on incident light with weaker light intensity, a larger nonlinear effect is obtained, and a stable light soliton with space-time (PT) symmetry is obtained.
The four-energy-level inverted Y-shaped rydberg cold atom system with the widened service life has the energy levels of atoms of |1>＝|5S1/2,F＝1>，|2>＝|5S1/2,F＝2>，|3>＝|5P3/2,F＝3>And |4>＝|60S1/2>Wherein 5 and 60 represent the number of principal quantums, S1/2Denotes the S orbit with a spin quantum number of 1/2, F denotes the total angular momentum, P3/2Represents the P orbit with a spin quantum number of 3/2. A bundle of pull ratio frequency of A S-1Weak detection light field omegapAnd a bundle of pull ratio frequencies of B S-1Strongly controlled light field omegacCoupled respectively to |1>→|3>And |2>→|3>A bundle of pull ratio frequencies of C S-1Auxiliary light field omegaaCoupling |3>→|4>Their field distribution functional relationship Ep≤Ea＜＜Ec(ii) a Wherein A, B, C is a preset value.
The specific implementation comprises the following substeps:
step 1: the method comprises the following steps of trapping a Reidberg atomic gas in a magneto-optical trap, wherein the ambient temperature of the atomic gas is in the order of nanometer Kelvin, and the Doppler effect caused by the mass center movement and the thermal movement of atoms is negligible;
step 2: will have a ratio frequency of B S-1The control light field of the spatial modulation is incident into the gas according to a preset direction, and the frequency coupling energy level is |3>→|4>A transition of (c);
and step 3: will have a pull ratio frequency of A S-1Detected light field omegapSum-to-ratio frequency of C S-1Auxiliary light field omegaaAfter focusing and collimating, the light beam reversely propagates in the gas;
and 4, step 4: locking the frequency of the detection light field on a transition line of a rydberg atomic gas atomic energy level |1> → |3>, controlling the frequency of the light field to be adjusted to be close to the transition line of the rydberg atomic gas atomic energy level |2> → |3>, applying DHz to the detection light field, and modulating FHz to the modulation amplitude; wherein D, F is a preset value;
and 5: in the whole process, the optical power is kept and controlled to be unchanged, the frequency of the detection light is scanned near a transition line of atomic energy level |1> → |3> of the atomic gas of the Reedberg, the transmission light intensity and the phase of the detection light after passing through the atomic gas are detected, and then demodulation is carried out to obtain the stable optical soliton.
Theoretical and experimental studies show that the cold atoms in the rydberg can establish an optical nonlinear system with strong and long optical path. By introducing Electromagnetic Induction Transparency (EIT) of the gas of the cold atoms in the Reidberg, the absorption of the resonant medium to the incident light with weaker light intensity is eliminated by the interference between the atomic quantum states induced by the control light with larger light intensity through the interaction of the light and the cold atoms, and a larger nonlinear effect is obtained to obtain the stable optical solitons. Different from the classical nonlinear material method, the optical soliton obtained by the invention not only has space-time (PT) symmetry, but also supports low speed (the group velocity is hundreds of meters per second) of non-local weak light (nano watt level), so that the optical soliton with the characteristic can be more concerned and applied.
Compared with the prior art, the invention has the beneficial effects that:
(1) the invention provides a method for generating stable LBs based on a Reedberg cold atom decorated EIT. The method obtains stable LBs (ground state optical solitons, dipolar optical solitons, quadrupole solitons and vortex optical solitons) and dynamic characteristics thereof by regulating and controlling a real part and an imaginary part of PT symmetrical potential and Kerr non-local nonlinear coefficients. Analysis shows that the optical solitons not only have an ultra-slow propagation speed, but also have extremely low generated power.
(2) The method provided by the invention opens up a development approach of non-Hermite nonlinear optics, and particularly utilizes controllable PT symmetrical optical potential and non-local Kerr nonlinear manipulation LBs to realize stable PT symmetrical optical solitons with non-local weak light and low speed characteristics, so that the stable PT symmetrical optical solitons can be widely applied to the technical fields of optical communication and optical transmission.
(3) The method provided by the invention is simple and easy to understand, convenient to realize and strong in practicability, can be used for adjusting related parameters according to actual conditions, and provides powerful support for deep application and development of the optical solitons in the technical field of optical communication.
Drawings
FIG. 1 is a schematic diagram of a four-level inverted Y-shaped Reedberg cold atom system with extended lifetime for an embodiment of the present invention;
FIG. 2 is a schematic diagram of an experimental scheme corresponding to the method of the present invention and a schematic diagram of propagation directions of light fields;
fig. 3 is a characteristic diagram of the ground state optical soliton (a) and the dipolar optical soliton (d) realized by the method of the present invention. The (a1, d1) is a cross section, (a2, d2) is a field mode diagram, and (a3, d3) is a phase diagram.
Detailed Description
In order to facilitate the understanding and implementation of the present invention for those of ordinary skill in the art, the present invention is further described in detail with reference to the accompanying drawings and examples, it is to be understood that the embodiments described herein are merely illustrative and explanatory of the present invention and are not restrictive thereof.
For convenience of explaining the method for generating the low-speed stable light solitons with weak light, the four-energy-level inverted-Y-shaped rydberg cold atom system with a widened lifetime is introduced in the embodiment as shown in FIG. 1, and the embodiment selects88Sr is selected as the four-level inverted Y-shaped Reedberg cold atom system with the lifetime widened88Sr atomThe four energy levels of the son are respectively |1>＝|5S1/2,F＝1>，|2>＝|5S1/2,F＝2>，|3>＝|5P3/2,F＝3>And |4>＝|60S1/2>. A bundle of pull ratio frequency of A S-1Weak detection light field omegapAnd a bundle of pull ratio frequencies of B S-1Strongly controlled light field omegacCoupled respectively to |1>→|3>And |2>→|3>A bundle of pull ratio frequencies of C S-1Auxiliary light field omegaaCoupling |3>→|4>Their field distribution functional relationship Ep≤Ea＜＜Ec(ii) a The quantum effect of the optical field is not significant and can be handled as a classical electromagnetic field. Another incoherent pump light (gamma)21) For this system, the control field and the auxiliary field are spatially modulated. Delta3For single-photon detuning, Δ2And Δ4For two-photon detuning, the decorated Reidberg EIT scheme (Δ)3+Δ4＞＞Ωa). This example studies that the density of the gas at the rydberg atoms is small and the local non-linearity caused by the interaction between light and atoms cannot be neglected.
The specific implementation of the embodiment comprises the following steps:
step 1: a gas of a Reedberg atom (88Sr) is confined in a Magneto-optical trap (MOT), the ambient temperature of atomic gas is in the order of nano Kelvin, and the Doppler effect caused by the mass center movement and the thermal movement of atoms is negligible;
step 2: will have a pull ratio frequency of B S-1Of the spatial modulation of (2) the control light field omegacIncident into the gas in a predetermined direction, and frequency-coupled to an energy level |3>→|4>A transition of (c);
and step 3: will have a pull ratio frequency of A S-1Detected light field omegapSum-to-ratio frequency of C S-1Auxiliary light field omegaaAfter focusing and collimating, the light beam reversely propagates in the gas;
and 4, step 4: locking the frequency of the detection light field on a transition line of a rydberg atomic gas atomic energy level |1> → |3>, controlling the frequency of the light field to be adjusted to be close to the transition line of the rydberg atomic gas atomic energy level |2> → |3>, and applying shallow amplitude frequency modulation with the modulation frequency of DHz and the modulation amplitude of FHz to the detection light field;
and 5: in the whole process, the optical power is kept and controlled to be unchanged, the frequency of the detection light is scanned near a transition line of atomic energy level |1> → |3> of the atomic gas of the Reedberg, the transmission light intensity and the phase of the detection light after passing through the atomic gas are detected, and then demodulation is carried out to obtain the stable optical soliton.
The weak detection light field omega of the present embodimentpHas a value range of 106<A<3×106Strong control of light field omegacHas a value range of 107<B<3×107Auxiliary light field omegaaThe range of the value of the draw ratio frequency is 5 multiplied by 106<C<1.5×107The modulation frequency has a value range of 103<D<104The value range of the modulation amplitude is 107<F<108。
Fig. 2 is a schematic diagram of an experimental scheme corresponding to this embodiment and a schematic diagram of propagation directions of respective optical fields. The whole big sphere is a mode-locked super atom, the dotted circular inner sphere is a Reidberg atom, omegap、ΩaAnd omegacIn parallel in opposite directions in the gas of the rydberg atoms.
A schematic representation of the blockage effect of the reed castle is shown in fig. 2. The excitation of atoms within the occluding sphere is hindered by long range interactions between the rydberg atoms, the boundaries of which are represented by the dashed circles in this embodiment. Only one atom (the hollow sphere in the center of the dotted circle) in each occluding sphere is excited to the rydberg state, and the remaining atoms (the hollow spheres in the dotted circle) cannot be excited to the rydberg state due to the occluding effect. The kinetics of the light-rydberg atom interaction system is described in terms of hamiltonian under the heisenberg representation:
Figure BDA0002815481830000051
Figure BDA0002815481830000052
is the system Hamiltonian, NaIs the atomic gas density, r represents the distance between the rydberg atoms,
Figure BDA0002815481830000053
is the Hamiltonian of the r atom position, d3r represents the triple integral over space and t represents time.
Under the approximation of electric dipoles and spin waves, the main equation of the system density matrix evolution is as follows:
Figure BDA0002815481830000054
wherein
Figure BDA0002815481830000055
Being a density matrix, Γ is a relaxation matrix, which describes atomic state spontaneous emission and atomic system decoherence; i represents an imaginary unit,
Figure BDA0002815481830000056
Representing the planck constant.
Under paraxial and slowly varying envelope approximations, the maxwell's equations for probe light are:
Figure BDA0002815481830000057
wherein omegapFor detecting the optical contrast ratio frequency, c is the speed of light, omegapTo detect the optical frequency, z, x, y represent three dimensional coordinates in space.
Figure BDA0002815481830000058
For detecting the optical polarizability, wherein(1)Linear polarizability, which is a symmetric potential with respect to PT,
Figure BDA0002815481830000059
and
Figure BDA00028154818300000510
for local and non-local third-order nonlinear polarizabilities,
Figure BDA00028154818300000511
and
Figure BDA00028154818300000512
for local and non-local fifth order nonlinear polarizabilities,
Figure BDA0002815481830000061
and
Figure BDA0002815481830000062
depending on the interaction between the light and the atoms,
Figure BDA0002815481830000063
and
Figure BDA0002815481830000064
then depends on the interaction between the rydberg atoms, such as the interaction potential V (r-r') between the rydberg atoms and the atomic gas density NaAnd the like.
The dimensionless nonlinear equation of the detection field pulse satisfies:
Figure BDA0002815481830000065
wherein psi ═ omegap/ψ0To detect the typical rabi frequency of the field pulses, s-z/(2L)diff),r⊥＝(x,y,0),(ξ,η)＝(x,y)/R⊥Coefficient of dispersion
Figure BDA0002815481830000066
Wherein
Figure BDA0002815481830000067
R⊥Typical radius of curvature of the probe field pulse. gamma-2W1|ψ0|2LdiffIs in photo-atomic phaseThe nonlinear coefficients of the local Kerr effect of the interaction contributions,
Figure BDA0002815481830000068
the system non-local scale coefficient is represented, pi is PT symmetrical potential, and V is long-range interaction potential between rydberg atoms.
A step fourier method can be used to solve the stable digital solution of equation (4). In the present invention, the present embodiment adopts88Sr as the inverted "Y" type four-level atomic system in fig. 1, the parameters involved in the proposed method are chosen as follows: r⊥＝12μm,τ0＝1.1×10-6s,τ21＝0.2πMHz,Γ3＝2π×106MHz,Γ4＝Γ34＝2π×16.7kHz,Δ2＝1.67×106s-1,Δ3＝9.67×107s-1,Δ4＝1.36×107s-1,Na＝1.0×1012cm-3,Ωc＝1.5×107s-1,Ωa＝1.0×107s-1,V0＝21.17。
Fig. 3 is a characteristic diagram of the ground state optical soliton (a) and the dipolar optical soliton (d) realized by the method provided by the invention. The (a1, d1) is a cross section, (a2, d2) is a field mode diagram, and (a3, d3) is a phase diagram. Therefore, the method provided by the invention can generate stable PT symmetrical optical solitons and realize the stable transmission of the ultra-low-speed low-power optical solitons.
The method provided by the invention has the advantages that: the invention provides a Reedberg cold atom decoration state EIT method based stable PT symmetrical optical solitons, which solves the problem that the stable optical solitons are difficult to generate in the technical field of optical communication, and the realized PT symmetrical optical solitons have the characteristics of ultra-low speed and low power. The optical soliton realized by the invention has wide application prospect in the technical field of optical communication.
It should be understood that the above description of the preferred embodiments is given for clarity and not for any purpose of limitation, and that various changes, substitutions and alterations can be made herein without departing from the spirit and scope of the invention as defined by the appended claims.

Claims (1)

1.一种产生弱光低速稳定光孤子的方法，其特征在于：通过非相干泵浦光Γ21作用于寿命加宽的四能级倒Y型里德堡冷原子系统，利用控制光诱导的原子量子态之间的干涉来消除共振介质对光强较弱的入射光的吸收，获得较大的非线性效应，得到稳定PT对称光孤子；1. a method for producing weak light low-speed stable optical solitons, characterized in that: acting on a four-level inverted Y-type Rydberg cold atom system with extended lifetime by incoherent pump light Γ21 , using controlled light-induced The interference between the atomic quantum states can eliminate the absorption of the incident light with weak light intensity by the resonance medium, obtain a large nonlinear effect, and obtain a stable PT symmetrical optical soliton; 所述寿命加宽的四能级倒Y型里德堡冷原子系统，原子的能级分别为|1>＝|5S1/2,F＝1>，|2>＝|5S1/2,F＝2>，|3>＝|5P3/2,F＝3>，和|4>＝|60S1/2>，其中，5和60表示主量子数，S1/2表示自旋量子数为1/2的S轨道，F表示总角动量、P3/2表示自旋量子数为3/2的P轨道；一束拉比频率为A S-1的弱探测光场Ωp和一束拉比频率为B S-1的强控制光场Ωc分别耦合|1>→|3>和|2>→|3>，一束拉比频率为CS-1的辅助光场Ωa耦合|3>→|4>，它们的场分布函数关系Ep≤Ea＜＜Ec；其中，A、B、C为预设值；In the four-level inverted Y-type Rydberg cold atomic system with extended lifetime, the atomic energy levels are |1>=|5S 1/2 , F=1>, |2>=|5S 1/2 , F=2>, |3>=|5P 3/2 , F=3>, and |4>=|60S 1/2 >, where 5 and 60 represent principal quantum numbers and S 1/2 represent spin quantum numbers The S orbital with a number of 1/2, F is the total angular momentum, P 3/2 is a P orbital with a spin quantum number of 3/2; a beam of weak probe light field Ω p with a Rabi frequency of AS -1 and a The strong control light field Ω c with the beam-rabi frequency of BS -1 is coupled to |1>→|3> and |2>→|3> respectively, and an auxiliary light field Ω a of the beam-rabi frequency of CS -1 is coupled| 3>→|4>, their field distribution function relationship E p ≤E a <<E c ; wherein, A, B, C are preset values; 所述方法具体实现包括以下子步骤：The specific implementation of the method includes the following sub-steps: 步骤1：将里德堡原子气体囚禁在一个磁光阱里，原子气体的环境温度在纳开尔文量级，原子的质心运动和热运动带来的多普勒效应忽略不计；Step 1: The Rydberg atomic gas is trapped in a magneto-optical trap. The ambient temperature of the atomic gas is on the order of nanokelvin, and the Doppler effect caused by the motion of the center of mass and thermal motion of the atom is negligible; 步骤2：将拉比频率为B S-1的空间调制的控制光场按预设方向入射到上述气体中，频率耦合能级|3〉→|4〉的跃迁；Step 2: The spatially modulated control light field whose Rabi frequency is BS -1 is incident into the above-mentioned gas according to the preset direction, and the frequency coupling energy level |3>→|4>transitions; 步骤3：将拉比频率为A S-1的探测光场Ωp和拉比频率为C S-1的辅助光场Ωa经过聚焦和准直后在上述气体中反向传播；Step 3: The probe light field Ω p with the Rabi frequency AS -1 and the auxiliary light field Ω a with the Rabi frequency CS -1 are back-propagated in the above gas after focusing and collimating; 步骤4：将探测光场频率锁定在里德堡原子气体原子能级|1>→|3>的跃迁线上，控制光场频率调整在里德堡原子气体原子能级|2>→|3>的跃迁线附近，对探测光场施加调制频率DkHz，调制幅度FMHz的浅幅调制；其中，D、F为预设值；Step 4: Lock the detection optical field frequency on the transition line of the Rydberg atomic gas atomic energy level |1>→|3>, and control the optical field frequency to adjust to the Rydberg atomic gas atomic energy level |2>→|3> Near the transition line, apply a modulation frequency DkHz to the detection light field, and a shallow amplitude modulation of the modulation amplitude FMHz; wherein, D and F are preset values; 步骤5：整个过程中维持控制光功率不变，在里德堡原子气体原子能级|1>→|3>的跃迁线附近扫描探测光频率，检测探测光经过原子气体后的透射光强和相位，再解调即获得稳定光孤子。Step 5: Keep the control optical power unchanged during the whole process, scan the frequency of the probe light near the transition line of the atomic energy level |1>→|3> of the Rydberg atomic gas, and detect the transmitted light intensity and phase of the probe light after passing through the atomic gas , and then demodulate to obtain stable optical soliton.
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CN103399446A (en) * 2013-07-30 2013-11-20 吉林大学 All-optical wavelength converter of optical solitons on basis of weak light regulation

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