CN112051696A - Miniaturized compression source generating device - Google Patents
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- CN112051696A CN112051696A CN202010851959.1A CN202010851959A CN112051696A CN 112051696 A CN112051696 A CN 112051696A CN 202010851959 A CN202010851959 A CN 202010851959A CN 112051696 A CN112051696 A CN 112051696A
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Abstract
本发明涉及一种小型化压缩源产生装置,属于连续变量非经典光场产生设备技术领域,包括激光源、光隔离器件、光学谐振腔和光反射器件;所述激光源输出的激光经光隔离器件后,入射到光学谐振腔内,在光学谐振腔内发生参量上转换后,产生的倍频光从光学谐振腔内输出后,经光反射器件反射后沿原路返回光学谐振腔,并作为泵浦光在光学谐振腔内与非线性晶体发生参量下转换,产生的基频压缩光从光学谐振腔射出后,返回光隔离器件,并经光隔离器件输出。本发明装置在小功率激光注入下,无需额外倍频腔,仅通过单个光学腔实现了高质量的压缩态光场的产生,结构紧凑,易于调节,实用性强,易于产品化和批量化生产,可以应用于量子精密测量、生物测量以及量子成像等前沿领域。
The invention relates to a miniaturized compressed source generating device, belonging to the technical field of continuous variable non-classical light field generating equipment, comprising a laser source, an optical isolation device, an optical resonant cavity and an optical reflection device; the laser output from the laser source passes through the optical isolation device Then, it is incident into the optical resonator, and after the parametric up-conversion occurs in the optical resonator, the generated frequency-doubling light is output from the optical resonator, reflected by the light reflection device, and returns to the optical resonator along the original path, and acts as a pump. The Pu light is parametrically down-converted with the nonlinear crystal in the optical resonator, and the generated fundamental frequency compressed light is emitted from the optical resonator, returns to the optical isolation device, and is output through the optical isolation device. The device of the present invention realizes the generation of high-quality compressed state optical field only through a single optical cavity without additional frequency doubling cavity under low-power laser injection, compact structure, easy adjustment, strong practicability, and easy productization and mass production , which can be applied to cutting-edge fields such as quantum precision measurement, biological measurement and quantum imaging.
Description
技术领域technical field
本发明属于连续变量非经典光场产生技术领域,具体是一种结构紧凑,实用性强的小型化压缩源产生装置。The invention belongs to the technical field of continuous variable non-classical light field generation, in particular to a miniaturized compression source generation device with compact structure and strong practicability.
背景技术Background technique
连续变量压缩态光场是一种重要的非经典光场,可将光场的某一可观测物理量的量子起伏降低至标准量子极限以下,它的产生一直以来是连续变量量子信息领域最基础和最热点的的研究内容之一,被广泛应用于引力波探测、光学精密测量、量子信息科学等众多研究领域。The continuous variable squeezed state light field is an important non-classical light field, which can reduce the quantum fluctuation of an observable physical quantity of the light field to below the standard quantum limit. One of the hottest research contents, it is widely used in many research fields such as gravitational wave detection, optical precision measurement, and quantum information science.
目前,参量下转换是压缩光最有效的产生方式,基于这种方式可以获得高质量压缩光,但是此方法需要倍频腔产生倍频光,通过倍频光泵浦光学参量振荡器,以获得压缩态光场。由于倍频腔的加入,需要额外的腔长、相位等锁定装置庞大,此系统结构较为复杂;利用参量上转换也可以获得压缩态光场,其优点在于可以获得较短波长光束的压缩态,装置简单有利于实际应用,但是其缺点在于所获得的压缩光的压缩度不高,无法满足实际需要。At present, parametric down-conversion is the most effective way to generate compressed light, and high-quality compressed light can be obtained based on this method, but this method requires a frequency-doubling cavity to generate frequency-doubling light, and pumping an optical parametric oscillator through the frequency-doubling light to obtain Squeezed light field. Due to the addition of the frequency doubling cavity, additional locking devices such as cavity length and phase are required, and the structure of the system is relatively complex; the compressed state light field can also be obtained by using parametric up-conversion. The advantage is that the compressed state of the shorter wavelength beam can be obtained, The simplicity of the device is beneficial to practical application, but the disadvantage is that the compression degree of the obtained compressed light is not high, which cannot meet the actual needs.
发明内容SUMMARY OF THE INVENTION
本发明克服现有技术存在的不足,所要解决的技术问题为:提供一种小型化压缩源产生装置,在小功率激光注入下,无需额外倍频腔,通过单个光学腔产生高质量的压缩态光场。The invention overcomes the shortcomings of the prior art, and the technical problem to be solved is: to provide a miniaturized compressed source generating device, which can generate a high-quality compressed state through a single optical cavity without an additional frequency-doubling cavity under the injection of a low-power laser. light field.
为了解决上述技术问题,本发明采用的技术方案为:一种小型化压缩源产生装置,包括激光源、光隔离器件、光学谐振腔和光反射器件;所述激光源输出的激光经光隔离器件后,入射到光学谐振腔内,在光学谐振腔内发生参量上转换后,产生的倍频光从光学谐振腔内输出后,经光反射器件反射后沿原路返回光学谐振腔,并作为泵浦光在光学谐振腔内与非线性晶体发生参量下转换,产生的基频压缩光从光学谐振腔射出后,返回光隔离器件,并经光隔离器件输出。In order to solve the above technical problems, the technical scheme adopted in the present invention is: a miniaturized compressed source generating device, including a laser source, an optical isolation device, an optical resonant cavity and a light reflection device; , incident into the optical resonator, after the parametric up-conversion occurs in the optical resonator, the generated frequency-doubled light is output from the optical resonator, reflected by the light reflective device, and then returned to the optical resonator along the original path, and used as a pump The light is parametrically down-converted with the nonlinear crystal in the optical resonator, and the generated fundamental frequency compressed light is emitted from the optical resonator, returns to the optical isolation device, and is output through the optical isolation device.
所述光隔离器件为光学隔离器或者为光纤环路器。The optical isolation device is an optical isolator or an optical fiber circulator.
所述光学谐振腔包括非线性晶体和组成四镜环形腔的第一腔镜、第二腔镜、第三腔镜和第四腔镜,所述第一腔镜和第二腔镜为平凹镜,第三腔镜和第四腔镜为平面腔镜,所述第一腔镜为输入输出耦合镜,其外端面镀有基频光和倍频光双增透膜,内端面可使基频光和倍频光透过。The optical resonant cavity includes a nonlinear crystal and a first cavity mirror, a second cavity mirror, a third cavity mirror and a fourth cavity mirror that form a four-mirror ring cavity, and the first cavity mirror and the second cavity mirror are plano-concave mirror, the third cavity mirror and the fourth cavity mirror are plane cavity mirrors, the first cavity mirror is an input and output coupling mirror, and its outer end surface is coated with double antireflection coatings for fundamental frequency light and frequency-doubling light, and the inner end surface can Frequency light and frequency doubled light are transmitted.
所述第二腔镜、第三腔镜和第四腔镜对基频光和倍频光的反射率大于99.9%,所述非线性晶体镀的两端面均镀有基频光和倍频光双波段减反膜。The reflectivity of the second cavity mirror, the third cavity mirror and the fourth cavity mirror to the fundamental frequency light and the frequency doubled light is greater than 99.9%, and both ends of the nonlinear crystal are coated with the fundamental frequency light and the frequency doubled light. Dual-band anti-reflection coating.
所述第一腔镜的内端面对基频光的透过率为10%,对倍频光的透过率为20%。The transmittance of the inner end of the first cavity mirror to the fundamental frequency light is 10%, and the transmittance to the frequency doubled light is 20%.
所述光学谐振腔的其中一面腔镜上固定设置在第一压电陶瓷上,所述第一压电陶瓷用于调节光学谐振腔的腔长。One of the cavity mirrors of the optical resonant cavity is fixedly arranged on the first piezoelectric ceramic, and the first piezoelectric ceramic is used to adjust the cavity length of the optical resonant cavity.
所述光反射器件包括双色镜,基频光反射镜和倍频光反射镜,且所述倍频光反射镜固定设置在第二压电陶瓷上,从所述光学谐振腔输出的基频光和倍频光经双色镜后分开,分开后的基频光和倍频光分别经基频光反射镜和倍频光反射镜反射后返回双色镜,再经双色镜原路后返回光学谐振腔。The light reflecting device includes a dichroic mirror, a fundamental frequency light reflecting mirror and a frequency-doubling light reflecting mirror, and the frequency-doubling light reflecting mirror is fixedly arranged on the second piezoelectric ceramic, and the fundamental frequency light output from the optical resonant cavity The frequency-doubling light and the frequency-doubling light are separated by the dichroic mirror, and the separated base-frequency light and frequency-doubling light are reflected by the base-frequency light mirror and the frequency-doubling light mirror, respectively, and then return to the dichroic mirror, and then return to the optical resonator through the original path of the dichroic mirror. .
所述双色镜靠近光学谐振腔的一面对倍频光增透,基频光高反,另一面对倍频光增透。One side of the dichroic mirror close to the optical resonant cavity is anti-reflection for the frequency-doubling light, the fundamental frequency light is highly reflected, and the other side is anti-reflection for the frequency-doubling light.
所述双色镜靠近光学谐振腔的一面对倍频光的透射率大于97%,基频光反射率大于99.9%,另一面对倍频光反射率小于0.5%。The transmittance of the frequency-doubling light on one side of the dichroic mirror close to the optical resonant cavity is greater than 97%, the reflectivity of the fundamental frequency light is greater than 99.9%, and the reflectivity of the other side of the frequency-doubling light is less than 0.5%.
激光源、光隔离器件、光学谐振腔和光反射器件固定在一个方便移动的光学隔振平台上。The laser source, optical isolation device, optical resonator and optical reflection device are fixed on a convenient moving optical vibration isolation platform.
本发明与现有技术相比具有以下有益效果:本发明通过对参量上转换产生的倍频光的反馈,在单个光学谐振腔内同时实现参量上转换和参量下转换,只需要注入小功率的基频光,即可以获得压缩度高的压缩光,因此本发明提供一种小型化压缩源产生装置,在小功率激光注入下,无需额外倍频腔,通过单个光学腔产生高质量的压缩态光场。实验证实,注入25mW的基频光,可以获得5dB的真空压缩光;而且本装置无需锁定泵浦光和种子光的相对相位,仅需锁定光学谐振腔的腔长,锁定装置简洁,实验系统易于调节,操作简便。结构紧凑,易于调节,实用性强,易于产品化和批量化生产,可以应用于量子精密测量、生物测量以及量子成像等前沿领域。Compared with the prior art, the present invention has the following beneficial effects: the present invention realizes parametric up-conversion and parametric down-conversion simultaneously in a single optical resonant cavity by feeding back the frequency-doubling light generated by parametric up-conversion, and only needs to inject low-power The fundamental frequency light can obtain the compressed light with high compression degree. Therefore, the present invention provides a miniaturized compressed source generating device, which can generate high-quality compressed state through a single optical cavity without additional frequency doubling cavity under low-power laser injection. light field. Experiments have confirmed that 5dB vacuum compression light can be obtained by injecting 25mW of fundamental frequency light. Moreover, the device does not need to lock the relative phases of the pump light and the seed light, but only needs to lock the cavity length of the optical resonator. The locking device is simple and the experimental system is easy to use. Adjustable and easy to operate. The compact structure, easy adjustment, strong practicability, easy productization and mass production, can be applied to frontier fields such as quantum precision measurement, biological measurement and quantum imaging.
附图说明Description of drawings
图1是本发明实施例提供的一种小型化压缩源产生装置的原理框图;Fig. 1 is the principle block diagram of a kind of miniaturized compressed source generation device provided by the embodiment of the present invention;
图2是本发明实施例提供的一种小型化压缩源产生装置的光路示意图;2 is a schematic diagram of an optical path of a miniaturized compressed source generating device provided by an embodiment of the present invention;
图3是本发明产生的在分析频率为0-10MHz范围内压缩态光场的测量结果图;Fig. 3 is the measurement result graph of the compressed state light field in the range of 0-10MHz that the analysis frequency that the present invention produces;
图4是本发明实施例产生的压缩光在分析频率为2MHz处压缩态光场的测量结果图;Fig. 4 is the measurement result graph of the compressed state light field of the compressed light generated in the embodiment of the present invention at the analysis frequency of 2MHz;
1—激光源, 2—光隔离器件, 3—光学谐振腔, 4—光反射器件,5—平台,6—第一偏振分束棱镜,7—法拉第旋光器,8—第二偏振分束棱镜,9—第一腔镜,10—第二腔镜,11—第三腔镜,12—第四腔镜,13—基频光,14—倍频光,15—双色镜,16—基频光高反镜,17—倍频光高反镜,18—压缩光。1—laser source, 2—optical isolation device, 3—optical resonant cavity, 4—light reflection device, 5—platform, 6—first polarization beam splitter prism, 7—Faraday rotator, 8—second polarization beam splitter prism , 9—first cavity mirror, 10—second cavity mirror, 11—third cavity mirror, 12—fourth cavity mirror, 13—fundamental frequency light, 14—frequency doubled light, 15—dichroic mirror, 16—fundamental frequency Light high mirror, 17 - frequency doubled light high mirror, 18 - compressed light.
具体实施方式Detailed ways
为使本发明实施例的目的、技术方案和优点更加清楚,下面将对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本发明的一部分实施例,而不是全部的实施例;基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。In order to make the purposes, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below. Obviously, the described embodiments are part of the embodiments of the present invention, not All the embodiments; based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative work, all belong to the protection scope of the present invention.
如图1所示,本发明实施例提供了一种小型化压缩源产生装置,包括:激光源1、光隔离器件2、光学谐振腔3和光反射器件4,所述激光器1输出激光;所述光隔离器件2用于将光学谐振腔产生的压缩光输出;所述光学谐振腔3用于产生压缩态光场;所述光反射器件4将基频光13和倍频光14反射进入所述光学谐振腔3,产生压缩态光场。为了使得系统能够稳定输出压缩光且适用于多种应用场景,将以上的各部分元件固定在一个方便移动的小型隔振平台5上。As shown in FIG. 1, an embodiment of the present invention provides a miniaturized compressed source generating device, including: a laser source 1, an optical isolation device 2, an
本实施例中,所述激光源1输出的激光经光隔离器件2后,入射到光学谐振腔3内,在光学谐振腔3内发生参量上转换后,产生的倍频光从光学谐振腔3内输出后,经光反射器件4反射后沿原路返回光学谐振腔3,并作为泵浦光在光学谐振腔3内与非线性晶体发生参量下转换,产生的基频压缩光从光学谐振腔3射出后,返回光隔离器件2,并经光隔离器件2输出。In this embodiment, the laser output from the laser source 1 is incident into the
如图2所示,为本发明实施例提供的一种小型化压缩源产生装置的光路示意图,具体地,本实施例中,所述光学谐振腔3包括非线性晶体和组成四镜环形腔的第一腔镜9、第二腔镜10、第三腔镜11和第四腔镜12,所述第一腔镜9和第二腔镜10为平凹镜,第三腔镜11和第四腔镜12为平面腔镜,所述第一腔镜9为输入输出耦合镜,其外端面镀有基频光和倍频光双增透膜,内端面可使基频光和倍频光透过。具体地,所述第一腔镜9的内端面对基频光的透过率为10%,对倍频光的透过率为20%。此外,第一腔镜9的内端面对基频光和倍频光的透过率也可以根据需要进行设置,只需要具有透过率即可。所述第二腔镜10、第三腔镜11和第四腔镜12对基频光和倍频光的反射率大于99.9%。光学谐振腔3内的非线性晶体为尺寸为1*2*10mm的PPKTP晶体,晶体的两面均镀有基频光和倍频光减反膜,PPKTP晶体的温度由商用控温仪控制在相位匹配点,控温精度为0.01摄氏度。As shown in FIG. 2 , it is a schematic diagram of an optical path of a miniaturized compression source generating device provided in an embodiment of the present invention. Specifically, in this embodiment, the optical
所述光学谐振腔3的其中一面腔镜上固定设置在第一压电陶瓷上,所述第一压电陶瓷用于对光学谐振腔3的腔长进行主动控制,即锁定光学谐振腔3的腔长。如图2所示,本实施例中,所述光隔离器件2为两个偏振分束棱镜和一个法拉第旋光器的组合而成的光学隔离器,此外,光隔离器件2也可以为光纤环路器。One of the cavity mirrors of the
进一步地,如图2所示,所述光反射器件4包括双色镜15,基频光反射镜16和倍频光反射镜17,且所述倍频光反射镜17固定设置在第二压电陶瓷上,从所述光学谐振腔3输出的基频光和倍频光经双色镜15后分开,分开后的基频光和倍频光分别经基频光反射镜16和倍频光反射镜17反射后返回双色镜15,再经双色镜15原路后返回光学谐振腔3。所述双色镜15靠近光学谐振腔3的一面对倍频光增透,基频光高反,另一面对倍频光增透。所述双色镜15靠近光学谐振腔3的一面对倍频光的透射率大于97%,基频光反射率大于99.9%,另一面对倍频光反射率小于0.5%。通过第二压电陶瓷,可以扫描泵浦光与种子光间的相对相位,即倍频光与基频压缩光间的相对相位,通过扫描相位,可以监视经典增益。Further, as shown in FIG. 2 , the light reflecting device 4 includes a
本实施例中,由所述激光源1出射的1080nm基频光经过所述光隔离器件2后,注入到所述光学谐振腔3内,通过标准PDH 稳频技术锁定所述光学谐振腔3的腔长后,所述光学谐振腔3稳定输出540nm倍频光14,第一腔镜9反射的基频光13和所述光学谐振腔3输出的倍频光14经过双色镜15分开,分别由基频光高反镜16和倍频光高反镜17反射后,返回并经过双色镜15后进入所述光学谐振腔3产生压缩光18,产生的压缩光18经第一腔镜9输出后,返回光隔离器件,并由所述光隔离器件2输出,使用平衡零拍探测装置可以对压缩光进行探测。In this embodiment, the 1080 nm fundamental frequency light emitted from the laser source 1 passes through the optical isolation device 2 and is injected into the
如图2所示,为本发明实施例提供的一种小型化压缩源产生装置的光路示意图:由所述激光器1出射的1080nm基频光经过所述光隔离器2(本实施例中所使用的光隔离器为偏振分束棱镜和法拉第旋光器的组合)后,注入到所述光学谐振腔3内,通过标准PDH 稳频技术锁定所述光学谐振腔3的腔长后,所述光学谐振腔3稳定输出540nm倍频光14,作为输入输出镜的第一腔镜9反射的基频光13和所述光学谐振腔3输出的倍频光14经过双色镜15分开,分别由第一高反镜16和第二高反镜17反射,进入所述光学谐振腔3产生压缩光18,产生的压缩光18由所述光隔离器2输出,使用平衡零拍探测装置进行探测。As shown in FIG. 2, it is a schematic diagram of the optical path of a miniaturized compression source generating device provided by an embodiment of the present invention: the 1080 nm fundamental frequency light emitted by the laser 1 passes through the optical isolator 2 (used in this embodiment) The optical isolator is a combination of a polarizing beam splitter prism and a Faraday rotator), injected into the
如图3所示,为本发明实施例中产生的真空压缩态光场的测量结果,此时光学谐振腔腔前注入功率为25mW,扫描频率为0-10MHz。其中,(a)为反压缩,(b)为散粒噪声基准,(c)为压缩,(d)电子学噪声,结果表明在0-10MHz范围内我们均制备得到了压缩光。As shown in FIG. 3 , which is the measurement result of the vacuum compressed state optical field generated in the embodiment of the present invention, the injection power in front of the optical resonator cavity is 25 mW, and the scanning frequency is 0-10 MHz. Among them, (a) is the inverse compression, (b) is the shot noise benchmark, (c) is the compression, and (d) is the electronic noise. The results show that we can prepare the compressed light in the range of 0-10MHz.
如图4所示,为本发明实施例中产生的真空压缩态光场的测量结果,此时光学谐振腔的注入功率为25mW,测量的分析频率为2MHz。其中,(a)表示散粒噪声基准,(b)表示压缩光随本地光相位变化的噪声功率曲线,结果表明压缩态光场的压缩度为5dB。本发明设计的小型化压缩源在低注入功率的情况下获得了稳定的压缩光的输出。As shown in FIG. 4 , it is the measurement result of the vacuum compressed state optical field generated in the embodiment of the present invention. At this time, the injection power of the optical resonator is 25 mW, and the measured analysis frequency is 2 MHz. Among them, (a) represents the shot noise reference, and (b) represents the noise power curve of the compressed light with the local optical phase. The results show that the compression degree of the compressed light field is 5dB. The miniaturized compression source designed by the present invention obtains a stable output of compressed light under the condition of low injection power.
本发明通过将光学谐振腔输出的倍频光反射回光学谐振腔参与参量下转换,使用单个光学谐振腔便实现了以往两个光学谐振腔才能实现的结果,该装置的获得缩小了压缩源的体积,有助于将压缩态光场广泛应用于现实生活的方方面面。In the present invention, the frequency-doubling light output by the optical resonator is reflected back to the optical resonator to participate in the parametric down-conversion, and a single optical resonator is used to achieve the results that could only be achieved by two optical resonators in the past. volume, which helps to apply squeezed-state light fields to all aspects of real life.
需要加以说明的是,可以在上述实施例的基础上采用包括但不限于波长为1550nm,1342nm,1064nm和795nm的激光器作为激光源来实施本发明。It should be noted that, on the basis of the above-mentioned embodiments, the present invention can be implemented by adopting, but not limited to, lasers with wavelengths of 1550 nm, 1342 nm, 1064 nm and 795 nm as laser light sources.
最后应说明的是:以上各实施例仅用以说明本发明的技术方案,而非对其限制;尽管参照前述各实施例对本发明进行了详细的说明,本领域的普通技术人员应当理解:其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分或者全部技术特征进行等同替换;而这些修改或者替换,并不使相应技术方案的本质脱离本发明各实施例技术方案的范围。Finally, it should be noted that the above embodiments are only used to illustrate the technical solutions of the present invention, but not to limit them; although the present invention has been described in detail with reference to the foregoing embodiments, those of ordinary skill in the art should understand that: The technical solutions described in the foregoing embodiments can still be modified, or some or all of the technical features thereof can be equivalently replaced; and these modifications or replacements do not make the essence of the corresponding technical solutions deviate from the technical solutions of the embodiments of the present invention. scope.
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN114361922A (en) * | 2021-12-17 | 2022-04-15 | 济南量子技术研究院 | All-fiber bright compressed light source based on optical parameter down-conversion |
CN115683365A (en) * | 2022-12-28 | 2023-02-03 | 安徽鲲腾量子科技有限公司 | Tunable quantum beat frequency interference device based on quantum frequency up-conversion |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105867046A (en) * | 2016-06-02 | 2016-08-17 | 山西大学 | Device and method for generating photo-communication waveband continuous variable quantum entanglement source |
CN107561819A (en) * | 2017-09-04 | 2018-01-09 | 山西大学 | A kind of squeezed vacuum state light field generating means and method |
CN109632128A (en) * | 2018-12-07 | 2019-04-16 | 山西大学 | A kind of device and method measuring optics cavity double resonance temperature condition |
CN110068978A (en) * | 2019-04-30 | 2019-07-30 | 山西大学 | A kind of self-compensating non-classical optical state generator of phase |
CN111474802A (en) * | 2020-05-09 | 2020-07-31 | 山西大学 | Device for simultaneously generating compressed-state light field and entangled-state light field |
-
2020
- 2020-08-21 CN CN202010851959.1A patent/CN112051696B/en active Active
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105867046A (en) * | 2016-06-02 | 2016-08-17 | 山西大学 | Device and method for generating photo-communication waveband continuous variable quantum entanglement source |
CN107561819A (en) * | 2017-09-04 | 2018-01-09 | 山西大学 | A kind of squeezed vacuum state light field generating means and method |
CN109632128A (en) * | 2018-12-07 | 2019-04-16 | 山西大学 | A kind of device and method measuring optics cavity double resonance temperature condition |
CN110068978A (en) * | 2019-04-30 | 2019-07-30 | 山西大学 | A kind of self-compensating non-classical optical state generator of phase |
CN111474802A (en) * | 2020-05-09 | 2020-07-31 | 山西大学 | Device for simultaneously generating compressed-state light field and entangled-state light field |
Non-Patent Citations (2)
Title |
---|
KUI LIU ETC.: "High-fidelity heralded quantum squeezing gate based on entanglement", 《OPTICS EXPRESS》 * |
何亚亚等: "795nm真空压缩的实验产生及猫态模拟", 《量子光学学报》 * |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN114361922A (en) * | 2021-12-17 | 2022-04-15 | 济南量子技术研究院 | All-fiber bright compressed light source based on optical parameter down-conversion |
CN115683365A (en) * | 2022-12-28 | 2023-02-03 | 安徽鲲腾量子科技有限公司 | Tunable quantum beat frequency interference device based on quantum frequency up-conversion |
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