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Spatial Multiplexing of Squeezed Light by Coherence Diffusion

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Spatial Multiplexing of Squeezed Light by Coherence Diffusion Spatial multiplexing of squeezed light by coherence diffusion Jian Sun,1 Weizhi Qu,1 Eugeniy Mikhailov,2 Irina Novikova,2 Heng Shen,3, ∗ and Yanhong Xiao1, y 1Department of Physics, State Key Laboratory of Surface Physics and Key Laboratory of Micro and Nano- Photonic Structures (Ministry of Education), Fudan University, Shanghai 200433, China 2Department of Physics, College of William and Mary, Williamsburg, Virginia 23185, USA 3Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, UK Spatially splitting nonclassical light beams is in principle prohibited due to noise contamination during beam splitting. We propose a platform based on thermal motion of atoms to realize spatial multiplexing of squeezed light. Light channels of separate spatial modes in an anti-relaxation coated vapor cell share the same long-lived atomic coherence jointly created by all channels through the coherent diffusion of atoms which in turn enhances individual channel's nonlinear process responsible for light squeezing. Consequently, it behaves as squeezed light in one optical channel transferring to other distant channels even with laser powers below the threshold for squeezed light generation. An array of squeezed light beams was created with low laser power ∼ mW. This approach holds great promise for applications in multi-node quantum network and quantum enhanced technologies such as quantum imaging and sensing. Spatially splitting a beam of classical light is a rou- quantum properties of the optical fields. tine process to distribute the light energy in optics, and For light squeezing, we consider a double-Λ scheme can be conveniently done by a beam splitter made of typically used for squeezed light and photon-pair gener- glass or crystal. However, such an operation for a quan- ation in atom ensembles [12, 13] in absence of an op- tum state of light is nontrivial since a conventional beam tical cavity thanks to the atomic coherence which has splitter introduces noise contamination from the vacuum, been proved to enhance nonlinear interactions [14] and destroying the quantum property of the light. As a con- reduce laser power requirements. In our system we take sequence, when spatially separated multiple nonclassical advantage of the long-lived spin coherence created be- sources are needed, such as in multi-node quantum net- tween Zeeman sublevels, which is known to enhance the works [1, 2], and studies of multi-partite entanglement nonlinear magneto-optical rotation and polarization self- for continuous variables [3{6], one has to duplicate sev- rotation effects (PSR) [15]. The latter can be used to eral setups, each including a parametric nonlinear crystal generate squeezed vacuum in an orthogonal polarization and a cavity to generate one beam of squeezed light or if the linearly polarized light propagates through the PSR one photon pair. How to scalably produce an array of medium [16], due to the enhanced cross-phase modula- nonclassical light beams therefore becomes a question of tion between the left and right circularly polarized com- great interest to both fundamental studies of quantum ponents of the x-polarized laser field, interacting with the optics and applications in quantum communications and optical transitions j1i ! j3; 4i and j2i ! j3; 4i as shown quantum imaging with high spatial resolution [7{9]. in Figure 1(b). Alternatively, such interaction can be de- In this paper, we propose a scheme and report scribed as a degenerate four-wave-mixing (FWM) process the proof-of-principle experiment to spatially multiplex where the driving laser serves as the pump twice in the squeezed light using fast moving atoms. The essence is FWM cycle, generating a pair of degenerate y-polarized to employ the transport of long-lived atomic coherence photons, as shown in the energy diagram redrawn in within an anti-relaxation coated vapor cell, combined the linear atomic basis. These quantum correlated y- with coherence-enhanced nonlinear atom-light interac- polarized photon pairs can be treated as a quadrature- tion. Multiple spatially separated laser beams (channels) squeezed y-polarized vacuum, whereas the whole light are shined into the cell, and serve as the mutual optical field is in a polarization squeezed state [16{20]. arXiv:1811.11647v3 [quant-ph] 20 Dec 2018 pumping or state preparation for each other to create the In our proposal, two (or more) illuminated interac- atomic coherence, and further leads to the generation of tion regions, named optical channels, and the dark re- squeezing in all optical channels. A striking phenomenon gion outside of the laser beams in the cell are considered is the observation of squeezing in an optical channel with (Figure 1(a)), with each channel undergoing the above the laser power below the squeezing threshold when a double-Λ process [21]. The spin dynamics of the moving distant beam is introduced. Previously, such coherence atoms can be described by a set of coupled differential transport has been used to demonstrate anti-parity-time equations taking into account the atomic coherence ex- symmetric optics [10] and a slow light beamsplitter [11] change between different regions, as well as the Langevin for classical light, with however no evolvement of the noise operators. The effective coherence exchange be- tween the optical channels is driven by the slow evolution of the ground state spin of atoms in the dark region, and the optical coherence transfer between channels is negli- 87 ∗Electronic address: [email protected] gible as it decays within 20 ns (for Rb). Since FWM yElectronic address: [email protected] within either channel typically has a faster cycle than 2 (a) (b) (a) HWP PBS B field QWP HWP HWP BPD Cell BPD (b) FIG. 2: Proof-of-principle two-channel squeezed light result. |4 |4 > Δ > Δ Measured minimal-quadrature noise spectra for both channels |3> δ |3> δ with the other channel on or off, obtained by a spectrum analyzer. The input laser powers for Ch1 and Ch2 before the g -g 1 1 cell are 4.5 mW and 11 mW, respectively. The laser frequency g2 g2 ay ay 87 0 Ωx Ωx is 348 MHz blue-detuned from Rb D1 line F = 2 to F = 2 transition. The noise power is normalized to the shot noise |1> |2> |x> |y> level; the spectrum analyzer is set to the resolution bandwidth (RBW) 10 kHz, video bandwidth (VBW) = 10 Hz, each trace FIG. 1: Schematics for spatial multiplexing of squeezed light. is averaged 200 times. (a) Experiment schematics. Two spatially separated optical channels (Ch1 and Ch2), formed by x-polarized laser beams propagating along z, interact with Rb atoms inside an anti- relaxation coated vapor cell, and then have their quantum fore the cell to ensure the same polarization of all beams. fluctuations individually analyzed by balanced photodetec- All laser beams are slightly focused via a 1-meter-focal- tors (BPD) in a homodyne configuration. PBS: polariza- length lens before the cell. The linearly polarized input tion beam splitter; HWP: Half-wave plate; QWP: Quarter- laser also played the role of the local oscillator (LO) at wave plate, used a phase retarder here to rotate the quan- the output for quantum noise measurements of squeez- tum noise ellipse. (b) The double-Λ four-level interaction ing [22{24]. schemes. A x-polarized driving laser is near resonant with the 0 Since the average time between atom-wall collisions is 5S1=2;F = 2 ! 5P1=2;F = 1; 2 transition. In the circular basis (left diagram), the driving laser is treated as a superpo- about 100 µs and the transit time through the light beam sition of the left- and right-circularly polarized components, with diameter of 1.5 mm is ∼ 5 µs, the long-lived ground driving the dipole transitions between the Zeeman sublevels state atomic spin (coherence lifetime about 30 ms) can of the ground state and both excited states: j1i ! j3; 4i (with thus endure nearly a thousand wall collisions [25], which the single photon Rabi frequencies g1, g2 ) and j2i ! j3; 4i establishes within the entire cell a steady state distribu- (with Rabi frequencies g2, −g1) correspondingly. The energy tion of coherence and population attributed to optical levels can be redrawn in the linear atomic basis (right dia- pumping by all the optical channels [26, 27]. It is then gram) with jxi = p1 (j1i + j2i) and jyi = p1 (j1i − j2i) to 2 2 expected that turning on one channel can enhance coher- highlight the FWM description of the PSR. The x polariza- ence within the entire cell hence light squeezing in an- tion drives jxi ! j3i and jyi ! j4i, whereas the y polarization other channel due to effectively increased average optical drives jxi ! j4i and jyi ! j3i, as determined by the Clebsch- pumping rate, which was verified by Figure 2. In contrast Gordan coefficients of 87Rb. The detuning of laser light from the j1i ! j3i transition is denoted as δ, and the hyperfine to the nearly shot-noise-limited (SNL) output from Ch1 splitting between the two excited states is ∆ = 814.5 MHz. (∼ 4.5 mW input power) in absence of Ch2, squeezed light is observed below ∼ 100 kHz when switching on Ch2 (∼ 11 mW input power), with 0.45 dB squeezing the slow spin dynamics, as implied by the much broader detected at 40 kHz. Similarly, as shown, the minimal noise spectrum of squeezing, FWM in all channels es- noise for Ch2 is also reduced upon turning on Ch1. sentially sees and is boosted by the same collective spin To fully characterize such noise reduction by a remote state, causing the simultaneous quantum noise reduction laser beam, we investigate the dependence of quantum or light squeezing in all channels. noise on the laser detuning and laser power.
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