Efficient All-Optical Switching Using Slow Light within a Hollow Fiber

Phys. Rev. Lett. 102, 203902
(a) Schematic of the experimental setup. (b) Schematic detail of the fiber loading. Inside the fiber, the atoms are transversely trapped by an optical trap formed by a single beam guided by the fiber. After exiting the top end of the fiber the divergent beam creates a funnel potential guiding the atoms into the fiber core from a distance up to 100μm. The atomic cloud is moved into this region by a magnetic guide consisting of four current-carrying wires that fan out from the fiber tip. (c) Scanning electron microscope image of the fiber cross section. The diameter of the central hollow region is 7μm. (d) Transmission through the fiber loaded with 3000 atoms as a function of probe detuning from the (5S1/2,F=1)(5P1/2,F=2) transition. Red points show the absorption profile with the dipole trap on continuously. Comparison to the calculated profile based on the dipole trap parameters (solid red line) confirms that the atoms are loaded inside the fiber. Black points show the observed absorption profile when probe and dipole trap are modulated as shown in (e). Here, a homogeneous broadening is caused solely by the large optical depth of the system.(a) Schematic of the experimental setup. (b) Schematic detail of the fiber loading. Inside the fiber, the atoms are transversely trapped by an optical trap formed by a single beam guided by the fiber. After exiting the top end of the fiber the diverg... Show more

In analogy with an electronic transistor, an all-optical switch is a device in which one light beam can fully control another. Realization of efficient all-optical switches is a long-standing goal in optical science and engineering [1]. If integrated with modern fiber-optical technologies, such devices may have important applications for optical communication and computation in telecommunication networks. Optical switches operating at a fundamental limit of one photon per switching event would further enable the realization of key protocols from quantum information science [2].

Typically, interactions of light beams in nonlinear media are very weak at low light levels. Strong interactions between few-photon pulses require a combination of large optical nonlinearity, long interaction time, low photon loss, and tight confinement of the light beams. Here, we present a fiber-optical switch that makes use of an optically dense medium containing a few hundred cold atoms trapped inside the hollow core of a photonic-crystal fiber (PCF) [3] within dimensions d of a few micrometers. Near atomic resonance, the interaction probability p between a single atom and a single photon of wavelength λ, which scales as pλ2/d2, approaches a few percent. In this system, the properties of slowly propagating photons under conditions of electromagnetically induced transparency (EIT) [4–6] can be manipulated by pulses containing p-1100 photons [7–10].

(a) Four-state atomic system for nonlinear saturation based on incoherent population transfer. (b) Transmission of the probe as a function of the number of incident pump photons with exponential fit. 50% reduction of probe transmission is achieved with 300 pump photons.(a) Four-state atomic system for nonlinear saturation based on incoherent population transfer. (b) Transmission of the probe as a function of the number of incident pump photons with exponential fit. 50% reduction of probe transmission is achieved wi... Show more

Simultaneous implementation of all requirements for few-photon nonlinear optics has until now only been feasible in the context of cavity quantum electrodynamics (QED) [11–14]. However, these experiments remain technologically challenging and must compromise between cavity bandwidth, mirror transmission and atom-photon interaction strength. Consequently, large nonlinearities in these systems are accompanied by substantial input and output losses. Our alternative cavity-free approach uses propagating fields in a PCF. Hollow-core PCFs filled with molecular gas have been used for significant enhancements of efficiency in processes such as stimulated Raman scattering [15] and four-wave mixing [16], as well as observations of EIT [17]. Recently, both room-temperature and ultracold atoms have successfully been loaded into PCFs [18–21] and EIT with less than a micro-Watt control field has been reported [18,19].

Our apparatus [Fig. 1(a)] makes use of a 3 cm-long piece of single-mode hollow-core PCF vertically mounted inside an ultrahigh vacuum chamber. A laser-cooled cloud of Rb87 atoms is collected into a magneto-optical trap, focused with a magnetic guide, and loaded into the hollow core of the PCF. Once inside, the atoms are radially confined by a red-detuned dipole trap formed by a single beam guided by the fiber. The small mode diameter allows for strong transverse confinement (trapping frequencies ωt/2π50100kHz) and deep trapping potential ( 10mK) at guiding light powers of a few milliwatts.

(a) Three-level Λ-scheme used for EIT in the mesoscopic atomic medium. (b) Both probe and control field are broken into a set of 100 synchronized pulses sent through the fiber during the off-times of the dipole trap. The probe pulses have Gaussian envelopes with rms width tp150ns. (c) Probe transmission through the fiber without (black data points) and with (red data points) control field (each data point corresponds to 100 individual pulses). Solid lines are fits of Eq. (2). (d) Individual probe pulse shape and delay. The EIT pulse (red) is delayed by 100ns compared to the reference pulse (black), for control pulses containing 3500 photons. Data points represent the average number of photons detected in a 30 ns time bin. (e) Observed transmission of the probe pulses on resonance as a function of average number of photons in the 1μs control field pulse and the prediction (gray line) based on Eq. (2).(a) Three-level Λ-scheme used for EIT in the mesoscopic atomic medium. (b) Both probe and control field are broken into a set of 100 synchronized pulses sent through the fiber during the off-times of the dipole trap. The probe pulses have Gaussian e... Show more

To probe the atoms in the fiber, we monitor the transmission of a very low power ( 1pW) probe beam through the PCF [Fig. 1(a)]. The signature of atoms inside the PCF are absorption profiles associated with atomic resonance lines. If the atoms are probed inside the dipole trap, we observe a unique profile shown in Fig. 1(d). The dipole trap introduces a power dependent, radially varying ac-Stark shift, which results in broadening and frequency shift of the absorption profile [red data points in Fig. 1(d)]. Comparison with the calculated profile based on the dipole trap parameters verifies that the atoms are loaded inside the fiber. For the experiments described below, we avoid the broadening of the atomic transition by synchronous square-wave modulation of the dipole trap and the probe beam with opposite phase [Fig. 1(e)] at a rate much higher than the trapping frequency. When using this technique and scanning the probe laser over a particular hyperfine transition, we observe a typical absorption profile as shown in Fig. 1(d) (black data points). The shape of this resonance is completely determined by the natural line profile of the transition Tnat=exp(-OD/[1+4(δpΓe)2]), where Γe is the linewidth of the excited atomic state and δp=ωp-ω0 is the detuning of the probe laser from resonance. The optical depth is defined as OD=2Neff(σeg/A), where Neff is the effective number of atoms in the fiber (corresponding to all atoms localized on the fiber axis), σeg is the atomic absorption cross section for the probed transition, and A=πw02 is the beam area. Note that the optical depth for a given number of atoms inside the fiber does not depend upon the length of the atomic cloud. The measured beam waist of guided light inside the fiber is w0=1.9±0.2μm. This means that 100 atoms inside the fiber create an optically dense medium ( OD=1). The profile shown in Fig. 1(d) yields OD=30, which corresponds to 3000 atoms loaded into the fiber.

We now consider nonlinear saturation based on incoherent population transfer in our mesoscopic atomic ensemble. The transmission of the probe beam, coupled to a cycling atomic transition, |2|4, is controlled via an additional pump beam transferring atoms from an auxiliary state |1 into |2 [Fig. 2(a)]. Initially, the state |2 is not populated, and the system is transparent for the probe beam. The incident pump beam, resonant with the |1|3 transition, is fully absorbed by the optically dense atom cloud, thereby transferring atoms into the |2 state, where they then affect the propagation of the probe beam. As demonstrated in Fig. 2(b), we achieve a 50% reduction of the probe transmission with only 300 pump photons. This corresponds to 150 atoms being transferred into the |2 state, which is sufficient to cause the observed absorption of the probe beam.

(a) Four-level system for nonlinear optical switching. (b) Timing sequences for probe, control, and switch fields. (c) Probe transmission through the fiber without (red) and with (blue) the switch field present. Solid lines are fits of Eq. (2). (d) Observed transmission versus average number of switch photons per pulse. The solid gray line is the prediction based on Eq. (2). The transmission is normalized to the EIT transmission in the absence of the switch photons. (e) Truth table of the switch, showing the detected photons in the output port of the switch system as a function of presence (denoted by 1) or absence (denoted by 0) of the probe and switch pulses. Data are presented for probe pulses containing on average 2 photons and 1/e attenuation of transmission in the presence of the switch photons.(a) Four-level system for nonlinear optical switching. (b) Timing sequences for probe, control, and switch fields. (c) Probe transmission through the fiber without (red) and with (blue) the switch field present. Solid lines are fits of Eq. (2). (d) O... Show more

Next, we turn to coherent interaction between few atoms and photons in our system. First, we demonstrate EIT [4,5], where atomic coherence induced by a control beam changes the transmission of a probe beam. The essence of this phenomenon is the creation of a coupled excitation of probe photons and atomic spins (“dark-state polariton”) [22] that propagates through the atomic medium at greatly reduced group velocity [6]. We consider the three-state Λ-configuration shown in Fig. 3(a). In the absence of the control field, our medium is completely opaque at resonance [Fig. 3(c), black data points]. In contrast, when the copropagating control field is added, the atomic ensemble becomes transparent near the probe resonance [Fig. 3(c), red data points]. Figure 3(d) shows the profile of individual pulses and their transmission and delay due to reduced group velocity vg inside the atomic medium. For probe pulses with rms width tp150ns we observe a group delay td approaching 100 ns, corresponding to a reduced group velocity of vg3km/s. Remarkably, Fig. 3(e) shows that control pulses containing as few as 104 photons are sufficient to achieve almost complete transparency of the otherwise opaque system.

The sensitive nature of the quantum interference underlying EIT enables strong nonlinear coherent interaction between the dark-state polariton and additional light fields, which can be viewed as an effective photon-photon interaction [7,8,10]. An efficient nonlinear optical switch can be realized by adding to the EIT Λ-system a switch field coupling the state |2 to an excited state |4 [Fig. 4(a)] [9]. In this scheme, the switching photons interact with flipped atomic spins (state |2) within the dark-state polariton, causing a simultaneous absorption of a probe and a switch photon [23,24]. Switching is achieved when all three light fields involved (probe, control, and switching field) are overlapping within the atomic cloud [Fig. 4(b)]. In the absence of the switching field [red data in Fig. 4(c)], we observe high transmission of the probe beam on resonance due to EIT. When the switch field is turned on, this transmission is reduced. The strength of the reduction depends on the number of photons contained in the switch pulse [Fig. 4(d)]. Experimentally, we observe best switching results for switch pulses of length tstp+td. We find a 50% reduction of the initial transmission for a total number of 700 switch photons per pulse. Figure 4(e) presents the truth table of our switch, where the system acts as a logic gate for the incoming probe and switch pulses. As seen from Fig. 4(d), a contrast of over 90% between the “on” and “off” state of the switch, desirable for practical applications, can be achieved with a moderate increase of the number of switch photons.

We now analyze the nonlinear behavior of our atomic medium. When the resonant control and switching pulses are longer than the weak probe pulse, the effect of the atomic medium on such probe pulses with carrier frequency ωp is given by Eout(t)=12πdωEin(ω)×eı(OD/2)f(ω)e-ıωt, where Ein(ω) is the Fourier transform of the slowly varying envelope Ein(t) of the probe pulse, normalized such that Nin=dt|Ein(t)|2, with Nin being the number of input photons. The frequency dependent atomic response to probe light f(ω) is given by [8,9]

where Ωs,c are the Rabi frequencies of the switch and control fields. The complex detunings δij are defined as δij=δp+ıγij, with γij being the coherence decay rates between levels i, j and δp=ωp-ω13, where ω13 is the frequency of the |1|3 transition. We consider input pulses with Gaussian envelope Ein(t)e-(t2/4tp2), in which case the transmission through our atomic medium is

We fit expression (2) to observed absorption profiles such as the ones shown in Fig. 3(c) and 4(c) to extract the control and switch Rabi frequencies, optical depth, and ground state decoherence rate. We next use these parameters to compare our observed EIT and nonlinear optical switch data to the theoretical prediction in Fig. 3(e) and 4(d). In both cases, we find excellent agreement between our experimental data and the theoretical model. In the relevant case of resonant probe field, Eq. (2) can be approximated by

Here, Ns is the number of switch photons and μs,p are switch and probe transition dipole matrix elements, respectively. Furthermore, we have assumed ΩsΩc, γ12=0, γ13γ24 and used td=L/vg=ODγ13|Ωc|2, with L being the length of the medium. For the investigated case of a relatively weak probe transition and resulting OD3, the delay time is small ( tdtp) and the probe pulse is never fully stored inside the medium. If the OD is increased, tdtp and the whole probe pulse is contained inside the medium as a dark-state polariton in mostly atomic form. Then, a switch photon number NsAλ2 causes 1/e attenuation of the probe pulse. This ideal limit can be easily understood. In the case of a single slow probe photon, the polariton contains only a single atomic spin. Consequently, absorption of a single switch photon, which occurs with probability pλ2A, is required to destroy this coherent atomic excitation.

Our experimental demonstrations introduce a novel physical system that opens up unique prospects in quantum and nonlinear optics. Our system can be used to implement efficient photon counting [25,26] by combining photon storage with spin-flipped atom interrogation via a cycling transition. Further improvements in nonlinear optical efficiency are possible by either simultaneously slowing down a pair of pulses to enable long interaction time [27] or using stationary-pulse techniques [28,29]. In the former case, the threshold number of switch photons would be reduced to Ns1ODAλ2 [27], while in the latter case the probability of interaction between two single photons scales as ODλ2A [29]. Thus, with a relatively modest improvement of atom loading resulting in optical depth OD>100, achieving nonlinear interaction of two guided photons appears within reach. Finally, the present demonstration opens up the possibility to create strongly interacting many-body photon states [30], which may give new insights into the physics of nonequilibrium strongly correlated systems.


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About the Authors

Image of M. Bajcsy
Image of S. Hofferberth
Image of V. Balic
Image of T. Peyronel
Image of M. Hafezi
Image of A. S. Zibrov
Image of V. Vuletic
Image of M. D. Lukin

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