Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:1606.00562 · Physical Review A

Creation of two-photon states via interactions between Rydberg atoms during light storage

Julius Ruseckas, Ite A. Yu, Gediminas Juzeliūnas

Published Feb 3, 2017• 13 citations
arXivHTMLPDF

Abstract

A scheme for photon pair generation based on the storage and retrieval of slow light in an atomic medium is proposed. The second-order correlation function, determined by the atom-atom interaction and the storage time, is shown to be a sensitive optical tool for probing the atomic interaction potential.
DOI
10.1103/physreva.95.023807

Related papers

Engineering two-photon states via interaction between Rydberg atoms during the light storage

Julius Ruseckas, Ite A. Yu, Gediminas Juzeliūnas

We propose a new method to create two-photon states in a controllable way using interaction between the Rydberg atoms during the storage and retrieval of slow light. A distinctive feature of the suggested procedure is that the slow light is stored into a superposition of two atomic coherences under conditions of electromagnetically induced transparency (EIT). Interaction between the atoms during the storage period creates entangled pairs of atoms in a superposition state that is orthogonal to the initially stored state. Restoring the slow light from this new atomic state one can produce a two photon state with a second-order correlation function determined by the atom-atom interaction and the storage time. Therefore the measurement of the restored light allows one to probe the atom-atom coupling by optical means with a sensitivity that can be increased by extending the storage time. As a realization of this idea we consider a many-body Ramsey-type technique which involves pi/2 pulses creating a superposition of Rydberg states at the beginning and the end of the storage period. In that case the regenerated light is due to the resonance dipole-dipole interaction between the atoms in the Rydberg states.

•Jun 2, 2016•0 citations

Storage of a Single Photon in a Highly Non-Linear Medium Based on Rydberg Atoms

Auxiliadora Padrón-Brito, Pau Farrera, Emanuele Distante +3 more

Photons are very good candidates to carry quantum information due to their negligible interactions. However, photon-photon interactions are needed to process photonic quantum information. This is very useful for quantum repeater applications [1], in which the success probability of entanglement swapping can be highly increased if the Bell-state measurement is performed deterministically. In the case of photons, it requires mapping them in a non-linear medium at the single-photon level. This strong non-linearity has been demonstrated by using Rydberg atoms, which are atoms excited to states with a high principal quantum number. However, previous experiments with Rydberg atoms have been implemented with weak coherent input states of light [2, 3]. Hence, the mapping of true single photons to a medium with strong single-photon non-linearity is, so far, an outstanding goal. In this work, we have demonstrated the storage and retrieval of a paired single photon on a highly non-linear medium based on atoms excited to Rydberg levels. More recently, we have also enhanced the non-linearity of our ensemble to the single photon-level, as witnessed by the antibunching of a stored and retrieved incoming coherent field [3]. This will allow the storage of a single photon in a medium with single-photon non-linearity.

Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)•Jun 1, 2019•0 citations

Storage and retrieval of a single photon emitted by a quantum memory on a highly excited Rydberg state

Emanuele Distante, Pau Farrera, Auxiliadora Padrón-Brito +3 more

Summary form only given. Strong interaction between two single photons [1], is a long standing and important goal in quantum photonics. This would enable a new regime of nonlinear optics and unlock several applications in quantum information science, including photon-photon gates and deterministic Bell-state measurements for quantum networking. In the context of quantum networks [2], a particularly important case is to achieve strong interaction between single photons from independent photon pairs that can be stored in quantum memories. So far, most of the efforts towards nonlinear effects at the single-photon level have been realized using weak classical input light.In this contribution, we demonstrate the storage and retrieval of a paired single photon emitted by an ensemble quantum memory in a strongly nonlinear medium based on highly excited Rydberg atomic excitations [3,4]. We demonstrate that non-classical correlations between the two photons persist after the retrieval from the Rydberg ensemble. We show that our Rydberg cold atomic ensemble displays optical nonlinearity with input pulses containing few tens of photons. Our results [5], mark an important step towards deterministic photonphoton interactions, and may enable deterministic Bell-state measurement with multimode quantum memories.

Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)•Jun 1, 2017•2 citations

A quantum light-matter interface with Rydberg polaritons in a cold atomic ensemble

Emanuele Distante

Nonlinear optics at the single-photon level enables deterministic photonphoton interaction, a long-standing goal in quantum photonics science. Besides its implication in fundamental aspects of physics, this would unlock several applications in quantum information science. A relevant example are deterministic Bell state measurements, which find a prominent application in long-distance quantum communications using quantum repeater architecture. Toward this goal, we built a highly nonlinear system based on Rydberg excited states of a cold atomic ensemble and electromagnetically induced transparency (EIT). Our work first focuses on the storage of weak coherent light pulses in the atomic ensemble analysing the resulting nonlinear response of the medium. Then we demonstrate storage and retrieval of a paired single photon by coupling the Rydberg ensemble with a second remote cold atomic based quantum memory. Our set-up is based on magneto-optically trapped 87Rb atoms cooled down to temperature of 50 to 100 μK, with a cloud density of 10 ^(10) cm^(-3). Using EIT, light pulses are slowed down, stored as Rydberg collective atomic excitation and retrieved. We characterize EIT, slow-light and light-storage on a variety of Rydberg states, from the 26S up to the 80S. Depending on the state, the typical storage efficiency observed is of the order of few percents at a storage time of ~200 ns while the typical 1/e coherence time is of ~2us. By studying the optical response at different mean probe photon number, we have examined the Rydberg induced nonlinearity in EIT, slow-light and stored-light case for different Rydberg states. In particular, we have measured the nonlinear Rydberg induced dephasing of a stored collective Rydiberg state. For few microseconds storage time we have measured nonlinear response at the order of tens of photons. Our results show that light-storage enhances the nonlinear response of the atomic ensemble when compared to the slow light case, this possibly facilitating photonic quantum information processing using Rydberg excited atoms. Finally, we have used a separated cold atomic quantum memory to generate pair of correlated single photons. One photon of the pair is stored as single collective Rydberg atomic excitation and we show that non-classical correlations between the two photons and the single-photon statistic persist after the retrieval from the Rydberg ensemble. This result marks an important step towards deterministic photon-photon interactions. At the same time, linking a quantum memory with a highly nonlinear system may enable deterministic distribution of entanglement over long-distance using quantum repeaters. Un dels objectius que la fotònica quàntica persegueix des de temps ençà és la interacció determinista entre fotons, fenomen que podria assolir-se gràcies als avanços en l'òptica no-lineal a nivell de fotó únic. Aquests avanços, a més de les seves implicacions en la física fonamental, possibilitarien diferents aplicacions de la informació quàntica. A mode d'exemple, es podrien portar a terme mesures d'estat de Bell deterministes que facilitessin un funcionament eficient de l'arquitectura dels repetidors quàntics. En aquest projecte, i seguint aquesta línia, hem construït un sistema altament no-lineal basat en estats excitats de Rydberg d'un gas d'àtoms freds i hem aplicat el fenomen de la transparència induïda electromagnèticament (EIT). En un primer moment, ens hem focalitzat en l'emmagatzematge de polsos febles de llum coherent dins el núvol atòmic i en l'anàlisi de la resposta no-lineal del medi. Després, hem demostrat el emmagatzematge i la posterior recuperació d'un fotó emparellat (que forma part d'una parella de fotons correlacionat) gràcies a l'acoblament del nostre sistema d'àtoms Rydberg amb una altra memòria quàntica basada en conjunt diferenciat d'àtoms freds. El nostre dispositiu es compon d'àtoms de 87Rb dins una trampa magneto-òptica que han estat refredats a una temperatura de 50uK amb una densitat de 10^(10) cm^(-3). Utilitzant EIT, alentim els polsos de llum, els emmagatzemem en forma d'excitacions col·lectives a nivells de Rydberg i, posteriorment, els recuperem. Després, caracteritzem la llum lenta i l'emmagatzematge de fotons. Per fer-ho, utilitzem diferents estats de Rydberg: des de el 26S fins al 80S. En funció de l'estat, l'eficiència d'emmagatzematge observada és típicament de l'ordre de 2-8% en un temps ~200 ns, mentre que el temps de coherència 1/e típic és de 2us. A través de l'estudi de la resposta òptica a diferents escales de fotons, hem examinat la no-linealitat induïda per les interaccions dipolo-dipolo entre els estats de Rydberg a l'EIT i quins són els seus efectes, tant en la llum lenta, com en l'emmagatzematge. En concret, hem mesurat el desfasament quàntic induït per les interaccions dipolo-dipolo en els estats col·lectius de Rydberg. Al emmagatzemar-los durant uns microsegons, hem pogut mesurar les respostes no-lineals al nivell de desenes de fotons. Els nostres resultats demostren que l'emmagatzematge de la llum augmenta la resposta no-lineal del sistema atòmic respecte a la mera propagació a través del núvol d'àtoms facilitant, d'aquesta forma, el processament de la informació quàntica amb l'ús d'àtoms de Rydberg excitats. Per últim,hem acoblat el nostre sistema amb una altra memòria quàntica basada en àtoms freds que és capaç de generar parells correlacionats de fotons únics. Així, hem pogut demostrar que tant les correlacions no-clàssiques entre els fotons de la parella, com l'estadística que caracteritza el fotó únic, persisteixen després de l'emmagatzematge i la posterior recuperació d'un dels fotons de la parella dins del conjunt d'àtoms en forma d'excitació col·lectiva de Rydberg. Aquest resultat és un pas important cap a la demostració de les interaccions deterministes entre fotons. A la vegada, el fet d'acoblar una memòria quàntica amb un sistema altament no-lineal podria facilitar la distribució determinista d'entrellaçament a llargues distàncies amb l'ús de repetidors quàntics.

•Mar 24, 2017•1 citation

Nonlinear quantum optics for spinor slow light

Julius Ruseckas, Viačeslav Kudriašov, Algirdas Mekys +3 more

We investigate quantum nonlinear effects at a level of individual quanta in a double-tripod atom-light coupling scheme involving two atomic Rydberg states. In such a scheme the slow light coherently coupled to strongly interacting Rydberg states represents a two-component or spinor light. The scheme provides additional possibilities for the control and manipulation of light quanta. A distinctive feature of the proposed setup is that it combines the spin-orbit coupling for the spinor slow light with an interaction between the photons, enabling generation of the second probe beam even when two-photon detuning is zero. Furthermore, the interaction between the photons can become repulsive if the one-photon detunings have opposite signs. This is different from a single-ladder atom-light coupling scheme in which the interaction between the photons is attractive for both positive and negative detunings as long as the Rabi frequency of the control beam is not too high.

arXiv:1805.00144•Physical Review A•Jul 27, 2018•5 citations

‘Storage of Light’ in a Fast-Light Atomic Medium

A. M. Akulshin, A. Lezama, Blake Orr +3 more

We demonstrate both experimentally and by numerical modelling based on the optical Bloch equations that storage and retrieval of optical pulses are remarkably similar in fast-and slow-light atomic media with ground-state Zeeman coherences.

Slow and Fast Light (SL)•Jan 1, 2006•0 citations
We propose a new method to create two-photon states in a controllable way using interaction between the Rydberg atoms during the storage and retrieval of slow light. A distinctive feature of the suggested procedure is that the slow light is stored into a superposition of two atomic coherences under conditions of electromagnetically induced transparency (EIT). Interaction between the atoms during the storage period creates entangled pairs of atoms in a superposition state that is orthogonal to the initially stored state. Restoring the slow light from this new atomic state one can produce a two photon state with a second-order correlation function determined by the atom-atom interaction and the storage time. Therefore the measurement of the restored light allows one to probe the atom-atom coupling by optical means with a sensitivity that can be increased by extending the storage time. As a realization of this idea we consider a many-body Ramsey-type technique which involves pi/2 pulses creating a superposition of Rydberg states at the beginning and the end of the storage period. In that case the regenerated light is due to the resonance dipole-dipole interaction between the atoms in the Rydberg states.
Photons are very good candidates to carry quantum information due to their negligible interactions. However, photon-photon interactions are needed to process photonic quantum information. This is very useful for quantum repeater applications [1], in which the success probability of entanglement swapping can be highly increased if the Bell-state measurement is performed deterministically. In the case of photons, it requires mapping them in a non-linear medium at the single-photon level. This strong non-linearity has been demonstrated by using Rydberg atoms, which are atoms excited to states with a high principal quantum number. However, previous experiments with Rydberg atoms have been implemented with weak coherent input states of light [2, 3]. Hence, the mapping of true single photons to a medium with strong single-photon non-linearity is, so far, an outstanding goal. In this work, we have demonstrated the storage and retrieval of a paired single photon on a highly non-linear medium based on atoms excited to Rydberg levels. More recently, we have also enhanced the non-linearity of our ensemble to the single photon-level, as witnessed by the antibunching of a stored and retrieved incoming coherent field [3]. This will allow the storage of a single photon in a medium with single-photon non-linearity.
Summary form only given. Strong interaction between two single photons [1], is a long standing and important goal in quantum photonics. This would enable a new regime of nonlinear optics and unlock several applications in quantum information science, including photon-photon gates and deterministic Bell-state measurements for quantum networking. In the context of quantum networks [2], a particularly important case is to achieve strong interaction between single photons from independent photon pairs that can be stored in quantum memories. So far, most of the efforts towards nonlinear effects at the single-photon level have been realized using weak classical input light.In this contribution, we demonstrate the storage and retrieval of a paired single photon emitted by an ensemble quantum memory in a strongly nonlinear medium based on highly excited Rydberg atomic excitations [3,4]. We demonstrate that non-classical correlations between the two photons persist after the retrieval from the Rydberg ensemble. We show that our Rydberg cold atomic ensemble displays optical nonlinearity with input pulses containing few tens of photons. Our results [5], mark an important step towards deterministic photonphoton interactions, and may enable deterministic Bell-state measurement with multimode quantum memories.
Nonlinear optics at the single-photon level enables deterministic photonphoton interaction, a long-standing goal in quantum photonics science. Besides its implication in fundamental aspects of physics, this would unlock several applications in quantum information science. A relevant example are deterministic Bell state measurements, which find a prominent application in long-distance quantum communications using quantum repeater architecture. Toward this goal, we built a highly nonlinear system based on Rydberg excited states of a cold atomic ensemble and electromagnetically induced transparency (EIT). Our work first focuses on the storage of weak coherent light pulses in the atomic ensemble analysing the resulting nonlinear response of the medium. Then we demonstrate storage and retrieval of a paired single photon by coupling the Rydberg ensemble with a second remote cold atomic based quantum memory. Our set-up is based on magneto-optically trapped 87Rb atoms cooled down to temperature of 50 to 100 μK, with a cloud density of 10 ^(10) cm^(-3). Using EIT, light pulses are slowed down, stored as Rydberg collective atomic excitation and retrieved. We characterize EIT, slow-light and light-storage on a variety of Rydberg states, from the 26S up to the 80S. Depending on the state, the typical storage efficiency observed is of the order of few percents at a storage time of ~200 ns while the typical 1/e coherence time is of ~2us. By studying the optical response at different mean probe photon number, we have examined the Rydberg induced nonlinearity in EIT, slow-light and stored-light case for different Rydberg states. In particular, we have measured the nonlinear Rydberg induced dephasing of a stored collective Rydiberg state. For few microseconds storage time we have measured nonlinear response at the order of tens of photons. Our results show that light-storage enhances the nonlinear response of the atomic ensemble when compared to the slow light case, this possibly facilitating photonic quantum information processing using Rydberg excited atoms. Finally, we have used a separated cold atomic quantum memory to generate pair of correlated single photons. One photon of the pair is stored as single collective Rydberg atomic excitation and we show that non-classical correlations between the two photons and the single-photon statistic persist after the retrieval from the Rydberg ensemble. This result marks an important step towards deterministic photon-photon interactions. At the same time, linking a quantum memory with a highly nonlinear system may enable deterministic distribution of entanglement over long-distance using quantum repeaters. Un dels objectius que la fotònica quàntica persegueix des de temps ençà és la interacció determinista entre fotons, fenomen que podria assolir-se gràcies als avanços en l'òptica no-lineal a nivell de fotó únic. Aquests avanços, a més de les seves implicacions en la física fonamental, possibilitarien diferents aplicacions de la informació quàntica. A mode d'exemple, es podrien portar a terme mesures d'estat de Bell deterministes que facilitessin un funcionament eficient de l'arquitectura dels repetidors quàntics. En aquest projecte, i seguint aquesta línia, hem construït un sistema altament no-lineal basat en estats excitats de Rydberg d'un gas d'àtoms freds i hem aplicat el fenomen de la transparència induïda electromagnèticament (EIT). En un primer moment, ens hem focalitzat en l'emmagatzematge de polsos febles de llum coherent dins el núvol atòmic i en l'anàlisi de la resposta no-lineal del medi. Després, hem demostrat el emmagatzematge i la posterior recuperació d'un fotó emparellat (que forma part d'una parella de fotons correlacionat) gràcies a l'acoblament del nostre sistema d'àtoms Rydberg amb una altra memòria quàntica basada en conjunt diferenciat d'àtoms freds. El nostre dispositiu es compon d'àtoms de 87Rb dins una trampa magneto-òptica que han estat refredats a una temperatura de 50uK amb una densitat de 10^(10) cm^(-3). Utilitzant EIT, alentim els polsos de llum, els emmagatzemem en forma d'excitacions col·lectives a nivells de Rydberg i, posteriorment, els recuperem. Després, caracteritzem la llum lenta i l'emmagatzematge de fotons. Per fer-ho, utilitzem diferents estats de Rydberg: des de el 26S fins al 80S. En funció de l'estat, l'eficiència d'emmagatzematge observada és típicament de l'ordre de 2-8% en un temps ~200 ns, mentre que el temps de coherència 1/e típic és de 2us. A través de l'estudi de la resposta òptica a diferents escales de fotons, hem examinat la no-linealitat induïda per les interaccions dipolo-dipolo entre els estats de Rydberg a l'EIT i quins són els seus efectes, tant en la llum lenta, com en l'emmagatzematge. En concret, hem mesurat el desfasament quàntic induït per les interaccions dipolo-dipolo en els estats col·lectius de Rydberg. Al emmagatzemar-los durant uns microsegons, hem pogut mesurar les respostes no-lineals al nivell de desenes de fotons. Els nostres resultats demostren que l'emmagatzematge de la llum augmenta la resposta no-lineal del sistema atòmic respecte a la mera propagació a través del núvol d'àtoms facilitant, d'aquesta forma, el processament de la informació quàntica amb l'ús d'àtoms de Rydberg excitats. Per últim,hem acoblat el nostre sistema amb una altra memòria quàntica basada en àtoms freds que és capaç de generar parells correlacionats de fotons únics. Així, hem pogut demostrar que tant les correlacions no-clàssiques entre els fotons de la parella, com l'estadística que caracteritza el fotó únic, persisteixen després de l'emmagatzematge i la posterior recuperació d'un dels fotons de la parella dins del conjunt d'àtoms en forma d'excitació col·lectiva de Rydberg. Aquest resultat és un pas important cap a la demostració de les interaccions deterministes entre fotons. A la vegada, el fet d'acoblar una memòria quàntica amb un sistema altament no-lineal podria facilitar la distribució determinista d'entrellaçament a llargues distàncies amb l'ús de repetidors quàntics.
We investigate quantum nonlinear effects at a level of individual quanta in a double-tripod atom-light coupling scheme involving two atomic Rydberg states. In such a scheme the slow light coherently coupled to strongly interacting Rydberg states represents a two-component or spinor light. The scheme provides additional possibilities for the control and manipulation of light quanta. A distinctive feature of the proposed setup is that it combines the spin-orbit coupling for the spinor slow light with an interaction between the photons, enabling generation of the second probe beam even when two-photon detuning is zero. Furthermore, the interaction between the photons can become repulsive if the one-photon detunings have opposite signs. This is different from a single-ladder atom-light coupling scheme in which the interaction between the photons is attractive for both positive and negative detunings as long as the Rabi frequency of the control beam is not too high.