## Abstract

We demonstrate a new generation mechanism for polarisation- and colour-entangled photon pairs. In our approach we tailor the phase-matching of a periodically poled KTP crystal such that two downconversion processes take place simultaneously. Relying on this effect, our source emits entangled bipartite photon states, emerging intrinsically from a single, unidirectionally pumped crystal with uniform poling period. Its property of being maximally compact and luminous at the same time makes our source unique compared to existing photon-entanglement sources and is therefore of high practical significance in quantum information experiments.

## Introduction

Quantum entanglement is regarded as a key feature for new information technologies such as quantum key distribution^{1}, dense coding^{2}, teleportation^{3} or one-way quantum computing^{4}. In particular, most experiments and applications rely on photonic entanglement, taking advantage of long coherence times, good controllability and favourable detection methods. The most common generation technique relies on spontaneous parametric downconversion (SPDC) in a *χ*^{(2)} nonlinear crystal.

Up to this point photon-entanglement sources suffered from the compromise of being *either* compact *or* efficient. A very popular approach makes use of a *β*-barium borate (BBO) crystal to generate cones of down-converted photons whose lines of intersection are the spatial modes of polarisation-entangled photon states^{5, 6}. Although this source consists of a very simplistic setup— it uses only a single unidirectionally pumped crystal and is therefore very convenient to assemble— it allows for only moderate count rates since the generated photons are emitted spatially into a cone and only a small intersection is coupled into single-mode fibres. The rates can be improved by collapsing the cones into quasi-Gaussian modes propagating collinearly with the pump. However, in order to generate entanglement in this setup, *two* crystals, arranged in a crossed fashion^{7}, are needed. In addition, only a short propagation length is allowed as not to suffer from walk-off effects, thereby limiting the maximal production rate again. (As a side note, however, the non-collinear geometry of BBO-based sources has been demonstrated favourable for the generation of hyperentangled states^{8, 9}. These states, among other interesting properties, allow for a convenient way to perform Bell-state analysis^{10, 11}).

The first truly collinear SPDC sources^{12} appeared with the advent of quasi-phase-matching (QPM) in SPDC, allowing for a wider choice of wavelengths for the generated photon pairs, longer crystals, better mode matching with single-mode fibres and hence higher production rates. In order to generate (polarisation) entanglement, most existing QPM sources are either assembled in a single-pass & double-crystal or single-crystal & double-pass configuration. The most common double-crystal scheme is the Mach-Zehnder configuration^{13, 14} where both crystals are pumped individually and the output is combined subsequently. Apart from higher costs and the elaborate effort of aligning two crystals, this type of setup also requires a stable phase relation to be kept between the two paths^{15}. Alternatively, the two crystals can be placed behind one another with the second crystal being rotated by 90° with respect to the first one^{16, 17}. In this realisation, the optimal focussing- and collection geometries cannot be satisfied for both crystals simultaneously, especially for long crystals and highly non-degenerate wavelengths of the produced photons. Due to the above disadvantages of the double-crystal configurations, a single-crystal & double-pass geometry, based on a Sagnac interferometer, is widely used nowadays^{18,19,20,21}. The remaining issues with this setup are a larger footprint and difficult alignment of the counter-propagating beams, especially for non-degenerate wavelengths^{22}. Recently polarisation entanglement has also been demonstrated in a single-crystal & single-pass fashion where the periodic pattern of the QPM period is altered to support two different SPDC modes at the same time. This method is mainly applied in conjunction with optical waveguides where either the first and second section of the waveguide shows a different poling period^{23}, or a more complex pattern in which the two different periods are interleaved^{24}. Apart from the time- and cost-extensive crystal manufacturing process, these promising approaches are at current state very sensitive to manufacturing imperfections and suffer from moderate count rates due to unsatisfying waveguide coupling.

Our new concept of creating entanglement combines most of the advantages of the previous schemes. At heart it uses a single nonlinear crystal with a uniform grating period for QPM which is also suitable for short-pulsed excitation. The setup offers high coupling efficiencies due to its collinear design and is still as compact and simplistic as a BBO source, requiring only one crystal pumped from one direction. The alignment process is therefore straightforward even for highly non-degenerate SPDC. By varying the pump wavelength, the emitted photon pairs can be wavelength-tuned to near degeneracy.

## Collinear double-downconversion

Spontaneous parametric downconversion is a quantum-mechanical process where a shortwave photon (usually referred to as *pump*) decays into two longwave daughter photons (*signal* and *idler*) by interaction with a nonlinear medium. In general the three fields interfere destructively within the medium and no measurable output is generated. This is caused by a non-zero momentum-difference vector

where *n* represent the respective refractive indices. Quasi-phase-matching is a technique which allows for a positive energy transfer from pump to signal and idler fields throughout the medium. In this approach destructive interference of the three interacting fields is avoided by an alternating nonlinearity coefficient *d*_{eff} of the material. In particular, ferro-electric poling of the crystal is used to toggle *d*_{eff} between positive and negative values in integer multiples of a specific length along the crystal, the poling periodicity Λ. Consider a collinear process where pump, signal and idler each propagate along the crystal’s *x*-axis. The amplitude for a downconversion in a crystal with length *L* reads

where $\mathcal{N}$ is a normalisation constant, *d*_{eff} is the effective nonlinearity coefficient for the specific process and ${\stackrel{\u02c6}{a}}_{s,i}^{\u2020}$ are the respective creation operators. Moreover, *μ* is the *pump envelope amplitude*, often represented by a Gaussian distribution:

where *λ*_{
p
} = (1/*λ*_{
s
} + 1/*λ*_{
i
})^{−1} by energy conservation and *λ*_{
p0} is the central pump wavelength. Finally, *ψ* is the *quasi*-*phase*-*matching amplitude*

with Δ*k*_{
m
} being the phase-mismatch vector represented as

where *m* is an odd integer (positive or negative), referred to as the QPM order. Quasi-phase-matching is achieved when the amplitude *ψ* is maximised. This is the case when the sinc function equals one or, equivalently, when Δ*k*_{
m
} = 0. From this requirement and from (5) follows the poling periodicity:

Note that the momentum difference Δ*k* can be both positive and negative (Fig. 1). Accordingly the QPM order *m* will be positive or negative respectively in order to preserve positivity of the crystal periodicity Λ. So more precisely, the quasi-phase-matching amplitude actually reads

where the subscripts + and − correspond to a positive/negative QPM order *m* in equation (5). This modifies the SPDC amplitude (2) to the state

where |*α*|^{2} + |*β*|^{2} = 1. While in most experimental setups only one of the two terms contributes to the amplitude, there are specific configurations (crystal type, wavelengths, polarisations) where neither of both terms can be neglected. It is important to note that in this case a single periodically poled crystal with a given grating Λ and pumped by a laser with given centre wavelength *λ*_{
p0} can be used to phase-match up to *two* different SPDC processes with distinct wavelength pairs being generated— provided the respective momentum-difference vectors Δ*k* carry the same length but different signs. This property, collinear double-downconversion (CDDC), is the key to our novel entangled-photon source.

## Intrinsic entanglement

The *joint spectral intensity* (JSI) of an SPDC process is the probability distribution function of specific signal and idler wavelength pairs being emitted. It is represented as the square over the joint spectral amplitude (JSA) which is the product of pump- and phase-matching envelope amplitude:

with *λ*_{
p
} = (1/*λ*_{
s
} + 1/*λ*_{
i
})^{−1}. Graphically, when intensity over signal and idler wavelength is plotted, the JSI can be understood as the intersection of the envelope intensities |*μ*|^{2} and |*ψ*|^{2}, as illustrated in Fig. 2a. When a periodically poled crystal allows for phase-matching of both positive and negative Δ*k* in a given wavelength range, the pump intensity |*μ*|^{2} intersects with *two* constituents of *ψ*(*λ*_{
s
},*λ*_{
i
}), namely |*ψ*_{+}|^{2} and |*ψ*_{−}|^{2}, as shown in Fig. 2b. In this case the setup will generate photons with four distinct wavelengths: one pair with ${\lambda}_{{s}_{+}}$, ${\lambda}_{{i}_{+}}$ and joint spectral intensity JSI_{+} and another one with ${\lambda}_{{s}_{-}}$, ${\lambda}_{{i}_{-}}$ and JSI_{−} (Fig. 2c).

Consider now a type-II downconversion where signal and idler radiation are orthogonally polarised and define, without loss of generality, the signal photons to be polarised horizontally. Under careful configuration of the setup, the two centre wavelengths of one pair can be brought to coincide with those of the respective counterparts of the other, orthogonally polarised, pair, hence

as illustrated in Fig. 2d. When the wavelengths of the two pairs cannot be told apart, entanglement emerges from the lost information whether a generated pair originates from |Ψ_{+}> or |Ψ_{−}>. So when the two joint spectral distributions become interchangeable in wavelength, the SPDC amplitude (8) becomes entangled in polarisation and wavelength. When we label the shortwave daughter photons as blue (*B*) and the longwave ones as red (*R*), the state can (in a simplified form) be written as

with all creation operators acting on the same spatial mode due to the collinearity of the downconversion. Depending on experimental requisition this state can be reduced to both a *polarisation*-entangled state

or *frequency*-entangled state

where the photons are spatially separated into mode 1 and 2 by a dichroic mirror (12) or a polarising beamsplitter (13). The amplitudes *α* and *β* = |*β*|*e*^{iθ} are complex numbers which fulfil the normalisation condition |*α*|^{2} + |*β*|^{2} = 1. Note that in general the effective nonlinearity *d*_{eff} of the two superimposed SPDC processes is not of equal magnitude, so neither will be |*α*| and |*β*|. In addition, the two JSI distributions might come in different spectral bandwidths which has to be compensated using sufficiently narrow bandpass filters in order to avoid spectral distinguishability. This will further influence the magnitude of the two amplitudes.

## Numerical investigation of CDDC-entanglement in ppKTP

Using our software ‘QPMoptics’^{25}, we discovered a large variety of configurations allowing for generation of intrinsic entanglement using CDDC in periodically poled potassium titanyl phosphate (KTiOPO_{4}, ppKTP). These configurations are depicted in Fig. 3. The figure shows that the generated wavelengths *λ*_{
B
} and *λ*_{
R
} approach each other as the crystal periodicity Λ gets longer. This brings the advantage of equal group velocities in the two SPDC processes, since differences in the wavelength dispersion can be neglected. Moreover, due to overlapping bandwidths for photons with same polarisation (see right inset in Fig. 3), no measures such as bandpass-filtering have to be taken in order to preserve coherent overlap of the two JSI’s. This gives rise to the possibility of a highly efficient colour-entanglement source with signal and idler in the vicinity of ${\lambda}_{s,i}\sim 1$ μm. Since no filtering is required, this source would be very promising in terms of brightness and visibility. However, the degeneracy wavelength lies at around 1100 nm, invisible to common avalanche photo diodes, and would require superconducting nanowire detectors to be counted efficiently. For the first demonstration of intrinsic entanglement from CDDC we therefore decided on highly non-degenerate polarisation-entangled photon pairs at roughly ${\lambda}_{B}\sim 900$ nm and ${\lambda}_{R}\sim 1300$ nm which can be detected efficiently with available Silicon and InGaAs photo diodes respectively.

## Experiment

The experimental setup is depicted in Fig. 4. A 10 mm long, periodically poled KTP crystal was pumped with a *λ*_{
p0} = 532.3 nm continuous-wave laser, generating photon pairs at *λ*_{
B
} = 904.3 nm and *λ*_{
R
} = 1293.9 nm. The photons were separated according to their wavelength using a dichroic mirror, coupled into single-mode fibres and detected by avalanche photo diodes. Even though the centre-wavelengths of the generated photon pairs can be matched very accurately, entanglement visibility is undermined by spectral distinguishability due to different bandwidths of the two JSI’s. This distinguishability could be overcome by insertion of a narrow tunable bandpass filter (BPF) in the arm of the longwave photon (*λ*_{
R
}). The spectra of the down-converted photons before and after bandpass filtering are illustrated in Fig. 5. For our experiment it turned out that the process with higher nonlinearity (and therefore SPDC amplitude) is also the one with greater spectral bandwidth. Therefore, insertion of a bandpass filter reduced the greater one of the two amplitudes and matched the coefficients |*α*| and |*β*| to each other such that we ended up with an almost maximally entangled state:

Due to different group velocities within the crystal, the relative time delays between the shortwave and longwave photon differ, according to whether the pair originates from |Ψ_{+}>or |Ψ_{−}> (see Table 1), therefore diminishing coherent superposition of the two SPDC processes. This effect could be compensated using birefringent calcite wedges. The very same wedges were also used for tuning of the phase angle *θ* of the entangled state (14).

Using single-photon counters in both arms, we measured a coincidence rate of 1200 counts/s/mW. Taking into account coupling- and detection losses, this corresponds to a pair-generation rate of approximately 5.5 × 10^{5} counts/s/mW and a spectral brightness of 3.4 × 10^{6} counts/s/mW/THz. (To give a comparison with up-to-date single-crystal & single-pass entanglement sources, the— to our knowledge— brightest BBO-based source^{6} yielded a measured coincidence rate of up to 900 counts/s/mW, a pair-generation rate of 1.1 × 10^{4} counts/s/mW and a spectral brightness of 4.5 × 10^{3} counts/s/mW/THz). We measured polarisation correlations in the H/V basis (0° and 90°) and in the diagonal basis (±45°), depicted in Fig. 6. After subtraction of the background coincidences, we achieved visibilities of *V*_{
H/V
} = 0.999(4) and *V*_{+/−} = 0.971(6) respectively. The average visibility is therefore *V*_{avg} = 0.985(4) which exceeds the non-locality threshold of $\mathrm{1/}\sqrt{2}\approx 0.71$ by more than 71 standard deviations. (Before subtraction of the background we measured *V*_{
H/V
} = 0.985(3), *V*_{+/−} = 0.950(5) and therefore *V*_{avg} = 0.967(3)). We measured a CHSH parameter^{26} of *S* = 2.817(22) (*S* = 2.778(21) before subtraction of the background pairs), therefore violating the CHSH inequality by approximately 38 standard deviations. After removal of the tunable bandpass filter, the coincidence rate could be increased to 1970 counts/s/mW under the cost of a lower visibility in the diagonal basis: *V*_{+/−} = 0.733(12), therefore *V*_{avg} = 0.865(6). The heralding efficiency of the longwave photon amounts to 45.1% which is a drastic advance compared to other highly non-degenerate entangled-photon sources (e.g. 20%^{17} or 10%^{22}).

## Conclusion and Outlook

We presented the theoretical concept and first experimental demonstration of a novel collinear entangled-photon source, consisting of a single unidirectionally pumped nonlinear crystal. Using the collinear double-downconversion effect in periodically poled crystals, this concept can be used to generate both, polarisation- and colour-entangled photon states. Numerical evaluations revealed a broad range of wavelength pairs this type of source could generate. In our particular experimental setup we successfully generated polarisation-entangled pairs of 904.3 nm and 1293.9 nm wavelength, achieving coincidence rates of 1200 counts/s/mW and an average visibility of *V*_{avg} = 0.985(4). However, we found that pairs in the vicinity of $\lambda \sim 1$ μm would feature even better spectral and temporal indistinguishability due to coinciding bandwidths and group velocities in the medium. This would enhance the entanglement visibility and allow for significantly higher count rates, since no bandpass-filtering would be required to match the bandwidths. Moreover, we numerically investigated four other crystals in the *mm2* point group and discovered a large number of additional promising implementations of our method (Laudenbach *et al*. Numerical investigation of photon-pair generation in periodically poled *M*TiO*X*O_{4} (*M* = K, Rb, Cs; *X* = P, As). *Manuscript submitted*).

Due to its collinear and very compact design, our novel source will set new standards in terms of scalability as it is required for example in multi-photon experiments.

## Methods

A detailed description of the experimental setup is provided in the caption of Fig. 4. The wavelength spectra of our generated photons (Fig. 5) were measured using an optical spectrum analyser (OSA) in conjunction with our single-photon detectors. In its normal operation mode, the OSA measures the wavelength-resolved optical power with a built-in detector which, however, is not sensitive enough to resolve single photons. We therefore operated the OSA as a monochromator by replacing the internal detector with a fibre output that we connected to an external single-photon detector. A self-written Labview program was used to control the monochromator’s diffraction grating and log the count rate with respect to the coupled wavelength.

Before planning and conducting this experiment, we performed a thorough numerical search for possible realisations of our novel concept. Apart from type-II downconversion in periodically poled KTP, we initially investigated two other popular nonlinear materials, namely lithium niobate (LiNbO_{3}, ppLN) and lithium tantalate (LiTaO_{3}, ppLT) but were unable to find experimentally feasible setups using these media. However, in recent numerical investigations, we discovered a large variety of possible implementations of our novel concept using other nonlinear materials in the *mm2* point group (isomorphic to KTP). These results help to make new favourable wavelength configurations accessible (Laudenbach *et al*. Numerical investigation of photon-pair generation in periodically poled *M*TiO*X*O_{4} (*M* = K, Rb, Cs; *X* = P, As). *Manuscript submitted*).

The experiment was designed using our SPDC-simulation software QPMoptics^{25}. Table 1 provides a direct comparison of the numerically simulated spectra with the measured ones as well as the photons’ individual group delays and relative time delays.

In order to obtain an estimate on the pair-generation rate PR, we took into account that the measured single-count rates SR of the bluer (B) and redder (R) arm as well as the measured coincidence rate CR are attenuated by imperfect coupling efficiency *μ* and detection efficiency *η*:

This allows us to express the coupling efficiencies as follows:

The pair-generation rate is then

The spectral brightness is the pair-generation rate per optical pump power *P* per photon bandwidth *B*:

## Additional Information

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## Acknowledgements

We gratefully acknowledge invaluable help from Florian Stierle, Alexander Sanchez de la Cerda and Christoph Pacher. This work was funded by the Austrian Research Promotion Agency (Österreichische Forschungsförderungsgesellschaft, FFG) through KVQ (No. 4642983). Moreover, we acknowledge support from the European Commission, via EQUAM (No. 323714), PICQUE (No. 608062), GRASP (No. 613024), QUCHIP (No. 641039) and the Austrian Science Fund (FWF) through START (Y585-N20).

## Author information

### Affiliations

#### Security & Communication Technologies, Center for Digital Safety & Security, AIT Austrian Institute of Technology GmbH, Donau-City-Str. 1, 1220, Vienna, Austria

- Fabian Laudenbach
- , Sebastian Kalista
- , Michael Hentschel
- & Hannes Hübel

#### Quantum Optics, Quantum Nanophysics & Quantum Information, Faculty of Physics, University of Vienna, Boltzmanngasse 5, 1090, Vienna, Austria

- Fabian Laudenbach
- & Philip Walther

### Authors

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### Contributions

F.L. conceived the concept and theoretical foundations of the experiment and performed the numerical search for possible realisations. H.H. operated as the project leader and, together with M.H., developed the schedule, methodology and detailed procedure of the experiment. Moreover, M.H. contributed to the experimental setup. S.K. assembled the source and performed most measurements. P.W. contributed the theoretical analysis of the polarisation- and frequency-entangled state. The manuscript draft was written by F.L. and all co-authors contributed to the final version.

### Competing Interests

F.L. and the AIT will be holding a share of a possible commercial distribution of the SPDC-simulation software ‘QPMoptics’ by a third-party retailer.

### Corresponding author

Correspondence to Fabian Laudenbach.

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