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Space product information carriers

Space product information carriers

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Mode division multiplexing MDM is mooted as a technology to address future bandwidth issues and has been successfully demonstrated in free space using spatial modes with orbital angular momentum OAM. To further increase the data transmission rate, more degrees of freedom are required to form a densely packed mode space.

Here we move beyond OAM and demonstrate multiplexing and demultiplexing using both the radial and azimuthal degrees of freedom. We achieve this with a holographic approach that allows over modes to be encoded on a single hologram, across a wide wavelength range, in a wavelength independent manner. Our results offer a new tool that will prove useful in realizing higher bit rates for next generation optical networks.

Since the beginning of the 21st century there has been a growing interest in increasing the capacity of telecommunication systems to eventually overcome our pending bandwidth crunch. Significant improvements in networks transmission capacity has been achieved through the use of polarization division multiplexing PDM and wavelength division multiplexing WDM techniques and also through implementing high order modulation formats 1 , 2 , 3.

However, it might not be possible to satisfy the exponential global capacity demand in the near future. One potential solution to eventually cope with bandwidth issues is space division multiplexing SDM 4 , 5 , 6 and in particular the special case of mode division multiplexing MDM , which was first suggested in the s 7. In MDM based communication systems, each spatial mode, from an orthogonal modal basis, can carry an independent data stream, thereby increasing the overall capacity by a factor equal to the number of modes used 8.

A particular mode basis for data communication is orbital angular momentum OAM 9 , 10 which has become the mode of choice in many studies due to its topical nature and ease of detection with phase-only optical elements 11 , More recent reports have shown free space communication with a bit rate of 1.

But, by taking into account the effects of atmospheric turbulence on the crosstalk and system bit error rate BER in an OAM multiplexed free space optics FSO link, experimental results have indicated that turbulence-induced signal fading will significantly deteriorate link performance and might cause link outage in the strong turbulence regime 16 , 17 , Recently, Zhao et al. Indeed, OAM is only a subspace of the full space of Laguerre Gaussian LG beams where modes have two degrees of freedom: an azimuthal index and a radial index p , the former responsible for the OAM.

The addition of the radial degree of freedom certainly increases the bandwidth capacity, since for each value of an infinite number of p values can be used to have access to many more information channels.

In this study, we demonstrate a new holographic tool to realise a communication link using a densely packed LG mode set incorporating both radial and azimuthal degrees of freedom. Our subset of the LG modes were successfully used as information carriers over a free space link to illustrate the robustness of our technique. The information is recovered by simultaneously detecting all modes employing a single hologram.

Although our scheme is a proof-of-concept, it provides a useful basis for increasing the capacity of future optical communication systems.

The mode size is a function of the indices and is given by. Such modes are shape invariant during propagation and are reduced to the special case of the Gaussian beam when. This full set of modes can be experimentally generated using complex-amplitude modulation.

In this way, the amplitude and phase of the modes set Eq. Moreover, the holograms can be multiplexed into a single hologram to generate multiple modes simultaneously. Figure 1 a shows the generated holograms to create the desired subset of modes for this experiment.

Their corresponding theoretical intensity profile can be seen in Fig. The information is propagated through free space and reconstructed in the second stage with a modal filter. The modes generated in this way were encoded using three different wavelengths onto a single hologram, in a wavelength independent manner and sent through free space. At the receiver, we were able to identify with high fidelity any of the encoded modes in a single real time measurement, using a wavelength independent multimode correlation filter on a single SLM 22 , 23 , This involves superimposing a series of single transmission functions t n r , each multiplied with a unique carrier frequency K n to produce a final transmission function T r.

In the Fourier plane the carrier frequencies K n manifest as separate spatial coordinates as illustrated in Fig. This approach allows multiple LG modes to be generated and detected simultaneously producing a high data transmission rate.

The experimentally generated modes are used to encode and decode information in our multiplexing and demultiplexing scheme as shown in Fig. Here we demonstrate that the propagation dynamics, divergence being one example, is governed by the beam quality factor 25 and that modes with the same index will propagate in an identical manner regardless of the radial component p. To show this, we encoded information in the set of modes that incorporates both degrees of freedom, created as described before.

Moreover, we multiplex the above mentioned subset of modes on three different wavelengths to increase our de encoding basis set from 35 to The data are encoded using these mode set and transferred in free space. This information is recovered by projecting the propagated information onto a modal filter. The modal filter consists of multiplexed holograms displayed on a second SLM SLM-2 and a CCD camera, capable of identifying with high accuracy any of the input modes see experimental details.

The intermodal crosstalk for the chosen modes, this is, the crosstalk between the input modes and the output modes was computed by measuring, for each input mode, the on-axis intensity of every output mode and normalized so that the total intensity adds up to unity Fig. As can be seen, the crosstalk between the different modes is very low and is independent of the p value.

In a real scenario, where modes propagate over long distances, intermodal crosstalk would become an issue and the addition of compensating methods, as adaptive optics, would be needed. For each input mode we measure the output cross talk for all hundred and five output modes. The correlation coefficient is a dimensionless number that measures the similarity between two images, being 0 for nonidentical images and 1 for identical images.

A quantification of the similarity between sent and received images is done using 2D image correlation. The value of the correlation coefficient ranges from 0 for nonidentical images to 1 for identical images. The information encoding is performed in three different ways.

In the first one, applied to grayscale images, we specifically assign a particular mode and a particular wavelength to the gray-level of each pixel forming the image. In this approach we are able to reach different levels of gray. In a second approach, applied to color images, each pixel is first decomposed into its three color components red, blue and green. In this approach only 35 levels of saturation can be reached with a total number of generated modes.

Finally, in the third we implement multi-bit encoding [see Fig. In this scheme, levels of contrast are achieved by multiplexing eight different modes on a single hologram. Each of the possible permutations, of these 8 modes, representing a particular gray level. Upon arrival to the detector each permutation is uniquely identified and the information is decoded to its 8-bit form to reconstruct the image.

This approach was extended to high contrast color images by using a particular wavelength for each primary color intensity, achieving a total rate of 24 bits per pixel. The reliability of our technique was further tested by transmitting different complex images containing all levels of saturation in each RGB component.

Here we only show the results for one image Fig. Very recently it was pointed out that OAM multiplexing is not an optimal technique for free-space information encoding and that OAM itself does not increase the bandwidth of optical communication systems 19 , It has also been suggested that MDM, requires a complete mode set for a real bandwidth increment. Indeed, in all work to date only the azimuthal component of transverse modes, that gives rise to OAM, has been used in multiplexing schemes.

Here we point out that the propagation dynamics beam size, divergence, phase shift etc. The M 2 can be viewed as a mode index: modes with the same index e.

It is clear that one mode set will be as good as any other at least in terms of perturbation-free communication , provided that the elements are orthogonal and regardless of whether it carries OAM or not. Moreover, by implementing MDM on different wavelengths, we demonstrate that it is possible to expand the overall transmission capacity by several orders of magnitude. The number of carrier channels would be given by the number of optical modes times the number of wavelengths.

In our experiment we generated 35 optical modes and combined this with 3 different wavelengths, creating a basis set of modes. These modes are used as information carriers in a proof-of-concept free space link, capable of transmitting and recovering information in real time with very high fidelity.

Figure 4 is an example of the many images transmitted in our link. Each image is sent pixel by pixel, for this, the information of colour saturation of each pixel, is encoded using our mode set. Its simplicity linked to the versatility of SLMs, capable of operating in a wide range of the spectrum as well as with broad band sources, allowed us to generate customized digital hologram to encode and decode the information. Furthermore, the designed correlation filters are wavelength insensitive which allows the technique to operate in a large spectrum, compared to existing mode de multiplexers which are extremely wavelength sensitive, such as the photonic lantern.

This approach can be extended to a wider range of wavelengths and to a higher number of modes, both limited by physical properties of the SLM as for example spatial resolution and wavelength operating range. The use of polarization could be potentially an additional degree of freedom and could possibly double the overall transmission capacity of the system.

Even though here we have used our modes as information carriers, this experiment establishes the basis for this technique to be incorporated into standard communication systems. In this case each mode would represent a channel that can be modulated and detected with conventional technology. This technique allowed us to incorporate the radial component of LG beams as another degree of freedom for mode division multiplexing. By combining both degrees of freedom, radial and azimuthal, with wavelength-division multiplexing, we are able to generate over information channels using a single hologram.

As a proof-of-concept, we implemented different encoding techniques to transmit information, with very high accuracy, in a free space link that employs conventional technology such as SLMs and CCD cameras.

Our approach can be implemented in both, free space and optical fibres, facilitating studies towards high bit rate next generation networks. Additionally, our technique could also be extended to other type of orthogonal modes regardless of their OAM content, as for example Hermite-Gaussian beams. Afterwards it is decomposed into its different wavelength components by means of a grating. The SLM is split into three independent screens, one for each beam and controlled independently.

Each third is addressed with a hologram representing a Laguerre-Gaussian mode , where p is the radial index and the azimuthal index [see Fig.

For this experiment we use 35 different modes [see Fig. It should be stressed that the selection of the modes was made arbitrary and does not exclude any other combinations. These modes were encoded via complex amplitude modulations, a technique that allows for the generation of modes with purities higher than 0.

Additionally, we added blazed gratings to each hologram and spatially filtered the first diffraction order to generate wavelength independent holograms. Even though here we only used the first 35 LG modes, similar results would be obtained in using higher order modes and a larger set of modes, the limit is only imposed by the spatial resolution of the SLM. This SLM is also split into three independent screens, each of which is addressed with a multiplexed hologram.

This hologram consists of the complex conjugated of all 35 modes, encoded with different spatial carrier frequencies [see Fig.

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Optical communication beyond orbital angular momentum

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