Semiconductor quantum dots (QDs) are well established as sub-Poissonian sources of entangled photon pairs. To improve the utility of a QD light source, it would be advantageous to extend their emission further into the near infrared, into the low absorption wavelength windows utilised in long-haul optical telecommunication. Initial experiments succeeded in interfering O-band (1260—1360 nm) photons from an InAs/GaAs QD with dissimilar photons from a laser, an important mechanism for quantum teleportation. Interference visibilities as high as 60 ± 6 % were recorded, surpassing the 50 % threshold imposed by classical electrodynamics. Later, polarisation-entanglement of a similar QD was observed, with pairs of telecom-wavelength photons from the radiative cascade of the biexciton state exhibiting fidelities of 92.0 ± 0.2 % to the Bell state. Subsequently, an O-band telecom-wavelength quantum relay was realised. Again using an InAs/GaAs QD device, this represents the first implementation of a sub-Poissonian telecom-wavelength quantum relay, to the best knowledge of the author. The relay proved capable of implementing the famous four-state BB84 protocol, with a mean teleportation fidelity as high as 94.5 ± 2.2 %, which would contribute 0.385 secure bits per teleported qubit. After characterisation by way of quantum process tomography, the performance of the relay was also evaluated to be capable of implementing a six-state QKD protocol. In an effort to further extend the emitted light from a QD into the telecom C-band (1530—1565 nm), alternative material systems were investigated. InAs QDs on a substrate of InP were shown to emit much more readily in the fibre-telecom O- and C-bands than their InAs/GaAs counterparts, largely due to the reduced lattice mismatch between the QD and substrate for InAs/InP (~3 %) compared to InAs/GaAs (~7 %). Additionally, to minimize the fine structure splitting (FSS) of the exciton level, which deteriorates the observed polarisation-entanglement, a new mode of dot growth was investigated. Known as droplet epitaxy (D-E), QDs grown in this mode showed a fourfold reduction in the FSS compared to dots grown in the Stranski-Krastanow mode. This improvement would allow observation of polarisation-entanglement in the telecom C-band. In subsequent work performed by colleagues at the Toshiba Cambridge Research Labs, these D-E QDs were embedded in a p-i-n doped optical cavity, processed with electrical contacts, and found to emit entangled pairs of photons under electrical excitation. The work of this thesis provides considerable technological advances to the field of entangled-light sources, that in the near future may allow for deterministic quantum repeaters operating at megahertz rates, and in the further future could facilitate the distribution of coherent multipartite states across a distributed quantum network.

[pt] O bunching de fótons é um dos mais celebrados efeitos de interferência de dois fóotons, associado à tendéncia de fótons indistinguíveis de tomarem o mesmo caminho quando há uma superposição dos pacotes de onda em um combinador de feixes óptico simétrico. Nós exploramos o fenômeno de interferência de dois fótons e mostramos que: a característica espectral de uma fonte de luz pode ser determinar através da técnica de Espectroscopia de Transformada de Fourier de Poucos Fótons de alta resolução que se mostra como uma técnica útil para a caracterização espectral de fontes ópticas débeis abaixo do limite coberto por técnicas clássicas de batimento heteródino; uma fonte de fótons com estatística sub-Poisson, a Fonte de Fótons Anunciadas com Óptica Linear, pode ser construída baseada apenas em óptica linear e estados coerentes atenuados uma vez que os anúncios sejam sintonizados nos picos de coincidência de um interferograma de Hong-Ou-Mandei quando o interferômetro é alimentado com estados em frequências diferentes; uma modificação do interferômetro de Hong-Ou-Mandel produz um aumento no número de coincidências, ao invés de sua diminuição, quando os pacotes de onda estão perfeitamente superpostos no interferômetro e o anúncio de fótons sintonizados nesse pico gera um feixe com distribuição sub-Poisson. A descrição matemática de cada experimento é detalhada e uma revisão extensa das ferramentas teóricas e práticas necessárias para o entendimento dos resultados é apresentada. / [en] Photon bunching is one of the most celebrated effects of two-photon interference, related to the tendency of indistinguishable photons to take the same path when there is a wave-packet overlapping in a symmetric beam splitter. Photon antibunching, the counterpart of photon bunching is, on turn, a desired effect in many applications such as single-photon generation. We explore the two-photon interference phenomena and show that: the spectral characteristics of a light source can be determined with a high resolution Few-Photon Fourier Transform Spectroscopy which proves to be a useful asset for spectral characterization of faint optical sources below the range covered by classical heterodyne beating techniques; a sub-Poisson photon source, the Linear-Optic Heralded Photon Source, can be constructed based only on linear optics and weak coherent states by time-tuning a Hong-Ou-Mandel interferometer fed with frequency-displaced coherent states and yields a second-order correlation function at zero time below one; a modified version a the Hong-Ou-Mandel interferometer produces a peak of coincidences instead of dip when the wave-packets are perfectly overlapped and the announcement of photons time-tuned to this coincidence peak yield an antibunched photon stream. The mathematical description of each experiment is detailed and an extensive review of the most important theoretical and practical tools for understanding of the results is presented.