Table of Links
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III. EXPERIMENTAL SETUP
The laser (TOPTICA-TopMode 405) with a center wavelength of 405 nm and bandwidth of 0.01 pm emits a Gaussian beam. The beam passes through a half-wave plate (HWP) followed by a polarising beam splitter (PB...
Table of Links
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III. EXPERIMENTAL SETUP
The laser (TOPTICA-TopMode 405) with a center wavelength of 405 nm and bandwidth of 0.01 pm emits a Gaussian beam. The beam passes through a half-wave plate (HWP) followed by a polarising beam splitter (PBS). This combination gives a control over the intensity of the beam. A 50cm lens (L1) is used to focus the beam on a Type-I Bismuth Borate (BiBO) crystal of length 5 mm. The pump power before the nonlinear crystal is 5 mW. Two correlated degenerate spontaneous parametric down-converted photons are generated in the crystal in a non-collinear geometry assisted via angle tuning. The photon pairs are collimated by a 10 cm lens (L2) and separated by a prism mirror (PM) to interfere in a Mach Zehnder like setup as shown in Fig. 1. In one of the paths, a motorized translation stage MTS25-Z8, with a resolution of 29 nm, is added to compensate for the extra delay, if any. The two output ports of the beam splitter are initially used to show a HOM dip [29] as shown in Fig. 2.
\ Once the two polarisation entangled qubits are generated as described in the theoretical section, one can simply detect one of the qubits in the detector following path “X”. The other qubit is measured in H-V polarisation basis (path “Y” and “Z”). Measuring this other qubit in coincidence with the photon in path “X” generates random numbers as it gets detected either in the H polarisation (bit 0) or V polarisation (bit 1) at a particular instant with a 50:50 probability as shown in Fig. 1 (c) .The detectors (SPCM-800-14FC with a dark count of 100 counts per second) are identical in all three arms. To see measurement-device independence on the detector side, the diagram of the setup is slightly modified after the beam splitter to take projective measurements using quarter wave plate (QWP), HWP and a PBS combination as shown in Fig. 1 (a). On the contrary, to show the source independence, HOM curve is used as a certification technique. it’s visibility serves as a parameter for source-independence. Thus, a high visibility of the HOM curve is desired. In our case, we achieved a visibility of 97%. Since no phase information is required to generate bit streams, random bit-streams generated from maximally mixed state of a bipartite system and single photon source are identical. The extra phase information in the entangled case helps in providing security against attacks on the source. After calibration of data points A and B (as highlighted in Fig. 2) using the HOM curve, we generate entangled states at these data points.
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IV. RESULTS AND DISCUSSION
In this study, we have generated two datasets of 4.5 million (M) bit streams from the experimental setup shown in Fig. 1. The data is recorded for two different cases: Dataset A is recorded at the point of highest visibility of the HOM curve of Fig. 2), which represents a maximally entangled state, and Dataset B is recorded 700 nm away from dip point which degrades the quality of the above entangled quantum state. After post-processing using Toeplitz hash function, the length of random numbers is reduced from 4.5 M to 1.2 M.
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\ The datasets are tested against NIST-STS for quality of statistical randomness, and the results are highlighted in Table I. Kolmogorov-Smirnov test (KS test) is performed on sets with
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\ multiple p-values to provide an overall p-value indicating that they are normally distributed. Every test in Table I, shows a test-static p ≥ 0.01, suggesting that the generated dataset is statistically random.
\ The dataset A and B are obtained from two different quantum states, therefore having different “quantum information”. Here, we have used CHSH inequality (S) as one such quantifier of entanglement, as given in Eq. (2). The CHSH violation is measured from the direct observation as discussed in Ref. [13] and alternatively by estimating the density matrix using Bayesian and MLE quantum state tomographic techniques as in Ref.[26, 27].
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\ The results in Table I indicate a high confidence that both the datasets have statistically independent random bit-streams. Additionally, the results shown in Table II, prove the quantum correlation. The table, although indicating quantum signature, shows some inconsistency amongst different values. This discrepancy arises due to two reasons. One that Bayesian estimation is better than MLE in cases where right prior is known (Dataset A in our case). Secondly, the effect of sampling can bias the Bayesian estimation (Dataset B in our case).
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\ For Dataset B, right prior is not known. This requires further investigation. However, the result provided in this study positively concludes that the QRNG developed using entangled polarisation entangled photon pair is statistically random and secure against source and detector side attacks as indicated by HOM dip visibility and CHSH value respectively. A contrasting difference between our technique and randomness expansion protocols is that we have performed sequential measurements bunched together for a quantum correlation quantifier, while the semi-device independent protocols sparse them in generation and test rounds with some bias picked from a quantum source.
\ One open problem with random numbers is to investigate whether unpredictability and statistical properties are interrelated. To address this query, we performed scrambling operations at different lengths. One can use a quantifier from information theory, specifically min-entropy [30], defined as:
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V. CONCLUSION
In this article, we have provided a sanity check of the quantum source (HOM dip) and investigated the working of a fully device-independent quantum random number generator. One can put a constraint on resources and translate the fully deviceindependent scheme to measurement device-independent or source-independent quantum random number generator protocols with automation of HWPs and calculation of smooth conditional min-entropy (based on density matrix). Other quantifiers like entanglement measure/witness can be used to define new protocols in semi-device independent regime or for higher dimensions. Also, it is theoretically proven that the visibility of the HOM curve is equal to the purity of input photons [31]. This provides a correlation between closeness to the dip point and the amount of CHSH Bell violation as indicated by Table II. Physically, it means that relative phase information between two photons is used to prove device independence and thus, preventing attacks on QRNGs from Eve. Here device independence checks can be relaxed to cases where HOM serves as a check for source independence or CHSH Bell parameter serves as a security check for measurement device independence. Sending the qubit which is being traced out here, to another party, post-processing to consider loss over the channel and together with the addition of local operations using classical communication (LOCC) can convert this random number generation scheme to device-independent quantum key distribution scheme.
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:::info Authors:
(1) Vardaan Mongia, Quantum Science and Technology Laboratory, Physical Research Laboratory, Ahmedabad, 380009, India and Dept. of Physics, Indian Institute of Technology Gandhinagar, Gujarat, 382355, India;
(2) Abhishek Kumar, Space Weather Laboratory, Physical Research Laboratory, Ahmedabad, 380009, India;
(3) Shashi Prabhakar, Quantum Science and Technology Laboratory, Physical Research Laboratory, Ahmedabad, 380009, India;
(4) Anindya Banerji, Center for Quantum Technologies, National University of Singapore, Singapore 117543;
(5) R.P. Singh, Quantum Science and Technology Laboratory, Physical Research Laboratory, Ahmedabad, 380009, India.
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:::info This paper is available on arxiv under CC BY 4.0 DEED license.
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