Towards higher precision and operational use of optical homodyne tomograms

We present the results of an operational use of experimentally measured optical tomograms to determine state characteristics (purity) avoiding any reconstruction of quasiprobabilities. We also develop a natural way how to estimate the errors (including both statistical and systematic ones) by an analysis of the experimental data themselves. Precision of the experiment can be increased by postselecting the data with minimal (systematic) errors. We demonstrate those techniques by considering coherent and photon-added coherent states measured via the time-domain improved homodyne detection. The operational use and precision of the data allowed us to

[1]  Gerard 't Hooft Determinism in Free Bosons , 2001 .

[2]  O'Connell,et al.  Necessary and sufficient conditions for a phase-space function to be a Wigner distribution. , 1986, Physical review. A, General physics.

[3]  J. Fiurášek,et al.  A high-fidelity noiseless amplifier for quantum light states , 2010, 1004.3399.

[4]  Optical tomography of photon-added coherent states, even and odd coherent states, and thermal states , 2011, 1102.1067.

[5]  Alessandro Zavatta,et al.  Probing Quantum Commutation Rules by Addition and Subtraction of Single Photons to/from a Light Field , 2007, Science.

[6]  V. Dodonov Upper bounds on the relative energy difference of pure and mixed Gaussian states with a fixed fidelity , 2011, 1112.2308.

[7]  Beck,et al.  Measurement of the Wigner distribution and the density matrix of a light mode using optical homodyne tomography: Application to squeezed states and the vacuum. , 1993, Physical review letters.

[8]  Iwo Bialynicki-Birula Formulation of the uncertainty relations in terms of the Rényi entropies , 2006 .

[9]  Granino A. Korn,et al.  Mathematical handbook for scientists and engineers. Definitions, theorems, and formulas for reference and review , 1968 .

[10]  Alessandro Zavatta,et al.  Experimental nonclassicality of single-photon-added thermal light states , 2007, 0704.0179.

[11]  Fidelity for qubits and photon states in tomographic probability representation , 2009 .

[12]  V. Man'ko,et al.  Optical tomography of Fock state superpositions , 2011, 1101.1689.

[13]  D. W. Scott On optimal and data based histograms , 1979 .

[14]  V. Dodonov REVIEW ARTICLE: `Nonclassical' states in quantum optics: a `squeezed' review of the first 75 years , 2002 .

[15]  Positive-type functions on groups and new inequalities in classical and quantum mechanics , 2010 .

[16]  Alfréd Rényi,et al.  Probability Theory , 1970 .

[17]  A. Furusawa,et al.  Optical homodyne tomography with polynomial series expansion , 2011, 1107.0526.

[18]  D. A. Trifonov Generalizations of Heisenberg uncertainty relation , 2001 .

[19]  H. Paul,et al.  Measuring the quantum state of light , 1997 .

[20]  V. Man'ko,et al.  Distances between quantum states in the tomographic-probability representation , 2009, 0911.1414.

[21]  Vogel,et al.  Determination of quasiprobability distributions in terms of probability distributions for the rotated quadrature phase. , 1989, Physical review. A, General physics.

[22]  State extended uncertainty relations , 2000, quant-ph/0005086.

[23]  W. Heisenberg Über den anschaulichen Inhalt der quantentheoretischen Kinematik und Mechanik , 1927 .

[24]  S. Solimeno,et al.  Homodyne estimation of quantum state purity by exploiting the covariant uncertainty relation , 2010, 1012.3297.

[25]  E. Wigner On the quantum correction for thermodynamic equilibrium , 1932 .

[26]  Michael G. Raymer,et al.  Sampling of photon statistics and density matrix using homodyne detection , 1996 .

[27]  Ł. Rudnicki Shannon entropy as a measure of uncertainty in positions and momenta , 2011, 1108.3828.

[28]  M. Kim,et al.  Experimental demonstration of the bosonic commutation relation via superpositions of quantum operations on thermal light fields. , 2009, Physical review letters.

[29]  V. Man'ko,et al.  Measuring microwave quantum states: tomogram and moments , 2011, 1104.3857.

[30]  I. Bialynicki-Birula,et al.  Uncertainty relations for information entropy in wave mechanics , 1975 .

[31]  Alessandro Zavatta,et al.  Non-classical field characterization by high-frequency, time-domain quantum homodyne tomography , 2005 .

[32]  G. Hooft How a wave function can collapse without violating Schroedinger's equation, and how to understand Born's rule , 2011, 1112.1811.

[33]  A. Toigo,et al.  Quantum homodyne tomography as an informationally complete positive-operator-valued measure , 2008, 0807.3437.

[34]  V. Dodonov Comparing energy difference and fidelity of quantum states , 2011, 1112.4200.

[35]  M. Markov Invariants and the evolution of nonstationary quantum systems , 1989 .

[36]  V. Man'ko,et al.  Dynamic symmetries and entropic inequalities in the probability representation of quantum mechanics , 2011, 1102.2497.

[37]  Francesco Marin,et al.  Time-domain analysis of quantum states of light: noise characterization and homodyne tomography , 2002 .

[38]  M. Bellini,et al.  Quantum-to-Classical Transition with Single-Photon-Added Coherent States of Light , 2004, Science.

[39]  V. Man'ko,et al.  Probability Description and Entropy of Classical and Quantum Systems , 2011 .

[40]  M. A. Marchiolli,et al.  Dynamical squeezing of photon-added coherent states , 1998 .

[41]  Z. Hradil Quantum-state estimation , 1996, quant-ph/9609012.

[42]  M. A. Man'ko Entropic inequalities in classical and quantum domains , 2010 .

[43]  W. Vogel,et al.  Nonclassicality quasiprobability of single-photon-added thermal states , 2011, 1101.1741.

[44]  V. I. Man'ko,et al.  Symplectic tomography as classical approach to quantum systems , 1996 .

[45]  V. Pereira,et al.  Quantum Statistics of the Squeezed Vacuum by Measurement of the Density Matrix in the Number State Representation. , 1996, Physical review letters.

[46]  M. Bellini,et al.  Single-photon excitation of a coherent state: Catching the elementary step of stimulated light emission , 2005, quant-ph/0508094.

[47]  A. Lvovsky,et al.  Continuous-variable optical quantum-state tomography , 2009 .

[48]  I. Hirschman,et al.  A Note on Entropy , 1957 .

[49]  E. Sudarshan,et al.  Does the uncertainty relation determine the quantum state , 2006, quant-ph/0604044.

[50]  G. Agarwal,et al.  Nonclassical properties of states generated by the excitations on a coherent state , 1991 .

[51]  V. Man'ko,et al.  Two-mode optical tomograms: a possible experimental check of the Robertson uncertainty relations , 2012, 1202.0434.

[52]  Probability representation and state-extended uncertainty relations , 2011 .

[53]  S. Olivares,et al.  Full characterization of Gaussian bipartite entangled states by a single homodyne detector. , 2008, Physical review letters.

[54]  New uncertainty relations for tomographic entropy: application to squeezed states and solitons , 2006, quant-ph/0607200.

[55]  M. Kim,et al.  Scheme for proving the bosonic commutation relation using single-photon interference. , 2008, Physical review letters.

[56]  How can we check the uncertainty relation , 2012, 1201.6628.

[57]  Timothy C. Ralph,et al.  A Guide to Experiments in Quantum Optics , 1998 .

[58]  M. Bellini,et al.  Implementation of single-photon creation and annihilation operators: experimental issues in their application to thermal states of light , 2009 .

[59]  A. Ibort,et al.  An introduction to the tomographic picture of quantum mechanics , 2009, 0904.4439.

[60]  Cleve Moler,et al.  Mathematical Handbook for Scientists and Engineers , 1961 .

[61]  V. Man'ko,et al.  A possible experimental check of the uncertainty relations by means of homodyne measuring photon quadrature , 2008, 0811.4115.