3 Maggio 2005, IEN Galileo Ferraris Anno Mondiale della Fisica L’eredità di Einstein

1. Giacomo Mauro D’Ariano Università degli Studi di Pavia Recenti sviluppi della Meccanica Quantistica: dalla tomografia quantistica alla caratterizazione dei rivelatori quantistici • 3 Maggio 2005,IEN Galileo Ferraris • Anno Mondiale della Fisica • L’eredità di Einstein • Alcuni recenti progressi

2. “Measuring” the quantum state

3. The quantum state • It contains the whole information in-principle available on the system. • Quantum complementarity forbids to obtain all the possible information from the same measurement: if we are measuring the wave aspects of the system, we are missing out on all its particle aspects. • Thus, to recover the state, we need to perform a set of incompatible measures on an ensemble of equally prepared systems.

4. Pre-history: “measuring” the state Wolfgang Pauli [1958]:The mathematical problem, as to whether for given functions W(q) and W(p) the wave function ψ, if such function exists is always uniquely determined, has still not been investigated in all its generality.

5. Pre-history: “measuring” the state Eugene Paul Wigner [1983]:There is no way to determine what the wave function (or state vector) of a system is— if arbitrarily given,there is no way to “measure” its wave function. Clearly, such a measurement would have to result in a function of several variables, not in a relatively small set of numbers ... In order to verify the [quantum] theory in its generality, at least a succession of two measurements are needed. There is in general no way to determine the original state of the system, but having produced a definite state by a first measurement, the probabilities of the outcomes of a second measurement are then given by the theory.

6. Pre-history: “measuring” the state Bernard d’Espagnat [1976]: The question of determining which operators correspond to observables and which do not is a very difficult one. At the present time, no satisfactory answer appears to be known. Neverthless, it is interesting to investigate the relationship of this question to another, similar one: “What are the systems whose density matrices are measurable?” Should we, for instance, say that if a given type of systems corresponding to a given Hilbert space has a measurable density matrix, then all the Hermitean operators defined on that space are measurable? And is the reverse proposition true? What do we mean when we say that the density matrix corresponding to a given type of system is measurable? Let an ensemble E of a sufficiently large number of this type be given. Let us first separate it into subensembles Eλ, the elements of which are chosen at random in E. If from the results of appropriate measurements on the Eλ, we can derive the value of every element of the matrix ρ that describes E in some fixed representation, we say that ρ is measurable.

7. “Measuring” the quantum state of a syngle system • O. Alter, and Y. Yamamoto, Inhibition of the Measurement of the Wave Function of a Single Quantum System in Repeated Weak Quantum Nondemolition Measurements, Phys. Rev. Lett. 74 4106 (1995). • Y. Aharonov, J. Anandan, L. Vaidman, Meaning of the Wave Function, Phys. Rev. A 47 4616 (1993); See also the Comment: W. G. Unruh, Reality and Measurement of the Wave Function, Phys. Rev. A 50 882 (1994). • M. Ueda and M. Kitagawa, Phys. Rev. Lett. Reversibility in Quantum Measurement Processes,68 3424 (1992). • A. Imamoglu, Logical Reversibility in Quantum-Nondemolition Measurements,Phys. Rev. A 47 R4577 (1993). • A. Royer, Reversible Quantum Measurements on a Spin 1/2 and Measuring the State of a Single System, Phys. Rev. Lett. 73 913 (1994); Errata, Phys. Rev. Lett. 74 1040 (1995). • G. M. D'Ariano and H. P. Yuen, On the Impossibility of Measuring the Wave Function of a Single Quantum System, Phys. Rev. Lett. 76 2832 (1996) [NO CLONING]

8. “Measuring” the quantum state • No cloning theorem <---> It is impossible to determine the state of a single quantum system. • To “measure the state” we need an ensemble of equally prepared identical quantum systems.

9. “Measuring” the quantum state • How to measure concretely the matrix elements of the quantum state? • In order to determine the density matrix, one needs to measure a “complete” set of observables, the quorum, [Fano, d’Espagnat, Royer,...] • The problem remained at the level of mere speculation for many years... • It entered the realm of experiments only in 1994, after the experiments by Raymer’s group in the domain of Quantum Optics.

10. “Measuring” the quantum state • For particles, it is difficult to devise concretely measurable translational observables—other than position, momentum and energy. • Quantum optics: unique opportunity of measuring all possible linear combinations of position Q and momentum Pof a harmonic oscillator, here a mode of the electromagnetic field. • Such a measurement is achieved by means of a balanced homodyne detector, which measures the quadrature of the field at any desired phase with respect to the local oscillator (LO).

11. Homodyne Detector

12. Homodyne Tomography K. Vogel, H. Risken, Phys. Rev. A 40 2847 (1989)

13. Homodyne Tomography

14. Problems with the Radon transform • The inverse Radon transform is nonanalytical • One needs a cutoff, which gives an uncontrollable bias in the matrix elements

15. Exact method It is possible to bypass the Radon transform and obtain the density matrix elements by simply averaging suitable functions on homodyne outcomes G. M. D'Ariano, C. Macchiavello and M. G. A. Paris, Phys. Rev. A 50 4298 (1994)

16. In the same way different representations of the state can be “experimentally” inequivalent Exact method Measurement statistical errors on the density matrix elements can make them useless for the estimation of ensemble averages

17. Exact method Robust to noise, such as gaussian noise from loss or nonunit quantum efficiency Bound for quantum efficiency for estimation of the density matrix in the Fock basis

18. Exact method G. M. D'Ariano, U. Leonhardt and H. Paul, Phys. Rev. A 52 R1801 (1995)

21. Exact method Multimode field: full joint multimode density matrix via random scan over LO modes G. D'Ariano, P. Kumar, M. Sacchi, Phys. Rev. A 61, 13806 (2000)

22. Tomography of a twin beam M. Vasilyev, S.-K. Choi, P. Kumar, and G. M. D'Ariano, Phys. Rev. Lett. 84 2354 (2000)

23. Tomography of a twin beam M. Vasilyev, S.-K. Choi, P. Kumar, and G. M. D'Ariano, Phys. Rev. Lett. 84 2354 (2000) Marginal distributions for the signal and idler beams

24. Tomography of a twin beam

25. Exact method: adaptive techniques The estimators are not unique, and can be “adapted” to data to minimize the rms error G. M. D'Ariano and M. G. A. Paris, Phys. Rev. A 60 518 (1999)

26. Max-likelihood techniques Maximize the likelihood function of data Positivity constraint via Cholesky decomposition Statistically optimally efficient! Drawbacks: exponential complexity with the number of modes; estimation of parameters of the density operator only K. Banaszek, G. M. D'Ariano, M. G. A. Paris, M. Sacchi, Phys. Rev. A 61, 010304 (2000) (rapid communication)

27. Angular momentum tomography G. M. D'Ariano, L. Maccone, and M. Paini , J. Opt. B 577 (2003)

28. General approach: theory of operator frames (frames on Banach spaces): the operator form of wavelet theory General quantum tomography G. M. D'Ariano, Scuola "E. Fermi" on Experimental Quantum Computation and Information,  F. De Martini and C. Monroe eds. (IOS Press, Amsterdam 2002) pag. 385.

29. General quantum tomography • Any quantum system • Any observable • Many modes, or many quantum systems • Unbiasing noise ... The method is very powerful: G. M. D'Ariano, Scuola "E. Fermi" on Experimental Quantum Computation and Information,  F. De Martini and C. Monroe eds. (IOS Press, Amsterdam 2002) pag. 385.

30. Pauli Tomography

31. Tomography of quantum operation of a device

32. Tomography of quantum operation of a device G. M. D'Ariano, and P. Lo Presti, Phys. Rev. Lett. 86 4195 (2001)

33. Tomography of quantum operation of a device Fork scheme Twin beam

34. Tomography of quantum operation of a device F. De Martini, M. D'Ariano, A. Mazzei, and M. Ricci, Phys. Rev. A 87 062307 (2003)

35. Tomography of quantum operation of a device F. De Martini, M. D'Ariano, A. Mazzei, and M. Ricci, Phys. Rev. A 87 062307 (2003)

36. Tomography of quantum operation of a device Faithful states • Is it possible to make a tomography of a quantum operation using entangled mixed states, or even separable states? • Answer: yes! as long as the state is faithful.

37. Tomography of quantum operation of a device Faithful states M. D'Ariano and P. Lo Presti,Phys. Rev. Lett. 91 047902-1 (2003)

38. Tomography of quantum operation of a device M. D'Ariano and P. Lo Presti,Phys. Rev. Lett. 91 047902-1 (2003)

39. Tomography of quantum operation of a device M. D'Ariano and P. Lo Presti,Phys. Rev. Lett. 91 047902-1 (2003)

40. Quantum Calibration We can perform a complete quantum calibrationof a measuring apparatus experimentally, without knowing its functioning!

41. Quantum Calibration How we describe a measuring apparatus?

42. pre calibration Quantum Calibration G. M. D'Ariano, P. Lo Presti, and L. Maccone, Phys. Rev. Lett. 93 250407 (2004)

43. Quantum calibration of a photocounter G. M. D'Ariano, P. Lo Presti, and L. Maccone, Phys. Rev. Lett. 93 250407 (2004)

44. Quantum calibration of a photocounter G. M. D'Ariano, P. Lo Presti, and L. Maccone, Phys. Rev. Lett. 93 250407 (2004)

45. G. M. D’Ariano and L. Maccone (submitted to Discrete Tomography and Applications, N.Y. City, June 13-15(2005) Quantum tomography for imaging

46. Conclusions • Quantum tomography is a method to measure experimentally the quantum state, or any ensemble average. • There is a setup for any quantum system. • Robust to noise. • Statistically efficient. • Can be used for fully calibrating devices and measuring apparatuses. Robust to input state. • Maybe useful also for ACT.

47. www.qubit.it

48. THE END