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arXiv:quant-ph/0608066 · Physical Review A

Interaction-free measurement with an imperfect absorber

Hiroo Azuma

Published Nov 17, 2006• 13 citations
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Abstract

We consider interaction-free measurement (IFM) with imperfect interaction. In the IFM proposed by Kwiat et al., we assume that the interaction between an absorbing object and a probe photon is imperfect, so that the photon is absorbed with probability $1\ensuremath{-}\ensuremath{\eta}$ $(0\ensuremath{\leqslant}\ensuremath{\eta}\ensuremath{\leqslant}1)$ and it passes by the object without being absorbed with probability $\ensuremath{\eta}$ when it approaches close to the object. We derive the success probability $P$ that we can find the object without the photon absorbed under the imperfect interaction as a power series in $1∕N$ and show the following result: Even if the interaction between the object and photon is imperfect, we can let the success probability $P$ of the IFM get close to unity arbitrarily by making the reflectivity of the beam splitter larger and increasing the number of the beam splitters. Moreover, we obtain an approximating equation of $P$ for large $N$ from the derived power series in $1∕N$.

DOI
10.1103/physreva.74.054301

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We consider interaction-free measurement (IFM) with imperfect interaction. In the IFM proposed by Kwiat et al., we assume that the interaction between an absorbing object and a probe photon is imperfect, so that the photon is absorbed with probability 1\ensuremath−\ensuremathη1\ensuremath{-}\ensuremath{\eta}1\ensuremath−\ensuremathη (0\ensuremath⩽\ensuremathη\ensuremath⩽1)(0\ensuremath{\leqslant}\ensuremath{\eta}\ensuremath{\leqslant}1)(0\ensuremath⩽\ensuremathη\ensuremath⩽1) and it passes by the object without being absorbed with probability \ensuremathη\ensuremath{\eta}\ensuremathη when it approaches close to the object. We derive the success probability PPP that we can find the object without the photon absorbed under the imperfect interaction as a power series in 1∕N1∕N1∕N and show the following result: Even if the interaction between the object and photon is imperfect, we can let the success probability PPP of the IFM get close to unity arbitrarily by making the reflectivity of the beam splitter larger and increasing the number of the beam splitters. Moreover, we obtain an approximating equation of PPP for large NNN from the derived power series in 1∕N1∕N1∕N.
In this paper, we consider interaction-free measurement (IFM) with imperfect interaction. In the IFM proposed by Kwiat et al., we assume that interaction between an absorbing object and a probe photon is imperfect, so that the photon is absorbed with probability 1-\\eta (0\\leq\\eta\\leq 1) and it passes by the object without being absorbed with probability \\eta when it approaches close to the object. We derive the success probability P that we can find the object without the photon absorbed under the imperfect interaction as a power series in 1/N, and show the following result: Even if the interaction between the object and the photon is imperfect, we can let the success probability P of the IFM get close to unity arbitrarily by making the reflectivity of the beam splitter larger and increasing the number of the beam splitters. Moreover, we obtain an approximating equation of P from the derived power series in 1/N.
Recently, it has been pointed out that it is possible to make a quantum-mechanical interaction-free measurement (IFM), in which the existence of an object in a given region of space may be determined seemingly without interacting with it.1,2 In the embodiment first proposed by Elitzur and Vaidman,3 a standard Michelson interferometer is aligned so that incident single photons (obtained in our experiment by using parametric downconversion; see Fig. 1) must exit by the same port in which they entered, in the absence of any object within the interferometer. The presence of an object (e.g., the mirror leading to detector DB) in one of the arms completely changes the possible outcomes because the constructive interference is interrupted. Now it is possible that the photon will exit from the other exit port, to detector DIfm. By detecting the photon in this case, one can claim with certainty that an object was within the interferometer, even though the photon could not have interacted with it. If the beam splitter has a very low reflectivity, then the fraction of IFMs approaches 1/2.
"Interaction-free measurements" (IFM) originate from the latest quantum interferometric technologies. The latest research of quantum optics demonstrates, by using the complementary wavelike and particlelike natures of photons, it is possible to make interaction-free measurements by which the presence of an object can be determined with no photons being absorbed. The paper introduces the concept of "Interaction-free Measurement" (IFM), the original Elitzur-Vaidman scheme, the "High Efficiency Interaction-free Measurement", the application of quantum Zeno effect and the improved scheme proposed by Kwiat et al. The EV scheme is implemented in a Mach-Zehnder interferometer. Theoretically this paper also draws a conclusion in IFM feasibility by analyzing the wave functions of photon at various locations in the interferometer.
Summary form only given.The purpose of an interaction-free measurement is to detect the presence of an object without letting any energy quanta be absorbed by the object. In this work we present interaction-free measurement results using a Fabry-Perot interferometer as a measurement apparatus. If the cavity of the interferometer is empty, an incoming photon will be transmitted through the interferometer. If an absorbent is placed between the mirrors, the photon will be reflected by the first mirror. By detecting which way the photon takes, we will gain information about the presence of the absorbent without losses/interaction. For a perfect measurement, the figure of merit will be equal to the mirror reflectivity R. Thus, in theory, one can approach the perfect interaction-free measurement simply by increasing R.
It is now well-understood that the complementary wave- and particle-like natures of quanta enable one to make measurements that are “interaction-free” -- one can determine the presence or absence of an object, even a completely absorbing object, without any photons being absorbed. The first proposal of such a scheme was limited to an efficiency of 50% -- at most half of the measurements could be interaction free [1]. By using an application of the Quantum Zeno effect, one can in fact have the fraction of interaction-free measurements arbitrarily close to one [2].
Summary form only given.Using the complementary wave-like and particle-like natures of photons, one can make interaction-free measurements (IFM)-the presence of an object can be determined with no photons being absorbed. By using an application of the quantum Zeno effect (weakly and repeatedly testing for the object's presence so that the otherwise coherent evolution of the interrogating photon is inhibited), we have demonstrated the feasibility of IFMs with an efficiency of >85%, higher than that possible in the original IFM scheme, where, at most, half of the measurements could be interaction free. We also investigate various interaction-free imaging systems, demonstrate imaging with a resolution <5 /spl mu/m, and define the limits to these systems. We also discuss in which sense interaction-free measurements really are not.