{"id":3156,"date":"2015-03-10T06:12:39","date_gmt":"2015-03-10T06:12:39","guid":{"rendered":"http:\/\/revoscience.com\/en\/?p=3156"},"modified":"2015-03-10T06:12:39","modified_gmt":"2015-03-10T06:12:39","slug":"quantum-sensors-advantages-survive-entanglement-breakdown","status":"publish","type":"post","link":"https:\/\/www.revoscience.com\/en\/quantum-sensors-advantages-survive-entanglement-breakdown\/","title":{"rendered":"Quantum sensor\u2019s advantages survive entanglement breakdown"},"content":{"rendered":"

Preserving the fragile quantum property known as entanglement isn\u2019t necessary to reap benefits.<\/strong><\/em><\/span><\/p>\n

\"In<\/a>
In the researchers’ new system, a returning beam of light is mixed with a locally stored beam, and the correlation of their phase, or period of oscillation, helps remove noise caused by interactions with the environment.
Illustration: Jose-Luis Olivares\/MIT<\/figcaption><\/figure>\n

CAMBRIDGE, Mass. —\u00a0The extraordinary promise of quantum information processing \u2014 solving problems that classical computers can\u2019t, perfectly secure communication \u2014 depends on a phenomenon called \u201centanglement,\u201d in which the physical states of different quantum particles become interrelated. But entanglement is very fragile, and the difficulty of preserving it is a major obstacle to developing practical quantum information systems.<\/span><\/p>\n

In a series of papers since 2008, members of the Optical and Quantum Communications Group at MIT\u2019s Research Laboratory of Electronics have argued that optical systems that use entangled light can outperform classical optical systems \u2014 even when the entanglement breaks down.<\/span><\/p>\n

Two years ago, they\u00a0showed<\/span><\/a>\u00a0that systems that begin with entangled light could offer much more efficient means of securing optical communications. And now, in a paper appearing in\u00a0Physical Review Letters<\/em>, they demonstrate that entanglement can also improve the performance of optical sensors, even when it doesn\u2019t survive light\u2019s interaction with the environment.<\/span><\/p>\n

\u201cThat is something that has been missing in the understanding that a lot of people have in this field,\u201d says senior research scientist Franco Wong, one of the paper\u2019s co-authors and, together with Jeffrey Shapiro, the Julius A. Stratton Professor of Electrical Engineering, co-director of the Optical and Quantum Communications Group. \u201cThey feel that if unavoidable loss and noise make the light being measured look completely classical, then there\u2019s no benefit to starting out with something quantum. Because how can it help? And what this experiment shows is that yes, it can still help.\u201d<\/span><\/p>\n

Phased in<\/strong><\/span><\/p>\n

Entanglement means that the physical state of one particle constrains the possible states of another. Electrons, for instance, have a property called spin, which describes their magnetic orientation. If two electrons are orbiting an atom\u2019s nucleus at the same distance, they must have opposite spins. This spin entanglement can persist even if the electrons leave the atom\u2019s orbit, but interactions with the environment break it down quickly.<\/span><\/p>\n

In the MIT researchers\u2019 system, two beams of light are entangled, and one of them is stored locally \u2014 racing through an optical fiber \u2014 while the other is projected into the environment. When light from the projected beam \u2014 the \u201cprobe\u201d \u2014 is reflected back, it carries information about the objects it has encountered. But this light is also corrupted by the environmental influences that engineers call \u201cnoise.\u201d Recombining it with the locally stored beam helps suppress the noise, recovering the information.<\/span><\/p>\n

The local beam is useful for noise suppression because its phase is correlated with that of the probe. If you think of light as a wave, with regular crests and troughs, two beams are in phase if their crests and troughs coincide. If the crests of one are aligned with the troughs of the other, their phases are anti-correlated.<\/span><\/p>\n

But light can also be thought of as consisting of particles, or photons. And at the particle level, phase is a murkier concept.<\/span><\/p>\n

\u201cClassically, you can prepare beams that are completely opposite in phase, but this is only a valid concept on average,\u201d says Zheshen Zhang, a postdoc in the Optical and Quantum Communications Group and first author on the new paper. \u201cOn average, they\u2019re opposite in phase, but quantum mechanics does not allow you to precisely measure the phase of each individual photon.\u201d<\/span><\/p>\n

Improving the odds<\/strong><\/span><\/p>\n

Instead, quantum mechanics interprets phase statistically. Given particular measurements of two photons, from two separate beams of light, there\u2019s some probability that the phases of the beams are correlated. The more photons you measure, the greater your certainty that the beams are either correlated or not. With entangled beams, that certainty increases much more rapidly than it does with classical beams.<\/span><\/p>\n

When a probe beam interacts with the environment, the noise it accumulates also increases the uncertainty of the ensuing phase measurements. But that\u2019s as true of classical beams as it is of entangled beams. Because entangled beams start out with stronger correlations, even when noise causes them to fall back within classical limits, they still fare better than classical beams do under the same circumstances.<\/span><\/p>\n

\u201cGoing out to the target and reflecting and then coming back from the target attenuates the correlation between the probe and the reference beam by the same factor, regardless of whether you started out at the quantum limit or started out at the classical limit,\u201d Shapiro says. \u201cIf you started with the quantum case that\u2019s so many times bigger than the classical case, that relative advantage stays the same, even as both beams become classical due to the loss and the noise.\u201d<\/span><\/p>\n

In experiments that compared optical systems that used entangled light and classical light, the researchers found that the entangled-light systems increased the signal-to-noise ratio \u2014 a measure of how much information can be recaptured from the reflected probe \u2014 by 20 percent. That accorded very well with their theoretical predictions.<\/span><\/p>\n

But the theory also predicts that improvements in the quality of the optical equipment used in the experiment could double or perhaps even quadruple the signal-to-noise ratio. Since detection error declines exponentially with the signal-to-noise ratio, that could translate to a million-fold increase in sensitivity.<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"

Preserving the fragile quantum property known as entanglement isn\u2019t necessary to reap benefits. CAMBRIDGE, Mass. —\u00a0The extraordinary promise of quantum information processing \u2014 solving problems that classical computers can\u2019t, perfectly secure communication \u2014 depends on a phenomenon called \u201centanglement,\u201d in which the physical states of different quantum particles become interrelated. But entanglement is very fragile, […]<\/p>\n","protected":false},"author":6,"featured_media":3157,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[17],"tags":[],"class_list":["post-3156","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-research"],"featured_image_urls":{"full":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"thumbnail":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01-150x150.jpg",150,150,true],"medium":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01-300x200.jpg",300,200,true],"medium_large":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"large":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"1536x1536":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"2048x2048":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"ultp_layout_landscape_large":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"ultp_layout_landscape":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"ultp_layout_portrait":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",600,400,false],"ultp_layout_square":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",600,400,false],"newspaper-x-single-post":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"newspaper-x-recent-post-big":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",540,360,false],"newspaper-x-recent-post-list-image":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",95,63,false],"web-stories-poster-portrait":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",639,426,false],"web-stories-publisher-logo":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",96,64,false],"web-stories-thumbnail":["https:\/\/www.revoscience.com\/en\/wp-content\/uploads\/2015\/03\/MIT-Quantum-Sensor-01.jpg",150,100,false]},"author_info":{"info":["Amrita Tuladhar"]},"category_info":"Research<\/a>","tag_info":"Research","comment_count":"0","_links":{"self":[{"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/posts\/3156","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/users\/6"}],"replies":[{"embeddable":true,"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/comments?post=3156"}],"version-history":[{"count":0,"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/posts\/3156\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/media\/3157"}],"wp:attachment":[{"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/media?parent=3156"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/categories?post=3156"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.revoscience.com\/en\/wp-json\/wp\/v2\/tags?post=3156"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}