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	<title>biomedical imaging &#8211; Science</title>
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	<title>biomedical imaging &#8211; Science</title>
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		<title>Metasurface and Nanoparticle Screens Turn Infrared Light into Visible Images</title>
		<link>https://scienmag.com/metasurface-and-nanoparticle-screens-turn-infrared-light-into-visible-images/</link>
		
		<dc:creator><![CDATA[Denise Maddox]]></dc:creator>
		<pubDate>Sat, 12 Sep 2026 22:15:02 +0000</pubDate>
				<category><![CDATA[Technology and Engineering]]></category>
		<category><![CDATA[all-optical infrared imaging screens]]></category>
		<category><![CDATA[biomedical imaging]]></category>
		<category><![CDATA[chemical fingerprint imaging using nanostructures]]></category>
		<category><![CDATA[core-shell nanoparticles]]></category>
		<category><![CDATA[flat optics]]></category>
		<category><![CDATA[hybrid metasurface and nanoparticle architecture]]></category>
		<category><![CDATA[infrared imaging]]></category>
		<category><![CDATA[infrared imaging for telescopes and biomedical applications]]></category>
		<category><![CDATA[infrared to visible light conversion]]></category>
		<category><![CDATA[lanthanide nanoparticles]]></category>
		<category><![CDATA[light conversion]]></category>
		<category><![CDATA[low-cost infrared-to-visible conversion technologies]]></category>
		<category><![CDATA[metasurface-based optical imaging]]></category>
		<category><![CDATA[metasurfaces]]></category>
		<category><![CDATA[nanoparticle-assisted infrared upconversion]]></category>
		<category><![CDATA[nanoparticle-enhanced metasurface devices]]></category>
		<category><![CDATA[Nanophotonics]]></category>
		<category><![CDATA[night vision]]></category>
		<category><![CDATA[optical computing]]></category>
		<category><![CDATA[overcoming infrared detection limitations]]></category>
		<category><![CDATA[photoluminescence]]></category>
		<category><![CDATA[thermal signature detection with metasurfaces]]></category>
		<category><![CDATA[upconversion]]></category>
		<category><![CDATA[visible light emission from infrared photons]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=199140</guid>

					<description><![CDATA[Researchers have developed hybrid screens that combine metasurfaces with lanthanide-doped nanoparticles to convert infrared light directly into bright, processable visible images.]]></description>
										<content:encoded><![CDATA[<p>Infrared light is everywhere. It carries the heat signatures of living bodies, the chemical fingerprints of molecules, and the faint whispers of the universe arriving through telescopes. Yet the human eye, and nearly every consumer camera ever built, is blind to it. For decades, the standard workaround has been to convert infrared photons into electrical signals with specialized detectors, then reconstruct an image electronically. That approach works, but it is expensive, often requires cooling to cryogenic temperatures, and imposes a bottleneck between the optical world and the electronic readout. A research team reporting in Light: Science &amp; Applications has now demonstrated a fundamentally different route: an all-optical imaging screen that converts infrared light directly into visible light, using a hybrid architecture that pairs engineered metasurfaces with lanthanide-doped nanoparticles.</p>
<p>The concept behind the new work is known as infrared-to-visible upconversion. Instead of detecting infrared photons electronically, an upconversion device absorbs them and re-emits their energy at shorter, visible wavelengths, where ordinary silicon sensors and even the naked eye can see it. The trick has been demonstrated before in bulk crystals and optical fibers, but those systems typically demand intense laser pumping, operate only in narrow spectral bands, and offer little spatial control over the conversion process. The result is a technology that has remained largely confined to laboratory demonstrations rather than practical imaging systems. The new study tackles each of these limitations by rethinking the device at the level of nanostructure design.</p>
<p>At the heart of the approach are lanthanide-doped upconversion nanoparticles, most commonly built from a sodium yttrium fluoride host lattice doped with ions such as ytterbium and erbium or ytterbium and thulium. These ions form a cascade: the sensitizer ion, typically ytterbium, absorbs a near-infrared photon around 980 nanometers and transfers that energy stepwise to an activator ion, which accumulates the excitation and finally emits a visible photon. Because the energy levels of lanthanide ions are shielded by outer electron shells, the emission is sharp, stable, and remarkably resistant to photobleaching. The nanoparticles can be synthesized with controlled sizes and shell architectures, and core-shell designs that physically separate dopant ions suppress a major loss channel known as surface quenching, in which excitation energy leaks away at particle surfaces before it can produce light.</p>
<p>On their own, however, these nanoparticles are inefficient. The transitions that lanthanide ions undergo are formally forbidden by quantum-mechanical selection rules, which makes absorption weak, and the stepwise energy transfer process competes with numerous decay pathways. This is where the metasurface enters. A metasurface is a two-dimensional array of engineered nanostructures, often metallic or dielectric pillars and antennas, patterned at a scale smaller than the wavelength of light. By adjusting the geometry, spacing, and material composition of these building blocks, researchers can sculpt how light behaves at the surface: concentrating it into tiny volumes, redirecting it, filtering specific wavelengths, or imposing precise phase shifts across a wavefront. Metasurfaces have already revolutionized flat optics, enabling ultrathin lenses and holograms, and the new work harnesses that same design freedom to supercharge upconversion.</p>
<p>The hybrid screens described in the study integrate the two components so that the metasurface acts as an optical antenna system for the nanoparticles. Resonant modes supported by the metasurface trap incoming infrared light near the surface, dramatically increasing the local electromagnetic field intensity exactly where the nanoparticles sit. Because upconversion is a nonlinear process, in which the emission rate scales steeply with excitation intensity, even a modest field enhancement translates into a large boost in output. The metasurface can also be tuned to match the absorption bands of the sensitizer ions and to extract the emitted visible light efficiently, reducing the losses that would otherwise trap the upconverted photons inside the structure. The researchers report that this combined electromagnetic and photonic engineering yields imaging screens with substantially enhanced brightness and sensitivity compared with films of nanoparticles alone.</p>
<p>What elevates the work from a materials demonstration to an imaging technology is the spatial dimension. Because metasurfaces are patterned with lithographic precision, the hybrid screens can be designed to do more than simply brighten an image. The authors show that the screens can impose controlled phase and amplitude modifications on the upconverted visible light, effectively performing optical processing at the moment of conversion. In one configuration, the screen functions as a direct infrared imager: infrared light from a scene strikes the screen, is converted locally into visible emission, and the resulting visible image can be captured with an ordinary camera or viewed directly. In another configuration, the metasurface patterning enables edge enhancement, a computational imaging operation in which the outlines and boundaries of objects are emphasized, all performed passively in optics without any digital processing.</p>
<p>This ability to merge light conversion with analog optical computation in a single thin film points toward a compelling vision of the future of imaging. Conventional infrared cameras chain together optics, detectors, amplifiers, and processors, each stage adding cost, weight, latency, and power consumption. A hybrid upconversion screen collapses much of that chain into a passive optical element. The infrared image is converted, enhanced, and even pre-processed before a single electron is moved. Such screens could be produced as coatings on standard camera lenses, integrated into smartphone modules, or deployed as large-area viewing panels that make invisible laser beams, thermal signatures, or biomedical fluorescence directly visible to the eye.</p>
<p>The potential applications span an unusually wide range. In night vision, low-cost, uncooled upconversion screens could complement or replace bulky image intensifier tubes, offering a lighter and potentially cheaper alternative for both military and civilian use. In medicine, near-infrared light penetrates tissue more deeply than visible light and scatters less, and upconversion nanoparticles are already explored as imaging probes and as agents for light-triggered therapies; screens that convert scattered near-infrared light into visible images could improve surgical guidance and diagnostics. In telecommunications, silicon photonic circuits and optical fibers operate in the near-infrared, and efficient, fast upconversion could allow infrared signals to be inspected visually or routed with visible-light components. In industrial settings, the screens could reveal hot spots, gas absorption features, or defects that are invisible under ordinary illumination, while in fundamental research they could serve as diagnostic foils for characterizing infrared laser beams and photonic devices.</p>
<p>The authors are candid about the challenges that remain before such devices become routine. Upconversion efficiency, even with metasurface enhancement, still falls short of what high-speed, low-light imaging would demand, and the nonlinear nature of the process means performance degrades at low illumination levels, precisely where night-vision applications matter most. The spectral bandwidth of lanthanide-based conversion is inherently narrow, tied to the discrete energy levels of the ions, so covering the broader infrared spectrum, including the mid-infrared region where thermal imaging lives, will require different material combinations or multi-resonant metasurface designs. Response time is another consideration: the excited-state lifetimes that make lanthanides stable emitters also limit how quickly the screens can follow rapidly changing scenes. Scaling the nanofabrication from centimeter-scale laboratory samples to large, uniform, low-cost panels is an engineering task in its own right.</p>
<p>Nevertheless, the demonstration marks a meaningful step in the convergence of two of nanophotonics&#8217; most productive threads: flat metasurface optics and lanthanide luminescence. By treating the upconversion screen not as a passive phosphor but as an actively engineered optical element, the researchers have shown that the conversion of invisible light into visible images can be made brighter, more controllable, and more functional than previously imagined. If the efficiency and bandwidth gaps can be closed through continued materials and design refinement, hybrid metasurface-nanoparticle screens could reshape how we see the invisible half of the electromagnetic spectrum, turning infrared imaging from a specialized electronic undertaking into something as simple and ubiquitous as a sheet of smart glass.</p>
<p><strong>Subject of Research:</strong> Hybrid metasurface–lanthanide nanoparticle screens for enhanced infrared-to-visible upconversion imaging</p>
<p><strong>Article Title:</strong> Enhanced infrared-to-visible upconversion imaging via metasurface–lanthanide nanoparticle hybrid screens</p>
<p><strong>Article References:</strong> Sefidmooye Azar, N., Parry, M., Qi, X., Lee, C., Lee, W. S. L., Russell, B., Luo, W., de Gille, R. W., Nelson, D., Balendhran, S., Meng, J., Tan, H., Bonin, G. O., Choi, D.-Y., Schuck, P. J., Chan, E. M., Cohen, B. E., Neshev, D. N., &amp; Crozier, K. B. (2026). Enhanced infrared-to-visible upconversion imaging via metasurface–lanthanide nanoparticle hybrid screens. <em>Light: Science &amp;amp; Applications, 15</em>(1), Article 377. <a href="https://doi.org/10.1038/s41377-026-02449-5" rel="noopener noreferrer">https://doi.org/10.1038/s41377-026-02449-5</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1038/s41377-026-02449-5" rel="noopener noreferrer">10.1038/s41377-026-02449-5</a></p>
<p><strong>Keywords:</strong> upconversion, metasurfaces, lanthanide nanoparticles, infrared imaging, nanophotonics, night vision, optical computing, core-shell nanoparticles, photoluminescence, flat optics, biomedical imaging, light conversion</p>
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		<post-id xmlns="com-wordpress:feed-additions:1">199140</post-id>	</item>
		<item>
		<title>Digitized Laser Pulse Trains Offer Precise Control of Quantum Systems</title>
		<link>https://scienmag.com/digitized-laser-pulse-trains-offer-precise-control-of-quantum-systems/</link>
		
		<dc:creator><![CDATA[Katie Riggs]]></dc:creator>
		<pubDate>Sat, 12 Sep 2026 16:12:45 +0000</pubDate>
				<category><![CDATA[Mathematics]]></category>
		<category><![CDATA[adiabatic passage]]></category>
		<category><![CDATA[applications of digitized laser pulses in quantum computing]]></category>
		<category><![CDATA[biomedical imaging]]></category>
		<category><![CDATA[coherent control of atoms and molecules]]></category>
		<category><![CDATA[laser intensity effects on quantum systems]]></category>
		<category><![CDATA[laser pulse choreographing for quantum experiments]]></category>
		<category><![CDATA[laser pulse sequencing in quantum systems]]></category>
		<category><![CDATA[laser pulses]]></category>
		<category><![CDATA[laser-based quantum technology advancements]]></category>
		<category><![CDATA[molecular physics]]></category>
		<category><![CDATA[multiphoton processes]]></category>
		<category><![CDATA[novel methods in quantum control engineering]]></category>
		<category><![CDATA[precision quantum state manipulation]]></category>
		<category><![CDATA[Quantum Computing]]></category>
		<category><![CDATA[quantum control]]></category>
		<category><![CDATA[quantum information processing with laser pulses]]></category>
		<category><![CDATA[quantum laser pulse control]]></category>
		<category><![CDATA[Quantum sensing]]></category>
		<category><![CDATA[quantum states]]></category>
		<category><![CDATA[quantum system energy state engineering]]></category>
		<category><![CDATA[spectroscopy]]></category>
		<category><![CDATA[Stevens Institute of Technology]]></category>
		<category><![CDATA[Svetlana Malinovskaya]]></category>
		<category><![CDATA[weak laser pulses for quantum control]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=196171</guid>

					<description><![CDATA[Stevens Institute of Technology researchers have calculated that a train of twelve weak, precisely timed laser pulses can control quantum systems as effectively as one intense pulse, avoiding disruptive multiphoton processes.]]></description>
										<content:encoded><![CDATA[<p>Quantum technologies promise to transform medicine, sensing, computing and communications, but they all depend on a delicate feat of engineering: coaxing atoms and molecules into exactly the energy states a researcher wants, and no others. The standard tool for the job is the laser, whose tightly synchronized light waves can nudge quantum systems with extraordinary precision. Yet the very intensity that makes lasers so useful can also be their undoing. Now, researchers at Stevens Institute of Technology and their collaborators have proposed a novel way to sidestep this fundamental tension, using a carefully choreographed sequence of weak laser pulses to achieve what previously demanded a single, powerful blast of light.</p>
<p>The work, led by Svetlana Malinovskaya, professor at the Charles V. Schaefer, Jr. School of Engineering and Science at Stevens, addresses a problem that has long plagued experimentalists working at the frontier of quantum control. &#8220;A laser is a device that creates a very narrow, highly directional beam of light,&#8221; Malinovskaya explains. &#8220;Unlike sunlight or light from regular bulbs or flashlights that scatters in all directions, a laser produces light in which all waves move together in a highly synchronized way allowing the light to be very focused and controlled with remarkable precision.&#8221;</p>
<p>When such a light wave reaches a quantum system, its packets of energy, called photons, are absorbed by the atoms and molecules in that system, lifting them into higher-energy states. This is precisely the mechanism by which scientists manipulate quantum behavior. But there is a catch. If the laser field is too intense, a single atom or molecule may interact with several photons at once. These simultaneous interactions, known as multiphoton processes, open additional pathways between the system&#8217;s energy levels, scrambling the intended dynamics and rendering the quantum system difficult, sometimes impossible, to predict or control.</p>
<p>&#8220;By shining laser light on molecules, we can excite molecular vibrations in a controlled way and learn about molecular properties,&#8221; says Malinovskaya. &#8220;But when very strong laser fields are used for precise quantum control, they can also trigger unwanted multiphoton processes allowing the molecule to access many different states and pathways, making its behavior much more difficult to predict and control.&#8221; In other words, the instrument of control becomes an instrument of chaos, and the very act of measurement or manipulation contaminates the result.</p>
<p>That unpredictability is more than an inconvenience; it is a roadblock for the technologies hoping to capitalize on quantum mechanics. &#8220;That&#8217;s not what we need, particularly for the precision measurements required in quantum computing or quantum sensing,&#8221; Malinovskaya says. &#8220;In those systems, every photon counts.&#8221; Quantum computers rely on the faithful preparation and manipulation of quantum states to perform calculations, while quantum sensors extract exquisitely faint signals from their environment, and even a small number of stray photon interactions can corrupt a computation or drown a measurement in noise. The ideal solution would use just enough light to steer a quantum system where it needs to go, without any excess energy spilling over into unwanted channels.</p>
<p>In their new study, Malinovskaya and her collaborators propose to do exactly that with what they describe as a &#8220;digitized&#8221; laser pulse. Their calculations show that a train of twelve short, low-intensity laser pulses can produce the same net effect on a quantum system as one long, intense pulse, but without pushing the atoms or molecules into the undesirable states that plague high-intensity approaches. The idea is conceptually similar to replacing a single powerful hammer blow with a rapid series of precisely timed taps that, together, accomplish the same task with far less collateral disturbance.</p>
<p>&#8220;Instead of using one very strong laser pulse, we suggest mimicking its effects with a carefully programmed sequence—or train—of weak pulses,&#8221; Malinovskaya explains. &#8220;Each pulse carries much less energy, but its timing, intensity, frequency and phase are precisely calculated and controlled.&#8221; According to the team&#8217;s analysis, this sequence of gentle nudges can drive the same gradual transfer of a quantum system from one state to another that a much stronger pulse would produce. The desired outcome is preserved, while the laser intensity at each step remains low enough to keep multiphoton processes from ever gaining a foothold.</p>
<p>The method is an outgrowth of a well-established control strategy known as adiabatic passage, in which a quantum system is guided slowly and smoothly between energy states so that it remains stable against small imperfections. By digitizing that smooth evolution into discrete steps, the researchers retain the robustness of the adiabatic approach while shedding its traditional dependence on high peak laser intensities. The result, described in a paper titled &#8220;Digitizing ultrafast adiabatic passage with a pulse train&#8221; published in the Journal of the Optical Society of America B on September 10, 2026, offers a theoretical blueprint that, if borne out experimentally, could reshape how quantum control experiments are designed across a wide range of platforms.</p>
<p>The potential applications stretch across the quantum technology landscape. Quantum sensors, quantum computers and quantum simulators all depend on reliable preparation and manipulation of quantum states, and the pulse-train technique could make those operations more accurate and repeatable. In molecular physics and spectroscopy, where intense laser pulses often generate background effects that interfere with measurements, the lower-intensity approach could yield cleaner data and sharper insights into molecular structure and behavior. The implications extend beyond physics laboratories as well: in biology and medicine, laser-based technologies are widely used for imaging and disease diagnosis, and reducing pulse intensity offers a straightforward way to minimize damage to sensitive cells and tissues, opening a path to safer optical diagnostics and therapies.</p>
<p>For now, the technique remains theoretical, but the paper lays out all of the necessary calculations in full detail, providing experimenters with a concrete roadmap. &#8220;The next step will be to actually test it,&#8221; Malinovskaya says. &#8220;When demonstrated experimentally, this approach will open a new way to precisely control quantum systems with weaker laser fields, making it easier to use in practical applications.&#8221; If the laboratory results match the theory, the digitized pulse train could become a standard tool in the quantum engineer&#8217;s kit, helping to bring the promise of quantum technologies—from unimaginably powerful computers to sensors capable of detecting the faintest whispers of nature—closer to everyday reality, one carefully timed pulse at a time.</p>
<p><strong>Subject of Research:</strong> Digitized ultrafast adiabatic passage using low-intensity laser pulse trains for precise quantum state control</p>
<p><strong>Article Title:</strong> Stevens researchers take step toward more precise, practical quantum technologies</p>
<p><strong>Article References:</strong> Stevens researchers take step toward more precise, practical quantum technologies. (n.d.). <a href="https://www.eurekalert.org/news-releases/1143235" rel="noopener noreferrer">Original publication</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> Not provided</p>
<p><strong>Keywords:</strong> quantum control, laser pulses, multiphoton processes, adiabatic passage, quantum computing, quantum sensing, spectroscopy, molecular physics, quantum states, biomedical imaging, Stevens Institute of Technology, Svetlana Malinovskaya</p>
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