Tuesday, September 12, 2006

Screening for Terrorism - Scientific American

For a few weeks in July, a commuter rail station in New Jersey enjoyed the same screening protection as that surrounding the soldiers and civilians in Baghdad’s Green Zone. Using millimeter waves–wavelengths of light shorter than infrared but longer than x-rays–a walk-through portal produced images of passengers before they boarded the trains. Like an x-ray, the technology creates a revealing picture that can highlight items, such as plastic guns, that typical transit security sensors fail to detect. And, essential for transit hubs such as New Jersey’s Exchange Place Station, which serves at least 200,000 passengers a day, it does so quickly.

Portal
A passenger walks through a millimeter wave portal in a New Jersey commuter train station.

Be they trains, planes or automobiles, the world’s transportation network needs better protection. In the U.S. alone, Government Accountability Office investigators snuck bomb components through more than 20 airports and the recent roll-up of a terror plot in the U.K. highlighted the inability of current technologies to detect items such as liquid explosives or their precursors. But a slew of new devices could help fill this security gap, including millimeter-wave cameras.

Developed by companies ranging from industry heavyweights General Electric (GE) and L-3 Communications to smaller firms such as QinetiQ, millimeter wave detectors work in one of two ways: active or passive. Active devices bombard people with millimeter waves to reveal what may be hidden inside clothing, whereas passive devices rely on collecting the ambient waves in the environment. “Millimeter wave covers a broad range of frequencies–from 30 to 300 GHz. At some, the sky illuminates the object, the image being collected in much the same way as an optical camera,” explains John Salkeld, QinetiQ’s director of optronics. “At others, you can pick up emission from the human body.”

Whether active or passive, millimeter waves’ real attraction lies in what it is not: overly revealing. But revealing is exactly what security experts desire for passenger and luggage screening. And for that, x-ray remains the best probing wave. Already, x-ray machines form the core of checked baggage security, peering inside suitcases much as doctors peer inside bodies using CAT scans. Carry-on baggage screening also enhances x-ray imagery by overlaying color-specific highlights that identify the type of material.

millimeter wave image
Millimeter wave provides an image that can reveal concealed items.
Carry-on luggage is a cluttered affair, however, and adding so-called backscatter x-ray machines–those that pick up the x-rays scattered by materials, rather than just those that pass through or are absorbed–can help clarify images. These devices can detect items otherwise obscured in baggage (such as the water bottle glowing to the right of the normal colored x-ray image above). Such x-rays have been offered as a solution for passenger screening as well, though radiation and privacy concerns have limited their application in the U.S.

Besides seeing what passengers bring on board, security officials also want to sniff them. The most common “smelling” devices are trace detection portals, known as puffers, which work by loosening particles on a passenger’s clothing with blasts of air and then analyzing them for traces of explosives or other suspicious chemicals. But the machines have proved susceptible to malfunction, prompting a halt in their installation at airports, and some experts question their effectiveness. “Airplane security stops the sloppy and the stupid,” argues Bruce Schneier, chief technology officer of Counterpane Internet Security. Puffer makers, though, are quick to defend their technology. “It doesn’t take much to be sloppy,” counters Jay Hill, chief technology officer for GE Security. “We’re talking about picogram concentrations.”

Regardless of whether terrorists are sloppy or stupid, they do have a wide array of explosive tools at their disposal: from highly volatile chemical bombs manufactured from relatively common ingredients, such as the hexamethylene triperoxide diamine (HMTD) suspected in the foiled London terror plot, to the military grade plastic explosive Semtex. Because of the problems with existing puffers, some security experts are looking at alternatives, such as quadrupole resonance, terahertz detectors and neutron bombardment machines.

Color imaging
Color coding reveals materials in a traditional x-ray image but backscatter pierces the clutter to highlight a hidden bottle.
Quadrupole resonance machines, in development for shoe scanners and other applications, hit an object with radio waves of varying frequencies, as do terahertz detectors. This injects energy into the material in question, which it releases when the pulse stops. By analyzing the frequency that comes back, scanners can precisely identify the material, whether solid, liquid or gas. Neutron bombardment works much the same way, shooting neutrons into an object and analyzing the gamma rays that return. Such technologies are already in use by bomb squads but might find a useful place in transportation security. “We would integrate it as a secondary system,” says Sean Moore, vice president of sales and marketing at neutron-based machine-maker HiEnergy Technologies. “You always have those bags that need to be rescreened.”

Determining how many bags–or passengers–should qualify for more screening is the difficult balance of any security procedure: screen too many, and the utility of the transportation is compromised; screen too few, and its security is. “They have done the analysis on what is a minimum threat quantity that would be the minimum amount necessary if placed strategically to cause a catastrophic event,” explains Peter Kant, vice president for global government affairs for detection device maker Rapiscan Systems. “All the machines are tested towards that threat quantity.” In other words, if the machine is too lenient it will not make it into use, but if it is too stringent it will not find application either.

And critics charge that much of transportation security development is targeted at past threats, such as shoe bombs, not at future, untried tactics. It may also be providing a perverse incentive. “If you look at the history of aviation security, starting with the Cuban hijackings in the ’60’s, each security measure put in place may have deterred things for a while but ended up raising the bar,” offers R. John Hansman, director of M.I.T.’s International Center for Air Transportation. “It would be much more effective to have more random screenings with more types of devices. From a deterrence standpoint, an attacker does not know what screen will be used.”

Advanced terror detection technologies remain expensive and sometimes difficult to use, challenges that will have to be overcome before they can find widespread deployment, but they are useful in liberating the most important part of any transportation security scheme: security officers themselves. “You might want to be getting more technology out there to free up the people to do other things like behavioral pattern recognition, interfacing with passengers,” notes Craig Coy, president and chief operating officer of the Homeland Security Group at L-3 Communications. Technology may be able to help here as well, via biometric devices that read a person’s physical signals for signs of agitation or other warnings.

“In this world, our technology development cycle has to be faster than the bad guy’s learning cycle,” adds Randy Null, chief technology officer at the Transportation Security Administration. “[But] we clearly would like to find people before we have to find items.” Technology can detect bombs or other terrorist devices but it is the people behind the machines–and behind the intelligence rendering this last line of defense redundant–that truly protect.

By David Biello


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Smart fibres measure optical and thermal signals

They may look unconventional but the photosensitive fibre structures being developed at MIT promise a new way to measure the amplitude and phase of an optical signal. Rob van den Berg talks to the team to find out more.

Using a combination of lenses, filters, beam splitters and detectors to measure an optical field could be a thing of the past thanks to Yoel Fink and his group at Massachusetts Institute of Technology, US. The team has developed a geometric approach to obtaining both the amplitude and phase of an optical field using tough photosensitive fibres woven into lightweight two- and three-dimensional structures (Nature Materials 25 June).

Fink and colleagues say that these fibres do not suffer from the same constraints as their classic glass counterparts and enable access to optical information on unprecedented length and volume scales. What's more, the group has shown that by changing the chemical composition of the fibres, they can be made to detect heat, vibrations and even specific chemical components.

Ayman Abouraddy is a research scientist in Fink's group that has been pioneering the smart fibre work over the last few years. "The basic principle behind these fibres is very simple," Abouraddy told OLE. "The core consists of a light-sensitive semiconductor chalcogenide glass. Along the full length and in intimate contact with this semiconductor material are four thin strips of metal, usually tin. When light or heat impinges on the fibre, photons are absorbed and electron-hole pairs may be generated. These are collected by the electrodes producing an electrical response."

In order to protect the fibres from the environment, a resilient polymer insulator, such as polyethersulphone, covers the semiconductor core and metal electrodes. Combining these three different materials – a semiconductor, a metal and a polymer – is not as difficult as it sounds. Just like their standard glass counterparts, these "smart" fibres are produced from a macroscopic preform, approximately 30 cm long and 3–4 cm in diameter.

Smart fibre fabrication

The fabrication process begins by preparing cylindrical rods of the glassy semiconductor material. A cylindrical shell of polymer having an inner diameter equal to that of the glass rod is prepared with four slits removed from the walls for the metal electrodes.

The glass rod is inserted into the polymer shell and a polymer sheet is then rolled around the resulting cylinder to provide a protective cladding. This is then consolidated into an integrated structure by heating under vacuum. Finally, the cylinder is put in a standard drawing tower producing hundreds of metres of fibre. This maintains the geometry and structure of the macroscopic preform and contacts are formed at the glass/metal interfaces.

"It is very important that the thermo-mechanical properties, such as the melting temperatures of the different materials, are properly matched otherwise the fibre drawing process fails," explained Abouraddy. "People have assumed that it would be impossible to integrate materials with highly different electrical and optical properties into the same fibre because they would have different thermo-mechanical properties. We have shown that this is not necessarily the case."

The fibres are mechanically tough, yet flexible, lightweight and protected (both electrically and chemically) from environmental effects. Arranging them into a closed-surface sphere creates an omnidirectional light-detection system capable of discerning the direction of illumination over 4πsr.

A more sophisticated detection scheme results from using two-dimensional arrays or webs. With a single fibre web, Abouraddy explains that it is possible to reconstruct the intensity distribution of an arbitrary optical field using an algorithm similar to that used in computerized axial tomography (CAT) scans.

"We illuminate a 32 × 32 fibre web with a simple image using a white-light lamp and each fibre records the total intensity of the light along its entire length," said Abouraddy. "In order to reconstruct an estimate of the optical intensity distribution that impinges on the web, we record a set of rotated projections and use a back-projection algorithm."

In the case of fibre webs, these projections can be obtained by rotating the web or alternatively, rotating the object that is being imaged. The image reconstruction improves as more projections are taken into account.

A unique advantage of this detector is the fact that no lens is needed because of the large dimensions used (relative to the wavelength of the light). And, as Abouraddy explains, with two parallel fibre webs it even becomes possible to reconstruct both the amplitude and the phase distributions of an incoming field. "Once the amplitude of a field is known in two different planes, the phase can be obtained using an iterative algorithm," he said.

Abouraddy is convinced that this approach will eventually lead to non-interferometric, lensless imaging, when a larger number of fibres are included in the web to form images of objects in more detail. "The system has an infinite depth of focus," he said. "An image of the object is formed regardless of the distance of the object from the webs, provided that the diffracted field at the locations of the two webs is intercepted."

According to Abouraddy, the image reproduces the object with its physical dimensions and also determines its physical distance from the webs. "Instead of choosing and positioning lenses and detector arrays to perform an optical field measurement, you now only have to design the proper geometrical constructions of polymeric, light-sensitive fibres," he added.

Changing the chemical composition

Abouraddy is keen to point out that the method is by no means limited to measurements in the optical domain. Changing the chemical composition allows the team to tune the electronic bandgap of the semiconducting material. For example, by including germanium, the material becomes sensitive to slight changes in temperature.

The team believes that there are already numerous potential applications for the thermally sensitive fibres. By weaving them into large arrays, for example, he says that thermal information over areas as large as tens of square metres can be obtained with cm2 resolution.

Spatially resolved thermal sensing enables failure detection in systems where the failure mechanism is linked to a change in temperature, such as chemical reactors or car tyres. An intriguing application involves the thermal monitoring of the body of large aircraft or measuring the skin temperature of the space shuttle beneath its thermal tiles.

The method could also be used for thermal monitoring of battlefield soldiers by medical staff. "By weaving these fibres into the clothing of soldiers we can allow them to thermally sense both the environment and their own body," said Abouraddy. "Our optically sensitive fibres may detect the tiny dots of laser light used by snipers for aiming. If a soldier is hit by a bullet, blood will rush to the wound leading to a local increase in temperature, which can be monitored."

Fibres used for infrared laser beam delivery, regardless of the guiding mechanism or materials used, must transport significant power densities through their core. This leads to another important application: self-monitoring of the fibres' condition.

Defects in fibres tend to be highly localized but even a small defect within such a high-power optical transmission line can result in an unintentional energy release with potentially catastrophic consequences. High-power infrared light travelling through the fibre will accumulate at the defect site, heating up the region and eventually leading to failure. The research team has demonstrated that it is possible to localize these defects with high precision (Nature Materials November 2005).

The Fink group was fast in coming up with a promising application of such a local temperature probe. In 2002, the group unveiled a photonic bandgap (PBG) fibre to efficiently guide high-power infrared radiation at 10.6 µm from a CO2 laser (Nature 12 December 2002). Today, these have been incorporated into a device (recently approved by the FDA for use in patients) that enables surgeons to efficiently remove cancerous tissue from the lungs using infrared laser light.

Structural perturbations such as fibre bends also tend to increase the overall losses through coupling to both higher-order propagating modes and to localized defects. "This may happen, for instance, when the fibre enters the throat," explained Abouraddy. "My colleague Mehmet Bayindir came up with the idea to surround these PBG fibres with extra layers just like those used for thermal sensing. This allows us to sense the escape of light via the heat generated as soon as it occurs and switch off the treatment laser immediately."

These applications highlight the value of combining various functionalities into a single smart fibre. And there are yet more promising prospects by going beyond the optical and thermal regimes.

"This is a very flexible process. We have found many more combinations of materials that are compatible and can be drawn into fibres," concluded Abouraddy. "You could think of adding completely different functionalities to the fibres, such as pressure sensitivity, or the ability to detect specific chemicals, just by tuning the chemical composition of the chalcogenide glass and the polymer and designing a suitable fibre structure."

About the author

Rob van den Berg is a freelance science journalist based in the Netherlands.


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Saturday, September 09, 2006

Micromachined waveguide antennas for 1.6 THz

J.W. Bowen, S. Hadjiloucas, B.M. Towlson, L.S. Karatzas,
S.T.G. Wootton, N.J. Cronin, S.R. Davies, C.E. McIntosh,
J.M. Chamberlain, R.E. Miles and R.D. Pollard
A new type of horn antenna for operation at 1.6 THz, that can befabricated monolithically with 1/4-height micromachined waveguide, is described. Height limitations imposed by the micromachining process are overcome by removing a tapered slot in the upper surface of a scalar horn, allowing the E-plane fields to extend outside the confines of the metallic structure before radiation, with a consequent reduction in E-plane beamwidth. 1.6 THz radiation pattern measurements for different designs show that, while there is scope for further optimisation, 3 dB beamwidths of 24° and 17.5° in the E- and H-planes, respectively, can be achieved.

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Diamagnetic Response of Metallic Photonic Crystals at Infrared and Visible Frequencies

Xinhua Hu,1 C. T. Chan,2 Jian Zi,3 Ming Li,1 and Kai-Ming Ho1
1Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
2Department of Physics, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China
3Surface Physics Laboratory (National Key Lab), Fudan University, Shanghai 200433,

We show analytically and numerically that diamagnetic response (effective magnetic permeability miu_e <>

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Friday, September 08, 2006

On-chip gratings improve stability of laser diodes

Quintessence Photonics has written gratings into its infrared laser diodes that narrow the emission spectra and reduce temperature sensitivity. As Paul Rudy explains, this makes the diodes ideal for medical applications and could lead to cheaper diode-pumped systems.

The combination of compactness, low running cost and excellent electrical-to-optical efficiency has enabled high-power edge-emitting laser diodes to serve many applications in industrial, medical and defence markets. A growing number of these lasers are directly addressing “thermal” applications such as printing, medical and plastics welding, but the majority have a well-defined emission spectra and are used as sources to pump solid-state and fibre-laser systems.

The advantages of diode pumping over lamp pumping are well known, and include increased system efficiency, greater reliability and lower cost of ownership. However, these systems cannot deliver the temperature-independent performance of lamp-pumped designs because of the laser’s lack of stability. Instead, thermal management and temperature control of the diode are needed to precisely tune its emission wavelength. But even with this control, the linewidths produced are insufficiently narrow for some applications.


It is critical to improve the stability and spectral narrowing of high-power laser diodes so that they can simultaneously deliver the efficiency associated with diode pumping and temperature stability provided by lamp pumping. If these objectives are met at a well-defined wavelength, then laser system design- ers can improve the decvice’s compactness, efficiency, power and beam quality while reducing its thermal-management cost.

Fig. 1

The improvements would also mean that these lasers could be used directly for scientific and medical pumping applications, such as Raman spectroscopy and enhanced magnetic resonance imaging, which require precise tuning of narrow emission wavelengths to hit atomic or molecular absorption spectra.

Various methods have already been used to improve the spectral brightness, stability and accuracy of laser diodes. These approaches include various external techniques using either volume Bragg gratings, external lenses and bulk gratings, or seed lasers in master oscillator power amplifiers. However, all of these approaches require sensitive and high-precision alignment, costly additional lasers and/or optics and specially designed coatings. On-chip solutions are possible with internal distributed feedback gratings similar to those that are used in singlemode telecom lasers. However, it is difficult to transfer this technology to high-power multimode lasers because multimode devices require more complex grating designs to capture and lock the large number of transverse modes.

Recently, Quintessence Photonics Corporation (QPC) has overcome these challenges and demonstrated a range of high-power lasers operating at 808, 976, 1470, 1535 and 1550 nm, which are fabricated at our headquarters in Sylmar, CA. These MOCVD-grown InP-based and GaAs-based lasers feature internal gratings that narrow the spectral linewidth, reduce wavelength-temperature sensitivity, and ensure that the device operates at the required wavelength.

High-power laser diodes are usually constructed by inserting a gain-producing active stripe into the device’s resonant Fabry-Pérot cavity. Aside from defining a periodic “comb” of resonant frequencies, the cavity provides no wavelength control. The emission wavelength is controlled by the active layer’s gain spectrum. Unfortunately, this gain spectrum is “flat”, has a characteristic width of typically 20 nm, and is strongly temperature dependent. This makes for a spectrally broad laser output, particularly at high power fluxes, which is highly dependent on the operating temperature. The emission wavelength can typically vary by 0.3 nm/°C.

However, when the on-chip grating is added to select the longitudinal mode, temperature sensitivity is governed by the changes in refractive index of the grating region, and is reduced to 0.1 nm/°C or less.

These devices are fabricated in a similar way to conventional laser diodes, with the gratings defined by optical lithography into a photoresist, followed by etching, or formed during a growth and re-growth process.

The InP and GaAs lasers have different grating geometries that are designed through extensive modelling, but use similar processes to write the gratings. After the design has been optimized, the total processing time for the grating-based lasers is only slightly longer than that for conventional emitters. Our development has led us to believe that high-power grating-based lasers promise excellent manufacturing yields through improved targeting of the wavelength, which leads to reduced yield loss compared with conventional laser diodes.

When 808 nm pump lasers are sold, it is typically with a 3 nm centre wavelength tolerance, a spectral width of less than 2-4 nm and a 0.3 nm/°C temperature tuning coefficient. However, for common gain media, such as neodymium-based crystals, absorption peaks can be as narrow as 1 nm. This means that system manufacturers have to control the operating temperature to within 0.1 °C to correctly tune and maintain the appropriate emission wavelength. Unfortunately, the diode red-shifts as it ages, and to maintain efficient lasing the diode has to be increasingly cooled, often until it reaches the dew point. Once this point is reached, catastrophic damage to the laser’s mirrors can occur.

QPC released 808 nm lasers in June with 100 μm wide stripes that avoid these issues by using internal gratings to deliver the performance described in the table above. These lasers have much narrower laser emission widths than their Fabry-Pérot cousins (see figure 1), and have great promise for Raman spectroscopy, pumping alkali vapours for medical imaging and atomic vapour lasers, and simplifying neodymium-based diode pumped systems.

In the 915-976 nm regime, high-power laser diodes are used to pump fibre lasers that have a typical centre wavelength tolerance of 5 nm, a spectral width of less than 5 nm and a temperature tuning coefficient of 0.3 nm/°C. The fibre laser’s absorption spectrum has a relatively weak broad peak of 915-960 nm, and a peak that is three to four times a strong at 976 nm. Using this shorter wavelength peak is not ideal for a growing number of pulsed fibre laser applications, because longer lengths of fibre increase nonlinear losses. Until now, the choice has been between using an uncooled diode to pump the broad but weak absorption peak, or a temperature-controlled laser to excite the stronger and narrower 976 nm peak. However, our 976 nm single-emitting device shows that it is possible to enjoy the benefits of pumping strong but narrow peaks without the need for high precision temperature controls.

Laser diodes emitting between 1.4 and 1.6 μm are used for various applications, including pumping Er:YAG lasers that are used for range finding, materials processing and aesthetic medical treatments. Er:YAG sources, which emit in the eye-safe regime, are also becoming widely used to reduce the impact of potentially hazardous unintended scattered radiation from either laser sources, optical delivery systems and targets. Applications are plentiful in the industrial, defence and medical markets.

For Er:YAG pumping, lasers operating at 0.9-1.0 μm can be used, but optical conversion is more efficient at 1532 nm where there is a 1 nm-wide absorption peak. This peak can be pumped using typical high-power temperature-controlled InP lasers that have a 10 nm spectral width and 0.35 nm/°C temperature tuning, but it can also be excited with increased efficiency with our grating-based laser bars.

Fibre laser sources

High-power fibre lasers often use several expensive amplifying stages, but this could be avoided by using 1550 nm single frequency, single transverse mode diodes that can deliver sufficient power. At higher powers, singlemode operation has been demonstrated in tapered devices. However, producing more power while maintaining a near diffraction-limited performance and narrow linewidth is challenging, because of yield losses owing to beam quality deterioration at high powers, and filamentation at relatively low powers. These issues have been addressed with QPC’s high-power 1550 nm laser, which contains a buried heterostructure singlemode waveguide and a tapered gain region. The waveguide acts as a mode filter, but once the beam is fed into the tapered gain region the mode can freely diffract and be amplified by a tapered electrical contact. These lasers can deliver more than 1.5 W at 28% wall-plug efficiency, using a 5 A drive current. Spectral linewidth is limited by the test equipment, but was measured at less than 6 MHz, and suppression of the sidemodes is more than 50 dB.

The combination of our range of diodes’ spectral brightness, stability and spatial brightness opens the door to deployment in tasks such as the seeding and core pumping of fibre systems, as well as providing the source for second harmonic generation of light for biotech and display applications. And even higher output powers could be reached while maintaining diffraction-limited performance if emitters can be coherently combined. Our motivation is to expand the number of pumping and direct diode applications with enhanced performance, increased temperature stability and reduced system complexity, while maintaining the device’s compactness, low running cost and excellent efficiency.

Acknowledgments

Part of this work was supported by the Naval Air Warfare Center Weapons Division and by the US Army.

• This article originally appeared in the August issue of Compound Semiconductor magazine.


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Thursday, September 07, 2006

Photonic crystals go magnetic

Physicists in Germany have made a new type of photonic crystal by fine-tuning the magnetic, rather than the electric, properties of a material.

Stefan Linden of the Karlsruhe Research Institute and colleagues at Karlsruhe University made a novel type of photonic crystals from pairs of gold wires, which act as artificial magnetic atoms. The discovery has opened up new ways to manipulate light on the nanoscale, the scientists claim (Phys.Rev.Lett. 97 083902).

Photonic crystals are nanostructured materials in which periodic variations of some property - usually, the material's electric permittivity - produce a "photonic band gap". This affects how photons propagate through the material. This effect is similar to how a periodic potential in semiconductors affects the flow of electrons by defining allowed and forbidden energy bands. In particular, photons with wavelengths or energies in the photonic band gap cannot travel through the crystal, which allows scientists to control and manipulate the flow of light by introducing carefully selected defects.

Until now, all photonic crystals operating with visible light have worked by modifying a material's electric permittivity - a measure of the extent to which a material concentrates electrostatic lines of flux. Although the same effects are expected for periodic modulations of the magnetic permeability ("mu") - which is a measure of how a material responds to a magnetic field - all known natural substances have a ("mu") of 1 for visible light. This means that researchers have not been able to make photonic crystals that operate through variations in the magnetic permeability.

Now, however, Linden and colleagues have found a way round this problem by using "metamaterials". These are composite structures made from tiny rods, ensembles of metal rings and the like, in which the individual components act as "artificial atoms". Metamaterials therefore have very different properties from their component parts, including values of ("mu") not equal to 1.

In the current work, the researchers used pairs of gold wires a mere 220 nm wide and 100 micrometres long, separated by a 50 nm thick layer of magnesium fluoride, to create a one-dimensional periodic lattice of artificial "magnetic atoms". This was then placed on a quartz-based slab, which acts as a waveguide to channel light along certain paths, to create a 1D "magnetic" photonic crystal.

"Our findings are a proof of principle for the concept of a magnetic photonic crystal," says Linden. "However, there still is a long way till we can utilize it as a real-world application." The ability to use both electrical permittivity and magnetic permeability will give physicists more design freedom. It could even lead to new effects such as three-dimensional photonic bands - a prerequisite if photonic crystals are to fulfil their potential - made of stacks of one-dimensional magnetic photonic crystals. The team is now trying to fabricate 3D metamaterials based on its 1D structures.

About the author

Bob Swarup is a science writer for physicsweb.org


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Generation of coherent terahertz pulses in ruby at room temperature

Elena Kuznetsova,1 Yuri Rostovtsev,1 Nikolai G. Kalugin,1 Roman Kolesov,1 Olga Kocharovskaya,1 and Marlan O. Scully1,2

1Institute for Quantum Studies and Department of Physics, Texas A&M University, College Station, Texas 77843, USA
2Princeton Institute for Material Science and Department of Mechanical and Aerospace Engineering, Princeton University, New Jersey 08544, USA

(Received 8 May 2006; published 29 August 2006)

We have shown that a coherently driven solid state medium can potentially produce strong controllable short pulses of THz radiation. The high efficiency of the technique is based on excitation of maximal THz coherence by applying resonant optical pulses to the medium. The excited coherence in the medium is connected to macroscopic polarization coupled to THz radiation. We have performed detailed simulations by solving the coupled density matrix and Maxwell equations. By using a simple V-type energy scheme for ruby, we have demonstrated that the energy of generated THz pulses ranges from hundreds of pico-Joules to nano-Joules at room temperature and micro-Joules at liquid helium temperature, with pulse durations from picoseconds to tens of nanoseconds. We have also suggested a coherent ruby source that lases on two optical wavelengths and simultaneously generates THz radiation. We discussed also possibilities of extension of the technique to different solid-state materials.

URL: http://link.aps.org/abstract/PRA/v74/e023819

doi:10.1103/PhysRevA.74.023819

PACS: 42.50.Gy, 42.65.Ky


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Wednesday, September 06, 2006

Theory of the ultrafast nonlinear response of terahertz quantum cascade laser structures

C. Weber, F. Banit, S. Butscher, and A. Knorr
Institut für Theoretische Physik, Nichtlineare Optik und Quantenelektronik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
A. Wacker
Fysiska Institutionen, Lunds Universitet, Box 118, 22100 Lund, Sweden

(Received 9 March 2006; accepted 10 July 2006; published online 30 August 2006)

Using density matrix theory, the linear and ultrafast nonlinear optical properties of a recently developed terahertz quantum cascade laser are investigated. All relevant excitation regimes, from coherent Rabi flopping up to the scattering dominated stationary response, are covered by the theory. It is shown that the coherence transfer between different periods is important to describe optical effects. ©2006 American Institute of Physics


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Saturday, September 02, 2006

Gap structures and wave functions of classical waves in large-sized two-dimensional quasiperiodic structures

Y. Lai,1 Z. Q. Zhang,1 C. H. Chan,2 and L. Tsang2

1Department of Physics, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong
2Department of Electronic Engineering, City University of Hong Kong, Kowloon, Hong Kong

(Received 8 May 2006; published 30 August 2006)

By using the sparse-matrix canonical-grid method, we performed large-scale multiple-scattering calculations to study the gap structures and wave functions of classical waves in two-dimensional quasiperiodic structures. We observed many interesting phenomena arising from the quasiperiodic long-range order. In particular, a self-similar wave function with resonant structures was observed at a band edge. Our findings indicate that two-dimensional quasiperiodic systems exhibit a universal behavior that applies to both electrons (or phonons) in discrete lattices and classical waves in continuous media.

URL: http://link.aps.org/abstract/PRB/v74/e054305

doi:10.1103/PhysRevB.74.054305

PACS: 71.23.Ft, 43.40.+s, 42.70.Qs, 61.44.Br


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Excitation wavelength dependence of terahertz emission from semiconductor surface

Masato Suzuki and Masayoshi Tonouchi
Institute of Laser Engineering, Osaka University, 2-6 Yamadaoka, Suita, Osaka 565-0871, Japan
Ken-ichi Fujii
Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan
Hideyuki Ohtake and Tomoya Hirosumi
Aisin Seiki Co., Ltd., Kojiritsuki, Hitotsugi-cho, Kariya 448-0003, Japan

(Received 30 January 2006; accepted 1 July 2006; published online 30 August 2006)

The authors have measured terahertz radiation from InSb, InAs, and InGaAs excited by femtosecond optical pulses at wavelengths of 1560, 1050, and 780 nm. The amplitude of the terahertz field strongly depends on the pump wavelengths. Among the materials, the InSb emitter shows the largest terahertz emission amplitude at high power 1560 nm excitation, whereas 780 nm excitation provides the weakest. With increasing photon energy, the increase in emission amplitude from InAs is less as compared to that from InGaAs. The decrease from InSb and InAs originates in low mobilities of L or X valley carriers generated by intervalley scatterings. ©2006 American Institute of Physics


doi:10.1063/1.2338430

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'Lumalive' textile presents variable LED display

A novel display-embedded textile from Philips Research can turn clothes into walking dynamic advertisements.

Philips Research, Eindhoven, Netherlands, is expecting to impress visitors at this year's IFA show (Internationale Funkausstellung, 1-6 September, Berlin, Germany) with the world's first demonstration of promotional jackets and furniture featuring the company's Lumalive technology.

Lumalive textiles allow the creation of fabrics that can carry dynamic advertisements, graphics and constantly changing color surfaces. Philips stand at the IFA show in Hall 22 will be a showcase for Lumalive textile products that will be worn by Philips' staff and embedded into booth furniture of the "Future Zone".

Although the technology has been developed only recently -early prototypes were exhibited at IFA 2005- Philips Research has made progress in fully integrating Lumalive fabrics into garments. The first-generation jackets are ready for commercialization by companies partnering with Philips Research, particularly those in the promotional industry looking for a new, high-impact medium.

Lumalive fabrics feature flexible arrays of colored LEDs integrated into the fabric - without compromising the softness or flexibility of the cloth. The light emitting textiles can carry dynamic messages, graphics or multicolored surfaces. Fabrics such as drapes, cushions or sofa coverings become active when they illuminate in order to enhance the observer's mood and positively influence his/her behavior.

The jackets are said to be comfortable to wear, and the Lumalive fabrics only become obvious when they light up to display various vivid colored patterns, logos, short text messages or even full color animations.

The electronics, batteries and LED arrays are fully integrated and invisible to the observer and wearer. The jackets feature panels of up to 200x200 mm2, although the active sections can be scaled up to cover much larger areas such as a sofa.

"Taking the Lumalive fabrics from prototypes to integrated products has been a major challenge," said Bas Zeper, managing director of Photonic Textiles, Philips Research. "The light emitting textiles have to be flexible, durable and operated by reasonably compact batteries. Fitting all that into a comfortable, lightweight garment is a considerable engineering success."

"Last year Philips Research showed our research prototypes; this year the jackets and furniture represent versions that are ready to go into commercial production, and include integrated power sources and control electronics," added Zeper.

The products include features that make them practical for daily use. For example, when integrating the Lumalive fabrics into the garment, Philips Research has made the parts that can't be easily washed - such as the batteries and control electronics-simple to disconnect and reconnect after the garment has been cleaned. Even the light-emitting layer can be easily removed and refitted to the jacket.

Philips Research is inviting potential partners to discuss the commercialization potential of the material at IFA 2006 where the company's booth is acting as a showcase for the technology and a focal point for discussions.

About the author

Matthew Peach is a contributing editor to optics.org and Optics & Laser Europe


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Luxtera claims first single chip dual XFP transceiver

Will permit economically-feasible fiber-to-chip connectivity. Technology is "the future" of optical interfaces, developer claims.

Luxtera, based in Carlsbad, Ca, US, a developer of CMOS photonic technology has announced a single-chip integrated photonics-electronics device implemented in a standard CMOS process.

The technology integrates high-performance optics and mainstream electronics on a single die, bringing fiber connectivity directly to a chip.

"Fabrication in a standard, high volume 0.13 micron SOI-CMOS process makes fiber optics feasible and economical for everyday applications," the company states. Additional digital logic can be integrated into the same chip with optical devices, reducing both device size and power consumption.

The technology incorporates two lasers and photodetectors mounted directly on a monolithic CMOS die that also includes all logic equivalent to two complete XFP modules including TransImpedance Amplifiers (TIA), Mach-Zehnder modulators, as well as transmit and receive Clock and Data Recovery (CDR) circuits. This complete single chip solution is one-quarter the size of existing XFP module solutions.

Luxtera is currently sampling prototype devices for preliminary testing by strategic development partners. The company will launch a commercial transceiver product line based on the technology early in 2007.

Initial product offerings will comprise multi-port transceivers for communications, storage, and computing applications.

The first commercial application is expected to be high speed, high bandwidth enterprise data communications. Driven by the high bandwidth capabilities of new multi-core, high performance processors, the need for low cost, low latency and low power 10G, and faster interconnects is here, the company adds.

"The potential impact on the industry of combining photonic and electronic elements on a single CMOS die is substantial," said Lawrence Gasman, president of CIR. "Many applications, including those in the cost sensitive consumer markets, will benefit from the improvements in cost, power consumption and size."

"CMOS Photonics technology will enable the widespread adoption of 10G interconnects, which today are very expensive to deploy, by driving the cost of 10G optical ports to well below $100."

As a result of Luxtera's technology, the cost of optical interfaces are reaching those of copper with the added benefits of lower power, lower latency, smaller footprint, longer reach and less expensive cabling. For complete link solutions, the technology provides 7X power reduction, 40X reach, 100X lower latency with scalability to 1000X the bandwidth of 10GBASE-T.

"This technology is the future of optical interfaces," said Marek Tlalka, vice president of marketing at Luxtera. "Traditional discrete optical solutions are bulky and costly. Emerging 10G copper interfaces are also bulky, power hungry and extremely limited in their reach. Our advanced developments eliminate these constraints to commercialization and, for the first time, render fiber optic performance at costs associated with copper interfaces a reality."

About the author

Matthew Peach is a contributing editor to optics.org and Optics & laser Europe.


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High output RGB sources promise laser TV 'by 2007'

Novalux says its new 750 mW red "Necsel" laser and 3 W green and blue models are paving the way for laser projection TV.

Novalux, Sunnyvale, Ca, has demonstrated its first Necsel laser arrays that emit more than 750 mW of red light. The company has also achieved a 3 W power output from its prototype blue and green arrays - double the power of previous devices.

The company says that these developments put Novalux on track to produce RGB (red, green, blue) Necsel lasers for integration into laser-based projection TVs.

"Demonstrating 750-mW red Necsel arrays, along with meeting our 3 W target for green and blue, are significant milestones in our evolution," said Greg Niven, Novalux's VP marketing. "Our customers want all-Necsel RGB devices for incorporation into laser-based home cinema systems."

"Ultimately, this means 3 W per colour. Now that we've met the target with green and blue, red isn't far behind and will soon be at the same level. We're on track to support the TV companies' desire to be selling high-definition laser TVs featuring Necsel laser color by Christmas 2007."

Novalux say that Necsel RGB sources benefit TV manufacturers over other types of laser because they provide desirable output wavelengths and can cut overall system cost. Specifically, red Necsel arrays produce light at 620 nm - a wavelength that matches existing TV-screen phosphors.

Competing red edge-emitter laser technology can only go as low as 635 nm and has poor lifetime. In a Necsel system the same type of laser emits each of the three colors so they share the same device parameters. This uniformity results in simpler, more cost-efficient laser integration from drive electronics to imaging optics.

Novalux's prototype Necsel devices emit 3 W at 465 nm and 532 nm and 750nbsp;mW at 620 nm - all from a new package smaller than a matchbox. Necsel lasers' output is bright, speckle-free, and color-saturated, giving in clear, vibrant images that reach a larger color space than competing lighting technologies.

Novalux first introduced concept Necsel-based RPTVs during the 2006 Consumer Electronics Show (CES). These early units demonstrated the expanded color range and striking image contrast.

The company's latest prototypes, shown during Society for Information Display (SID) 2006, demonstrated even higher brightness, color-balanced, speckle-free, high-definition images on 52 inch screens. Ultimately, Novalux aims to enable home theater systems that marry over 200% of NTSC color coverage, high-brightness, high-resolution images, a thin, wide viewing angle architecture, and unsurpassed light source lifetime.

About Novalux

Founded in 1998, Novalux has developed proprietary Necsel (Novalux Extended Cavity Surface Emitting Laser) technology. This combines mass volume manufacturability with excellent optical performance. Necsel device attributes include bright, reliable, consistent, speckle-free light output from a compact, low-cost package, making them ideal for current- and next-generation display applications.

About the author

Matthew Peach is a contributing editor to optics.org and Optics & Laser Europe


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Friday, September 01, 2006

Laser Seeding of the Storage-Ring Microbunching Instability for High-Power Coherent Terahertz Radiation

J. M. Byrd, Z. Hao, M. C. Martin, D. S. Robin, F. Sannibale, R. W. Schoenlein, A. A. Zholents, and M. S. Zolotorev

Ernest Orlando Lawrence Berkeley National Laboratory, One Cyclotron Road, Berkeley, California 94720, USA

(Received 24 May 2006; published 18 August 2006)

We report the first observation of laser seeding of the storage-ring microbunching instability. Above a threshold bunch current, the interaction of the beam and its radiation results in a coherent instability, observed as a series of stochastic bursts of coherent synchrotron radiation (CSR) at terahertz frequencies initiated by fluctuations in the beam density. We have observed that this effect can be seeded by imprinting an initial density modulation on the beam by means of laser "slicing." In such a situation, most of the bursts of CSR become synchronous with the pulses of the modulating laser and their average intensity scales exponentially with the current per bunch. We present detailed experimental observations of the seeding effect and a model of the phenomenon. This seeding mechanism also creates potential applications as a high-power source of CSR at terahertz frequencies.

URL: http://link.aps.org/abstract/PRL/v97/e074802

doi:10.1103/PhysRevLett.97.074802

PACS: 41.60.Ap, 07.05.Tp, 07.57.Hm, 29.27.Bd

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Tracking the motion of charges in a terahertz light field by femtosecond X-ray diffraction

A. Cavalleri1,2, S. Wall1, C. Simpson1, E. Statz3, D. W. Ward3, K. A. Nelson3, M. Rini4 and R. W. Schoenlein4

In condensed matter, light propagation near resonances is described in terms of polaritons, electro-mechanical excitations in which the time-dependent electric field is coupled to the oscillation of charged masses1,2. This description underpins our understanding of the macroscopic optical properties of solids, liquids and plasmas, as well as of their dispersion with frequency. In ferroelectric materials, terahertz radiation propagates by driving infrared-active lattice vibrations, resulting in phonon-polariton waves. Electro-optic sampling with femtosecond optical pulses3,4,5 can measure the time-dependent electrical polarization, providing a phase-sensitive analogue to optical Raman scattering6,7. Here we use femtosecond time-resolved X-ray diffraction8,9,10, a phase-sensitive analogue to inelastic X-ray scattering11,12,13, to measure the corresponding displacements of ions in ferroelectric lithium tantalate, LiTaO3. Amplitude and phase of all degrees of freedom in a light field are thus directly measured in the time domain. Notably, extension of other X-ray techniques to the femtosecond timescale (for example, magnetic or anomalous scattering) would allow for studies in complex systems, where electric fields couple to multiple degrees of freedom14.

  1. Department of Physics, Clarendon Laboratory, University of Oxford, Oxford OX1 3PU, UK
  2. Central Laser Facility & Diamond Light Source, Rutherford Appleton Laboratory, Chilton, Didcot, OX11 0QX, UK
  3. Department of Chemistry, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
  4. Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA

Correspondence to: A. Cavalleri1,2 Correspondence and requests for materials should be addressed to A.C. (Email: a.cavalleri1@physics.ox.ac.uk).

Received 1 May 2006 |Accepted 30 June 2006


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Universal Features of Terahertz Absorption in Disordered Materials

S. N. Taraskin,1,2 S. I. Simdyankin,2 S. R. Elliott,2 J. R. Neilson,2,3 and T. Lo4

1St. Catharine's College, Trumpington Street, Cambridge CB2 1RL, United Kingdom
2Department of Chemistry, University of Cambridge, Cambridge CB2 1EW, United Kingdom
3Department of Materials Science and Engineering, Lehigh University, Bethlehem, Pennsylvania 18015, USA
4Teraview Ltd., Platinum Building, St. John's Innovation Park, Cambridge CB4 OW5, United Kingdom

(Received 10 March 2006; published 2 August 2006)

Using an analytical theory, experimental terahertz time-domain spectroscopy data, and numerical evidence, we demonstrate that the frequency dependence of the absorption coupling coefficient between far-infrared photons and atomic vibrations in disordered materials has the universal functional form, C(omega)=A+Bomega2, where the material-specific constants A and B are related to the distributions of fluctuating charges obeying global and local charge neutrality, respectively.

URL: http://link.aps.org/abstract/PRL/v97/e055504

doi:10.1103/PhysRevLett.97.055504

PACS: 63.50.+x, 61.43.Fs, 78.30.Ly

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The IRMMW-THz 2006 Conference

Joint 31st International Conference on Infrared and Millimeter Waves and 14th International Conference on Terahertz Electronics

September 18-22, 2006, Shanghai ,China

T
he IRMMW-THz 2006, currently in its 31st year, is the oldest continuous forum specifically devoted to the field of ultra high frequency electronics and applications. The scope of the conference extends from millimeter wave devices, components and systems to infrared detectors and instruments, and encompasses micro-scale structures to large-scale Tokamaks and Gyrotrons. In recent years the organizing committee has expanded the conference scope and the participating research communities with a special focus on terahertz techniques and applications, including both the traditional radio frequency domain and the new fast pulse time domain approaches to generating, detecting and using high frequency energy. The conference offers attendees a chance to hear and participate in a wide range of topic areas that span all aspects of Infrared, Terahertz and Millimeter-Wave technology and applications from quantum physics, chemistry and biology to radio astronomy and plasma physics.
The following is a representative list of topics to be covered at the conference:
  1. IR, THz, and MMW Sources, Detectors and Receivers
  2. Terahertz Devices, Components, Subsystems and Instruments; both Frequency and Time Domain.
  3. Novel Devices and Instruments for IR, THz and MMW
  4. IR, THz and MMW Spectroscopy, Instrumentation and Material Properties
  5. MMW and Submillimeter-Wave Radar and Communications
  6. Ultra High Speed MMW Digital Devices
  7. IR, THz and MMW Imaging
  8. MMW Systems, Transmission Lines and Antennas
  9. Gyro-Oscillators and Amplifiers, Plasma Diagnostics
  10. Free Electron Lasers and Synchrotron Radiation
  11. IR, THz and MMW Astronomy, Atmospheric and Environmental Science Applications
  12. Ultra-fast Components and Measurements in Chemistry and Physics
  13. IR, THz, and MMW Applications in Security and Industry.
  14. New IR, THz and MMW Applications in Biology and Medicine
  15. IR, THz and MMW Future Applications, Markets and Directions


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