Showing posts with label Warwick University. Show all posts
Showing posts with label Warwick University. Show all posts

Monday, July 13, 2020

Warwick leads breakthrough in terahertz imaging


Optical set up for single pixel transmission imaging of object R (Image: Warwick University)
https://www.theengineer.co.uk/warwick-university-terahertz-imaging/

A research team has reached a milestone towards developing single-pixel terahertz imaging technology for use in biomedical and industrial applications.
The team’s single-pixel terahertz camera is said to have reached 100 times faster acquisition than the previous state-of-the-art without adding any significant costs to the system or forgoing the sub-picosecond temporal resolution needed for medical applications.
The team, led by Prof. Emma Pickwell-Macpherson from Warwick University’s Department of Physics and involving Rayko Ivanov Stantchev and scientists from the The Chinese University of Hong Kong, have had their findings published in Nature Communications.
Terahertz (THz) radiation (T-rays) can see through materials including plastics, ceramics and clothes, making them potentially useful in non-invasive inspections. The low-energy photons of T-rays are non-ionising, making them very safe in biological settings such as security and medical screening.
THz technology is not, however, not widely used in commercial settings as the cost, robustness and ease of use is still lagging behind for commercial adoption.
For biomedical applications, very few clinical trials have been performed most notably due to the equipment not being user-friendly and imaging being too slow due to the need for measuring multiple terahertz frequencies for accurate diagnosis. Finally, equipment and running costs need to be within hospital budgets.
In a statement, Prof Emma Pickwell-Macpherson said: “We use what is called ‘a single-pixel camera’ to obtain our images. In short, we spatially modulate the THz beam and shine this light onto an object. Then, using a single-element detector, we record the light that is transmitted (or reflected) through the object we want to image. We keep doing this for many different spatial patterns until we can mathematically reconstruct an image of our object.”
According to Warwick University, the researchers have to keep changing the shape of the THz beam many times which means this method is usually slower compared to multi-pixel detector arrays. However, multi-pixel arrays for the terahertz regime usually lack sub-picosecond temporal resolution, require cryogenic temperatures to operate or incur large equipment costs. The setup developed by the Warwick team, which is based on a single-element detector, costs around £16,000, is robust, has sub-picosecond temporal resolution required for accurate diagnosis, and operates at room temperature.
“Our latest work improves upon the acquisition rate of single-pixel terahertz cameras by a factor of 100 from the previous state-of-the-art, acquiring a 32×32 video at six frames-per-second,” said Prof Pickwell-Macpherson. “We do this by firstly determining the optimal modulation geometry, secondly by modelising the temporal response of our imaging system for improvement in signal-to-noise, and thirdly by reducing the total number of measurements with compressed sensing techniques. In fact, part of our work shows that we can reach a five times faster acquisition rate if we have sufficient signal-to-noise ratio.”

Thursday, November 29, 2018

Varying graphene’s conductivity modulates THz wave


     Illustration of the device structure and its interaction with terahertz light . Credit: Xuequan
Lauren Barr 

https://physicsworld.com/a/varying-graphenes-conductivity-modulates-thz-wave/
Compared with other regions of the electromagnetic spectrum terahertz (THz), the frequency range between the infrared and the microwave, has been relatively neglected. A group from the Chinese University of Hong Kong and Warwick University have recently shown that broadband, large and fast modulation of THz beams is in fact possible, and can even be achieved with one very neat device.
Much effort has been spent designing cameras and spectrometers that operate at THz frequencies. They have already proved useful in airport security scanners, and for identifying underlying layers of old paintings.
One important component of these pieces of equipment are modulators, which control the amplitude or phase of a THz beam. These must operate quickly, consume little energy, give consistent modulation over a large frequency range, and produce large changes in the intensity or phase of a THz beam. Approaches so far include metamaterials, semiconductors and liquid crystal devices, none of which meet all the necessary requirements.

In comes Mr. Brewster…

In 1815 David Brewster published a paper describing the angle of incidence required to achieve zero reflection from a transparent body. Now over two hundred years later a team of scientists led by Jianbin Xu and Emma Pickwell-MacPherson have applied this knowledge, along with some more recent technological advances, to create a record-breaking THz modulator.
Pickwell-MacPherson commented, “Our first step was to demonstrate that broadband THz modulation can be achieved with a much lower change in the conductivity by employing  total internal reflection (TIR) geometry rather than transmission geometry (read more about it in Advanced Optical Materials). This has blossomed into the realization of several new device designs, with this latest one exploiting the Brewster angle.”
The device consists of a single stack of graphene, aluminium oxide (Al2O3) and titanium oxide (TiO­­x) on a quartz substrate. A p-polarized THz beam is reflected from the stack, and when Brewster’s angle is reached the reflection goes to zero. The addition of a layer of graphene here allows for an extra element of tunability. When a voltage is applied across the graphene between two gold contacts, the conductivity changes. This alters the Brewster angle for the stack, so for a given angle of incidence the reflected THz may be “switched on or off” by controlling the voltage.
R

Choose your mode of operation

Shining the p-polarized THz beam onto the device at an angle of 65°, and altering the voltage across the graphene from -12V to +14V, you can modulate the amplitude of the THz by between 99.3% and 99.9% across the entire frequency range of 0.5–1.6 THz. This range is limited by the experimental constraints; in theory even larger bandwidths could be achieved.
But that’s not the only option they have. The researchers took advantage of the fact that at angles greater than the Brewster angle, the reflected beam undergoes a 180° phase change. A THz beam incident at an angle of 68° will experience a phase change of at least 140° across the same frequency range when the voltage is changed from -12V to +16V. Across this range of voltages the Brewster angle varies between 72° and 64°.
Modulated terahertz time-domain waveform (red) and the modulation depth response (blue) to a 1 kHz square-wave electrical signal. Credit: Chen Xuequan.

The need for speed

The rise time of the modulation is around 1ms, so modulation frequencies of 1 kHz are easily achieved. However, if the modulation depth can be compromised, frequencies of up to 10 kHz can also be reached. Although other solid-state THz modulators operate at significantly higher frequencies of around 2.4 MHz, all is not lost as some small tweaks can improve the modulation frequency of this device. Currently it is limited by the resistance and capacitance of the layers between the gold contacts. By reducing the size to around 1 mm and replacing the TiOx with another layer of graphene, the modulation can reach speeds comparable to other devices.
Xu, who is Director of Materials Science and Technology Research Centre, the Chinese University of Hong Kong, explained that, “the additional benefit of this device is that it can be retrofitted into existing commercially available THz spectrometers.” This graphene-controlled Brewster angle THz modulator truly propels us into the future of THz technologies in real-life applications.