34 research outputs found

    Frequency tunable terahertz quantum cascade lasers

    Get PDF
    Terahertz (THz) quantum cascade lasers (QCLs) are compact solid–state sources of coheren radiation operating in the far–infrared (FIR) range of the electromagnetic spectrum. THz QCL ridge waveguides are typically Fabry–Pérot (FP) cavities and exhibit characteristic multiple–mode emission. However, widely tunable single–mode (SM) THz QCLs are ideally suited to many THz-sensing applications, such as trace gas detection, atmospheric observations and security screening. Tunable THz QCLs are also highly desirable for techniques like heterodyne mixing and self–mixing interferometry. SM emission from THz QCLs has been demonstrated using distributed feedback (DFB) cavities, photonic lattices (PLs) and photonic crystals (PhCs). Tunable THz QCLs have also been demonstrated using various techniques, such as external coupled mirrors, variation of growth parameters, deposition of nitrogen gas and dielectric materials, and aperiodic PLs. In this study, SM emission from THz QCLs is obtained from PLs patterned with electron beam lithography (EBL). This lithography based processing has the advantage of integrated device processing. Spectral performance of the PLs was simulated using finite element modelling (FEM) and coupled mode theory. A frequency stopband centred at the characteristic Bragg frequency was computed with emission predicted outside this stopband. Spectral emission of experimentally fabricated devices was observed outside the stopband, as was predicted from simulations. The design of the THz QCLs with PL was modified to investigate frequency tenability by depleting carriers under the PL metallised sections using a three–section device. A bulk Drude model was used to simulate the variation of refractive index as a function of carrier concentration. The PLs were deposited such that they form a Schottky junction and a thin depletion layer at the active material interface. The PLs were driven with an independent external electrical connection. An electrical model was designed, which explained the experimentally observed behaviour. This electrical model was used to calculate the depletion layer and the redistribution of carriers under the PL. The resulting variation in the refractive index was computed using FEM. A 15–20 GHz shift in the Bragg frequency was predicted using the Drude model. The frequency stopband was also predicted to reduce from ~90 GHz to ~77 GHz with carrier depletion and a ~5–6 GHz shift in the stopband band edge was predicted. In an exemplar device, a tuning of 15 GHz was observed. A change in spectral power density (SPD) amongst modes was observed in all other devices. A different approach towards the realisation of a frequency tunable THz QCLs was adopted based on two–coupled cavities. This design was based on a Vernier selection rule and promised a wide band tuning from a small refractive index perturbation. One of the two cavities formed the lasing section, while the other formed a tuning section. A thermal tuning mechanism based on a localised Joule heating was used to tune frequency of the coupled–cavity. THz QCLs with coupled–cavities were modelled using transfer matrices and a bulk thermal model. Two devices were designed to exhibit a blue shift in frequency when the shorter of the coupled–cavities acted as a tuning element. The frequency spacing of the devices were ~15 and ~25 GHz respectively. The devices were also optimised such that a reversal in tuning direction is observed by swapping the functions of the lasing and tuning cavities. A monotonic discrete frequency hopping with a blue shift of ~50 and ~85 GHz was observed from the two devices. A red shift in frequency was also observed as the lasing and tuning cavities were swapped. Additionally, since the tuning element is isolated from the lasing section, the power emission of the lasing section was unaffected by the tuning current. The coupled cavity designs were further optimised to disrupt the monotonic frequency hopping to obtain a quasi–continuous frequency tuning. Unlike, the discrete tuning design, this detuned design required variation of current at the lasing and tuning cavities simultaneously, along with a variation in heat sink temperature. Spectral behaviour was modelled using the same transfer matrices, bulk thermal mode and coupled mode theory. Closely spaced discrete tuning over a range of ~67 and 100 GHz was observed from two devices, with continuous tuning of ~5 GHz observed at certain dominant modes. Continuous tuning was also investigated using coupled–cavities with an integrated PL. A continuous tuning of ~3 GHz was observed from experimental devices. Unlike the detuned coupled cavity devices, the power emission from these devices were unaffected by the tuning current. However, these devices are limited by a low tuning range

    Quasi-continuous frequency tunable terahertz quantum cascade lasers with coupled cavity and integrated photonic lattice

    Get PDF
    We demonstrate quasi-continuous tuning of the emission frequency from coupled cavity terahertz frequency quantum cascade lasers. Such coupled cavity lasers comprise a lasing cavity and a tuning cavity which are optically coupled through a narrow air slit and are operated above and below the lasing threshold current, respectively. The emission frequency of these devices is determined by the Vernier resonance of longitudinal modes in the lasing and the tuning cavities, and can be tuned by applying an index perturbation in the tuning cavity. The spectral coverage of the coupled cavity devices have been increased by reducing the repetition frequency of the Vernier resonance and increasing the ratio of the free spectral ranges of the two cavities. A continuous tuning of the coupled cavity modes has been realized through an index perturbation of the lasing cavity itself by using wide electrical heating pulses at the tuning cavity and exploiting thermal conduction through the monolithic substrate. Single mode emission and discrete frequency tuning over a bandwidth of 100 GHz and a quasi-continuous frequency coverage of 7 GHz at 2.25 THz is demonstrated. An improvement in the side mode suppression and a continuous spectral coverage of 3 GHz is achieved without any degradation of output power by integrating a π-phase shifted photonic lattice in the laser cavity

    Multi-spectral terahertz sensing: proposal for a coupled-cavity quantum cascade laser based optical feedback interferometer

    Get PDF
    We propose a laser feedback interferometer operating at multiple terahertz (THz) frequency bands by using a pulsed coupled-cavity THz quantum cascade laser (QCL) under optical feedback. A theoretical model that contains multi-mode reduced rate equations and thermal equations is presented, which captures the interplay between electro-optical, thermal, and feedback effects. By using the self-heating effect in both active and passive cavities, self-mixing signal responses at three different THz frequency bands are predicted. A multi-spectral laser feedback interferometry system based on such a coupled-cavity THz QCL will permit ultra-high-speed sensing and spectroscopic applications including material identification

    Optical feedback effects on terahertz quantum cascade lasers: modelling and applications

    Get PDF
    Terahertz (THz) quantum cascade lasers (QCLs) are compact sources of radiation in the 1–5 THz range with significant potential for applications in sensing and imaging. Laser feedback interferometry (LFI) with THz QCLs is a technique utilizing the sensitivity of the QCL to the radiation reflected back into the laser cavity from an external target. We will discuss modelling techniques and explore the applications of LFI in biological tissue imaging and will show that the confocal nature of the QCL in LFI systems, with their innate capacity for depth sectioning, makes them suitable for skin diagnostics with the well-known advantages of more conventional confocal microscopes. A demonstration of discrimination of neoplasia from healthy tissue using a THz, LFI-based system in the context of melanoma is presented using a transgenic mouse model. © (2016) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only

    Detection of terahertz frequency radiation via the photothermoelastic response of zincblende crystals

    Get PDF
    We present experimental evidence for a photothermoelastic response in zincblende crystals illuminated by quantum cascade laser sources in the frequency range 2.2–2.9 THz. Results obtained using an optically balanced sampling arrangement indicate a mechanism whereby the stress distribution established through localized heating of the crystal induces a change in optical birefringence via the photoelastic response of the crystal. A full mathematic model of this photothermoelastic mechanism in (110)-orientated crystals is presented, and shown to agree well with experimental measurements of the magnitude, and the orientational and spatial dependencies of the sampled signal in ZnTe and GaP crystals

    Origin of terminal voltage variations due to self-mixing in terahertz frequency quantum cascade lasers

    Get PDF
    We explain the origin of voltage variations due to self-mixing in a terahertz (THz) frequency quantum cascade laser (QCL) using an extended density matrix (DM) approach. Our DM model allows calculation of both the current–voltage (I–V) and optical power characteristics of the QCL under optical feedback by changing the cavity loss, to which the gain of the active region is clamped. The variation of intra-cavity field strength necessary to achieve gain clamping, and the corresponding change in bias required to maintain a constant current density through the heterostructure is then calculated. Strong enhancement of the self-mixing voltage signal due to non-linearity of the (I–V) characteristics is predicted and confirmed experimentally in an exemplar 2.6 THz bound-to-continuum QCL

    Gas spectroscopy with integrated frequency monitoring through self-mixing in a terahertz quantum-cascade laser

    Get PDF
    We demonstrate a gas spectroscopy technique, using self-mixing in a 3.4 terahertz quantum-cascade laser (QCL). All previous QCL spectroscopy techniques have required additional terahertz instrumentation (detectors, mixers, or spectrometers) for system pre-calibration or spectral analysis. By contrast, our system self-calibrates the laser frequency (i.e., with no external instrumentation) to a precision of 630 MHz (0.02%) by analyzing QCL voltage perturbations in response to optical feedback within a 0–800 mm round-trip delay line. We demonstrate methanol spectroscopy by introducing a gas cell into the feedback path and show that a limiting absorption coefficient of ∼1×10⁻⁴   cm⁻¹ is resolvable

    Discrete Vernier tuning in terahertz quantum cascade lasers using coupled cavities

    Get PDF
    Discrete Vernier frequency tuning of terahertz quantum cascade lasers is demonstrated using a device comprising a two-section coupled-cavity. The two sections are separated by a narrow air gap, which is milled after device packaging using a focused ion beam. One section of the device (the lasing section) is electrically biased above threshold using a short current pulse, while the other section (the tuning section) is biased below threshold with a wider current pulse to achieve controlled localized electrical heating. The resulting thermally-induced shift in the longitudinal cavity modes of the tuning section is engineered to produce either a controllable blue shift or red shift of the emission frequency. This discrete Vernier frequency tuning far exceeds the tuning achievable from standard ridge lasers, and does not lead to any corresponding change in emitted power. Discrete tuning was observed over bandwidths of 50 and 85 GHz in a pair of devices, each using different design schemes. Interchanging the lasing and tuning sections of the same devices yielded red shifts of 20 and 30 GHz, respectively

    Global, regional, and national burden of diabetes from 1990 to 2021, with projections of prevalence to 2050: a systematic analysis for the Global Burden of Disease Study 2021

    Get PDF
    Background Diabetes is one of the leading causes of death and disability worldwide, and affects people regardless of country, age group, or sex. Using the most recent evidentiary and analytical framework from the Global Burden of Diseases, Injuries, and Risk Factors Study (GBD), we produced location-specific, age-specific, and sex-specific estimates of diabetes prevalence and burden from 1990 to 2021, the proportion of type 1 and type 2 diabetes in 2021, the proportion of the type 2 diabetes burden attributable to selected risk factors, and projections of diabetes prevalence through 2050. Methods Estimates of diabetes prevalence and burden were computed in 204 countries and territories, across 25 age groups, for males and females separately and combined; these estimates comprised lost years of healthy life, measured in disability-adjusted life-years (DALYs; defined as the sum of years of life lost [YLLs] and years lived with disability [YLDs]). We used the Cause of Death Ensemble model (CODEm) approach to estimate deaths due to diabetes, incorporating 25 666 location-years of data from vital registration and verbal autopsy reports in separate total (including both type 1 and type 2 diabetes) and type-specific models. Other forms of diabetes, including gestational and monogenic diabetes, were not explicitly modelled. Total and type 1 diabetes prevalence was estimated by use of a Bayesian meta-regression modelling tool, DisMod-MR 2.1, to analyse 1527 location-years of data from the scientific literature, survey microdata, and insurance claims; type 2 diabetes estimates were computed by subtracting type 1 diabetes from total estimates. Mortality and prevalence estimates, along with standard life expectancy and disability weights, were used to calculate YLLs, YLDs, and DALYs. When appropriate, we extrapolated estimates to a hypothetical population with a standardised age structure to allow comparison in populations with different age structures. We used the comparative risk assessment framework to estimate the risk-attributable type 2 diabetes burden for 16 risk factors falling under risk categories including environmental and occupational factors, tobacco use, high alcohol use, high body-mass index (BMI), dietary factors, and low physical activity. Using a regression framework, we forecast type 1 and type 2 diabetes prevalence through 2050 with Socio-demographic Index (SDI) and high BMI as predictors, respectively. Findings In 2021, there were 529 million (95% uncertainty interval [UI] 500–564) people living with diabetes worldwide, and the global age-standardised total diabetes prevalence was 6·1% (5·8–6·5). At the super-region level, the highest age-standardised rates were observed in north Africa and the Middle East (9·3% [8·7–9·9]) and, at the regional level, in Oceania (12·3% [11·5–13·0]). Nationally, Qatar had the world’s highest age-specific prevalence of diabetes, at 76·1% (73·1–79·5) in individuals aged 75–79 years. Total diabetes prevalence—especially among older adults—primarily reflects type 2 diabetes, which in 2021 accounted for 96·0% (95·1–96·8) of diabetes cases and 95·4% (94·9–95·9) of diabetes DALYs worldwide. In 2021, 52·2% (25·5–71·8) of global type 2 diabetes DALYs were attributable to high BMI. The contribution of high BMI to type 2 diabetes DALYs rose by 24·3% (18·5–30·4) worldwide between 1990 and 2021. By 2050, more than 1·31 billion (1·22–1·39) people are projected to have diabetes, with expected age-standardised total diabetes prevalence rates greater than 10% in two super-regions: 16·8% (16·1–17·6) in north Africa and the Middle East and 11·3% (10·8–11·9) in Latin America and Caribbean. By 2050, 89 (43·6%) of 204 countries and territories will have an age-standardised rate greater than 10%.Peer ReviewedPostprint (published version
    corecore