Duc Tu Tu Tu

Dr. Duc Tu Tu Tu


Research Focus & Metrics

Academic Career Length

7Years (2020-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

View All Publications
29 September 2021 in Crystals
Verified
Journal Article
Open access
PDF file
DTDuc Tu Tu Tu
Duc Tu Tu Tu
YTYi-Chang Tsai
Yi-Chang Tsai
MLMinh Quoc Le
Minh Quoc Le
Shiao-Wei KuoShiao-Wei Kuo
Shiao-Wei Kuo
NLNgoc Diep Lai
Ngoc Diep Lai
Chia CHen HsuChia CHen Hsu
Chia CHen Hsu
Lanthanide (Ln3+)–doped upconversion nanoparticles (UCNPs) offer an ennormous future for a broad range of biological applications over the conventional downconversion fluorescent probes such as organic dyes or quantum dots. Unfortunately, the efficiency of the anti−Stokes upconversion luminescence (UCL) process is typically much weaker than that of the Stokes downconversion emission. Albeit recent development in the synthesis of UCNPs, it is still a major challenge to produce a high−efficiency UCL, meeting the urgent need for practical applications of enhanced markers in biology. The poor quantum yield efficiency of UCL of UCNPs is mainly due to the fol-lowing reasons: (i) the low absorption coefficient of Ln3+ dopants, the specific Ln3+ used here being ytterbium (Yb3+), (ii) UCL quenching by high−energy oscillators due to surface defects, impurities, ligands, and solvent molecules, and (iii) the insufficient local excitation intensity in broad-field il-lumination to generate a highly efficient UCL. In order to tackle the problem of low absorption cross-section of Ln3+ ions, we first incorporate a new type of neodymium (Nd3+) sensitizer into UCNPs to promote their absorption cross-section at 793 nm. To minimize the UCL quenching induced by surface defects and surface ligands, the Nd3+-sensitized UCNPs are then coated with an inactive shell of NaYF4. Finally, the excitation light intensity in the vicinity of UCNPs can be greatly enhanced using a waveguide grating structure thanks to the guided mode resonance. Through the synergy of these three approaches, we show that the UCL intensity of UCNPs can be boosted by a million−fold compared with conventional Yb3+–doped UCNPs.

1 September 2021 in Solar Energy
Verified
Journal Article
Closed access
DTDuc Tu Tu Tu
Duc Tu Tu Tu
HVHoang Vu
Hoang Vu
SSSeoyong Shin
Seoyong Shin
TTTran Quoc Tien
Tran Quoc Tien
NVNgoc Hai Vu
Ngoc Hai Vu


6 May 2022 in Energies
Verified
Journal Article
Open access
PDF file
DTDuc Tu Tu Tu
Duc Tu Tu Tu
KMkieu ngoc minh
kieu ngoc minh
QTQuoc Tien Tran
Quoc Tien Tran
TNThanh-Phuong Nguyen
Thanh-Phuong Nguyen
VHVu Hoang
Vu Hoang
NVNgoc Hai Vu
Ngoc Hai Vu
We have proposed a fruitful design principle targeting a concentration ratio (CR) >1000× for a typical high concentrating photovoltaics (HCPV) system, on account of a two-concentrator system + homogenizer. The principle of a primary dual-lens concentrator unit, completely analogous basic optics seen in the superposition compound eyes, is a trend not hitherto reported for solar concentrators to our knowledge. Such a concentrator unit, consisting of two aspherical lenses, can be applied to minify the sunlight and reveal useful effects. We underline that, at this stage, the CR can be attained by two orders of magnitude simply by varying the radius ratio of such two lenses known from the optics side. The output beam is spatially minimized and nearly parallel, exactly as occurs in the superposition compound eye. In our scheme, thanks to such an array of dual-lens design, a sequence of equidistant focal points is formed. The secondary concentrator consists of a multi-reflective channel, which can collect all concentrated beams from the primary concentrator to a small area where a solar cell is placed. The secondary concentrator is located right underneath the primary concentrator. The optical characteristics are substantiated by optical simulations that confirm the applicability of thousands-fold gain in CR value, ~1100×. This, however, also reduced the uniformity of the illumination area. To regain the uniformity, we devise a fully new homogenizer, hinging on the scattering principle. A calculated optical efficiency for the entire system is ~75%. Experimentally, a prototype of such a dual-lens concentrator is implemented to evaluate the converging features. As a final note, we mention that the approach may be extended to implement an even higher CR, be it simply by taking an extra concentrator unit. With simple design of the concentrator part, which may allow the fabrication process by modeling method and large acceptant angle (0.6°), we assess its large potential as part of a general strategy to implement a highly efficient CPV system, with minimal critical elaboration steps and large flexibility.

1 February 2021 in Journal of Porous Materials
Verified
Journal Article
Closed access
PDF file
DTDuc Tu Tu Tu
Duc Tu Tu Tu
TPThi Nhung Pham
Thi Nhung Pham
CHChia-Chen Hsu
Chia-Chen Hsu
HBHenri Benisty
Henri Benisty
NLNgoc Diep Lai
Ngoc Diep Lai

2 December 2020 in Biomedical Optics Express
Verified
Journal Article
Closed access
DTDuc Tu Tu Tu
Duc Tu Tu Tu
TLThanh-Thu Vu Le
Thanh-Thu Vu Le
CHChia-Chen Hsu
Chia-Chen Hsu
NLNgoc Diep Lai
Ngoc Diep Lai
CHChristophe Hecquet
Christophe Hecquet
HBHenri Benisty
Henri Benisty
We introduce a compact array fluorescence sensor principle that takes advantage of the long luminescence lifetimes of upconversion nanoparticles (UCNPs) to deploy a filter-free, optics-less contact geometry, advantageous for modern biochemical assays of biomolecules, pollutants or cells. Based on technologically mature CMOS chips for ∼10 kHz technical/scientific imaging, we propose a contact geometry between assayed molecules or cells and a CMOS chip that makes use of only a faceplate or direct contact, employing time-window management to reject the 975 nm excitation light of highly efficient UCNPs. The chip surface is intended to implement, in future devices, a resonant waveguide grating (RWG) to enhance excitation efficiency, aiming at the improvement of upconversion luminescence emission intensity of UCNP deposited atop of such an RWG structure. Based on mock-up experiments that assess the actual chip rejection performance, we bracket the photometric figures of merit of such a promising chip principle and predict a limit of detection around 10-100 nanoparticles.