Olivier Bernal

Dr. Olivier Bernal

orcid

Research Focus & Metrics

Academic Career Length

21Years (2006-Present)

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

Representative Publications

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1 February 2009
Verified
Conference Paper
Closed access
KCKunil Choe
Kunil Choe
OBOlivier Bernal
Olivier Bernal
DNDavid Nuttman
David Nuttman
MJMinkyu Je
Minkyu Je
Recently, there has been an increasing demand for SoCs in the biomedical field. In implantable applications, SoCs are designed under very stringent power and area constraints. The analog and mixed-signal circuits as well as digital circuits in those SoCs require a clock source, because clock-based signal-processing techniques, such as sampling and chopper stabilization, are often used. The primary clock source for such SoCs needs to provide good accuracy and long-term stability of the oscillation frequency foscto minimize variations and drifts of the system characteristics. A fairly pure clock signal is required to avoid signal distortion when sampling or chopping techniques are applied. Considering such a source is typically a free-running oscillator, and biomedical signals of typical interest reside at low frequencies, the close-in phase noise is important. For implantable biomedical sensor SoCs, due to high power consumption of quartz crystal oscillators and their bulky size, monolithic oscillators are preferred as a primary clock source. Relaxation oscillators can operate with low power and set their oscillation period Tosc in well-defined manner while consuming small silicon area. However, their performance is limited by process variations, noisy current sources, and noise and offset voltages of the comparators. Geraedts et al. presented an idea of subtracting a fixed charge packet and filtering out the comparator noise to improve the phase noise particularly at large offset frequencies. In this work, a self-clocked offset-cancellation scheme is presented for comparators in the relaxation oscillator, resulting in smaller frequency drifts and lower close-in phase fluctuations, which are more relevant parameters for primary clock sources in implantable biomedical SoCs.

13 August 2019 in IEEE Sensors Journal
Verified
Journal Article
Closed access
UZUsman Zabit
Usman Zabit
OBOlivier Bernal
Olivier Bernal
SASaqib Amin
Saqib Amin
MQMuhammad Farrukh Qureshi
Muhammad Farrukh Qureshi
AKArsalan Habib Khawaja
Arsalan Habib Khawaja
TBThierry Bosch
Thierry Bosch
In this paper, spectral processing of laser Self-Mixing (SM) interferometric signal phase has been carried out allowing better measurement accuracy for harmonic and arbitrarily shaped vibrations for an optical feedback based SM interferometric Laser Diode (LD) sensor. The resulting algorithm not only improves the measurement accuracy but also reduces the processing time (by a factor 3.45) as compared with a previous time-domain based displacement retrieval technique called the Phase Unwrapping Method (PUM). Fourier series based analysis of laser feedback phase is carried out to determine processing limits. The proposed algorithm has also been found to be robust against variation in optical feedback coupling C as well as additive noise. This use of spectral analysis not only increases the measurement accuracy but also retrieves information about target movement harmonics which can also be used in modal analysis applications of remote mechanical targets. Using an SM vibration sensor based on a LD emitting at 785nm, this technique has provided an average RMS error of 12.5 nm (while that of PUM is 39 nm RMS) for harmonic target vibrations of 5 µm amplitude. For reduced range of 1<C<2, an average RMS error of 8 nm (~λ/100) is obtained.

11 August 2016 in IEEE Sensors Journal
Verified
Journal Article
Closed access
OBOlivier Bernal
Olivier Bernal
HSHan Cheng Seat
Han Cheng Seat
UZUsman Zabit
Usman Zabit
FSFrederic Surre
Frederic Surre
TBThierry Bosch
Thierry Bosch
An innovative signal processing method based on custom-made wavelet transform (WT) is presented for robust detection of fringes contained in the interferometric signal of self-mixing (SM) laser diode sensors. It enables the measurement of arbitrarily-shaped vibrations even in the corruptive presence of speckle. Our algorithm is based on the pattern recognition capability of bespoke WTs for detecting SM fringes. Once the fringes have been correctly detected, phase unwrapping methods can be applied to retrieve the complete instantaneous phase of the SM signals. Here, the novelty consists in using two distinct mother wavelets Ψ r (t) and Ψ d (t) specifically designed to distinguish SM patterns as well as the displacement direction. The peaks, i.e. the maxima modulus of WT, then allow the detection of the fringes.

20 April 2020 in IEEE Sensors Journal
Verified
Journal Article
Closed access
SASaqib Amin
Saqib Amin
UZUsman Zabit
Usman Zabit
OBOlivier Bernal
Olivier Bernal
THTassadaq Hussain
Tassadaq Hussain
Self-Mixing interferometry (SMI) signal characteristics are highly dependent on both the operating optical regime and target surface. In this paper, a method is proposed to overcome some identified limitations of the even power scalable algorithm (EPSA) [1], such as the required operating regime to be weak feedback. In addition, by using the up-sampling techniques, the number of stages involved in the even-power scalable algorithm can be drastically increased without any data acquisition bandwidth modification. Here, 10 successive stages have been successfully implemented to achieve a theoretical resolution of λ0/213. It is further shown that the proposed method can handle and process weak, moderate and strong feedback regime as well as speckle affected SMI signals more efficiently. Lastly, FPGA based hardware emulation of EPSA is also done for later embedded implementation of this high-resolution algorithm. FPGA synthesis results show that the designed system can measure maximum target velocity up to 1.18 m/s while consuming total power of 1.4W.

25 May 2021 in IEEE Sensors Journal
Verified
Journal Article
Closed access
NANauman Ali
Nauman Ali
UZUsman Zabit
Usman Zabit
OBOlivier Bernal
Olivier Bernal
In this paper, a method is proposed to recover displacements with nanometric precision based on spectral analysis of the feedback phase of self-mixing laser interferometric signal. This method is an enhancement of the previously developed method called Time-domain Frequency-domain Signal Processing (TFSP) which could only recover target vibration(s) with greater than lambda/8 amplitude (where lambda is the laser’s wavelength) so long as at least one of the vibration’s components has an amplitude greater than or equal to lambda/2. Using TFSP reconstruction as a first approximation of the main target displacement combined with parameter (optical feedback factor C and linewidth enhancement factor alpha) estimation, the proposed method can provide a better in-depth analysis of the self-mixing signal spectrum and thus achieve the detection of even lower amplitude vibrations. Studies presented in the paper indicate that the proposed method does not require accurate parameter estimation. Experimental results obtained using a laser diode based self-mixing sensor with lambda = 785 nm show that the adding this method on top of TFSP allows to recover target vibrations with amplitude down to approximately lambda/32 with an average amplitude root-mean-square error of 1.56 nm, which corresponds to a 4 fold improvement over TFSP.

30 January 2020 in IEEE Sensors Journal
Verified
Journal Article
Closed access
OBOlivier Bernal
Olivier Bernal
UZUsman Zabit
Usman Zabit
FJFrancis Jayat
Francis Jayat
TBThierry Bosch
Thierry Bosch
In this paper, a method based on the inherent event-based sampling capability of the laser optical feedback interferometry (OFI) is proposed to recover sub-λ/2 displacement with a nanometric precision. The proposed method operates in open-loop configuration and relies on OFI’s fringe detection, thereby improving its robustness and ease of use. The measured white noise power spectral density is less than 100 pm/Hz with a corner noise frequency of approximately 80 Hz for a laser diode emitting wavelength λ0 of 785 nm placed at 30 cm of the target.