| dc.contributor | University of Limerick | |
| dc.contributor | Federal Institute of Mato Grosso do Sul | |
| dc.contributor | Universidade Estadual Paulista (Unesp) | |
| dc.date.accessioned | 2021-06-25T11:15:57Z | |
| dc.date.accessioned | 2022-12-19T22:43:37Z | |
| dc.date.available | 2021-06-25T11:15:57Z | |
| dc.date.available | 2022-12-19T22:43:37Z | |
| dc.date.created | 2021-06-25T11:15:57Z | |
| dc.date.issued | 2020-12-15 | |
| dc.identifier | OSA Continuum, v. 3, n. 12, p. 3424-3432, 2020. | |
| dc.identifier | 2578-7519 | |
| dc.identifier | http://hdl.handle.net/11449/208668 | |
| dc.identifier | 10.1364/OSAC.402485 | |
| dc.identifier | 2-s2.0-85105689326 | |
| dc.identifier | 2883440351895167 | |
| dc.identifier | 0000-0001-6320-755X | |
| dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/5389265 | |
| dc.description.abstract | Laser vibrometry has many applications in non-contact dynamic displacement and vibration measurement. A test beam reflected from a target and a reference beam are combined and detected by a photodiode; the photodetected signal is then processed to determine the target displacement and vibration. This paper describes the use of a 9 kHz measurement bandwidth system, consisting of a Michelson interferometer and self-correcting feedback synthetic-heterodyne signal processing technique, to measure the displacement impulse response of a commercial piezoelectric mirror shifter (PMS), consisting of a mirror mounted on a Piezoelectric transducer and a connecting 50 Ω electrical coaxial cable. The actual non-ideal applied impulse and measured impulse response data were used in conjunction with the instrument variable method to determine a Laplace domain linear transfer function approximation to the actual PMS transfer function. The best transfer function fitting, having a 84% normalized root mean square goodness of fit, was obtained using a 5-th order transfer function having two complex conjugate pole pairs, with associated natural frequencies of 6.29 and 6.79 kHz, and a single real pole. The transfer function zeros consisted of a single complex conjugate zero pair, having an antiresonance frequency of 6.38 kHz and a single real zero. Knowing the analytic transfer function of PMS based nanopositioners is useful for example in the design of closed-loop phase-locked interferometers for wideband sensing. | |
| dc.language | eng | |
| dc.relation | OSA Continuum | |
| dc.source | Scopus | |
| dc.title | Piezoelectric mirror shifter transfer function measurement, modelling, and analysis using feedback based synthetic-heterodyne Michelson interferometry | |
| dc.type | Artículos de revistas | |