Phase demodulation from a single carrier-frequency fringe pattern is becoming increasingly important particularly in areas of optical metrology such as dynamic interferometry, deflectometry and profilometry. The Fourier transform (FT) method and the spatial-carrier phase-shifting technique (SCPS) are two popular and well-established approaches to demodulation. However FT has the drawback of significant edge errors because of the Gibbs effect, whilst detuning errors for the local phase shift occur when SCPS is applied. A novel demodulation method based on pixel-level Lissajous figure and ellipse fitting (PLEF) is presented in this paper. Local demodulation in the spatial domain makes PLEF more flexible than the FT method, without spectral leakage. Based on a more adaptable approach, account is taken of variations in illumination and phase distribution over a few neighboring pixels. The mathematic demodulation model is of interest and has been demonstrated via simulation. Theoretical phase extraction error is as low as 10 −4 rad. Experiments further corroborate the effectiveness of the proposed method. In conclusion, various influencing factors, e.g. variations of background/modulation, phase amplitude, carrier frequency, additive noise that may affect the precision of PLEF are discussed in detail.Interferometry, deflectometry and profilometry are diagnostic tools frequently used in optical metrology to achieve highly accurate, non-contact and full-field measurements. Since the relevant physical information is usually encoded in the fringe phase, phase demodulation always plays a very critical role in fringe analysis. Temporal phase shifting (TPS) is a phase demodulation method, which has been used extensively in optical metrology since its introduction 1 .Phase shifting interferometry (PSI), for example, has already become a standard configuration of a modern high accuracy interferometer 2 . A well-calibrated phase shifter and stable environment are crucial factors to TPS due to equal steps conventionally used in phase-shifting algorithms (PSA) 3,4 . Though various kinds of generalized PSI have been put forward in recent years as a means of coping with random phase shift error caused by vibration 5-9 , it remains difficult to achieve real time phase demodulation in dynamic measurement operations since at least three interferograms are usually required in order to record and process data. Dynamic measurement is an attractive option not only in optical shop testing, e.g. high-aperture and long-distance primary mirror testing 10 but also in many other phase-demodulation operations, e.g. visual monitoring of cell culture in the biomedical domain 11 . With the exception of simultaneous phase shifting interferometry (SPSI) 12 , which is not our concern in this contribution, demodulation of a single shot fringe pattern is an attractive option. The spatial carrier-frequency (SCF) method is a good choice since implementation of spatial carrier-frequency interferometry (SCFI) is relatively easily accomplished on most advan...