This paper reports that Goos–Ha¨nchen (GH) shifts occurring on a symmetrical metal-cladding waveguide are experimentally identified.It was found that there exists a critical thickness of the upper metal layer,hcr,above which negative shift is observed and,reversely,positive shift occurs.Both positive and negative GH shifts near the critical thickness do not vary dramatically and can achieve a maximum on the submillimeter scale,which is different from simulated results using the stationary-phase method.It also shows that this critical thickness,hcr,can be obtained at the position for zero reflectivity by setting the intrinsic damping to be the same as the radiative damping.The GH effects observed near the critical thickness are produced by extreme distortion of the reflected beam profiles,which limits the amplitude of the GH shift and,further,the sensitivity of the GH optical sensor based on the symmetrical metal-cladding waveguide. This paper reports that Goos-Ha¨nchen (GH) shifts occurring on a symmetrical metal-cladding waveguide are experimentally identified. It was found there there a critical thickness of the upper metal layer, hcr, above which negative shift is observed and, reversely, positive shift occurs.Both positive and negative GH shifts near the critical thickness do not vary vary dramatically and can achieve a maximum on the submillimeter scale, which is different from simulated results using the stationary-phase method. , hcr, can be obtained at the position for zero reflectivity by setting the intrinsic damping to be the same as the radiative damping. the GH shift and, further, the sensitivity of the GH optical sensor based on the symmetrical metal-cladding waveguide.