“…The contribution from the sample bending to the PA signal is calculated by solving the thermoelastic equations, whereas the thermal diffusion contribution is attained by solving the heat conduction differential equation, as described in details in Refs. 12, 18-20. Assuming that all light is absorbed at the sample surface and considering no axial heat flux, the pressure fluctuation in the air chamber of a photoacoustic cell due to thermal diffusion (TD) and thermoelastic (TE) bending of a thermally thick sample, i.e., l s a s ) 1, is expressed in one-dimension by 12,[18][19][20] …”