Quantitative phase microscopy by digital holography provides direct access to the phase profile of a transparent subject with high precision. This is useful for observing phenomena that modulate phase, but are otherwise difficult or impossible to detect. In this letter, a carefully constructed digital holographic apparatus is used to measure optically induced thermal lensing with an optical path difference precision of less than 1 nm. Furthermore, by taking advantage of the radial symmetry of a thermal lens, such data are processed to determine the absorption coefficient of transparent media with precisions as low as 1×10 When a beam of incident light passes through a medium, that medium may absorb some energy of the beam. This absorbed energy causes a change in temperature of the absorbing region of the media, which diffuses to other parts of the medium in a way described by its thermal properties. Since the index of refraction is a temperature dependant property, the temperature gradient results in a refractive index gradient and, therefore, an optical path difference. This effect is referred to as thermal lensing and has been the focus of many other studies as an indicator of the optical and thermal properties of materials [1−3] . Due to the change in optical path length, a resulting phase shift can be detected at a plane on the far side of the medium. The description of this result can be simplified if the dimensions of the sample are such that the edge effects and container medium can be ignored relative to the effects in the sample medium itself. Such a model has previously been developed, and is known as the two-dimensional (2D) infinite model [4] . This model mathematically relates the resulting phase shift to the photothermal properties of the medium in a focused continuous wave (CW) excitation laser beam and an unfocused or collimated imaging beam, such as that used in this letter.The validity of the 2D infinite model is based on several assumptions, and the experimental design should take these into account. The sample cell path length should be comparable to the confocal parameter (twice the Rayleigh range) of the excitation beam to ensure that the spot size remains relatively constant through the sample. In addition, the sample cell dimensions should be large compared with the excitation beam radius so that both radial and axial edge effects can be ignored. The sample should absorb very little power to avoid convection effects. Finally, the temperature coefficient of the refractive index, dn dT , should be constant in the range of temperatures observed. With these assumptions in mind, the laser-induced change in temperature within the sample can be described. Using expressions for the heat generated in a sample by a Gaussian excitation beam and the corresponding solution to the heat transfer equation, a previous study [4] has derived the following relation:where r is the radial distance from the beam axis; t is the time of exposure to the excitation beam; P is the total excitation beam power at the...