In the quantum regime information can be copied with only a finite fidelity. This fidelity gradually increases to 1 as the system becomes classical. In this article we show how this fact can be used to directly measure the amount of radiated power. We demonstrate how these principles could be used to build a practical primary standard.Since its inception quantum mechanics has had a deep tie with radiometry, the science of measurement of electromagnetic radiation. The electrical substitution radiometer, developed by Lummer and Kurlbaum in 1892 [1], was used to observe the spectral distribution of a heated black body. In 1900 Max Planck was able to describe this distribution by assuming that electromagnetic radiation could only be emitted in multiples of an energy quantum E = h ν. This discovery not only provided an accurate law relating the radiated spectral density to temperature, but laid the foundations of quantum physics. The electrical substitution radiometer is still used as the primary standard for spectral radiance by many metrology laboratories. These systems have been improved over more than a century and can now achieve absolute uncertainties better than 10 −4 , when operated at relatively high powers [2].More recently, nonlinear optical effects such as Spontaneous Parametric Down Conversion have provided a new primary standard based on the correlations of quantum fields [3]. The accuracy of these techniques has improved by nearly one order of magnitude every ten years, and is currently of the order of 10 −3 . These systems are limited to the photon-counting regime, with a recent theoretical proposal for extension to higher photon rates [4].In this letter, we present a radiometer that overcomes these limitations and works over a broad range of powers: from the single photon level, up to several tens of nW (≈ 10 11 photons/s), i.e. from the quantum regime to the classical regime. In fact, our system is able to provide an absolute measure of spectral radiance by relying on a particular aspect of the quantum to classical transition: as the number of information carriers (photons) grows, so does the fidelity with which they can be cloned. For an optimal cloning machine [5][6][7][8][9] this relation can be derived ab initio [10,11] so that a measurement of the fidelity of the cloning process is equivalent, as we shall see below, to an absolute measurement of spectral radiance.Optimal cloning has been demonstrated in a variety of systems [6,8,9]. Stimulated emission in atomic systems is particularly practical as high gains can be easily achieved and the entire system can be implemented in-fibre which both ensures the presence of a single spatial mode and makes the system readily applicable, though not limited, to current telecom technology.Principle of operation -The aim of this experiment is to produce an absolute measurement of luminous power P in .We will do this by using an optimal Universal Quantum Cloning Machine (QCM). As we shall see such a device is able to directly relate a relative measurement of ...