We report a novel quantum random number generator based on the photon-number−path entangled state which is prepared via two-photon quantum interference at a beam splitter. The randomness in our scheme is of truly quantum mechanical origin as it comes from the projection measurement of the entangled two-photon state. The generated bit sequences satisfy the standard randomness test.PACS numbers: 03.67.Dd, 42.50.St, 42.50.Dv The need for generating random numbers arises in many scientific and engineering disciplines, in addition to obvious gaming industries. For instance, in quantum cryptography, the initial choices of the basis and the polarization state for the photon must be truly random for a secure system. Although mathematical algorithm may be used to obtain (pseudo-)random numbers which exhibit some statistical random behaviors, they are not truly random in the sense that the algorithmic method is deterministic in nature.Since randomness is inherent in quantum physics, a physical random number generator built upon a quantum mechanical process would offer true randomness. For example, consider a single-photon, |1 , entering a lossless 50/50 beam splitter via one of the two input ports. The state at the output ports of the beam splitter is easily calculated to be in quantum superposition, |ψ = (|1 t + |1 r )/ √ 2, where the subscripts t and r refer to the two output modes of the beam splitter. The singlephoton detectors placed at the output ports perform the projection measurement on the quantum state |ψ : when the t (r) detector clicks, we know that the quantum state has collapsed to |1 t (|1 r ). It is easy to see that each detector has 50% probability of registering the photon but, in the framework of quantum physics, it is not possible to predict which of the two detectors will click. Since the final outcome is non-deterministic and quantum mechanically random, this process may then be used to build a quantum random number generator (QRNG).The above discussion, hence, allows us to identify that the key elements that give rise to quantum mechanical randomness as the projection measurement and the quantum superposition state. In other words, quantum mechanical randomness arises from the projection measurement on a quantum superposition state.Obviously, the single-photon beam splitting scheme discussed above would make the ideal QRNG if properly implemented. Unfortunately, an efficient single-photon source which is essential for the beam splitter-based * Electronic address: yoonho@postech.ac.kr QRNG does not yet exist and the scheme, in practice, is implemented with attenuated optical pulses [1, 2, 3]. Thus, practical implementations of the beam splitterbased QRNG scheme do not properly realize the key elements for the QRNG.Recently, a number of alternative QRNG schemes have been reported in literature [4,5,6,7,8]. Some of these schemes make use of Poissonian statistics inherent in the photon emission and detection processes to extract random bit sequences [4,5,6]. The key elements of QRNG, i.e., projecti...