Quantum computation with photons requires efficient two photon gates. We put forward a two photon entangling gate which uses an intermediate atomic system. The system includes a single Rydberg atom which can switch on and off photon absorption in an ensemble using the dipole blockade. The gate is based in a counterfactual protocol. The mere possibility of an absorption that can only occur with a vanishing probability steers the photons to the desired final state.
I. QUANTUM COMPUTERS AND THEIR IMPLEMENTATIONSQuantum computers would be able to run new protocols and algorithms, some of them more efficient than any classical alternative [1]. There are several requisites for the practical implementation of a quantum computer: the data must be easy to prepare and read, the computer has to be able to perform any quantum logical operation and maintain coherence during the processing and the system must be scalable [2].There are many candidate systems, each with its own strong and weak points. An interesting family of proposals uses photons as information carriers [3]. Photons have long coherence times and good transmission properties, can be produced and detected with reasonable efficiency and the state of a single photon can be manipulated with standard linear optics equipment [4]. The main obstacle to quantum computation with photons is the creation of two photon gates.Controlled operations in which the state of one photon alters the state of a second photon are essential for universal quantum computation [5]. Two photon interaction is elusive. Most two photon gate proposals either require strongly nonlinear media with losses that can make the operation inefficient [6], need a number of resources that grows exponentially with the size of the system [7], or use measurement induced nonlinearities [8][9][10] that introduce a probabilistic element (the gates only work correctly with a certain low, theoretically bounded, probability [11,12]). Proposed alternatives also include the use of weak nonlinearities [13] or measurement assisted probabilistic gates [14].We propose a controlled sign gate in which the photon interaction is mediated by coupled Rydberg atoms. The proposal tries to make the atomic part as simple as possible. The gate is based on a version of the quantum Zeno effect, in which frequent measurement steers the evolution of a quantum state [15,16].
II. OPTICAL ENCODING: DUAL-RAILWe consider a dual-rail encoding representation. The basic logical quantum states |0 L and |1 L are encoded with a single photon in different orthogonal modes. One usual encoding uses orthogonal polarizations, like horizontally and vertically polarized photons so that |0 L ≡ |H and |1 L ≡ |V . We will use an alternative encoding with spatial separation. We define two paths, each containing a number state |n , where we can have n = 0 (no photons) or n = 1 (a single photon). We label the paths as up and down (with subindices U and D). There will only be one photon. The logical zero state is represented by a photon in the upper mode |0 ...