Photonic Quantum Information Processing OPTI 647: Lecture 3 Saikat Guha September 03, 2019
Associate Professor College of Optical Sciences Meinel 523 Outline for today
• Coherent states and linear optics • Quantizing the field • Distinguishing pure states General pure state of a single mode
Mode ( t ) , a quantum system, is excited in a coherent state ↵ , ↵ C | i 2 If we do ideal direct detection of mode ( t ) , the total number of photons K is a Poisson random variable of mean N
Mode ( t ) , a quantum system, is excited in a number state n ,n 0, 1,..., | i 2 { 1} If we do ideal direct detection of mode ( t ) , the total number of This orthogonality photons K = n (exactly so; K is not a random variable). (in the Hilbert A mode of ideal laser light is in a coherent state. state) is different Number (Fock) state of a given mode is very hard to produce from that of experimentally modes (in L2 norm space) There are infinitely many other types of “states” of the mode ( t ) . Coherent state and Fock state are just two example class of states n ,n 0, 1,..., Fock states of a mode are special: they form an orthonormal | i 2 { 1} basis that spans any general quantum state of that mode 1 1 | i m n = and = c n , c 2 =1 mn | i n| i | n| h | i n=0 n=0 X X Coherent state as a quantum state
↵ 2 Fock states can | | n 1 e 2 ↵ be thought of as ↵ = n infinite-length | i pn! | i unit-length n=0 ! column vectors X cn corresponding to 1 0 0 the orthogonal 0 1 0 axes of an 0 = 2 3 1 = 2 3 2 = 2 3 ... | i 0 | i 0 | i 1 infinite- 6 7 6 7 6 7 6 7 6 7 6 7 dimensional 6 7 6 7 6 7 4 5 4 5 4 5 vector space Ideal photon detection is a von Neumann quantum measurement described by projectors, n n ,n=0, 1,..., {| ih |} 1 Ideal direct detection on a coherent state ↵ produces outcome “n” | i N n 2 2 e N (i.e., n “clicks”) with probability, p = n ↵ = c = n |h | i| | n| n! Poisson detection statistics in a laser pulse is a result of the projection of the quantum state of the laser pulse—a coherent state–on to one of the Fock states Coherent states and “linear-optical transformations” (beam-splitters)