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Quantum Disentanglement Eraser M. Suhail Zubairy (with G. S. Agarwal and M. O. Scully) Department of Physics, Texas A&M University, College Station, TX 77843 Quantum Eraser Marlan O. Scully Texas A&M University Girish S. Agarwal Herbert Walther M. Suhail Zubairy Institute for Quantum Studies COMPLEMENTARITY (N. BOHR, 1927) • Two observables are “COMPLEMENTARY” if precise knowledge of one of them implies that all possible outcomes of measuring the other one are equally probable – POSITION-MOMENTUM – SPIN COMPONENTS – POLARIZATION • TRADITIONALLY Complementarity in quantum mechanics is associated with “Heisenberg’s uncertainty relations” [ x, p] i xp • However it is a more general concept!!! Scully, Englert, Walther, Nature 351, 111 (1991). Newsweek, June 19, 1995, p. 68 Erasing Knowledge! As Thomas Young taught us two Hundred years ago, photons interfere. But now we know that: Knowledge of path (1 or 2) is the reason why interference is lost. Its as if the photon knows it is being watched. But now we discover that: Erasing the knowledge of photon path brings interference back. “No wonder Einstein was confused.” Photon correlation experiment • Light impinging on atoms at sites 1 and 2. Scattered photons γ1 and γ2 produce interference pattern on screen. • Two-level atoms are excited by laser pulse and emit γ photons in the a → b transition (Fig. b). • Atom-scattered field system: 1 b1b2 ( 1 2 ) 2 • The state vector for the scattered photon from the ith atom: g k e ik ri i 1k k ( k ) i / 2 ______________________________ M. O. Scully and K. Druhl, PRA 25, 2208 (1982) 1 • Correlation function for the scattered field: 2 1 () G (r , t ) 1 2 E (r , t ) 0 2 1 0 E ( ) (r , t ) 1 0 E ( ) (r , t ) 2 2 1 2 1 (r , t ) 2 (r , t ) 2 (1) 2 • This is just the interference pattern associated with a Young’s double-slit experiment generalized to the present scattering problem. Note that when the γ1 and γ2 photons arrive at the detector at the ‘same time’, interference fringes are present. • Three-level atoms excited by a pulse l1 from |c> → |a> followed by emission of γ-photons in the |a> → |b> transition (Fig. c). • State of the coupled atom-field system: 1 1 b1c2 1 c1b2 2 2 • Field correlation function: 1 2 2 1 (r , t ) 2 (r , t ) 1* (r , t )2 (r , t ) b1c2 c1b2 c.c. 2 1 2 2 1 (r , t ) 2 (r , t ) 2 G (1) (r , t ) 2 • Which path information available - No fringes • Can we erase the information (memory) locked in our atoms and thus recover fringes? • Four-level system: a second pulse l2 takes atoms from |b> → |b’>. Decay from |b’> → |c> results in emission of Φphotons. • The second laser pulse l2 , resonant with |b>→ |b’> transition, transfers 100 percent of the population from |b> to |b’> (second laser pulse - π pulse). • State of the system after interacting with the l2 pulse is 2 1 b1' c2 1 c1b2' 2 2 • The ith atom decays to the |c> state via the emission of |Φi> photon. State vector after Φ-emission: 3 1 c1c2 1 1 2 2 2 • • • • • Scattered photons γ and γ result from a → b transition. Decay of atoms from b′→ c results in Φ photon emission Elliptical cavities reflect Φ photons onto a common photodetector. Electrooptic shutter transmits Φ photons only when switch is open. Choice of switch position determines whether we emphasize particle (shutter open) or wave (shutter • closed) nature of γ photon. • “Delayed choice” quantum eraser!!! U. Mohrhoff, Am. J. Phys. 64, 1468 (1996) “Delayed choice” quantum eraser experimental demonstration a • Pair of entangled photons is emitted from either atom A or atom B by atomic cascade emission. • ‘Clicks’ at D3 or D4 provide which path information (No interference fringes!!) • ‘Clicks’ at D1 or D2 erase the which path information (Fringes!!) • absence or restoration of interference can be arranged via an appropriately contrived photon correlation experiment. _______________________________________________ a Kim, Yu, Kulik, Shih, and Scully, PRL 84, 1 (2000) Experimental considerations • Distance LA, LB between atoms A, B and detector D0 << distance between atoms A,B and the beam splitter BSA and BSB where the which path or both paths choice is made randomly by photon 2 • When photon 1 triggers D0, photon 2 is still on its way to BSA, BSB • After registering of photon 1 at D0, we look at the subsequent detection events at D1, D2, D3, D4 with appropriate time delay • Joint detection events at D0 and Di must have resulted from the same photon pair • Interference pattern as a function of D0’ s position for joint counting rates R01 and R02 • No interference pattern for R03 and R04 Experimental setup a • The delayed choice to observe either wave or particle behavior of the signal photon is made randomly by the idler photon about 7.7 ns after the detection of the signal photon a Kim, Yu, Kulik, Shih, and Scully, PRL 84, 1 (2000) Experimental results a a Kim, Yu, Kulik, Shih, and Scully, PRL 84, 1 (2000) U. Mohrhoff, Am. J. Phys. 67, 330 (1999) Double-slit experiment with atoms • In the absence of laser-cavity system: (r ) 1 (r ) (r ) i 1 2 2 r is the center-of-mass coordinate and i denotes the internal state of the atom. • The probability density for particles on the screen: • Fringes!! P( R) 1 2 2 1 2 1* 2 2* 1 i i 2 Micromaser Which-Path Detector • State of the correlated atomic beam-maser system: (r ) • Probability density at the screen: P( R) • 1 2 2 1 2 1* 2 1102 0112 2* 1 0112 1102 2 Because <1102|0112> vanishes, P( R) • No fringes!! 1 1 (r ) 1102 2 (r ) 0112 b 2 1 2 2 1 2 2 b b Quantum Eraser a • Is it possible to retrieve the coherent interference crossterms by removing (‘erasing’) the which-path information contained in the detectors? • The answer is yes, but how can that be? The atom is now far removed from the micromaser cavities and so there can be no thought of any physical influence on the atom’s center-of-mass wave function. a Scully, Englert and Walther, Nature 351, 111 (1991) • • (r ) 1 1 (r ) 1102 2 (r ) 0112 b d 2 After absorbing a photon, the detector atom, initially in state |d> would be excited to state |e>. 1 (r ) (r ) (r ) b d 2 with (r ) • • Detector produces 1 1 (r ) 2 (r ); 1 1102 0112 2 2 1 (r ) 0102 e (r ) d b 2 i.e., the symmetric interaction couples only to the symmetric radiation state |+>; the antisymmetric state |-> remains unchanged. (r ) • Atomic probability density at the screen: 1 * ( R) ( R) * ( R) ( R) 2 P( R) • No interference fringes if the final state of the detector is unknown!! • Probability density Pe(R) for finding both the detector excited and the 2 Pe ( R) ( R) atom at R on the screen: Fringes → solid lines!! • Probability density Pd(R) for finding both the detector deexcited and the atom at R on the screen: P ( R) e Antifringes → broken line!! 1 2 2 1 ( R) 2 ( R) Re 1* ( R) 2 ( R) 2 ( R) 2 1 2 2 1 ( R) 2 ( R) Re 1* ( R) 2 ( R) 2 Quantum disentanglement erasersa • Involves at least three-subsystems A, B, T. • Entangled state of the AB subsystem: 1 AB 00 AB 11 AB 2 • Wave function of whole system: 1 ABT 00 AB 0 T 11 AB 1 T • State of the AB subsystem: 2 1 00 2 AB 00 11 AB 11 • Entanglement of subsystem AB is lost! • However if one erases the tag information, then the entanglement is restored. • Thus entanglement of any two particles that do not interact (directly or indirectly) never disappears but is encoded in the ancilla of the system. A projective measurement that seems to destroy such entanglement could always in principle be erased by uitable manipulation of the ancilla. aR. Garisto and L. Hardy, PRA 60, 827 (1999) • Entangled state of the AB subsystem: AB 1 00 2 AB 11 AB • Wave function of whole system: • Define ABT 1 00 2 T 1 0 T 1T 2 AB 0 T 11 AB 1T • Thus ABT 1 1 00 T 2 2 11 AB AB 1 00 T 2 11 AB • Measurement of the tagging qubit realizes the entangled state. AB • • AB system is given by the polarization, T is given by the path of particle 1. 1 At t0 t h s s 0 p h s s 1 p 1 2 1 2 1 1 2 1 1 h h h h 2 • After passage through polarizing beam splitter (PBS) • If we measure the spin of photons at this point, we obtain mixed state t • 1 h 2 h s s 0 p 0 s1s2 No entanglement!! 1 2 1 To reversibly erase the tagging information at t = 2, we perform the reverse of the operation of t=1. Entanglement is restored!! Cavity QED Implementation • Consider cavities A and B with |0> state and an atom 1 in excited state |a> passes through the two cavities • After passage through cavity A with interaction time corresponding to π/2 pulse: 1 1 0 2 A a 1 1 A b 1 0 B • After passage through cavity B with interaction time corresponding to π pulse: 1 1 0 2 A 1B1 A 0 B b 1 Entangled state!!! • Atom 2 (tagging qubit) now passes through cavity A • Atom 2 has dispersive coupling with cavity A, ca v A • Effective Hamiltonian: Η eff (g 2 / ) aa c c a a a a • Initially atom 2 is in state a b / 2 • After passage through cavity A, a quantum phase gate is made 3 e 1 2 -iΗ eff 2 1 g 2 1 i 0 A1B 1A0 B a2 0 A1B e 1A0 B , b2 2 2 _____________________________________ A. Rauschenbeutal et. al PRL 83, 5166 (1999). • Pass atom through classical field with (1 / 2 ) a2 b2 a2 (1 / 2 ) a2 b2 b2 • Resulting state (with η=π): 4 1 0 A1B a 21 A 0 B b 2 2 b • Entanglement between cavities A and B is controlled by atom 2!! 1 • Initial state: 1 1 0 2 A 1B1 A 0 B b 3 • After passage through cavity A: 1 b 1 a 0 0 2 3 2 B 3 B A • Phase shift: 3 1 b 3 1 B ei (t ) a 3 0 2 B 0 A • After passage through cavity B: 1 b3 ,1B a3 ,0 B ei (t ) ( a3 ,0 B b3 ,1B ) 0 A 2 1 b3 ,1B 1 ei (t ) a3 ,0 B 1 ei (t ) 0 A . 2 4 1 4 (t ) b3 ,1B 1 ei (t ) a3 ,0 B 1 ei (t ) 0 A . 2 Detection probabilities: 1 1 i ( t ) 2 Pa3 1 e 1 cos (t ) 4 2 1 Pb3 1 cos (t ) 2 Haroche et. al, Nature (2000) Quantum Eraser • Initial state: 2' • After passage through cavity A: 1 b 31B a 2 a 3 0 B b 2 2 0 b 1' 1 0 A1B a 21 A 0 B b 2 3' 1 b 3 1 B a 2 ei (t ) a 3 0 B b 2 • Phase shift: 2 2 A 3 . . 0 A . • After passage through cavity B: 4' 1 b3 ,1B a2 b2 ei (t ) a3 ,0 B a2 b2 ei (t ) 0 A . 2 • Detection probabilities: 1 1 P Tr a b e a b e 4 2 i ( t ) a 2 Pb 2 i ( t ) 2 2 1 2 • Restoration of fringes: a2 (1 / 2 ) a2 b2 5' 1 b2 (1 / 2 ) a2 b2 a ,0 a 1 e b 1 e b ,1 a 1 e b 1 e i ( t ) 2 2 1 Pa 2 { 3 2 i ( t ) i ( t ) 2 1 cos (t ) for a2 1 cos (t ) for b2 3 1 Pb 2 { B 2 i ( t ) 2 1 cos (t ) for a2 1 cos (t ) for b2 Quantum teleportation • Initial state is an entangled state between cavities A and B along with the tagged qubit T: 2' 1 0 2 A 1 B a 21 A 0 B b 2 b 1 . • We want to teleport the state of qubit C: C c0 0 c1 1 to cavity B • State of combined system ABCT is ABCT 1 [ c AC 2 2 2 1 2 2 c0 1 c1 0 0 c1 1 B AC 0 [ c AC 2 0 c0 1 c1 0 0 c1 1 B AC c0 1 c1 0 c 0 c 1 AC 0 1 AC B B B c0 0 c1 1 B AC c0 1 c1 0 AC where AC 1 01 10 ; AC 1 00 11 ; 2 1 a b 2 2 2 2 • A Bell-basis measurement of AC reduces the BT state to 1 1 c 0 0 c 1 1 c 0 c 1 2 BT 0 B 2 2 1 B 2 2 ] 2 0 B 2 1 B 2 B ] B Induced coherence without induced emission • Recall we produced: 3 e -iΗ eff 2 1 1 g 2 1 i 0 A1B 1A0B a2 0 A1B e 1A0 B , b2 2 2 2 • Interference terms are only partially erased in the reduced two-cavity density matrix ρAB, given by AB 1 1 0 A1B 0 A1B 1A0 B 1A0 B 0 A1B 1A0 B e i 1 c.c. 2 2 • Probabilities for finding the atom 3 in the excited and ground states: 1 cos cos Pa3 1 2 2 , Pb3 1 Pa3 . • For η≠π, we have the control of the interferences in unconditional measurements on atom 2. • Visibility of the fringes is equal to |sin(η/2)|. Brian Greene in The Fabric of the Cosmos (2004) These experiments are a magnificent affront to our conventional notions of space and time. . . . . . . . . .For a few days after I learned of these experiments, I remember feeling elated. I felt I'd been given a glimpse into a veiled side of reality. Table of Contents • • • • • • • • • • • • • • • • • • Quantum Disentanglement Eraser Quantum Eraser Complementarity (Bohr) Erasing Knowledge Photon Correlation Experiment Correlation Function Three-Level Atom Can we erase? Particle or Wave Restoration of Interference (Mohrhoff) Delayed Choice Experimental Considerations Experimental Set-up Experimental Results Objectivity, retrocausation (Mohrhoff II) Double-Slit Experiment Micromaser Which-Path Detector Quantum Eraser • • • • • • • • • • • • • • • • • Interference Fringes Atomic Probability Quantum Disentanglement Entangled State AB System Cavity QED Eraser Field Classical Field Initial State Detection Probabilities Quantum Eraser After Passage Quantum Teleportation ABCT Induced coherence Probabilities Fabric of the Cosmos