1.47k likes | 1.71k Views
Experiments With Entangled Photons. Paulo Henrique Souto Ribeiro Instituto de Física - UFRJ. Summer School of Optics Concépcion January/2010. Quantum Optics Group at IF/UFRJ. Group members. Experiments: Prof. Paulo Henrique Souto Ribeiro Prof. Stephen Patrick Walborn Theory:
E N D
Experiments With Entangled Photons Paulo Henrique Souto Ribeiro Instituto de Física - UFRJ Summer School of Optics Concépcion January/2010
Group members Experiments: Prof. Paulo Henrique Souto Ribeiro Prof. Stephen Patrick Walborn Theory: Prof. Luiz Davidovich Prof. Nicim Zagury Prof. Ruynet Matos Filho Prof. Fabricio Toscano Msc and PhD students: Adriana Auyuanet Larrieu, Adriano H. de Oliveira Aragão, Bruno de Moura Escher , Bruno Taketani, Daniel Schneider Tasca, Gabriel Horacio Aguilar, Osvaldo Jimenez farias, Gabriela Barreto Lemos, Rafael Chaves.
UFAL UFMG UFF UFRJ USP-SÃO PAULO
Part I - Simultaneity in parametric down-conversion - Violation of a classical inequality - Consequences of simultaneity: i) localized one-photon state; ii) the Hong-Ou-Mandel interferometer iii) measurement of the tunneling time
Parametric Down-conversion Espontaneous emission Twin Photons Stimulated emission
Parametric down-conversion: quantum state Time evolution Time evolution operator Time integral
Simultaneity in parametric down-conversion Quantum state for weak interaction
Simultaneity in parametric down-conversion Quantum state including some approximations
Simultaneity in parametric down-conversion Calculation of expectation values Electric field operator Intensity Coincidence
Simultaneity in parametric down-conversion: very simple view
Simultaneity in parametric down-conversion: very simple view Quantum state: simple version Electric field operator: plane wave, almost monochromatic Coincidence
Simultaneity in parametric down-conversion: very simple view Plane wave pumping field
Measurement of time delays s=168ps s=185ps
Simultaneity in parametric down-conversion: very simple view + detection filters Plane wave pumping field
Simultaneity in parametric down-conversion: very simple view + detection filters Interference filter: typical Dl = 10nm, Dw = 3.8 x 1013 Hz, Dt = 82 fs << 100ps
Simultaneity in parametric down-conversion: very simple view + timing resolution
Hong, Ou and Mandel Interferometer: single mode approach Beam splitter Input-output relations
Hong, Ou and Mandel Interferometer: single mode approach Two-photon input state Beam splitter Coincidence probability
Part II - Polarization entanglement - Bell’s inequalities - Entanglement measurement
Polarization entanglement: generation Kwiat et al. PRL 75, 4337 (1995)
Polarization entanglement: generation Kwiat et al. PRA 60, R773 (1999) White et al. PRL 83, 3103 (1999)
Polarization entanglement: generation Kwiat et al. PRA 60, R773 (1999) White et al. PRL 83, 3103 (1999)
Mixed states and entangled states Mixed state Pure entangled state
Bell inequality and Bell states Bell-CHSH inequality
Bell inequality and Bell states Bell states for the photon polarization Coincidence rate for f+:
Bell inequality and Bell states Bell states for the photon polarization Coincidence rate for f+:
Bell inequality and Bell states Maximal violation
Bell inequality and Bell states Maximal violation
Bell inequality and Bell states Maximal violation
Bell inequality and entanglement • Violation of a Bell inequality • Detects but does not quantify the • entanglement properly • - Some entangled states do not violate the • Bell inequality • Valid for dichotomic or dichotomized • systems
Quantum state tomography Take a set of measurements : Reconstruction of the density matrix
Quantum state tomography With r12 one can compute all quantities related to the system
Direct measurement of entanglement Concurrency: