Elementary condensed matter physics by Castro Neto A.H.

By Castro Neto A.H.

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The lineshape in Fig. ,fo) pair selections, along with a visual guide for the data. The apparent linewidth is significantly broader than that associated with the 5P state. The pairs of fv and fo used to obtain each point in Fig. 2(c) lead to substantially different detunings of the other 5P states and subsequently, varying optical pumping to the F=l ground state. Indeed, the theory model applied to the actual experiment conditions predicts significantly different ground state population transfer dynamics.

A. , in Gravitational wave andparticle astrophysics detectors, Eds J. H. Sanders, Proceedings of SPIE Vol5500 (SPIE, Bellingham, WA) 25,(2004). 33. B. , Phys. Rev. D 69 082004,(2004). 34. B. , Phys. Rev. D 69 122001,(2004). 36 35. B. , Phys. Rev. D 69 102001, (2004). 36. B. , Phys. Rev. D 69 122004, (2004). 37. B. , Phys. Rev. Lett. 94 181103, (2005). 38. V. , Astrophys. J . 601 L179 or arXiv:astro-ph/0312101v3,(2004). 39. T. , Class. Quantum Grav. 21 S1161, (2004). 40. P. Fritschel, in Gravitational Wave Detection, Eds M.

In parallel, capabilities in the generation and control of coherent light fields, including the generation of coherent optical bandwidth across the entire visible spectrum with spectral phase control and the maintenance of spectacularly long optical phase coherence time, permit the the full revelation of the quantum nature of light-matter interactions. In particular, the combination of ultracold atoms and phase-controlled ultra-wide-bandwidth optical frequency combs has had a profound impact to precision measurement science.

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