Self-rotation of resonant elliptically polarized light in collision
... Self-rotation in resonant atomic vapors, also caused by induced polarization of the medium, has been studied since the late 1960’s. The original interest in SR in atomic vapors was related to understanding the polarization of gas laser emission [17]. Later, SR was theoretically examined [18–21] in t ...
... Self-rotation in resonant atomic vapors, also caused by induced polarization of the medium, has been studied since the late 1960’s. The original interest in SR in atomic vapors was related to understanding the polarization of gas laser emission [17]. Later, SR was theoretically examined [18–21] in t ...
Realization of an Optomechanical Interface
... 3 1014 m= Hz. We observe that !m decreases with increasing lattice laser power, and measure !m =2 ¼ 244 kHz at P ¼ 76 mW. We attribute this to reduced tensile stress due to thermal expansion of the membrane, which is locally heated by the lattice laser [25]. The mechanical quality factor Q ¼ !m ...
... 3 1014 m= Hz. We observe that !m decreases with increasing lattice laser power, and measure !m =2 ¼ 244 kHz at P ¼ 76 mW. We attribute this to reduced tensile stress due to thermal expansion of the membrane, which is locally heated by the lattice laser [25]. The mechanical quality factor Q ¼ !m ...
chapter 2 photons and atoms
... for explaining virtually all known optical phenomena. For optical phenomena, this theory is also referred to as quantum optics. • it is possible to derive many of the quantum-mechanical properties of light and its interaction with matter by supplementing electromagnetic optics with a few simple rela ...
... for explaining virtually all known optical phenomena. For optical phenomena, this theory is also referred to as quantum optics. • it is possible to derive many of the quantum-mechanical properties of light and its interaction with matter by supplementing electromagnetic optics with a few simple rela ...
Second-order coupling between excited atoms and surface polaritons
... forces between atoms or molecules and macroscopic bodies are manifestations of the zero-point energy of the electromagnetic vacuum [1]. They occur even if the atom and the macroscopic body are in their respective (unpolarized) ground states [2] and can be understood—at least, in the nonretarded limi ...
... forces between atoms or molecules and macroscopic bodies are manifestations of the zero-point energy of the electromagnetic vacuum [1]. They occur even if the atom and the macroscopic body are in their respective (unpolarized) ground states [2] and can be understood—at least, in the nonretarded limi ...
Quantum State Control via Trap-induced Shape Resonance in
... The ability to arbitrarily manipulate the quantum state of a many-body ensemble represents the ultimate control of a physical system. This task has steadily advanced in atomic-molecular-optical systems with tremendous progress in cooling and trapping technology. This has led to the creation of Bose- ...
... The ability to arbitrarily manipulate the quantum state of a many-body ensemble represents the ultimate control of a physical system. This task has steadily advanced in atomic-molecular-optical systems with tremendous progress in cooling and trapping technology. This has led to the creation of Bose- ...
Physical Science Test #1 – Review Guide Properties of Matter
... 19. A __________________________ is made up of more than one kind of atom or molecule in the same place at the same time (but those atoms or molecules are NOT bonded together). 20. ________________________________ are made up of one kind of atom; for example: carbon, oxygen, hydrogen, sodium, or chl ...
... 19. A __________________________ is made up of more than one kind of atom or molecule in the same place at the same time (but those atoms or molecules are NOT bonded together). 20. ________________________________ are made up of one kind of atom; for example: carbon, oxygen, hydrogen, sodium, or chl ...
Precision spectroscopy using quantum superposition of atomic levels
... ion 9 Be+ , trapped in the rf Poul trap. This CNOT gate is a paradigm of quantum computing because sufficient for universal quantum computation is CNOT operation plus a simple qubit rotation. In CNOT gate on a single ion, quantum entanglement between internal atomic state and motional state are crucia ...
... ion 9 Be+ , trapped in the rf Poul trap. This CNOT gate is a paradigm of quantum computing because sufficient for universal quantum computation is CNOT operation plus a simple qubit rotation. In CNOT gate on a single ion, quantum entanglement between internal atomic state and motional state are crucia ...
Formula Charts
... T is the temperature in Kelvin R is the gas constant = 8.314 P is the pressure V is the volume in liters n represents moles R is the ideal gas constant T is the temperature in Kelvin PA is the partial pressure of “A” XA is the mole fraction of “A” PX is the partial pressure of “X” KE is the kinetic ...
... T is the temperature in Kelvin R is the gas constant = 8.314 P is the pressure V is the volume in liters n represents moles R is the ideal gas constant T is the temperature in Kelvin PA is the partial pressure of “A” XA is the mole fraction of “A” PX is the partial pressure of “X” KE is the kinetic ...
ppt of slides
... Atoms trapped in an optical lattice move due to quantum tunneling even if the potential depth of the lattice point exceeds the kinetic energy. Strongly interacting limit. However when the well depth is large then the interaction energy of the atoms become more than the hopping energy, then the atom ...
... Atoms trapped in an optical lattice move due to quantum tunneling even if the potential depth of the lattice point exceeds the kinetic energy. Strongly interacting limit. However when the well depth is large then the interaction energy of the atoms become more than the hopping energy, then the atom ...