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Preprint
... What does a trapped Bose-Einstein condensate look like? More precisely, how does it interact with light, and does this differ fundamentally from what one would naively expect from a similar collection of very cold atoms? In the early 1990s, before Bose-Einstein condensation was realized in atomic ga ...
... What does a trapped Bose-Einstein condensate look like? More precisely, how does it interact with light, and does this differ fundamentally from what one would naively expect from a similar collection of very cold atoms? In the early 1990s, before Bose-Einstein condensation was realized in atomic ga ...
Section 3.5 Ionic Compounds: Formulas and Names
... Molar Mass of a Compound • Also in chapter 2 we saw that the atomic mass in amu/atom was equal to the molar mass in g/mole. – This is because the definition for amu and mole are related to each other. ...
... Molar Mass of a Compound • Also in chapter 2 we saw that the atomic mass in amu/atom was equal to the molar mass in g/mole. – This is because the definition for amu and mole are related to each other. ...
Strongly Focused He+ Beam Source for Alpha Particle
... of alphas through injecting He0 beam into ITER.[3] As the result, it is found that a He− beam of 10 mA intensity and 1-1.5 MeV energy is required to obtain enough signal of neutralized alphas against noise induced by fusion produced neutrons. This beam intensity requirement has been adopted by the c ...
... of alphas through injecting He0 beam into ITER.[3] As the result, it is found that a He− beam of 10 mA intensity and 1-1.5 MeV energy is required to obtain enough signal of neutralized alphas against noise induced by fusion produced neutrons. This beam intensity requirement has been adopted by the c ...
Dynamical diffraction of atomic matter waves by crystals of light
... There are many publications deriving the dynamical diffraction theory for all kinds of different waves directly from the wave equation. The first derivation was done by Ewald @9# in 1917 for x-ray waves propagating inside a solid state crystal. The derivation for electron matter waves inside a cryst ...
... There are many publications deriving the dynamical diffraction theory for all kinds of different waves directly from the wave equation. The first derivation was done by Ewald @9# in 1917 for x-ray waves propagating inside a solid state crystal. The derivation for electron matter waves inside a cryst ...
- Phasics
... the laser–plasma coupling for a single, controlled filament of light and to underline the importance of the coupling among the numerous speckles within conventional multispeckled beams. © 2003 Optical Society of ...
... the laser–plasma coupling for a single, controlled filament of light and to underline the importance of the coupling among the numerous speckles within conventional multispeckled beams. © 2003 Optical Society of ...
PPT - Physics
... “The model we shall choose is not a popular one, through each other and fall apart (i.e. so that we will not duplicate too much of the no hard scattering). The outgoing work of others who are similarly analyzing particles continue in roughly the same various models (e.g. constituent interchange Part ...
... “The model we shall choose is not a popular one, through each other and fall apart (i.e. so that we will not duplicate too much of the no hard scattering). The outgoing work of others who are similarly analyzing particles continue in roughly the same various models (e.g. constituent interchange Part ...
Lattice dynamics in antimony and tellurium based phase
... of phonon spectroscopy and Mössbauer spectroscopy. The feasibility of nuclear forward scattering by the 68.7 keV nuclear resonance of 73 Ge was demonstrated and its suitability for the study of condensed matter was characterized. The Ge specific lattice dynamics are easily accessed in terms of the L ...
... of phonon spectroscopy and Mössbauer spectroscopy. The feasibility of nuclear forward scattering by the 68.7 keV nuclear resonance of 73 Ge was demonstrated and its suitability for the study of condensed matter was characterized. The Ge specific lattice dynamics are easily accessed in terms of the L ...
Full text - UvA/FNWI - University of Amsterdam
... In this chapter the main theory concerning the cooling and trapping of atoms using laser light and magnetic elds relevant for this thesis is described. To study the basic interaction between light and atoms a toy model is used where an atom is considered that has only two discrete energy levels. Th ...
... In this chapter the main theory concerning the cooling and trapping of atoms using laser light and magnetic elds relevant for this thesis is described. To study the basic interaction between light and atoms a toy model is used where an atom is considered that has only two discrete energy levels. Th ...
Kursat Sendur 2009 Opex2
... beam with a spherical nanoparticle located in a high refractive index medium. More recently, detailed analytical models have been published by Lerme et al. [5], Sendur et al. [4], and Mojarad et al. [6] based on generalized Mie theory. In these studies, a linearly polarized focused beam has been use ...
... beam with a spherical nanoparticle located in a high refractive index medium. More recently, detailed analytical models have been published by Lerme et al. [5], Sendur et al. [4], and Mojarad et al. [6] based on generalized Mie theory. In these studies, a linearly polarized focused beam has been use ...
CRANFIELD UNIVERSITY Edouard Berrocal MULTIPLE
... the combustion zone and generating fine spray droplets which subsequently vaporise and burn. When employing the appropriate spray device, the desired size, velocity, concentration and trajectory of droplets can be produced in such that the energy efficiency is optimized with a consequent reduction i ...
... the combustion zone and generating fine spray droplets which subsequently vaporise and burn. When employing the appropriate spray device, the desired size, velocity, concentration and trajectory of droplets can be produced in such that the energy efficiency is optimized with a consequent reduction i ...
Light Propagation with Phase Discontinuities
... Fig. 2. (A) Calculated phase and amplitude of scattered light from a straight rod antenna made of a perfect electric conductor (20). The vertical dashed line indicates the first-order dipolar resonance of the antenna. (B) A V-antenna supports symmetric and antisymmetric modes, which are excited, res ...
... Fig. 2. (A) Calculated phase and amplitude of scattered light from a straight rod antenna made of a perfect electric conductor (20). The vertical dashed line indicates the first-order dipolar resonance of the antenna. (B) A V-antenna supports symmetric and antisymmetric modes, which are excited, res ...
Ch 3 Student.pptx
... Molar Mass of a Compound • Also in chapter 2 we saw that the atomic mass in amu/atom was equal to the molar mass in g/mole. – This is because the definition for amu and mole are related to each other. ...
... Molar Mass of a Compound • Also in chapter 2 we saw that the atomic mass in amu/atom was equal to the molar mass in g/mole. – This is because the definition for amu and mole are related to each other. ...
Thomson scattering
... ħki + mivi = ħks + msvs where: mi,s = m0/(1-βi,s2)½ When incident wave has frequency ω such that ...
... ħki + mivi = ħks + msvs where: mi,s = m0/(1-βi,s2)½ When incident wave has frequency ω such that ...
Multi-particle simulation code for IBS - Indico
... • Particles are tracked from point to point in the lattice by their invariats (no phase tracking up to now). • At each point of the lattice the scattering routine is called. ...
... • Particles are tracked from point to point in the lattice by their invariats (no phase tracking up to now). • At each point of the lattice the scattering routine is called. ...
JHEP07(2007)083 - IHEP Diffractive Group
... equation for the colour-octet t-channel. This trick can make an impression that, say, the pomeron trajectory is not just a 2-gluon exchange (with account of interaction between these two gluons via “ladder rung exchanges”) but contains many-gluon configurations in the t-channel as well. However, the ...
... equation for the colour-octet t-channel. This trick can make an impression that, say, the pomeron trajectory is not just a 2-gluon exchange (with account of interaction between these two gluons via “ladder rung exchanges”) but contains many-gluon configurations in the t-channel as well. However, the ...
Total Internal Reflection Fluorescence
... (BFP) of the objective. The propagation direction of this collimated light is determined by the radial position of the focused spot in the BFP. Focused light at the center of the BFP will propagate vertically along the axis of the microscope, while light away from the center will propagate at an ang ...
... (BFP) of the objective. The propagation direction of this collimated light is determined by the radial position of the focused spot in the BFP. Focused light at the center of the BFP will propagate vertically along the axis of the microscope, while light away from the center will propagate at an ang ...
1 - Indico
... Dimension 4 effective operator with a 2-loop mixing angle [e.g. photon mixing with valley gauge boson] 1 GeV * (mixing angle)2 times phase space 10-12 sec lifetime ...
... Dimension 4 effective operator with a 2-loop mixing angle [e.g. photon mixing with valley gauge boson] 1 GeV * (mixing angle)2 times phase space 10-12 sec lifetime ...
Direct Evidence for a Magnetic f-Electron
... the f‐electron magnetic interactions of CeCoIn5 (Fig. 2D) and therefore that strong antiferromagnetic interactions occur between adjacent f‐electron moments (SI Section 1). Solution of Gap Equations with Magnetic f‐electron Interaction Kernel These interactions are hypothesized to ...
... the f‐electron magnetic interactions of CeCoIn5 (Fig. 2D) and therefore that strong antiferromagnetic interactions occur between adjacent f‐electron moments (SI Section 1). Solution of Gap Equations with Magnetic f‐electron Interaction Kernel These interactions are hypothesized to ...
232_1.PDF
... is excited to 2 MV/m to keep the bunch width below one hundred degrees. The new buncher is excited to an effective gradient of 1.7 MV/m so that the bunches entering the Afterburner have the same distribution in longitudinal phase space as the ones exiting the 400 MeV linac: 12 degrees full width and ...
... is excited to 2 MV/m to keep the bunch width below one hundred degrees. The new buncher is excited to an effective gradient of 1.7 MV/m so that the bunches entering the Afterburner have the same distribution in longitudinal phase space as the ones exiting the 400 MeV linac: 12 degrees full width and ...
https://www.cfa.harvard.edu/~hrs/icap2002/proceedings/Esry.pdf
... passes in and out of the threshold regime. The E 2 threshold law no longer applies near the resonance, and the rate tends to the limit imposed by unitarity — often comparable to or larger than the rates for boson systems. Feshbach resonances are, of course, extremely useful tools for the experimenta ...
... passes in and out of the threshold regime. The E 2 threshold law no longer applies near the resonance, and the rate tends to the limit imposed by unitarity — often comparable to or larger than the rates for boson systems. Feshbach resonances are, of course, extremely useful tools for the experimenta ...
Cross section (physics)
The cross section is an effective area that quantifies the intrinsic likelihood of a scattering event when an incident beam strikes a target object, made of discrete particles. The cross section of a particle is the same as the cross section of a hard object, if the probabilities of hitting them with a ray are the same. It is typically denoted σ and measured in units of area.In scattering experiments, one is often interested in knowing how likely a given event occurs. However, the rate depends strongly on experimental variables such as the density of the target material, the intensity of the beam, or the area of overlap between the beam and the target material. To control for these mundane differences, one can factor out these variables, resulting in an area-like quantity known as the cross section.