MOCK MODULAR FORMS AND QUANTUM MODULAR FORMS 1
... modular form, called f , as the holomorphic part of any harmonic Maass form M of weight k such that ξk (M ), called the shadow of f , is a cusp form. Thus, the mock theta functions of Ramanujan are weight 1/2 examples of Zagier’s mock modular forms. Denote the space of mock modular forms of weight k ...
... modular form, called f , as the holomorphic part of any harmonic Maass form M of weight k such that ξk (M ), called the shadow of f , is a cusp form. Thus, the mock theta functions of Ramanujan are weight 1/2 examples of Zagier’s mock modular forms. Denote the space of mock modular forms of weight k ...
Non-Abelian Anyons and Topological Quantum Computation
... is anti-symmetric. One cannot overemphasize, of course, the importance of the symmetry of the wavefunction, which is the root of the Pauli principle, superfluidity, the metallic state, Bose-Einstein condensation, and a long list of other phenomena. The limitation to one of two possible types of quan ...
... is anti-symmetric. One cannot overemphasize, of course, the importance of the symmetry of the wavefunction, which is the root of the Pauli principle, superfluidity, the metallic state, Bose-Einstein condensation, and a long list of other phenomena. The limitation to one of two possible types of quan ...
Electronic quantum optics beyond the integer quantum Hall effect
... [1, 2] aims at exploring the intimate nature of solid-state systems by generating, manipulating and measuring individual electronic wave-packets (WPs) ballistically propagating in mesoscopic devices, in the same spirit as is conventionally done for photons transmitted along wave-guides. This opens u ...
... [1, 2] aims at exploring the intimate nature of solid-state systems by generating, manipulating and measuring individual electronic wave-packets (WPs) ballistically propagating in mesoscopic devices, in the same spirit as is conventionally done for photons transmitted along wave-guides. This opens u ...
Advanced Placement Physics – B
... 48. Know the fields of highly symmetric charge distributions. 49. Understand the nature of electric fields in and around conductors. 50. Describe and sketch a graph of the electric field and potential inside and outside of a charged conducting sphere. 51. Understand induced charge and electrostatic ...
... 48. Know the fields of highly symmetric charge distributions. 49. Understand the nature of electric fields in and around conductors. 50. Describe and sketch a graph of the electric field and potential inside and outside of a charged conducting sphere. 51. Understand induced charge and electrostatic ...
Read PDF - Physics
... From these we obtain the three-photon coincidence probabilities for the AAA (−) and BBB (þ) combinations ...
... From these we obtain the three-photon coincidence probabilities for the AAA (−) and BBB (þ) combinations ...
Far-infrared-driven electron-hole correlations in a quantum dot with an internal... Roger Sakhel, Lars Jo¨nsson, and John W. Wilkins
... lead to qualitatively different optical properties for a correlated and an uncorrelated electron-hole pair. Since the word ‘correlation’ can have many meanings, we should make clear that in this paper correlation refers to the coupling between determinants caused by the Coulomb interaction. An FIR l ...
... lead to qualitatively different optical properties for a correlated and an uncorrelated electron-hole pair. Since the word ‘correlation’ can have many meanings, we should make clear that in this paper correlation refers to the coupling between determinants caused by the Coulomb interaction. An FIR l ...
Isosceles and Equilateral Triangles
... Proof of the Isosceles Triangle Theorem Begin with isosceles triangle XYZ. XY is congruent XZ. Draw XB, the bisector of the vertex angle YXZ Prove
... Proof of the Isosceles Triangle Theorem Begin with isosceles triangle XYZ. XY is congruent XZ. Draw XB, the bisector of the vertex angle YXZ Prove
Discovery of the Higgs Particle
... Though the full story is complicated, many important properties follow from two basic facts: (1) no two fermions can occupy the same state, which causes even slow-moving fermions to exert pressure on each other that bosons lack (known as Pauli’s exclusion principle), and (2) multi-particle interacti ...
... Though the full story is complicated, many important properties follow from two basic facts: (1) no two fermions can occupy the same state, which causes even slow-moving fermions to exert pressure on each other that bosons lack (known as Pauli’s exclusion principle), and (2) multi-particle interacti ...
Tessellations-KJK
... How to use functions of transformational geometry to manipulate shapes How to identify interior & exterior angles Angle properties for straight lines, equilateral triangles and other polygons How to identify a 2D shape They are working with an Euclidean Plane ...
... How to use functions of transformational geometry to manipulate shapes How to identify interior & exterior angles Angle properties for straight lines, equilateral triangles and other polygons How to identify a 2D shape They are working with an Euclidean Plane ...
Fulltext
... on the energy level splitting between the ground and first excited states. Particle Coulomb interactions are strong in small quantum dots with a high potential barrier. However, large quantum dots are considered in our case due to the requirement of a 1.3 µm emission wavelength. Therefore, the parti ...
... on the energy level splitting between the ground and first excited states. Particle Coulomb interactions are strong in small quantum dots with a high potential barrier. However, large quantum dots are considered in our case due to the requirement of a 1.3 µm emission wavelength. Therefore, the parti ...
