Coulombic interactions in the fractional quantum Hall effect: from
... We have formulated the theorem using operators in their exponentiated form: this makes them bounded, which avoids domain problems. For the sake of clarity we note how this result holds not only for position and momenta operators but also for any other operators satisfying the same conditions. This t ...
... We have formulated the theorem using operators in their exponentiated form: this makes them bounded, which avoids domain problems. For the sake of clarity we note how this result holds not only for position and momenta operators but also for any other operators satisfying the same conditions. This t ...
EMBEDDABLE QUANTUM HOMOGENEOUS SPACES 1
... Vaes [7, 9, 13]. We will be following the path begun by Vaes in [29], where he dealt with the generalization to the non-compact case of the quotient construction considered by Podleś. The task seems quite a lot more complicated than for compact quantum groups. We encounter many different classes of ...
... Vaes [7, 9, 13]. We will be following the path begun by Vaes in [29], where he dealt with the generalization to the non-compact case of the quotient construction considered by Podleś. The task seems quite a lot more complicated than for compact quantum groups. We encounter many different classes of ...
Quantum error correction
... This thesis intends to familiarise the reader with quantum error correction, and also show some relations to the well known concept of information – and the lesser known quantum information. Quantum information describes how information can be carried by quantum states, and how interaction with othe ...
... This thesis intends to familiarise the reader with quantum error correction, and also show some relations to the well known concept of information – and the lesser known quantum information. Quantum information describes how information can be carried by quantum states, and how interaction with othe ...
Spin-valley lifetimes in a silicon quantum dot with tunable valley
... Remarkably, silicon is also an ideal material to manipulate quantum information encoded in individual electron spins1–3. This is a consequence of the weak spin–orbit coupling and the existence of an abundant spin-zero isotope, which can be further enriched to obtain a ‘semiconductor vacuum’ in which ...
... Remarkably, silicon is also an ideal material to manipulate quantum information encoded in individual electron spins1–3. This is a consequence of the weak spin–orbit coupling and the existence of an abundant spin-zero isotope, which can be further enriched to obtain a ‘semiconductor vacuum’ in which ...
Time-Independent Perturbation Theory Atomic Physics Applications 1 Introduction
... (artificial atoms) closely mirror those of real atoms. In nuclear physics, precision atomic spectroscopy allows precise measurements of isotopic masses and other isotopic properties. In addition, as the most abundant element, much astronomical data is based on measuring the spectral lines of hydroge ...
... (artificial atoms) closely mirror those of real atoms. In nuclear physics, precision atomic spectroscopy allows precise measurements of isotopic masses and other isotopic properties. In addition, as the most abundant element, much astronomical data is based on measuring the spectral lines of hydroge ...
IO-IY
... 33. ssm Molybdenum has an atomic number of 2 = 42. Using the Bohr model, estimate the wavelength of the Kcx X-ray. 34. Interactive LearningWare 30.2 at www.wiley.comlcollege/cutnell reviews the concepts that are pertinent to this problem. By using the Bohr model, decide which element is likely to em ...
... 33. ssm Molybdenum has an atomic number of 2 = 42. Using the Bohr model, estimate the wavelength of the Kcx X-ray. 34. Interactive LearningWare 30.2 at www.wiley.comlcollege/cutnell reviews the concepts that are pertinent to this problem. By using the Bohr model, decide which element is likely to em ...
Partially Nondestructive Continuous Detection of Individual Traveling Optical Photons
... detection. The cross-correlation function gsp ¼ hns np i= hns ihnp i can be understood as the likelihood of measuring the signal twice: first measuring it nondestructively with our cavity QED system, which results in a detected probe photon (np ¼ 1), and then checking the first measurement by measur ...
... detection. The cross-correlation function gsp ¼ hns np i= hns ihnp i can be understood as the likelihood of measuring the signal twice: first measuring it nondestructively with our cavity QED system, which results in a detected probe photon (np ¼ 1), and then checking the first measurement by measur ...
Non-equilibrium steady state of sparse systems OFFPRINT and D. Cohen D. Hurowitz
... “quantum” case: see technical details below. Some technical details with regard to eq. (14) are in order (can be skipped in first reading). In the energy basis, H0 is a diagonal matrix with energy levels En . The state of the system is represented by the probability matrix, which can be rewritten as ...
... “quantum” case: see technical details below. Some technical details with regard to eq. (14) are in order (can be skipped in first reading). In the energy basis, H0 is a diagonal matrix with energy levels En . The state of the system is represented by the probability matrix, which can be rewritten as ...
On the Theory of Intramolecular Energy Transfer
... Poincare surfaces of section with Wigner distribution functions (calculated in a particular way). 25 One thus expects that, apart from tunnelling and interference contributions to any particular problem, there will be a close correspondence between various reduced properties calculated by averaging ...
... Poincare surfaces of section with Wigner distribution functions (calculated in a particular way). 25 One thus expects that, apart from tunnelling and interference contributions to any particular problem, there will be a close correspondence between various reduced properties calculated by averaging ...