Coherent-state analysis of the quantum bouncing ball
... Our current paper extends the literature of GaussianKlauder coherent states to include the case of a quantum particle confined to a semi-infinite gravity well, a system labeled the quantum bouncer 关16–21兴. The quantum bouncer satisfies at least two generic properties of one-dimensional quantum syste ...
... Our current paper extends the literature of GaussianKlauder coherent states to include the case of a quantum particle confined to a semi-infinite gravity well, a system labeled the quantum bouncer 关16–21兴. The quantum bouncer satisfies at least two generic properties of one-dimensional quantum syste ...
Spin and orbital Kondo effect in electrostatically coupled quantum dots S. L
... transparency region (VSD, h ≈ 0) corresponds to the spin Kondo effect at the dots (εi+ = εi–, 2*SU(2)). The enhanced conductance in this region, marked by the dark circle, is due to the orbital Kondo effect (ε1+ = ε2– for g1 = g2, or ε1+ = ε2+ for g1 = –g2). The orbital degeneracy for the same spin ...
... transparency region (VSD, h ≈ 0) corresponds to the spin Kondo effect at the dots (εi+ = εi–, 2*SU(2)). The enhanced conductance in this region, marked by the dark circle, is due to the orbital Kondo effect (ε1+ = ε2– for g1 = g2, or ε1+ = ε2+ for g1 = –g2). The orbital degeneracy for the same spin ...
Shamsul Kaonain
... The "braket" notation is a very compact formalism for linear algebra which was introduced by Paul Dirac. It was introduced by Dirac in order to describe in a uniform manner vectors and linear operators both in the abstract Hilbert space 1 ...
... The "braket" notation is a very compact formalism for linear algebra which was introduced by Paul Dirac. It was introduced by Dirac in order to describe in a uniform manner vectors and linear operators both in the abstract Hilbert space 1 ...
A little Big Bang
... The bosonic gas forms a Bose-Einstein condensate at low temperatures, only occupying a small volume in the trap, while the fermionic species remain large in size due to Pauli pressure. They form what is called a Fermi sea, with each atom occupying a different quantum state. It is especially striking ...
... The bosonic gas forms a Bose-Einstein condensate at low temperatures, only occupying a small volume in the trap, while the fermionic species remain large in size due to Pauli pressure. They form what is called a Fermi sea, with each atom occupying a different quantum state. It is especially striking ...
From Highly Structured E-Infinity Rings and Transfinite Maximally
... universe [40] which is used here directly and indirectly, is a clear cut example of noncommutative geometry as well as being a prototype of K-theory and Cantorian-E-infinity theory [12] [40]. Noting the well known intimate relationship of K-theory, n-categories and E-infinity algebra over operads [4 ...
... universe [40] which is used here directly and indirectly, is a clear cut example of noncommutative geometry as well as being a prototype of K-theory and Cantorian-E-infinity theory [12] [40]. Noting the well known intimate relationship of K-theory, n-categories and E-infinity algebra over operads [4 ...
The Quantum Theory of the Electron
... * Gordon, 'Z. f. Physik,' vol. 40, p. 117 (1926). p Klein, ' Z. f. Physik,' vol. 41, p. 407 (1927). : Jordan, 'Z. f. Physik,' vol. 40, p. 809 (1927); ...
... * Gordon, 'Z. f. Physik,' vol. 40, p. 117 (1926). p Klein, ' Z. f. Physik,' vol. 41, p. 407 (1927). : Jordan, 'Z. f. Physik,' vol. 40, p. 809 (1927); ...
Quantum Physics 2005 Notes-8 Three-dimensional Schrodinger Equation Notes 8
... What can we tell about L? • We can also show (homework!) that [L2,Lz]=0. • This tells us that there exists a complete set of eigenfunctions for both operators, or that we can measure both quantities simultaneously with infinite accruracy. • (We already knew that because we did the work to find the ...
... What can we tell about L? • We can also show (homework!) that [L2,Lz]=0. • This tells us that there exists a complete set of eigenfunctions for both operators, or that we can measure both quantities simultaneously with infinite accruracy. • (We already knew that because we did the work to find the ...
E + - IPAM
... energy at most E. – If for every probability C accepts is low, then every eigenstate of H has energy at least E+D. ...
... energy at most E. – If for every probability C accepts is low, then every eigenstate of H has energy at least E+D. ...
Paper - MaPhySto
... system were first formulated in cooperation with C.Aberg in [1]. 2. The description of continuous in time direct observation of a quantum system In this section we first consider the problem of description of continuous in time direct measurement of any quantum system. We use the clear and consisten ...
... system were first formulated in cooperation with C.Aberg in [1]. 2. The description of continuous in time direct observation of a quantum system In this section we first consider the problem of description of continuous in time direct measurement of any quantum system. We use the clear and consisten ...
Environment Assisted Quantum Transport in Organic Molecules
... trough the system. Once the electron enters the system it can leave the system only trough the exit. Unless some symmetry consideration forbids it the electron will leave the system with probability 1, so we have to find another characteristics. The next quantity is the average time τ an electron ne ...
... trough the system. Once the electron enters the system it can leave the system only trough the exit. Unless some symmetry consideration forbids it the electron will leave the system with probability 1, so we have to find another characteristics. The next quantity is the average time τ an electron ne ...
What is light? - Dipankar Home
... probing deeper into the nature of reality underlying quantum phenomena. Physicists taking this viewpoint say that a quantum entity such as an electron is actually a localised particle, but that its behaviour is guided by a physically real field satisfying the basic quantum mechanical equations. John ...
... probing deeper into the nature of reality underlying quantum phenomena. Physicists taking this viewpoint say that a quantum entity such as an electron is actually a localised particle, but that its behaviour is guided by a physically real field satisfying the basic quantum mechanical equations. John ...
Poster PDF (4.4mb)
... [2] Y.-J. Lin, R. L. Compton, K. Jimenez-Garcia, J. V. Porto, and I. Spielman, Nature 462, 628 (2009). [3] K. Jimenez-Garcia, L. J. LeBlanc, R. A. Williams, M. C. Beeler, A. R. Perry, and I. B. Spielman, Phys. Rev. Lett. 108, 225303 (2012). [4] M. Aidelsburger, M. Atala, S. Nascimbène, S. Trotzky, Y ...
... [2] Y.-J. Lin, R. L. Compton, K. Jimenez-Garcia, J. V. Porto, and I. Spielman, Nature 462, 628 (2009). [3] K. Jimenez-Garcia, L. J. LeBlanc, R. A. Williams, M. C. Beeler, A. R. Perry, and I. B. Spielman, Phys. Rev. Lett. 108, 225303 (2012). [4] M. Aidelsburger, M. Atala, S. Nascimbène, S. Trotzky, Y ...
Introduction to Quantum Mechanics and Multiplet Splitting in 1H
... If we once again consider the spinning nuclei, the magnetic field produced by the spin causes small changes in the electron distribution of its bonds. These in turn effect the electron distribution of neighboring bonds, which affect the neighboring nuclei. This process is known as spin-spin coupling ...
... If we once again consider the spinning nuclei, the magnetic field produced by the spin causes small changes in the electron distribution of its bonds. These in turn effect the electron distribution of neighboring bonds, which affect the neighboring nuclei. This process is known as spin-spin coupling ...