Nature 419, (51
... added to the potential well. It can be related to the s-wave scattering length a Ðand the ground-state wavefunction w(x) through U ¼ ...
... added to the potential well. It can be related to the s-wave scattering length a Ðand the ground-state wavefunction w(x) through U ¼ ...
Quantum Tic-Tac-Toe: A Genuine Probabilistic Approach
... because some problems that require a quantum description can only be successfully addressed if information can be accessed at the physical level used to encode it. The question that we ask in this paper is: How is this superior computational power manifesting itself in the context of quantum games? ...
... because some problems that require a quantum description can only be successfully addressed if information can be accessed at the physical level used to encode it. The question that we ask in this paper is: How is this superior computational power manifesting itself in the context of quantum games? ...
M15/03
... sequence (s0 (x), s1 (x), . . . , sm (x)), sm (x) > 0 we define w(x) = sm (x). Thus, w(x) is the cardinality of the highest shell of x. The width sequence of Pn0 is the sequence of integers (w(xn,0 ), w(xn,1 ), . . . , w(xn,2n−1 −1 )) We next display the width sequences of Pn0 for the first few valu ...
... sequence (s0 (x), s1 (x), . . . , sm (x)), sm (x) > 0 we define w(x) = sm (x). Thus, w(x) is the cardinality of the highest shell of x. The width sequence of Pn0 is the sequence of integers (w(xn,0 ), w(xn,1 ), . . . , w(xn,2n−1 −1 )) We next display the width sequences of Pn0 for the first few valu ...
Leftover Hashing Against Quantum Side Information
... entirely on probability theory and side information is, therefore (often implicitly), assumed to be represented by a classical system (modeled as a random variable).3 In fact, since hashing is an entirely “classical” process (a simple mapping from a random variable to another random variable ), one ...
... entirely on probability theory and side information is, therefore (often implicitly), assumed to be represented by a classical system (modeled as a random variable).3 In fact, since hashing is an entirely “classical” process (a simple mapping from a random variable to another random variable ), one ...
Spin signatures of exchange-coupled triplet pairs formed by singlet
... dips and means that δPL/PL for the higher-field anticrossing is closer to -1/4 than for the lower-field one. When the two triplets in a pair are equivalent, i.e. when their zero-field splitting tensors have the same orientation and D values, and their exciton g-values are identical, the total Hamilt ...
... dips and means that δPL/PL for the higher-field anticrossing is closer to -1/4 than for the lower-field one. When the two triplets in a pair are equivalent, i.e. when their zero-field splitting tensors have the same orientation and D values, and their exciton g-values are identical, the total Hamilt ...
Slide 1
... It may be that there is no new physics until we enter the TeV region (LHC). In which case we may well want a ~2 TeV linear collider. WW scattering is an excellent place to look for evidence of the new physics: With 1 year high luminosity should be able to measure WW cross-section differential in ...
... It may be that there is no new physics until we enter the TeV region (LHC). In which case we may well want a ~2 TeV linear collider. WW scattering is an excellent place to look for evidence of the new physics: With 1 year high luminosity should be able to measure WW cross-section differential in ...
.
... internal ion excitation j0; npn ¼ 1i ! j1; npn ¼ 0i, we assume that states j1i and j0i are connected by a metastable quadrupole electric transition. The reason for considering this kind of transition here is that, as opposed to step III above, there is a phase matching condition: the collective exci ...
... internal ion excitation j0; npn ¼ 1i ! j1; npn ¼ 0i, we assume that states j1i and j0i are connected by a metastable quadrupole electric transition. The reason for considering this kind of transition here is that, as opposed to step III above, there is a phase matching condition: the collective exci ...
CYCLOTRON RESONANCE IN HIGH MAGNETIC
... early 1950s 1−3 , the methods of far-infrared (FIR) and microwave magneto-optical spectroscopy [in the terahertz (THz) and gigahertz (GHz) frequency ranges] have been used for a variety of purposes — e.g. for determining band parameters of semiconductors, elucidating carrier scattering mechanisms, s ...
... early 1950s 1−3 , the methods of far-infrared (FIR) and microwave magneto-optical spectroscopy [in the terahertz (THz) and gigahertz (GHz) frequency ranges] have been used for a variety of purposes — e.g. for determining band parameters of semiconductors, elucidating carrier scattering mechanisms, s ...
“Magnus” force - Pacific Institute of Theoretical Physics
... Recall that we can always formulate the dynamics for the reduced density matrix as ...
... Recall that we can always formulate the dynamics for the reduced density matrix as ...
Quantum Algorithms for Estimating Gauss Sums and Calculating
... the entries xj ∈ Fp . If Fpr does not have a self-dual basis, we can use an almost self-dual basis to obtain the same complexity complexity. t u For general pr or n, it is not known how to implement the quantum Fourier transform exactly. Hence, the following results and the estimation algorithms of ...
... the entries xj ∈ Fp . If Fpr does not have a self-dual basis, we can use an almost self-dual basis to obtain the same complexity complexity. t u For general pr or n, it is not known how to implement the quantum Fourier transform exactly. Hence, the following results and the estimation algorithms of ...
