A Quantum Analog to Basis Function Networks
... being a linear combination of the basis. A set of examples is considered as a quantum system that undergoes unitary transformations to produce learning. The main result of the work is a quantum computational learning algorithm that is unique among quantum algorithms as it does not assume a priori kn ...
... being a linear combination of the basis. A set of examples is considered as a quantum system that undergoes unitary transformations to produce learning. The main result of the work is a quantum computational learning algorithm that is unique among quantum algorithms as it does not assume a priori kn ...
Wael`s quantum brain - Electrical & Computer Engineering
... 4. Generate new CRL file: Now, the QuantumOutput.xml file contains the results of the circuit along with their probabilities alpha2 and beta2. To generate the new CRL file, we need to run the following command. Ø java ReadWriteCrl MyCrlFile.crl QuantumOutput.xml The new CRL file with the name TestOu ...
... 4. Generate new CRL file: Now, the QuantumOutput.xml file contains the results of the circuit along with their probabilities alpha2 and beta2. To generate the new CRL file, we need to run the following command. Ø java ReadWriteCrl MyCrlFile.crl QuantumOutput.xml The new CRL file with the name TestOu ...
Quantum Coins, Dice and Children: Probability and Quantum Statistics
... In three of these cases B is selected, and since in two of them the remaining particle is also B, the answer to question (I) is 2/3, not 1/2. Again, we see that Bose statistics enhances the probability of finding two identical bosons in the same state. In the above, we have analyzed the problems by ...
... In three of these cases B is selected, and since in two of them the remaining particle is also B, the answer to question (I) is 2/3, not 1/2. Again, we see that Bose statistics enhances the probability of finding two identical bosons in the same state. In the above, we have analyzed the problems by ...
Quantized quasi-two-dimensional Bose-Einstein condensates with spatially modulated nonlinearity Deng-Shan Wang, Xing-Hua Hu,
... function (3), as shown in Fig. 4(b). It is shown that the energy levels of the atoms are only associated with the principal quantum number n. These are similar to energy level distribution of the energy eigenvalue problem for the linear harmonic oscillator described by linear Schrödinger equation. ...
... function (3), as shown in Fig. 4(b). It is shown that the energy levels of the atoms are only associated with the principal quantum number n. These are similar to energy level distribution of the energy eigenvalue problem for the linear harmonic oscillator described by linear Schrödinger equation. ...
A Quantum self-Routing Packet Switching
... • Also , it will not be possible to verify whether the received packet was intended for that output or not because the output address bits are removed by the nodes of the network • We can overcome the problem of verifying the received packets by keeping a copy of the output address in the data port ...
... • Also , it will not be possible to verify whether the received packet was intended for that output or not because the output address bits are removed by the nodes of the network • We can overcome the problem of verifying the received packets by keeping a copy of the output address in the data port ...
X. Xiao, J.C. Sturm, C.W. Liu, L.C. Lenchyshyn, M.L.W. Thewalt, R.B. Gregory, P. Fejes, "Quantum confinement effects in strained silicon-germanium alloy quantum wells," Appl. Phys. Lett.60, pp. 2135-2137 (1992).
... densitiesI Because no phonons are involved, the NP signal is an accurate measure of the band gap except for exciton binding energies at 4 K and renormalization effects due to the high-carrier densities in the plasmas at 77 K (about 10-20 meV). This NP signal will be used in this letter to track the ...
... densitiesI Because no phonons are involved, the NP signal is an accurate measure of the band gap except for exciton binding energies at 4 K and renormalization effects due to the high-carrier densities in the plasmas at 77 K (about 10-20 meV). This NP signal will be used in this letter to track the ...
Feynman lectures on computation
... • The unitary transformation U consists of a series of elementary quantum gates, single-, two-qubit... • The sequence of these quantum gates that are applied to the quantum input depends on the classical variables x and N complicatedly. • We need a classical computer processes the classical variable ...
... • The unitary transformation U consists of a series of elementary quantum gates, single-, two-qubit... • The sequence of these quantum gates that are applied to the quantum input depends on the classical variables x and N complicatedly. • We need a classical computer processes the classical variable ...
Simulation of Quantum Gates on a Novel GPU Architecture
... X = |0ih1| + |1ih0|, does project component |0i over the |1i one, and vice versa, following that its quantum application to a classic state 0 or 1 is equivalent to the logic operator NOT. The generalization to gates with more than one qubit is straightforward, resulting in an associated matrix of or ...
... X = |0ih1| + |1ih0|, does project component |0i over the |1i one, and vice versa, following that its quantum application to a classic state 0 or 1 is equivalent to the logic operator NOT. The generalization to gates with more than one qubit is straightforward, resulting in an associated matrix of or ...
UNITARY OPERATORS AND SYMMETRY TRANSFORMATIONS
... state, either |α and |β , use a measurement to guess which one. If |α and |β are not orthogonal, then no measurement perfectly distinguishes them, and we always have some constant probability of error. However, if we could make many copies of the unknown state, then we could repeat the optimal measu ...
... state, either |α and |β , use a measurement to guess which one. If |α and |β are not orthogonal, then no measurement perfectly distinguishes them, and we always have some constant probability of error. However, if we could make many copies of the unknown state, then we could repeat the optimal measu ...
CBO_Paper3_ConsciousnessandQuantumMechanics
... does not give the exact location of the particle. The square of the absolute value of the wave function will give the probability that a particle will be found at location (x,y,z) at time t. This is conflict with measurement. When an object is measured, an object is only in one state instead of all ...
... does not give the exact location of the particle. The square of the absolute value of the wave function will give the probability that a particle will be found at location (x,y,z) at time t. This is conflict with measurement. When an object is measured, an object is only in one state instead of all ...