Highly doubly excited S states of the helium atom
... We see from (1 1) that for extremely high excitation N -+ 00 of the inner electron we get two collinear configurations with minimum angle (cosO) -+ ( N - l ) / N % + I which corresponds to a configuration with both electrons on the same side of the nucleus (8 % 0", the 'frozen planet states', Richte ...
... We see from (1 1) that for extremely high excitation N -+ 00 of the inner electron we get two collinear configurations with minimum angle (cosO) -+ ( N - l ) / N % + I which corresponds to a configuration with both electrons on the same side of the nucleus (8 % 0", the 'frozen planet states', Richte ...
Geometric topology and connections with quantum field theory.
... [3]). The desired object is our space of elliptic bundles [3]. For a conformal field theory H, we defined the idea of stringy H-bundles on surfaces. Telegraphically speaking, an elliptic bundle is a stringy bundle on an elliptic curve E which is equivariant with respect to the action of E on itself, ...
... [3]). The desired object is our space of elliptic bundles [3]. For a conformal field theory H, we defined the idea of stringy H-bundles on surfaces. Telegraphically speaking, an elliptic bundle is a stringy bundle on an elliptic curve E which is equivariant with respect to the action of E on itself, ...
Evolving Quantum circuits - Portland State University
... [6,7,18,42,45]. This result is different from binary reversible logic, where the minimum universal gate is 3*3 [19,44] (all quantum gates are reversible and reversible gates have the same number of inputs and outputs and are one-to-one mappings, k*k gate has k inputs and k outputs). An interesting q ...
... [6,7,18,42,45]. This result is different from binary reversible logic, where the minimum universal gate is 3*3 [19,44] (all quantum gates are reversible and reversible gates have the same number of inputs and outputs and are one-to-one mappings, k*k gate has k inputs and k outputs). An interesting q ...
Quantum computing: An IBM perspective
... of seven atoms, we have a lot of new things that would happen that represent completely new opportunities for design. Atoms on a small scale behave like nothing on a large scale, for they satisfy the laws of quantum mechanics. So, as we go down and fiddle around with the atoms down there, we are work ...
... of seven atoms, we have a lot of new things that would happen that represent completely new opportunities for design. Atoms on a small scale behave like nothing on a large scale, for they satisfy the laws of quantum mechanics. So, as we go down and fiddle around with the atoms down there, we are work ...
Introduction to Renormalization Group Alex Kovner Valparaiso, December 12-14, 2013
... FIND A GIVEN FIELD CONFIGURATION φ(x) at time t. THERE IS STILL SCHROEDINGER EQUATION, BUT IT IS MUCH LESS USEFUL Ψ[φ] contains too much information, even knowing Ψ it is still hard work to get this information out. USUALLY WE ARE CONTENT WITH LESS. AS PARTICLE PHYSICISTS WE WANT SCATTERING AMPLITUD ...
... FIND A GIVEN FIELD CONFIGURATION φ(x) at time t. THERE IS STILL SCHROEDINGER EQUATION, BUT IT IS MUCH LESS USEFUL Ψ[φ] contains too much information, even knowing Ψ it is still hard work to get this information out. USUALLY WE ARE CONTENT WITH LESS. AS PARTICLE PHYSICISTS WE WANT SCATTERING AMPLITUD ...
Quantum Communications in the Maritime Environment
... determine the presence of an eavesdropper by randomly testing elements of their sifted keys and comparing their values. That is, Alice and Bob publicly agree on what bits they will use for testing, and publicly compare the values of the test bits. If the values are different, then they can presume t ...
... determine the presence of an eavesdropper by randomly testing elements of their sifted keys and comparing their values. That is, Alice and Bob publicly agree on what bits they will use for testing, and publicly compare the values of the test bits. If the values are different, then they can presume t ...
Reconstructing the dynamics of a movable mirror in a
... classical picture of this process [13, 14], setting the most appropriate scenario for the inference and study of the limitations to self-cooling due to quantum noise. While we defer to later the quantitative assessment of the problem, here we provide a very brief picture of the central point of our ...
... classical picture of this process [13, 14], setting the most appropriate scenario for the inference and study of the limitations to self-cooling due to quantum noise. While we defer to later the quantitative assessment of the problem, here we provide a very brief picture of the central point of our ...
Analysis of a Quantum Error Correcting Code using Quantum
... procedure to recover Alice’s original qubit. The CQP definition of Alice is as follows. Alice(a :b[Qbit], b :b[Qbit, Qbit, Qbit]) = (qbit y, z)a?[x : Qbit] . {x, z ∗= CNot} . {x, y ∗= CNot} . b![x, y, z] . 0 Alice is parameterized by two channels, a and b. In order to give Alice a general definition ...
... procedure to recover Alice’s original qubit. The CQP definition of Alice is as follows. Alice(a :b[Qbit], b :b[Qbit, Qbit, Qbit]) = (qbit y, z)a?[x : Qbit] . {x, z ∗= CNot} . {x, y ∗= CNot} . b![x, y, z] . 0 Alice is parameterized by two channels, a and b. In order to give Alice a general definition ...
Quantum-Secure Coin-Flipping and Applications
... irreversible. Hence, in order to produce a classical output, the simulator had to (partially) measure the quantum system without copying it beforehand, but then it would become generally impossible to reconstruct all information necessary for correct rewinding. For these reasons, no simple and strai ...
... irreversible. Hence, in order to produce a classical output, the simulator had to (partially) measure the quantum system without copying it beforehand, but then it would become generally impossible to reconstruct all information necessary for correct rewinding. For these reasons, no simple and strai ...
