Chapter 4 Orbital angular momentum and the hydrogen atom
... symmetric potentials und use the angular momentum operator to compute the energy spectrum of hydrogen-like atoms. ...
... symmetric potentials und use the angular momentum operator to compute the energy spectrum of hydrogen-like atoms. ...
2008 midtermkey - University of Victoria
... an electron from its surface via the photoelectric effect. What is the minimum energy (in J) needed for emission of one electron from manganese? A) 3.08 x 10–49 ...
... an electron from its surface via the photoelectric effect. What is the minimum energy (in J) needed for emission of one electron from manganese? A) 3.08 x 10–49 ...
Quantum Theory of the Coherently Pumped Micromaser
... Phase Properties of the Coherently Pumped Micromaser It is quite clear that the strong coherence present in this system also calls for an understanding of its features in terms of quantum phase. Studying the phase properties of quantum fields is arguably one of the most controversial subjects in phy ...
... Phase Properties of the Coherently Pumped Micromaser It is quite clear that the strong coherence present in this system also calls for an understanding of its features in terms of quantum phase. Studying the phase properties of quantum fields is arguably one of the most controversial subjects in phy ...
Majorana and the path-integral approach to Quantum Mechanics
... “slightly different classical motions” (the emphasis is given by Majorana himself), according to what specified by the Heisenberg’s uncertainty principle and mentioned just afterwards, is thus evidently related to that of the sufficiently wide integration region in Eq. (5) for quantum systems. In th ...
... “slightly different classical motions” (the emphasis is given by Majorana himself), according to what specified by the Heisenberg’s uncertainty principle and mentioned just afterwards, is thus evidently related to that of the sufficiently wide integration region in Eq. (5) for quantum systems. In th ...
Quantum Criticality - Subir Sachdev
... so it does not break the spin-inversion symmetry. It is not a ferromagnet, and we refer to it as a paramagnet. It is important to distinguish this quantum paramagnet from a thermal paramagnet obtained by simply raising a ferromagnet to a high temperature. In the thermal case, the spins are fluctuati ...
... so it does not break the spin-inversion symmetry. It is not a ferromagnet, and we refer to it as a paramagnet. It is important to distinguish this quantum paramagnet from a thermal paramagnet obtained by simply raising a ferromagnet to a high temperature. In the thermal case, the spins are fluctuati ...
quantum states satisfying classical probability constraints
... present examples of such bipartite states. We prove (proposition 2) that the nonseparable Werner state (5 ) is a DSO state for any dimension d ≥ 2 and represents a Bell class state if d ≥ 3. In sections 2.2, 2.3, for an arbitrary bipartite state, we derive (propositions 3, 4) new upper bounds of lin ...
... present examples of such bipartite states. We prove (proposition 2) that the nonseparable Werner state (5 ) is a DSO state for any dimension d ≥ 2 and represents a Bell class state if d ≥ 3. In sections 2.2, 2.3, for an arbitrary bipartite state, we derive (propositions 3, 4) new upper bounds of lin ...
QUANTUM THREE-PASS PROTOCOL: KEY DISTRIBUTION USING
... sequence of random bits. As a result, Eve will observe 0 or 1 with probability 1 2 . Therefore, the QTPP guarantees the confidentiality of communication. Eve cannot resend the intercepted data to Bob without errors. Also, the existence of Eve can be detected, because Eve’s intercept-resend attack in ...
... sequence of random bits. As a result, Eve will observe 0 or 1 with probability 1 2 . Therefore, the QTPP guarantees the confidentiality of communication. Eve cannot resend the intercepted data to Bob without errors. Also, the existence of Eve can be detected, because Eve’s intercept-resend attack in ...
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).
... between silicon and germanium following People.” For the Luttinger valence band parameters yl, y2, and y3, we follow Braunstein,20 and assume a linear variation of l/F, l/G, I/H, and l/H,, where F, G, H,, and H2 are k*p parameters originally introduced by Dresselhaus, Kip, and Kittel.21 That excelle ...
... between silicon and germanium following People.” For the Luttinger valence band parameters yl, y2, and y3, we follow Braunstein,20 and assume a linear variation of l/F, l/G, I/H, and l/H,, where F, G, H,, and H2 are k*p parameters originally introduced by Dresselhaus, Kip, and Kittel.21 That excelle ...
![arXiv:0803.3834v2 [quant-ph] 26 May 2009](http://s1.studyres.com/store/data/015940141_1-1e8e53e4d619ce68a74ed7b6b3742d1d-300x300.png)
Resilient Quantum Computation in Correlated Environments: A Quantum Phase Transition Perspective
... A similar argument can be applied to all of the remaining terms of Eq. (11). The critical condition is when D z 2 . In this particular case, correlations between hypercubes introduce logarithmic corrections to the stochastic part of Eq. (11). An irrelevant flow for indicates that the system i ...
... A similar argument can be applied to all of the remaining terms of Eq. (11). The critical condition is when D z 2 . In this particular case, correlations between hypercubes introduce logarithmic corrections to the stochastic part of Eq. (11). An irrelevant flow for indicates that the system i ...