Mechanical Proof of the Second Law of Thermodynamics Based on
... Increase) if non adiabatic transformations were considered. Based on the principles of microscopic (quantum or classical) mechanics here we prove that, provided the initial equilibrium satisfy the natural condition of decreasing ordering of probabilities, the expectation value of the volume entropy ...
... Increase) if non adiabatic transformations were considered. Based on the principles of microscopic (quantum or classical) mechanics here we prove that, provided the initial equilibrium satisfy the natural condition of decreasing ordering of probabilities, the expectation value of the volume entropy ...
Fractional @ Scaling for Quantum Kicked Rotors without Cantori
... double-kicked particle (2-DKP), found fractional scaling of momentum distributions with L @0:75 , i.e., characterized by one of the classical golden-ratio exponents, and in phase-space regions corresponding quite closely to those of [6]. It was argued that this too was evidence of the quantum sig ...
... double-kicked particle (2-DKP), found fractional scaling of momentum distributions with L @0:75 , i.e., characterized by one of the classical golden-ratio exponents, and in phase-space regions corresponding quite closely to those of [6]. It was argued that this too was evidence of the quantum sig ...
Quantum Lambda Calculus - Department of Mathematics and
... possible context. For example, the term M N only makes sense if M is a function; the term let hx, yi = M in N only makes sense when M is a pair; the term match P with (x 7→ M | y 7→ N ) only makes sense when P is a member of a disjoint union; and the term meas M only makes sense if M is a quantum bi ...
... possible context. For example, the term M N only makes sense if M is a function; the term let hx, yi = M in N only makes sense when M is a pair; the term match P with (x 7→ M | y 7→ N ) only makes sense when P is a member of a disjoint union; and the term meas M only makes sense if M is a quantum bi ...
Paper
... to study many-body phenomena because of the relative ease with which parameters in the model Hamiltonian can be tuned across a wide range [1,2]. Such studies have resulted in a better understanding of various phase transitions such as the Berezinskii-Kosterlitz-Thouless transition in two-dimensional ...
... to study many-body phenomena because of the relative ease with which parameters in the model Hamiltonian can be tuned across a wide range [1,2]. Such studies have resulted in a better understanding of various phase transitions such as the Berezinskii-Kosterlitz-Thouless transition in two-dimensional ...
Braid Topologies for Quantum Computation
... found which approximate any even number, 2m, of windings of the static quasiparticles. Figure 3(b) shows a twoqubit braid in which the pattern from Fig. 3(a) is used to weave the control pair through the target qubit. If the control qubit is in the state |0L i this weave does nothing, but if it is i ...
... found which approximate any even number, 2m, of windings of the static quasiparticles. Figure 3(b) shows a twoqubit braid in which the pattern from Fig. 3(a) is used to weave the control pair through the target qubit. If the control qubit is in the state |0L i this weave does nothing, but if it is i ...
How to Construct Quantum Random Functions
... Goldreich, Goldwasser, and Micali show how to build a pseudorandom function PRF from any length-doubling pseudorandom generator G. This construction is known as the GGM construction. Pseudorandom generators can, in turn, be built from any one-way function, as shown by Håstad et al. [HILL99]. The se ...
... Goldreich, Goldwasser, and Micali show how to build a pseudorandom function PRF from any length-doubling pseudorandom generator G. This construction is known as the GGM construction. Pseudorandom generators can, in turn, be built from any one-way function, as shown by Håstad et al. [HILL99]. The se ...
Quantum violation of classical physics in macroscopic systems
... macroscopic everyday world. While microscopic particles, such as photons, electrons or even large molecules, can nowadays be put into superposition or entangled states [17–19], the concept that a macroscopic object, such as a cat, could be in a superposition state, seems, in Schrödinger’s words, bur ...
... macroscopic everyday world. While microscopic particles, such as photons, electrons or even large molecules, can nowadays be put into superposition or entangled states [17–19], the concept that a macroscopic object, such as a cat, could be in a superposition state, seems, in Schrödinger’s words, bur ...
Doubly excited nonautoionizing P, D, and F states of helium with
... choice of 共A, B, C兲 in the framework of the HylleraasUndheim theorem. The present study is optimized in such a way that a particular set of optimized values of the nonlinear parameters can produce reasonably accurate energy levels for a particular partial-wave state. In Tables I–III, we have ...
... choice of 共A, B, C兲 in the framework of the HylleraasUndheim theorem. The present study is optimized in such a way that a particular set of optimized values of the nonlinear parameters can produce reasonably accurate energy levels for a particular partial-wave state. In Tables I–III, we have ...
A Theoretical Study of Atomic Trimers in the Critical Stability Region
... Elander. Without your help and efforts nothing would be done. My friend Doc. Sergey Levin is greatly acknowledged for his very important scientific help and guidance during these four years, and for his will to help me with everything else when needed. He taught me not only physics and mathematics b ...
... Elander. Without your help and efforts nothing would be done. My friend Doc. Sergey Levin is greatly acknowledged for his very important scientific help and guidance during these four years, and for his will to help me with everything else when needed. He taught me not only physics and mathematics b ...
Construction X for quantum error-correcting codes
... For x ∈ Fn4 let ||x|| = hx, xi be the norm of x. Note that ||x|| is always 0 or 1 and it equals the parity of wt(x). A subset S ⊂ Fn4 is called orthonormal if hx, y i = 0 for any two distinct x, y ∈ S and hx, xi = 1 for any x ∈ S. Proposition Let D be a subspace of Fn4 and assume that M is a basis f ...
... For x ∈ Fn4 let ||x|| = hx, xi be the norm of x. Note that ||x|| is always 0 or 1 and it equals the parity of wt(x). A subset S ⊂ Fn4 is called orthonormal if hx, y i = 0 for any two distinct x, y ∈ S and hx, xi = 1 for any x ∈ S. Proposition Let D be a subspace of Fn4 and assume that M is a basis f ...
School of Physics - The University of Sydney
... This unit is assessed through a final examination, a mid-term examination, assignments taken throughout the semester, participation in computational physics sessions and a project and computational test at the end of semester. Proof of identification is required at all examinations. Except where oth ...
... This unit is assessed through a final examination, a mid-term examination, assignments taken throughout the semester, participation in computational physics sessions and a project and computational test at the end of semester. Proof of identification is required at all examinations. Except where oth ...
On a measurement-free quantum lambda calculus with classical
... Notably, a configuration (the quantum generalisation of a term) is strongly normalising if and only if it is weakly normalising. Another remarkable feature of the calculus is given by the (quantum) standardisation theorem. Roughly speaking, for each terminating computation there is another ‘canonical ...
... Notably, a configuration (the quantum generalisation of a term) is strongly normalising if and only if it is weakly normalising. Another remarkable feature of the calculus is given by the (quantum) standardisation theorem. Roughly speaking, for each terminating computation there is another ‘canonical ...
Atomic Physics
... neutral, it also has 3 electrons. Bohr’s model is not applicable. If two electrons are stripped away, one ends up with the ion Li2+ . What is the ionization energy of Li2+ ? Solution: Since one has only one electron left, the Bohr’s model can be used. The ionization energy is found by putting n = 1 ...
... neutral, it also has 3 electrons. Bohr’s model is not applicable. If two electrons are stripped away, one ends up with the ion Li2+ . What is the ionization energy of Li2+ ? Solution: Since one has only one electron left, the Bohr’s model can be used. The ionization energy is found by putting n = 1 ...
Braid Topologies for Quantum Computation
... desired operation of this form [22]. However, unlike the single qubit case, actual implementation of this procedure is problematic. The space of unitary operations for six quasiparticles is parameterized by 87 continuous parameters, as opposed to 3 for the three quasiparticle case, and searching for ...
... desired operation of this form [22]. However, unlike the single qubit case, actual implementation of this procedure is problematic. The space of unitary operations for six quasiparticles is parameterized by 87 continuous parameters, as opposed to 3 for the three quasiparticle case, and searching for ...
For ULSI workshop. OUR SLIDES not ready. In PPT format.
... By iteratively applying the same input test vector (a probabilistic test) we are calculating the probability of getting the observed output. The input vectors are always vectors of pure states. Each successive iteration reduces the probability of obtaining a correct measurement for a faulty circuit. ...
... By iteratively applying the same input test vector (a probabilistic test) we are calculating the probability of getting the observed output. The input vectors are always vectors of pure states. Each successive iteration reduces the probability of obtaining a correct measurement for a faulty circuit. ...
