 
									
								
									t = |T – T c
									
... Quantum system: H = H(a+, a) in second quantization Hkin and Hpot do NOT commute => statics and dynamics couple, and need to be considered together! Technical solution: Divide [0,β] into infinitesimal sections parameterized by 0 ≤ τ ≤ β (“imaginary time”), making use of BCH, and represent Z as a fu ...
                        	... Quantum system: H = H(a+, a) in second quantization Hkin and Hpot do NOT commute => statics and dynamics couple, and need to be considered together! Technical solution: Divide [0,β] into infinitesimal sections parameterized by 0 ≤ τ ≤ β (“imaginary time”), making use of BCH, and represent Z as a fu ...
									Notes on Functional Analysis in QM
									
... of properties of a single function, whereas the former deals with spaces of functions[The modern concept of a function as a map f : [a, b]toR was only arrived at by Dirichlet as late as 1837, following earlier work by notably Euler and Cauchy. But Newton already had an intuitive grasp of this concep ...
                        	... of properties of a single function, whereas the former deals with spaces of functions[The modern concept of a function as a map f : [a, b]toR was only arrived at by Dirichlet as late as 1837, following earlier work by notably Euler and Cauchy. But Newton already had an intuitive grasp of this concep ...
									a simple explanation of search technique in quantum framework
									
... objective of a classical algorithm is to reduce the amplitude of non target states, where as a quantum search algorithm tries to amplify the amplitude of the target states. Here the term amplification indicates to increase the probability of the target state. The main idea of quantum search techniqu ...
                        	... objective of a classical algorithm is to reduce the amplitude of non target states, where as a quantum search algorithm tries to amplify the amplitude of the target states. Here the term amplification indicates to increase the probability of the target state. The main idea of quantum search techniqu ...
									lecture6.1
									
... 3*5=6, …, so 3 does not have a multiplicative inverse (mod 9) On the other hand, 4*2=8, 4*3=3, 4*4=7, 4*5=2, 4*6=6, 4*7=1, so 4-1=7 (mod 9) ...
                        	... 3*5=6, …, so 3 does not have a multiplicative inverse (mod 9) On the other hand, 4*2=8, 4*3=3, 4*4=7, 4*5=2, 4*6=6, 4*7=1, so 4-1=7 (mod 9) ...
									A fully self-consistent treatment of collective
									
... The study of the dynamical properties of quantum liquids has a storied history.1 The interplay of nuclear dynamics, particle statistics, dimensionality, disorder and temperature can lead to, or suppress, dramatic effects such as superfluidity in 4He and superconductivity in the superfluid Fermi liqu ...
                        	... The study of the dynamical properties of quantum liquids has a storied history.1 The interplay of nuclear dynamics, particle statistics, dimensionality, disorder and temperature can lead to, or suppress, dramatic effects such as superfluidity in 4He and superconductivity in the superfluid Fermi liqu ...
									Quantum Phase Transition and Emergent Symmetry in a Quadruple Quantum... Dong E. Liu, Shailesh Chandrasekharan, and Harold U. Baranger
									
... conductance is small because the phase shift is nearly zero in the LSS state [10]. For U0 large (U0 > 0:15), the conductance is also small and approaches zero as U0 ! 1, consistent with the argument in Ref. [8]. At intermediate values of U0 , there is a strikingly sharp conductance peak near the val ...
                        	... conductance is small because the phase shift is nearly zero in the LSS state [10]. For U0 large (U0 > 0:15), the conductance is also small and approaches zero as U0 ! 1, consistent with the argument in Ref. [8]. At intermediate values of U0 , there is a strikingly sharp conductance peak near the val ...
									The quantum query complexity of AC 0 - Washington
									
... The first quantum query lower bounds in [13, 6] showed that Grover’s algorithm for the OR is asymp√ totically optimal. In [7], Ambainis used the adversary method to prove an Ω( n) lower bound on the query complexity of an AND of ORs. Motivated in part by questions of the security of classical crypto ...
                        	... The first quantum query lower bounds in [13, 6] showed that Grover’s algorithm for the OR is asymp√ totically optimal. In [7], Ambainis used the adversary method to prove an Ω( n) lower bound on the query complexity of an AND of ORs. Motivated in part by questions of the security of classical crypto ...
									One-loop partition function of three
									
... loops and the ghost loops which arise from gauge fixing. In theories with topological degrees of freedom, such as Chern-Simons theory, this is typically the case. Given the similarities between three-dimensional gravity and Chern-Simons theory we therefore expect that the S piq may be non-trivial. T ...
                        	... loops and the ghost loops which arise from gauge fixing. In theories with topological degrees of freedom, such as Chern-Simons theory, this is typically the case. Given the similarities between three-dimensional gravity and Chern-Simons theory we therefore expect that the S piq may be non-trivial. T ...
									Complementarity in Quantum Mechanics and Classical Statistical
									
... Roughly speaking, complementarity can be understood as the coexistence of multiple properties in the behavior of an object that seem to be contradictory. Although it is possible to switch among different descriptions of these properties, in principle, it is impossible to view them, at the same time, ...
                        	... Roughly speaking, complementarity can be understood as the coexistence of multiple properties in the behavior of an object that seem to be contradictory. Although it is possible to switch among different descriptions of these properties, in principle, it is impossible to view them, at the same time, ...
									Quantum information processing with superconducting qubits in a
									
... this structure, the superconducting island with Cooperpair charge Q = 2ne is coupled to a segment of a superconducting ring via two Josephson junctions (each with capacitance CJ and Josephson coupling energy EJ0 ). Also, a voltage VX is coupled to the superconducting island through a gate capacitor ...
                        	... this structure, the superconducting island with Cooperpair charge Q = 2ne is coupled to a segment of a superconducting ring via two Josephson junctions (each with capacitance CJ and Josephson coupling energy EJ0 ). Also, a voltage VX is coupled to the superconducting island through a gate capacitor ...
									On the foundations of the theory of evolution
									
... view of physics, as developed recently in quantum mechanics. The notion of variation is examined. What is naturally selected for in the neo-Darwinian view are essentially forms of concrete and actual matter. We present a more general view in which forms of potentiality coexist with forms of actualit ...
                        	... view of physics, as developed recently in quantum mechanics. The notion of variation is examined. What is naturally selected for in the neo-Darwinian view are essentially forms of concrete and actual matter. We present a more general view in which forms of potentiality coexist with forms of actualit ...
 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									