Compendium of Theoretical Physics
... In the first chapter, Mechanics, we present the often overemphasized Newtonian approach to mechanics next to the Lagrange and Hamilton formulations. Each of these equivalent representations distinguishes itself by specific advantages: whereas Newton’s approach is most easily accessible using the conce ...
... In the first chapter, Mechanics, we present the often overemphasized Newtonian approach to mechanics next to the Lagrange and Hamilton formulations. Each of these equivalent representations distinguishes itself by specific advantages: whereas Newton’s approach is most easily accessible using the conce ...
Free Will as Involving Indeterminacy and Inconceivable Without It
... Far more difficult is a reconciliation of free will with indeterminism, given the force and widespread influence of van Inwagen’s Mind argument and the general “antipathy to chance” noted by William James. 9 It is this reconciliation that we will attempt in this article. The Case Against Indetermina ...
... Far more difficult is a reconciliation of free will with indeterminism, given the force and widespread influence of van Inwagen’s Mind argument and the general “antipathy to chance” noted by William James. 9 It is this reconciliation that we will attempt in this article. The Case Against Indetermina ...
De finetti theorems, mean-field limits and bose
... The purpose of these notes is to present as exhaustively and pedagogically as possible some recent mathematical results bearing on the Bose-Einstein condensation phenomenon observed in ultra-cold atomic gases. One of the numerous theoretical problems posed by these experiments is the understanding o ...
... The purpose of these notes is to present as exhaustively and pedagogically as possible some recent mathematical results bearing on the Bose-Einstein condensation phenomenon observed in ultra-cold atomic gases. One of the numerous theoretical problems posed by these experiments is the understanding o ...
Fluctuations of kinematic quantities in p+p interactions at the CERN
... Uncorrected ΦpT results for p+p collisions at beam momenta: 20, 31, 40, 80, 158 GeV/c were presented. Soon corrected results will be shown. Two-particle correlations in azimuthal angle and pseudo-rapidity: Two-particle correlations in ∆η and ∆φ were obtained for p+p interactions at 158 GeV/c both fo ...
... Uncorrected ΦpT results for p+p collisions at beam momenta: 20, 31, 40, 80, 158 GeV/c were presented. Soon corrected results will be shown. Two-particle correlations in azimuthal angle and pseudo-rapidity: Two-particle correlations in ∆η and ∆φ were obtained for p+p interactions at 158 GeV/c both fo ...
acta physica slovaca vol. 50 No. 1, 1 – 198 February 2000
... Received 10 November 1999, in final form 10 January 2000, accepted 13 January 2000 The work can be considered as an essay on mathematical and conceptual structure of nonrelativistic quantum mechanics (QM) which is related here to some other (more general, but also to more special and “approximative” ...
... Received 10 November 1999, in final form 10 January 2000, accepted 13 January 2000 The work can be considered as an essay on mathematical and conceptual structure of nonrelativistic quantum mechanics (QM) which is related here to some other (more general, but also to more special and “approximative” ...
Observation of Distinct Two-Photon Transition Channels in CdTe
... Semiconductor quantum dots (QDs) are nanomaterials represented by a three-dimensionally confined electron-hole system. Such tight spatial confinement provides interesting optical features, such as size-tunable absorption and emission, which are closely associated with new technologies spanning from ...
... Semiconductor quantum dots (QDs) are nanomaterials represented by a three-dimensionally confined electron-hole system. Such tight spatial confinement provides interesting optical features, such as size-tunable absorption and emission, which are closely associated with new technologies spanning from ...
in PPT
... this puts our Bell test exp’s into the “time-bin” regime (Gisin’s group) Experiments currently underway (4 stabilizations req’d) ...
... this puts our Bell test exp’s into the “time-bin” regime (Gisin’s group) Experiments currently underway (4 stabilizations req’d) ...
Robust dynamical decoupling
... distinguished from the environment. Its energy level splitting differs significantly from that of the bath. As a result, the coupling between them is much smaller than the difference of their energy level splittings. The interaction can then always be approximated by an Ising-type (zz) interaction, w ...
... distinguished from the environment. Its energy level splitting differs significantly from that of the bath. As a result, the coupling between them is much smaller than the difference of their energy level splittings. The interaction can then always be approximated by an Ising-type (zz) interaction, w ...
Fermionization of Spin Systems
... We will apply two kinds of fermionization to this model and we will see that both render the same excitation spectrum. We will also see that, depending on the kind of information needed, the one is more useful than the other, because of the differences in the approaches. Next we will go on to obtain ...
... We will apply two kinds of fermionization to this model and we will see that both render the same excitation spectrum. We will also see that, depending on the kind of information needed, the one is more useful than the other, because of the differences in the approaches. Next we will go on to obtain ...
Chapter 14.
... compares two 4-bit numbers ( S s3 s2 s1s0 and B b3b2b1b0 ). We first compare the Most Significant Bit (MSB), if s3 and b3 has different value ( s3 b3 1 ) and b3 1 , then we know B S . If s3 and b3 are the same ( s3 b3 0 ), then we need to move to the next significant bit. This can be ...
... compares two 4-bit numbers ( S s3 s2 s1s0 and B b3b2b1b0 ). We first compare the Most Significant Bit (MSB), if s3 and b3 has different value ( s3 b3 1 ) and b3 1 , then we know B S . If s3 and b3 are the same ( s3 b3 0 ), then we need to move to the next significant bit. This can be ...
Chapter 3 - THE FIRST LAW
... The Law of Oneness also tells us that via this field of intelligence, which is invisible to our ordinary eyes and pervades the whole of creation, we, like everything that exists within the Whole, are connected with everything else. Moreover, via this energy field, everything that exists is also con ...
... The Law of Oneness also tells us that via this field of intelligence, which is invisible to our ordinary eyes and pervades the whole of creation, we, like everything that exists within the Whole, are connected with everything else. Moreover, via this energy field, everything that exists is also con ...
Twenty years of the Weyl anomaly
... As chance would have it, my third postdoc brought me to King's College, London. at the same time as Steve Christensen, Paul Davies, Stanley Deser, Chris Isham and Steve Fulling. Bill Unruh was also a visitor. It was destined therefore to become a hot-bed of controversy and activity in Weyl anomalies ...
... As chance would have it, my third postdoc brought me to King's College, London. at the same time as Steve Christensen, Paul Davies, Stanley Deser, Chris Isham and Steve Fulling. Bill Unruh was also a visitor. It was destined therefore to become a hot-bed of controversy and activity in Weyl anomalies ...
Quiet Readout of Superconducting Flux States
... decoherence due to environmental noise, but back action from the required measuring device and intrinsic noise in the qubit itself results in decoherence that must be quantified and reduced. A dc Superconducting QUantum Interference Device (SQUID), which involves two Josephson junctions connected i ...
... decoherence due to environmental noise, but back action from the required measuring device and intrinsic noise in the qubit itself results in decoherence that must be quantified and reduced. A dc Superconducting QUantum Interference Device (SQUID), which involves two Josephson junctions connected i ...